£EPA
            United States
            Environmental Protection
            Agency
            Risk Reduction
            Engineering Laboratory
            Cincinnati OH 45268
EPA/600/2-90/025
June 1990
            Research and Development
Relationship of
Laboratory- and Field-
Determined Hydraulic
Conductivity in
Compacted Clay Layer

-------
                                                        EPA/600/2-90/025
                                                        June  1990
  RELATIONSHIP  OF  LABORATORY-  AND FIELD-DETERMINED HYDRAULIC
             CONDUCTIVITY  IN COMPACTED  CLAY  LAYER
                              by

                        A.  S.  Rogowski
             U.S. Department of Agriculture, ARS
             Northeast Watershed Research Center
             University Park, Pennsylvania 16802
             Interagency Agreement No. DW-12930303
                       Project Officer

                     Walter E.  Grube,  Jr.
Waste Minimization,  Destruction and  Disposal  Research  Division
            Risk Reduction Engineering Laboratory
                   Cincinnati, Ohio  45268
            RISK REDUCTION ENGINEERING LABORATORY
              OFFICE  OF  RESEARCH  AND  DEVELOPMENT
             U.S.  ENVIRONMENTAL  PROTECTION  AGENCY
                   CINCINNATI, OHIO  45268

-------
                                  DISCLAIMER
    The information in the document has been Bunded wholly or in part by the
United States Environmental  Protection Agency under assistance agreement
number DW-12930303 to the United States Department of Agriculture, ARS.  It
has been subject to the Agency's peer and administrative review and has been
approved for publication as  a  U.S.  EPA document.   Mention of trade names or
commercial  products does not constitute endorsement or recommendation for use.
                                       11

-------
                                   FOREWORD


    Today's rapidly developing and changing technologies and industrial
products and practices frequently carry with them the increased generation of
materials that, if improperly dealt with, can threaten both public health and
the environment.  The United States Environmental Protection Agency is charged
by Congress with protecting the Nation's land, air, and water resources.
Under a mandate of national environmental laws, the Agency strives to
formulate and implement actions leading to a compatible balance between  human
activities and the ability of natural  systems to support and nurture life.
These laws direct the U.S. EPA to perform research to define our environmental
problems, measure the impacts, and search for solutions.

    The Risk Reduction Engineering Laboratory is responsible for planning,
implementing, and managing research, development, and demonstration programs
to provide an authoritative, defensible engineering basis in support of  the
policies, programs, and regulations of the U.S. EPA with respect to drinking
water, wastewater, pesticides, toxic substances, solid and hazardous wastes,
and Superfund-related activities.  This publication is one of the products of
that research and provides a vital communication link between the researcher
and the user community.

    This report documents the spatial  variability of hydraulic conductivity,
measured by both infiltration and seepage, throughout an area of clayey  soil
compacted according to engineering specifications for landfill liners.   The
data emphasize the need for clear design specifications and high quality
construction of such earthen barriers  in waste management facilities.  This
report will be useful  to scientists, engineers, and regulatory staffs  who are
concerned with the actual hydraulic performance of soil  liners and soil  covers
constructed to protect the Nation's ground water.
                               E.  Timothy  Oppelt
                                   Director
                     Risk  Reduction  Engineering Laboratory
                                     iii

-------
                                     ABSTRACT                       • • >. •

     A study was begun in 1983 to characterize the areal variation in hydrau-
lic conductivity of a compacted clay liner.  A field-scale research facility
was constructed, consisting of a 30' x 75' area of clay soil compacted in
three layers to specifications commonly used in constructing clay liners.  The
facility was fully instrumented to measure infiltration, drainage, and soil
properties at numerous data collection points.  Preliminary studies were
initiated using sections of small barrels and larger caissons to verify the
performance of monitoring systems.  Results from these preliminary (prototype)
studies have shown that any perforations of the compacted soil, such as wells,
or access tubing for detectors to monitor wetting front advance, may result in
preferential water movement by gravity down the walls of these perforations.
To avoid this situation in the field-scale facility, access tubes were placed
horizontally to accommodate the nuclear probes used to measure changes in clay
density and porosity.  Underdrains were imbedded in the concrete support
structure to collect outflow, infiltration cylinders were installed to monitor
infiltration, and metal pedestals were placed on the clay surface to assess
swelling by measuring elevation changes.  Quality control observations
collected during the construction showed that on the average water content and
dry density of the compacted clay were close to design specifications, but the
spatial variability in these values was large.  Measured infiltration rates
and outflow rates obtained following ponding the field-scale facility were
poorly predicted by the prototype data from small barrels and larger caissons.
Initial data showed rapid breakthrough of percolate near the confining walls,
a feature that was also observed earlier in prototype studies.  The extent of
clay liner integrity and observed travel times reflect the effectiveness of a
field-scale clay liner in preventing possible ground water contamination.
Proper evaluation of flux rates and their distribution in time and space is
necessary to characterize the system.

     Flux values, computed from observed infiltration and outflow measurements
at 18M locations in a layer of compacted clay subsoil, were compared to effec-
tive flux values based on breakthrough time distributions for water and Br~
tracer over the same area.  Results suggested that both water and tracer move
at similar rates, but considerably faster than expected, on the basis of the
outflow flux alone, and that only a small fraction of the total pore space is
involved in active transport.  The ramifications of these findings are
explored against the background of effective porosity, degree of compaction,
and observed changes in bulk density with time.

     The experimental clay liner was ponded for 1 year.  During that time
inflow, outflow, and changes in density were routinely monitored at 250
locations.  Results suggested that initial increase and final leveling off of
the density values could be associated with water passing into the clay matrix
and attainment of the steady state.  Observed increases in density initially
were accompanied by increases in outflow which subsequently declined and
leveled off at twelve months.  These changes were associated with leaching and
precipitation of Fe and Mn.  Tracer breakthrough times were consistently
faster than water flow rates, although initial water breakthrough times
following ponding were similar to tracer breakthrough times.  Results suggest
that water and solutes moved in the clay through only a small portion of total
porosity.


                                      iv

-------
    Hydraulic conductivity distribution based on laboratory measurements
underestimated field measured hydraulic conductivity distribution  by a~factor
of five.  However, comparisons of individual  values at the same location could
differ by several  orders of magnitude.   Tt was found that the distribution  of
water content and density in the compacted clay was adequately described by
core samples and nuclear surface moisture-density probe data.  However,  the
water content and density data appeared to have little relationship to average
values of spatially distributed hydraulic conductivity.

    This report was submitted in fulfillment  of Interagency Agreement
No. DW-12930303 between the United States Environmental Protection Agency and
the United States Department of Agriculture,  Agricultural Research Service, k
This report covers a period from September 1983 to August 1988 and work  was
completed as of August 1988.

-------
                                   CONTENTS

                                                                           Page

Foreword	     ill
Abstract .	       iv
Figures	     viii
Plates	     xiv
Tables	     xv i
Acknowledgment 	 ........  	       xx

     1.  Introduction	       1
              Objectives and Approach	       2
              Literature Review (Phase I)	       3

     2.  Conclusions	       11

     3.  Recommendations	       13

     4.  Preliminary Studies	       14
              Design Criteria	       14
                   Clay Liner Materials		       20
                   Barrel Studies	       25
                   Caisson Prototypes	       32

     5.  Field Scale Studies 	       ty
              Testing Facility 	       49
                   Soil Materials	       54
              Liner Construction	       55
                   Experimental Procedures  	       56
                   Summary of Installation	  .       63
                   Site, Scale, and Spatial Relationships	       66
                   Surface Moisture and Density	       68
              Experimental Results 	  .       72
                   Preponded Stage 	       '72
                        Density	       72
                        Total Available Pore Space	       73
                   Ponded Stage	       77
                        Sampling Plan	       77
                        Average Values .....  	       78
                        Gradient	       82
                        Density	       82
                        Inflow and Outflow	       92
                             Initial infiltration	       95
                             Flow at a point	       95
                        Tracer Studies 	      104
                             Water and tracer breakthrough  ......      107
                             Effective porosity	      110
                             Macropore flow	      112
                             Tracer distributions	      115
                        Swelling	      116
                        Percolate Quality	      120
                                      VI

-------
                                                                          Page

     6.  Concluding Studies	     131
              Postponded Stage 	     131
              Laboratory Hydraulic Conductivity	     131
                   Flexible Membrane Method	     131
                   Comparative Analysis	     134
                   Distribution of Bulk Density and Water Content. . .     136
                        Veihmeier Tube Samples 	     137
                        Core Data	     137
     7.  Data Quality	     148
              Data Acquisition	     148
                   Analytical Procedures 	     152
                        Density	     152
                        CSE	     152
                        Leachate Drains	     153
                        Infiltration Rings 	     153
                        Liner	     153
                        Evaporation	     153
                   Data Reduction, Validation and Reporting  	     154
                   Internal QC Checks	     156
                   Final Density Check	     157
                   Inflow/Outflow Balance	     161
                   Statistical Stability Tests 	     161
                   Number of Samples 	 .....     165

Appendices

     A.  Literature.  ..... 	     169
     B.  Individual Readings 	    Disc
     C.  Statistics	    Disc
     D.  Tracers	    Disc
     E.  Laboratory	    Disc

Publications - Clay Liner	     203
                                      Vll

-------
                                   FIGURES

Number                                                                    Page

 1.1    Schematic representation of a variogram Y(h) ..........     7

 4.1    A platform for testing hydraulic properties of a 30 cm thick
          clay liner ..........................    14
 4.2    Standard proctor test on sieved material ............    22

 4.3    Standard proctor test on nonsieved material ...........    23

 4.4    Moisture characteristic of the clay liner material .......    24

 4.5    Permeability and infiltration measurements:  schematic diagram
          of the barrel, infiltration ring, inner and outer constant
          head devices .........................    29

 4.6    Infiltration rate x 10"? (m/s) in the inner ring of barrel
          #\ plotted as a function of time (days) ............    29

 4.7    Cumulative infiltration in the inner ring of barrel #1
          plotted as a function of time (days) .............    30

 4.8    Cumulative outflow from the inner bottom compartment
          of the barrel #1 plotted as a function of time (days) .....    30

 4.9    Cumulative inflow in the inner ring (0.05 m^) of barrel #1 as a
          function of the total pore volume below the infiltration ring
          plotted as a function of time (days) .............    31

 4.10   Cumulative outflow as a function of the total pore volume abpve
          the bottom inner compartment plotted as a function of time .  .    31

 4.11   Schematic diagram of the caisson study .............    32

 4.12   Swelling of clay liner given as percent of liner thickness and
          plotted as a function of time .................    37

 4.13   Comparison between cumulative infiltration in barrel #1 and
          caisson rings ......... . ............. .  .    37

 4.14   Typical water content with depth (access tube #1), caisson
          was flooded 41 days after being compacted. ... .......    38

 4.15   Improved version of clay liner prototype ............    41

 4.16   Comparison of observed swelling on prototype caisson 1 and 2
          studies ............................    45
                                     viii

-------
Number                         (Figures continues)

 5.1    Clay liner testing facility, similar to Figure 4.1 but in SI
          units showing additional detail on horizontal access tubes . .    49

 5.2    Experimental measuring grid for (a) bulk density,
          (b) infiltration and drainage, (c) swelling and
          evaporation	    50

 5.3    Standard proctor compaction test on till material used in
          the liner	    55

 5.4    Values of water content and dry density measured with the nuclear
          surface probe for the sheepsfoot roller, and with Eley
          volumeter, gravimetric samples for jackhammer and small
          vibratory roller; solid lines represent laboratory measured
          standard proctor compaction and saturation curves, dashed
          vertical lines give optimum water content (17.8$) and dashed
          horizontal lines represent 90$ of the maximum density
          (1754 kg/m3)	    64

 5.5    Distribution of water content (by wt) and dry densities (DD)
          on three compacted lifts measured with Troxler surface probe
          in the backscatter mode, shown against the background of
          proctor density at water content (opt), lines of maximums and
          line of saturation (.zero voids)	    65

 5.6    Geometry and scale considerations of Troxler dual gamma probe,
          Eley volumeter, and Troxler surface moisture-density probe
          in backscatter mode	    67

 5.7    Distribution of water content in lifts #1, #2 and #3 of the
          experimental clay liner based on small gravimetric grab
          samples, optimum (OPT) moisture content is 17.6$ by weight . .    68

 5.8    Distribution of water content in lifts #1, #2 and #3 of the
          experimental clay liner based on nuclear surface moisture
          gauge, optimum (OPT) moisture content was 17.8$ by weight. . .    69

 5.9    Distribution of dry bulk density in lifts #1, #2 and #3 of
          compacted clay liner in terms of standard proctor (PROCT)
          density (1754 kg/m3, 110 PCF)	    71

 5*10   Average density distribution over the clay liner 	    73

 5.11   An illustration of why the center portion of the clay liner
          may have received more passes than the sides	    74

 •5.12   Contours of average density (in kg/m3) adjusted to surface
          probe density values (a), and of surface probe moisture
          content (in kg/m3) (b), before ponding 	    75
                                      ix

-------
Number                         (Figures continued)

 5.13   Interpolated isopleths of the amount of water needed to
         saturate the liner (in kg/m3) at ponding ...........     76

 5.11*   Schematic representation of constant head Mariotte bottle
          assemblage ..........................    78

 5.15   Average wet density measured with dual gamma probe before and
          after ponding .........................    79

 5.16   Average ring infiltration rate during a one year study period.  .    80

 5.17   Average outflow rate during a one year study period .......    81

 5.18   Average infiltration and outflow rates for a ponded liner as
          a whole during the one year study period ...........    82

 5.19   Schematic representation of gradient parameters for compacted
          clay liner at Klingerstown, Pa ................    83

 5.20   Interpolated distribution of hydraulic gradient over the
          study area ..........................    83

 5.21   Interpolated contours of density two days (top), one week
          (middle), and one month (bottom) after ponding ........    86

 5.22   Distribution of standard counts for the dual density probe
          with time ...........................    87

 5.23   Net change  in density for consecutive readings at the site
          M#H, I#M, G#U and J#U, plotted as functions of time,
          dashed lines indicate possible extent of the error of
          measurement (±8.7 kg/m3) ........ .... .......    90
 5.2U   Cumulative change in density at the sites M#4, I#U, G#4 and
          J#4 plotted as functions of time, each value ( •) has an
          associated uncertainty of ± 8.7 kg/ra3 .............     91

 5.25   Spatial distribution of dual probe density values  (kg/m3)
          before ponding (a), and 2 days (b), 10 days (c), 1 month
          (d), 3 months (e), 6 months (f), 9 months  (g), and 1 yr
          (h) after ponding ................. .  .....     92

 5.26   Distribution of infiltration rings which showed  major, minor
          or slight leaks when fluorescein was added to  each ring.  ...     93

 5.27   Illustration of Philip's (1957) method for calculation of
          sorptivity S, and A-values . .  ................      96
                                        x

-------
Number                         (Figures continued)                        Page

 5.28   Ring inflow rate (R), drain outflow rate (D) and associated
         bulk density distribution to the east (Dg) and west (Dy)
          of the ring-drain, for the sites A3 (a), N8 (b) ........    98

 5.29   Ring inflow rate (R), drain outflow /ate (D) and associated
          bulk density distribution to the east (Dg) and west (Dy)
          of the ring-drain, for the sites H5 (a), FT (b) ........    99

 5.30   Comparison of hydraulic conductivity distributions computed
          from (ring) inflow and (drain) outflow at 3 months and 6
          months ............................   102

 5.31   Comparison of hydraulic conductivity distributions computed
          from ring inflow and drain outflow at 9 months and 1  year
          (13 months) ..... . ....................   103

 5.32   Comparison of hydraulic conductivity distributions computed
          from ring inflow and drain outflow averaged over time
          (6/27/85 to 4/30/86) . . . . .................
 5.33   Location of 15 infiltration rings and respective sampling
          areas (shaded) to which 1M Br~ solution had been added ....   105

 5.34   Logarithm (base 10) of relative (C/Co) breakthrough
          concentrations (logRC) of Br" pulses in hours (sumtime)
          at a particular drain (ID-B:AA6) and arrival times
          after applying Br" tracer to central ring (ID-A:AA7) .....   107

 5.35   Relative concentration of Br" in leachate from AA7 and
          surrounding drains (a), and from A3 and surrounding
          drains (b) ..........................   108

 5.36   Frequency histograms of breakthrough times (B-T time) for
          water (a) and Br" tracer (b) .................   109

 5.37   Distribution of breakthrough (first arrival) time (days) for
          water (a) and Br" tracer (b) in compacted, spatially
          variable clay liner .................... ..   110

 5.38   Distribution of effective porosity (Pe) in a compacted and
          ponded, spatially variable clay liner given as the percent
          of cross sectional -area (A), based on first arrival times
          of ponded water ........................   113

 5.39   Distribution in time of ring inflow (R), drain outflow (D),
          and bulk density in the east (Dg) and west (D^) of the
          primary ring and drain locations for the slow-flowing site
          F1 (a) and fast-flowing site G5 (b) ..............   114
                                      xi

-------
Number                         (Figures continued)                        Page

 5.40   Relative concentration of Br~ as leachate from site F1 and
         surrounding drains (a) and site G5 and surrounding
          drains (b)	   115

 5.41   Relative distribution of Br" tracer in soil around the sites
          F1 (a) and G5 (b) to which tracer has been applied	   117

 5.42   Relative distribution of Br" tracer in soil around the sites
          D7, L3, M7, and 01 to which the tracer has been applied. . .  .   118

 5.43   Relative distribution of Br~ tracer in soil around the sites
          Q5, S1, V8 and T5 to which the tracer has been applied ....   119

 5.41   Relative distribution of Br~ tracer in soil around the sites
          JO and 09 to which the tracer has been applied	   120

 5.45   Elevation changes in millimeters (mm) for the compacted clay
          liner 9 months after ponding; positive symbols indicate
          swelling, negative symbols are indicative of shrinkage.
          AAAA -2.50 to -2.00 mm; BBBB -2.00 to -1.50 mm; CCCC -1.50
          to -1.00 mm; DDDD -1.00 to -0.50 mm; EEEE -0.50 to 0.00 mm;
          FFFF 0.00 to 0.50 mm; GGGG 0.50 to 1.00 mm; HHHH 1.00 to
          1.50 mm; IIII 1.50 to 2.00 mm; JJJJ 2.00 to 2.50 mm; KKKK
          2.50 to 3.00 nun; LLLL 3.00 to 3.50 mm	   121

 5.46   Number of pore volumes leached through the clay liner at nine
          months, starred points indicate locations where leachate
          has been sampled monthly ..... 	   121

 5.47   Spatial distribution of electrical conductivity (EC)  in
          vimhos/cm (a), pH (b), and SOij mg/J, (c) in leachate  from
          drains (250) at 9 months	   125

 5.48   Spatial distribution of electrical conductivity (EC)  in
          ymhos/cm (a), pH (b), and SOij mg/!l (c) in leachate  from
          drains (250) at 12 months	   126

 5.49   Spatial distribution of K (a) and Na in mg/H (b) in leachate
          from drains at 9 months	   127

 5.50   Spatial distribution of K (a) and Na in mg/8, (b) in leachate
          from drains at 12 months	   128

 5.51   Spatial distribution of Ca (a) and Mg in rag/i (b) in  leachate
          from drains (250) at 9 months	   129

 5.52   Spatial distribution of Ca .(a) and Mg in mg/A (b) in  leachate
          from drains (250) at 12 months	   130
                                      xii

-------
Number                         (Figures continued)

 6.1    Chronological distribution of activities after the clay liner
          was drained ..................... .....   132

 6.2    Point to point comparison of laboratory hydraulic conductivity
          (K) with field derived values based on last (upper plots)
          and average (lower plots) observed ring and drain flux ....   135

 6.3    Rank to rank comparison of laboratory hydraulic conductivity
          (K) with field observed values based on last (upper plots)
          and average (lower plots) observed ring and drain flux ....   136

 6.4    Comparison between dual probe readings on 8/1/86 just after
          the clay liner was drained and on 8/18/86 just prior to
          when 3" core samples were taken ................   138

 6.5    Spatial distribution of the 3" core/dual probe density ratio
          on 8/18/86 in the compacted clay liner ............   140
 6.6    Contours of density (a) before ponding, (b) two days after
          ponding and (c) just prior to being drained
 6.7    Spatial distribution of the amount of water needed (in kg/m3)
          to saturate the clay liner before ponding, 2 days after
          ponding and just before being drained .............   142

 6.8    Changes in the degree of saturation at 3" (8cm) and water
          content by volume at 6" (25cm) in the drained clay liner
          with time ...........................   145

 6.9    An east to west transect of wet (a) and dry (b) density in 1"
          (2.5cm), depth increments as measured with the dual gamma
          probe on 3" (91cm) centers ..................   145

 6.10   An east to west transect of water contents by weight in 1"
          (2.5cm) depth increments measured gravimetrically .......   146

 7.1    Gravimetric balance performance data ..............   151

 7.2    Data processing flow chart ...................   154

 7t3    Distribution of dual density probe standard counts during the
          study period .........................   165

 7.4    Standard error of estimate as a function of the number of
          observations for ring infiltrometers .............   166

 7.5    Relative values of the standard error as a function of the
          number of observations for density, water content and
          hydraulic conductivity measurements ..............   168
                                    xiii

-------
                                    PLATES

Number                                                                    Page

 4.1    Elevated platform construction:  reinforced concrete footers . .    15

 4.2    Elevated platform construction:  finished platform 	    16

 4.3    Installation of the lower access tube prior to pouring of
          concrete floor on the platform	    16

 4.4    The 10m long access tubes were supported by brackets to keep
          them level	    17

 4.5    Location of lower access tubes after concrete floor has been
          poured; spacers show where upper tubes will go after the
          installation of the clay liner	    17

 4.6    Measurement of density in horizontal access tubes with dual
          gamma gauge	    18

 4.7    Distribution of infiltration rings on compacted clay liner, a
          few pedestals to monitor swelling can be seen in the
          background	    18

 4.8    Distribution of outflow ports equipped with moisture blocks
          (hanging wires) to indicate early arrival of breakthrough
          water	    19

 4.9    To test double ring infiltrometer geometry clay liner material
          was compacted in barrels (half drums)	    26

 4.10   Clay liner material was compacted using a scaled up version of
          Proctor compaction mold and drop hammer	    27

 4.11   An experimental set up to measure infiltration rate on
          compacted clay liner material	    28

 4.12   A bank of vertical access tubes for measurement of moisture
          and density with depth, and a ring for measuring
          infiltration rate in flooded caisson 	    33

 4.13   Additional details of optocator positioning and of the
          optocator pedestal for measurement of clay swelling,
          infiltratioin rings and access tubes shown in a
          flooded caisson	    34

 4.14   Constant head devices (cylinders) for infiltration rings and
          for the caisson itself (carboy) were placed on the outside
          of the caisson	    35

 4.15   Prototype liner being installed in caisson #2 study using
          mechanized compaction, neutron surface moisture/density
          gauge was used to monitor compaction	    42

                                       xiv

-------
Number                         (Plates continued)

 4.16   The prototype liner concrete box,  just showing, burlap covered
          bottom,  gypsum blocks located over drains and removable wooden
          wedges on the sides;  the bottom  horizontal access tube is
          barely visible in the center; raised metal ridge separates
          outer wall flow from  flow in the inner compartment;  constant
          head devices to be used with infiltration rings are  shown
          along the walls	    43

 5.1     Infiltration rings, a pedestal and a wooden walkway supported
          by access tubes were  installed in compacted clay liner ....    51

 5.2     The floor of the platform was sealed, and the bead of  the
          bentonite was placed  3'  away from the sidewalls,
          subsequently the floor was covered with burlap and a
          thin layer of sand	    52

 5.3     Bentonite panels are being placed  against sealed platform
          sidewalls, to minimize wall effects	    53

 5.4     Test plot is being compacted using a sheepsfoot roller 	    56

 5.5     Clay material was brought  in by trucks and spread on the
          platform with a large backhoe	    57

 5,6     After the required amount  of water was added,  it was
          incorporated into the clay by rototilling	    58

 5.7     Following  several passes with the  bulldozer and sheepsfoot
          roller,  each lift was smoothed out by large  vibratory
          roller prior to measurement of density 	    59

 5.8     Near the walls clay was compacted  using a "nervous turtle"
          roller (shown above)  and jackhammer (not shown)	    60

 5.9     Water content and density  were measured using  a nuclear
          moisture-density probe ...  	    61

 5.10   Prior to installation of the next  lift the clay surface was
          roughened by bulldozer treads	    62
                                     xv

-------
                                    TABLES

Number

 4.1    Average properties of the B-horizon of Hubblersburg
          cherty silt loam (Typic Hapludult, illitic or mixed
          mesic) developed on limestone, from PSU GP-10 file	      21

 4.2    Average surface and depth moisture and density readings. ...      35

 4.3    Results of gravimetric moisture sampling of the compacted
          clay liner in caisson 1	      40

 4.4    Electrical resistivity of gypsum blocks buried by respective
          drains (1 to 6) under the compacted clay ponded (time 0)
          on 10/9/84	      46

 4.5    Wet and dry bulk density (WD and DD) of compacted clay
          before ponding, measured with nuclear probes and
          gravimetrically	      47

 4.6    Water content measured gravimetrically and with nuclear
          probes on compacted clay prior to ponding	      47

 4.7    Wet bulk density (WD) of compacted clay as measured with
          horizontal access tubes and computed values of total
          available pore space (taps) before (0) and following
          (1, 3, 14 days) ponding	      48

 4.8    Outflow rates measured in inner (#5 and #6) and outer (#1, #2,
          #3 and #4) compartment drains	      48

 5.1    Selected properties of the till used as liner material as
          determined by supplier, our (NWRC), and EPA (HWERL) soil
          testing laboratories	•      54

 5.2    Clod size analysis of two large samples.	      55

 5.3    Cross sectional areas and volumes associated with monitoring
          of water flow, water content, and bulk density in the
          compacted clay liner 	 ......      66

 5.4    Distribution of water content (gravimetric) in clay liner
          computed from nuclear gauge data and point grab samples.  .  .      70

 5.5    Dry bulk density of the three lifts of compacted clay liner
          as a function of standard proctor compaction test	      71

 5.6    Statistics of 13 bulk density (wet) data sets taken
          continuously and consecutively following Installation
          on 11/1/84 and prior to ponding on 3/26/85	      72
                                       xvl

-------
 Number                          (Tables continued)                          Page

  5.7     Particle density of ground  fraction of  clay  liner  material .  .       72

  5.8     Average values of dry bulk  density and  water content
           by  weight	,	       84

  5.9     Selected statistics for the density distributions  before
           and after the clay liner  was ponded	      85

  5.10    Individual values of bulk density obtained using dual  gamma
        ,   probe on 9/25/85 (6 months after ponding)  	      88

  5.11    Summary of statistics for 9/25/85 bulk  density data (6 months
           after ponding) 	  .....     89

  5.12    Average infiltration rates  for selected times uncorrected
           (all) and corrected for ring area (area correction)  and
           leaking rings (leak rings omit)	     94

  5.13    Sorptivity, A-values, and saturated hydraulic conductivity
           based on initial (1000 sees) infiltration  rates  for
          .selected double rings (613 m2 area infiltrometers using
           Philip's (1957) method)	     97

  5.14    Selected statistics for the hydraulic conductivity
           distributions in time computed from nontransformed
:           (a)  and log-transformed (b) ring infiltration data
           for the ponded clay liner		    100

 •5.15    Selected statistics for the hydraulic conductivity
           distributions in time computed from nontransformed
           (a)  and log-transformed (b) drain outflow  data for
           the ponded clay liner	    101

  5.16   Amounts of 1M Br"1  diluted to 2000mil and applied to rings
           in  1, 2 or 3 (used) increments of 2000mX,;  applied
           concentration (Co)  in ppm and grams (g)	    106

  5.17   Laboratory values of hydraulic conductivity  compared with
           average field values of ring inflow and drain outflow	    111

  5.18   Breakthrough times (T^)  for Br" tracer  and water,  and
           cumulative tracer concentration (C/CO), recovered and
           computed effective  flux density (Qe)  values for  selected
           sites based on tracer breakthrough times and average 30
           cm  thickness of clay	    112

  5.19   Water quality changes as a result of passing  through
           experimental liner  	    122
                                     xvii

-------
Number                         (Tables  continued)

 5.20   Means and standard deviations,  'arid coefficient of variation
          (CV)  of leachate quality  parameters sampled at 9 and 12
          months after- ponding	   123

 5.21   Correlation matrix of leachate ^quality parameters a"t 9 and 12
          months following poridtng	   124

 6.1     Summary statistics for  laboratory and field evaluated hydraulic
          conductivity (x  10~9  m/sec)	   133

 6.2    Field values of hydraulic conductivity near the sites where
          defective cores  were  taken .	   134

 6.3    Statistics of the  3"  core data  compared with final dual
          probe (8/18) values	   139

 6.4    Statistics of the  wet density values obtained using 3" cores
          and Troxler surface moisture  density probe during construction
          (initial) and after the liner was drained (final)	   139

 6.5    Comparative statistics  for  wet  density values (kg/m2) obtained
          using 3" cores,  2"  cores, 6"  holes, excavations and K-cores.  .   139

 6.6    Statistics of the  ratio:   (3" core density/dual probe
          density)	   140

 6.7    Comparative statistics  for  the  amount of water needed to
          saturate the clay liner	   143

 6.8    Average swelling of clay	   143

 6.9    Statistics for the 2" cores, average and by layer	   144

 6.10   Comparative statistics  for  pesthole data 	   147

 7.1     Methods used and classical  data quality indicators for
          infiltration, evaporation and leachate rates, bulk
          density, and change of  surface elevation (CSE) 	   150

 7.2    Percent error as a function of  volume of leachate	   150

 7.3    Density data selected for QC/QA validation 	   158

 7.4    Example of density data record	   159

 7.5    Grouping summary	   160

 7.6    Summary density flagged validation values	   160

 7.7    Mass balance of inflow  and  outflow of clay liner water	   162
                                     xviii

-------
Number                         (Tables continued)                         Page

 7.8    Statistical stability and drift test - surface moisture gauge. .   163

 7.9    Personnel check, inflow measurements 	   16M

 7.10   Comparison of the relative values of standard error for density,
          moisture, and hydraulic conductivity measurements. . 	   167
                                      xix

-------
                               ACKNOWLEDGMENTS

     Special thanks and recognition go to the USDA-ARS personnel involved in
different aspects of this project, E. L. Jacoby, Jr., D. E. Simmons, W. M.
Yazujian, J. E. Donley, B. J. Chamberlin, C. W. Artz, P. J. Dockey and
students D. E. Gedon and R. M. Petery, T. Knerr and F. K. Reeser.  Mr.
Yazujian's, Mr. Jacoby's, and Mr. Simmons' contributons to the success of this
project were particularly outstanding.  The author acknowledges the support of
this study by the Land Pollution Control Division, Hazardous Waste Engineering
Research Laboratory, U. S. Environmental Protection Agency, Cincinnati, Ohio,
through Interagency Agreement No. DW129-303-03-01-0 with the Northeast
Watershed Research Center, Agricultural Research Service, U. S. Department of
Agriculture, University Park, Pennsylvania; D. Walter E. Grube, Jr. is the U.
S. EPA Project Officer.  This report has not been subjected to the EPA review
and therefore the contents do not necessarily reflect the views of the Agency
and no official endorsement should be inferred.
                                      XX

-------
                                  SECTION 1

                                 INTRODUCTION
     Installation of liners at sanitary landfills and hazardous waste sites
has been one of the commonly recommended methods of containment and control.
The primary function of a liner is to prevent, or limit the amount of leachate
that might ultimately reach the groundwater.  Thus, liners must have appropri-
ate properties to restrict, delay or dilute leachate migration so that a given
site may ideally provide an ultimate containment.  Desirable properties of
linear materials include (1) low permeability, (2) high adsorption capacity,
and (3) resistance to chemical, biological and mechanical breakdown.  These
desirable attributes work to enhance several physical and chemical processes
which will lessen the environmental consequences of contaminant migration.
The primary mitigating factors include dilution, time delay, and retardation.
The choice of liner material should be based on the extent to which these
factors operate to meet the desired performance criteria.

     Various treated and untreated soil mixtures have been utilized as liners
for waste sites:  compacted mixed clay soils, pure montmorillonite, montmoril-
lonite mixed with concrete, bentonite with an added polymer, as well as other
commercially available products.  Of these, the clay liners are the most
common.  Typically, clay liners are constructed in one of the following ways:

       (1) A commercial refined clay product is added to and mixed with
           the top few centimeters of native soil.

       (2) A nearby deposit of clay soil is excavated, hauled to, and
           compacted in place at the disposal site.

       (3) A native clay soil is compacted in place.

     Generally, a liner is covered with a layer of sand or soil to minimize
drying, and waste is placed on top of the soil varying in depth from 2 to 8
meters.  For municipal waste the density varies between 297-53^ kg/m3, for
many hazardous waste materials it is likely to be higher.  Taking 1000 kg/m3
as a likely number and adding to it the weight of cover cap, overburden
pressures on the liner might be on the order of 5 to 10 T/m^.  Since good
construction begins with adequate specifications, proper design is the single
most important factor in a successful liner installation.  Design procedures
need to take into account the Federal and State regulations and performance
standards.  While State requirements must meet the minimum Federal standards,
many go beyond to accommodate local conditions.  For example, the Pennsylvania
Department of Environmental Resources (DER) requires the following specifica-
tions be met if a native clay is to be used as a primary layer.

-------
                    Permeability:   < 10"? cm/sec
                    Thickness   :   60 cm
                    Compaction  :   95% standard proctor
                    Clay content:   greater or equal to 25%

In addition to the liners being compatible with the waste, the site must be
inspected and approved by the Department.  Quality testing is mandatory during
and upon completion of the installation.

     The least water content (by weight) at which the soil just flows under
its own weight is called the liquid limit (LL), while the smallest water
content (also by weight) at which the soil can still be rolled out into thin
(- 3mm) threads without crumbling is called the plastic limit (PL), the
difference between the tow (LL-PL) is taken as the plasticity index (PI) and
is given in units of water content by weight.  In general, liners should be
constructed of inorganic clays with a liquid limit greater or equal to 30 and
plasticity index greater or equal to 15, and with their respective cation
exchange characteristics carefully considered.  The liners should be compacted
wet of optimum water content using a sheepsfoot roller, and their clod size
should also be controlled.  Frequently  inadequate installation results in clay
liner failure.  Thus, a strict quality control of materials, equipment and
workmanship appears essential to ensure compliance with the engineering
specifications.

     Assuming a constant head of ponded water above a compacted clay liner the
flow rate through the liner should be proportioned to its hydraulic
conductivity.  As far back as 1856 Darcy established experimentally that the
volume of water (Q) flowing through a unit cross sectional area of a sandy
formation in a unit of time, was proportional to the difference in hydraulic
head (Ah) between the top and bottom of the formation.  Since the head at the
bottom of the formation of thickness L  is - zero, Ah is numerically equal to
the height of water ponded above the bottom, Ah/L is referred to as the
dimensionless gradient (i), and K the proportionality coefficient with units
of length/time, is the hydraulic conductivity.  Combining the above we get an
expression Q = Ki, known as Darcy's Law.


OBJECTIVES AND APPROACH

     The purpose of this study was to evaluate hydraulic conductivity of a
field scale clay liner and to compare the field observed values of the
hydraulic conductivity with the laboratory determined values of the hydraulic
conductivity.  Supplemental data were also to be gathered to support research
into factors potentially affecting leaching of the contaminants into the
groundwater.

     The specific objectives of this study were:

     (1) To document the present state-of-the-art for determining the in situ
         hydraulic conductivity of compacted clay soils.

     (2) To construct a field-scale test plot composed of recompacted clay
         soil, to install appropriate monitoring devices for measuring water

-------
         flow rate in compacted clay, and to determine the in situ hydraulic
         conductivity using selected permeants, verifying that accurate data
         can be obtained.

     (3) To compare the hydraulic conductivity values obtained on a field
         test site with those obtained in the laboratory on core samples,
         and if significant lack of agreement exists, to evaluate the
         factors responsible.

     The project was to proceed in three discrete phases.  The initial phase
(Phase I) was to include a literature review and methods evaluation to recom-
mend the most appropriate field scale procedure for measuring the hydraulic
conductivity in a compacted clay soil liner.  Particular emphasis was to be
placed on available methods addressing cohesive soils, undisturbed sites, and
large surface areas, as well as those that could provide data within a reason-
able time frame, remembering that hydraulic conductivity of the clay liner was
likely to be - 1 x 10~9 m/sec.  The output from Phase I was to be a literature
review report, with recommended approaches to construction of the field-scale
hydraulic conductivity measuring facilities.  In Phase II the field apparatus
for measuring flow and the prototype clay liner were to be designed and tested
for accuracy and performance.  In Phase III field-scale facility was to be
constructed and clay liner compacted and ponded according to standard industry
methods and procedures.  After the completion of the field phase, core samples
were to be removed from the site for laboratory determinations of hydraulic
conductivity.  This phase was to include long-term data collection, analysis
of field obtained results, and comparison with the laboratory values of deter-
mined hydraulic conductivity.


LITERATURE REVIEW (PHASE I)

     It is generally assumed that the denser the clay liner the lower its
permeability.  When constructing clay liners for containment of water the soil
material at a certain water content is compacted to a prespecified density.
The amount of compaction will vary with the water content.  For high values of
water content a test involving a standard number of blows will eliminate the
few air filled pores present.  Resulting density will be low and near to the
saturation density value.  If, however, the soil is quite dry, no amount of
compaction will substantially reduce the air filled porosity because there is
not enough water to provide lubrication and allow soil particles to pack
closer together.  Thus, the final dry density will also be low.  At some water
content in between these extremes there is a point, known as optimum water
content, when a compaction test such as Standard Proctor test will result in a
maximum dry density for a given amount of effort (i.e., number of blows,
height of fall, mass of weight) (Cooper and Cassie, 1978).

     The use of Standard Proctor test as a compaction measure assumes the same
aggregate size distribution for lab and field materials.  This need not be
necessarily so and large differences in water content between the lab and
field can occur (Cox, 1978).  Further modifications will take place as clay
adjusts to overburden stresses imposed on it by a combined load of waste and
cover cap.  Thus,  the equilibrium water content in the field may be different
from Standard Proctor test "optimum," and may also vary sufficiently over the

-------
area to cause differences in observed flow.   Although Cox (1978) investigated
the behavior of clays under extreme wet or dry conditions, his work shed
little light on clays compacted at or above the optimum water content.  The
optimum water content occurs at water contents less than saturation, with only
part of the void space occupied by water and the rest by air.  It is not known
whether under the conditions of optimum moisture and maximum density infiltrat-
ing water moves through the still empty, connected air voids or by displace-
ment through water-filled pores.

     According to Jumikis (1965) volume of solids, volume of water, and volume
of air, stabilize at the optimum water content and maximum dry density and
stay constant with total void space at the minimum.  Just above the optimum a
10$ increase in the relative volume of water may be accompanied by as much as
5Q% decrease in the air voids with little change in total « ^%) volume of
voids.  Considering results presented by Gary et al., (19^3) and accompanying
discussion by Kellog and Creager (Gary et al., 19^3) large decrease in perme-
ability can occur over the same range (just above optimum), suggesting that
primary pathways of water movement may be through relatively large air filled
and connected pores, while water in smaller pores of the clay matrix is more
or less immobilized.  This question has not been specifically addressed in
literature except indirectly by Gary et al., (19^3), Anderson and Low (1958),
Lambe (1955) and Mitchell et al., (1965).  It needs to be clarified whether
the pores through which water moves following compaction are the ones which
are predominantly air filled, or the ones which are predominantly water filled.
Gary et al., (19^3) state that optimum compaction means realignment of clay
platelets, while Lambe (1955) and Cary et al., (19^3) suggest that there is
little or no subsequent swelling as water is applied to the surface of remold-
ed clay.  Thus, the primary water conducting pores could well be the larger
pores which may initially be filled with air.  In either case, the flow would
be taking place only through a fraction of the total void space and in effect
constitute an unsaturated flow regime.  Some support for this view comes from
the work of Anderson and Low (1958) who suggest that the structure of adsorbed
water may also be different (i.e., less dense) from that of the free water.
The concept of field capacity (Burrows and Kirkham, 1958) in agricultural
soils, or nature of flow through coarse mine spoil (Rogowski and Weinrich,
1981) carries a similar connotation:  only certain pores conduct water.
Recent attempts to measure large pores in field soils (Clothier and White,
1981) may be a likely approach to clay liner permeability evaluation.

     Generally, a quantitative knowledge of clay liner properties is required
for prediction of hydrologic behavior at the hazardous waste sites.  The
choice of an approach may be dictated by the magnitude of spatial variability
and the distribution of hydrological properties.  Which properties should be
measured, what sample volumes should be taken, what locations and what sam-
pling frequency should be considered, are some of the aspects which need to be
resolved in characterizing a given clay liner.  Of prime importance in this
context are the objectives and the desired accuracy for which hydrologic
predictions are needed; this will influence the level of sophistication and
detail at which a site is sampled and the data analyzed.

     One source of  information to evaluate the suitability of a soil as clay
liner material is soil classification data.  Soil classification is based on
the premise that soil properties vary in space.  Soil surveys are then used to

-------
 identify  and delineate the  soil  boundaries  and  predict  extent and properties
 of individual horizons.  But  in  most  classification  schemes these boundaries
 remain  imprecisely defined.   The soil  survey  classification is based on the
 broad morphological  features  of  the landscape correlated to sampled profile
 properties  such as color, horizon, depth, structure,  and texture.
 Unfortunately, the extent and nature  of  variability  within a soil unit and
 associated  mapping purity are not always recorded.   As  a first approximation,
 properties  of soil series may be used  to select clay liner material.  However,
 it must be  realized  that the  criteria  used  in the classifying soils may not
 coincide  with those  affecting hydrologic response.   Furthermore,  appreciable
 spatial variability  in soil hydrological properties  has been observed within a
 soil series (e.g., Rogowski,  1972; Nielsen  et al., 1973;  Sharma et al.,  1980),
 and this  may affect  the areal response of remolded material.   Thus,  under  most
 conditions  field  characterization of an  in  place liner  is considered important
 and for this, field-oriented  methods are needed.  These methods should be
 simple, rapid, and reliable so that a  large number of measurements can be  made.
 For the ease of handling and  analyzing of data,  grid or transect  sampling
 schemes are preferred.

     The  choice of hydrological  properties  needed to  be determined and the
 extent  of detail  of  their characterization, depend largely on objectives and
 the choice  of model  to be used.  For detailed prediction  of water  distribution
 within  a  clay liner, a physically-based  deterministic model such  as a
 three-dimensional water flow  equation  for swelling soils  could be  used.  This
 however,  would require detailed  knowledge of  the spatial  distribution of the
 soil water  retention ij;(0) as  a function  of  water ratio  
-------
determination of approximate  K(ijj)  and  6(ip)  values for evaluation of spatial
variability and estimation of redistribution of applied water in a field soil.
Because K values in the  compacted  clay liner are expected to be very low (-
10~9 m/sec), it is doubtful to what  extent  this approach could be used.

     Considerable effort has  been  made in developing empirical methods to esti-
mate hydrological properties  based on  particle size analysis data.  Broad
scale hydrological classification  of agricultural soils of the USA is being
attempted by estimating  parameters appropriate to the Brooks and Corey model
of water retention (e.g.,  Rawls et al., 1982) as well as parameters suitable
for use in the Green and Ampt (1911) infiltration equation (Swartzendruber,
1987).  In the absence of soil hydrologic data, these approaches are likely to
have a wide appeal since they are  usually based on readily available
information.  The limitations of such  approaches to clay liner construction
should however be realized, particularly for soils with predominant structural
features.

     In general, soil systems, such  as a remolded clay liner, are extremely
complicated and highly variable at a scale  of individual aggregate, but such
complexity can be bypassed by measuring hydrological properties at a larger
scale.  Usually the variance  of a property  decreases with an increase in
volume of a sample.  The smallest  volume above which the variance no longer
decreases significantly  defines the  representative volume for that property
(Bear, 1972).  This is a theoretical concept, and in real world situations, it
may be difficult to define.  Ideally,  the representative volume should encom-
pass components of variability at several scales, in practice, however, hydro-
logic properties are measured on much  smaller samples and they are considered
points of a continuum.

     For comparative purposes and assuming  normality the magnitude of variabil-
ity is sometimes represented by the  coefficient of variation (CV).  In soils
coefficient of variation is found to be highest  (CV > 1.0) for transport
coefficients (hydraulic conductivity and diffusivity), medium (CV = 0.15-0.5)
for properties such as water contents  at selected water potential, and least
(CV < 0.15) for properties such as bulk density and total porosity (Warrick
and Nielsen, 1980).  The variability of a property can also be described by a
cumulative distribution function  (CDF), which  (if we assume a Gaussian model)
contains information about the mean and other moments, and these permit estima-
tion of  confidence intervals for  the property.  Assuming a CDF for a parameter
has important implications in computing the number of observations required to
estimate the mean with a specified precision  (Rogowski, 1972; Sharma, 1983),
and in determining the integrated hydrologic response of an area  (Sharma and
Luxmoore, 1979; Warrick and Amoozegar-Fard, 1979).

     In  traditional parametric analysis of variability a Gaussian or normal
model  is usually adopted.  Properties measured within an area are assumed
spatially independent of one another and observations are represented by their
mean,  standard deviation and other moments.  The  assumption of  spatial
independence, at least for points close by,  seldom holds for natural systems.
Geostatistical techniques  (e.g.,  Journel and Huijbregts, 1978)  and nonpara-
metric methods can then be employed to evaluate  the  degree of interdependence.
The spatial dependence of  neighboring  observations of  a property  Z measured  at

-------
  all points x and x+h as functions of the distance vector h can be expressed by
  the seraivariogram Y(h),
                                   N
Y(h)  = ^
                                            - Z(Xi+h)]2
(1.1)
  where N  is the number of pairs [Z(xi), Z(x^+h)] for a particular distance  (or
  time) increment h.  Thus, a semivariogram of a property describes the average
  rate of  change of Y(h) with distance and shows the variance  structure of
  observations.  These observations may or may not follow any  type of CDF, but
  should be additive  (Journel and Huijbregts,  1978).  An an idealized semivario-
  gram is  shown in Figure 1 .  The sill is an upper limit of a  variogram model
  where it levels off, while the distance at which the variogram model begins to
  level off is known  as the range in most applications.  The sill usually
  approaches a priori sample variance, while the range defines a neighborhood
  where the variable  is continuous.  With increasing separation distance h,  Y
  may increase and approach a constant value (sill) beyond some separation
  distance a (range). This indicates the extent of spatial dependence.  If  Y
  continues to increase with increasing h, information at larger separation
  distances may be required.  Often Y does not pass through the origin and at
 Spatial
Variance

 Y  (h)
 Random
 Variance
                         Variance = Sill
                             Nugget Effect
                                                              I
                                                             a.
                 Distance (h)   Between   Samples
           Figure  1.1.  Schematic representation of a variogram Y(h).

                                      7

-------
h=0 has some positive finite value called a nugget effect.  Such a nugget
effect usually suggests a spatial structure on a scale smaller than the sam-
pling interval h.  Once the spatial structure of the variable is defined by a
semivariogram, the values can be kriged to interpolate the distribution of a
property over an area or in space.

     Extensive reviews and discussion of laboratory and field techniques of
measuring permeability and related parameters are readily available in mono-
graphs (Black, 1965; Hagan et al.f 1967; USGS, 1977; Nielsen et al., 1972),
books (Bear et al., 1968;  Childs, 1968; Baver et al., 1972; Kirkham and
Powers, 1972; Hillel, 1971  and 1980),  journals (Bianchi and Haskell, 1970;
Ritchie et al., 1972; Alemi et al.,  1976;  Clothier and White, 1981).  Most
writings are concerned with permeability measurements in agricultural soils,
and the requirement that a flow rate be less than 10~9 m/sec, as specified for
clay liners, is of little practical  interest.  We have therefore, to turn to
engineering literature (Olson and Daniel,  1979),  particularly literature on
clay cores in earth dams and embankments as well as to novel approaches in
soil mechanics (Mitchell et al.,  1965; Lee, 1974; Zimmie and Riggs, 1981), and
to experimental and theoretical studies of shrinking and swelling systems
(Kemper, 1960, 196la,b; Sposito,  I975a,b,c) to get some idea what may be
involved.  These studies add new insights in a practical sense, to what has
been written before by Gary et al.,  (1943), Lambe (1955),  and Babcock (1963).

     Swelling clay soils do not behave in the same manner  as do nonswelling
materials.  Swelling soils, in addition to matric and gravitational potential
flows, will be subject to overburden potential and probably varying degree of
chemical potential depending on waste compatibility.  This, of course,  compli-
cates the situation considerably.  The effect of gravity on flow will be less
and vertical moisture profiles are likely to vary depending on clay thickness,
amount of swelling, and location with respect to the water table.  In shallow
profiles volume of water per unit volume of soil may increase, decrease, or
remain constant with depth, while, for deep profiles volume of water per unit
volume of soil will decrease.  These developments may markedly affect profile
permeability.  It is well known (Philip, 1969a,b) that surface macrotopography
does have a considerable influence on the equilibrium water content, but it is
not known to what extent microtopography of an essentially level clay liner
will affect its hydrology.  Much work has been done recently to predict the
behavior of swelling soils in response to water using the  fluid mechanics
approach (Philip, 1969a,b; Youngs and Towner, 1970; Philip, 1970; Talsma,
1974, 1977a,b; Talsma and Flint,  1958; Talsma and Lelij, 1976) or thermodynam-
ics approach (Babcock, 1963; Sposito,  1972, 1973, 1975a,b,c; Sposito et al.,
1976; Chu and Sposito, 1980.  Work done by Kemper and coworkers (i.e.,  Kemper
and Evans, 1963; Kemper and Rollins, 1966, etc.) addresses movement of water
across clay membranes as a function of concentration gradients.  When salt
solution is forced through a compacted clay a portion of electrolyte is
excluded from water films surrounding clay particles and remains behind at the
high pressure side increasing the concentration of salts and possibly affect-
ing permeability.  To what extent work on swelling systems is applicable to
our studies remains to be seen.
                                                       /
     When discussing aspects of structural stability Quirk (1978) pointed out
that in a soil containing illitic clay, the dominant pore peak occurred at

-------
3.5 nm (10~9 m).  However, volume changes during wetting usually lead to forma-
tion of planes of discontinuity and development of pores two to three orders
of magnitude larger than the original peak.  Recent work of Smalley (1978)
suggests that compaction at moistures slightly greater than optimum leads to
structural rearrangement of clay particles.  Particle realignment on wetting
and compaction in Leda/Champlain clays of eastern Canada was shown by Smalley
(1978) to result in considerable local variations in density.  Although ini-
tial open structure of these clays tended to be preserved by cementation of
short range bonds, bond breakage could subsequently result in complete struc-
tural collapse.

     Changes in hydraulic conductivity can be brought about by chemical and
physical reactions within the clay matrix.  Frenkel and Rhoades (1978) pointed
out that hydraulic conductivity can increase appreciably because of
dispersion, provided bulk density of the material and electrolyte level of
percolate are sufficiently low, flow rates are sufficiently high, and exchange-
able sodium is between 10 and 20%.  Under these conditions dispersion begins
to affect mechanics of transport and may lead to piping failures.  On the
other hand, if sufficient clay is present and exchangeable sodium is greater
than 25%, swelling will most likely reduce hydraulic conductivity.  At low
electrolyte levels in the percolate, if the bulk density and clay content are
sufficiently high, dispersion will lead to blocking of pores and reduction in
hydraulic conductivity.

     Thus, a system, such as a clay liner, may react in different ways and
require not only the specifications depending on location, clay type,  amount,
and water content, but also the knowledge of the particular waste chemistry.

     A basic experimental tool in field infiltration research is the ring
infiltrometer.  There are many different types and sizes that have been used
and modifications range from a double ring infiltrometer on one end of the
scale to an enclosed air entry permeameter and double tube permeameter at the
other.  Infiltration rate I within the rings is assumed to take place under
unit gradient conditions and calculations may involve fitting the S
(sorptivity) and A (coefficients) in Philip (1967) infiltration equation,

                                 I = St1/2 + At                         (1 .2)

where t is the time.  Straight line plot of I/t1/2 with respect to t^/2 gives
S as a y-axis intercept and coefficient A as a slope of the line.  A working
estimate of hydraulic conductivity (Ks) can then be obtained as,

                                     Ks = 3A                            (1.3)

     This relatively rapid method has been used by Talsma and Lelij (1976)  to
evaluate in situ infiltration rate and water movement on a swelling rice paddy
soil during prolonged ponding.  Measured values of hydraulic conductivity
ranged from 5.8 x 10"? to 1.12 x 10~5 cm/sec,  certainly within the range of
interest for clay liner studies.   Based on their average sorptivity of - 25
mm/day1/2 and average Ks value of - 2 mm/day (2.3 x 10~5 cm/sec) the plot of

-------
I/t1/2 vs t1 /2 was expected to be linear for about 3 days according to the
relation,

                                 t £ 0.02 (S/K)2                        (1.4)


It might therefore be anticipated that a linear behavior of I/t1/2 vs t1/2 for
a clay liner with K - 10~7 cm/sec is likely to be even longer.  If a ring is
large enough (> 30 cm diameter), or enclosed in a manner similar to an air
entry parameter, or a falling head infiltrometer (Daniel and Trautwein, 1986)
measurable infiltration rates can be readily calculated from the fall of water
level in a capillary, or by weight.

     Following ponding, and after the water drains a disc infiltrometer
(Clothier and While, 1981) can be used to check for the presence of large
pores.  Disc infiltrometer will allow water movement into the profile under a
known negative head and is used together with ponded values to see what propor-
tion of the larger pores are likely to be conducting water.  In agricultural
soils as much as 80 or 90% of flow can take place through the larger pores.
The "larger" pores in clay matrix are likely to be much smaller necessitating
the use of different membrane materials with higher impedance to induce higher
values of negative head.
                                      10

-------
                                  SECTION 2

                                 CONCLUSIONS
     The initial literature Review ('Phase I) has¥aised several questions.
The foremost among these was the evidence "that -flow''through compacted clay may
be very sensitive to the remolding water content and accompanying uncertainty
about the representativeness-and: effectiveness of standard co'mpaction
techniques.  Equally important was the potential'Existence and distribution of
preferential flow pathways.
                              •,- '"   •'*•:.'•*' <  ,;,'',' . •'  ;     '•!-, ;  '"   " •  '
     Preliminary studies (Phase I!) proved useful' in 'desi'gn of the''field
experiment and instrumentation. ' Resultsj suggested 'poterit'ial for leakage along
the walls of containment and sides of instruments.^ Some Swelling was also
observed; however, swelling infiltration and drainage rates from1;prototype
studies were"poor predictors of fleld'scale facility behavior. "!

     The large 10 x 25m, bridgelike• "platform'facility an'd a cbttipacted 0.3m
thick clay line (Phase 3) provided satisfactory data about the performance of
clay liners and relationship of field hydraulic conductivity to lab values.

     Clay liner was constructed from a B-horizon of a typical soil meeting the
EPA specifications.  In the course of analysis the soil was found to contain a
larger than expected number of coarse fragments.  However, no evidence was
found of preferential layering, or preferential distribution of these rock
fragments either because of natural tendencies or mechanized compaction of the
three lifts.  Sand layer on top of the clay liner acted as a moisture barrier
and prevented rapid drying.  Spatial measurements of evaporation needed to be
made to correct infiltration flux and for mass balance purposes.

     The considerable variability observed in the spatially distributed
infiltration, outflow and outflow chemistry on the compacted clay liner may
have been affected by the presence of preferential pathways of leachate flow
through the clay liner.

     Higher flow rates which originated in apparently unsaturated areas
suggested the presence of the preferential flow pathways.  Such pathways will
potentially pose a grave threat to underlying ground water quality even in the
presence of a clay liner.

     There was no correlation between laboratory and field derived values of
hydraulic conductivity on the point to point basis when values from the same
locations were compared.  However, when the distribution of laboratory values
was compared with the distribution of field values the results appeared to be
linearly correlated.  Laboratory distribution underestimated the field distri-
bution by approximately a factor of 5, despite the fact that individual obser-
vations varied as much as four orders of magnitude.
                                      11

-------
     Laboratory hydraulic conductivity values were not a good indicator of the
clay liner behavior.  Ring infiltrometers, despite problems, appeared to pro-
vide better estimates of potential outflow from below the compacted clay.
Unfortunately, using of the ring infiltrometers is time consuming.  Best esti-
mates of clay liner performance were obtained by following the conservative
tracer (Br~) movement, and breakthrough history.

     We have found little change in clay liner wet density with time suggest-
ing a very limited movement of water into the clay matrix.  Initial change,
however, just after flooding could be indicative of the extent of
macroporosity.

     Finally, we have found a surface moisture-density probe with capability
for direct transmission from shallow depths to be a quick and satisfactory
method of determining field distribution of moisture and density for individ-
ual lifts during construction.  Unfortunately, there appeared to be no
relationship between density and water content of the clay and the observed
values of hydraulic conductivity and the flow regime, as perceived by changes
in wet density, did not appear to be continuous but consisted of concurrent
alternating, filling and draining episodes distributed in space.

     The amount of available pore space in well compacted clay was very small,
and even a small change may be disproportionately large.  In our case minimal
swelling of - 2.4-mm could have accounted for - 20% increase in available pore
space in compacted clay.

     Far fewer (1/10 as many) samples were needed to characterize the compact-
ed clay liner density and water content compared with the number of samples
needed to characterize hydraulic conductivity with the same degree of
precision.   Considering that hydraulic conductivity per se did not appear to
be the primary controlling factor in the flow and breakthrough of water and
tracers in the compacted clay liner more effort is needed to characterize
potential distribution of the preferential flow pathways.
                                      12

-------
                                  SECTION 3

                               RECOMMENDATIONS


     Field constructed clay liners should have a layer of sand on the top and
the bottom, because sand acts as a capillary barrier for clay water, minimiz-
ing drying and outflow components.

     Specifications for liner construction should include an upper permissible
level of clods, aggregates and stones to be contained in the candidate
materials.  Clay liner materials are often derived from deeper horizons of
ordinary field soils.  Such materials,  particularly in the northeastern USA,
contain many coarse fragments.

     It is recommended that the integrity of compacted clay liners be tested
using a conservative tracer, ponded conditions and an underdrain catchment
system.  Because, despite adequate moisture and compaction, the moisture and
density readings did not appear to be correlated on a field scale with
observed hydraulic conductivity or the distribution of critically important
preferential flow paths.  However, the nuclear surface moisture-density probe
with a shallow direct transmission capacity appeared adequate for evaluating
distribution of moisture and density within individual compacted lifts of clay.

     In designing clay liner studies particular attention needs to be given to
potential flow along the walls of the containment facility or instrumentation
access ports.

     Judicious selection of liner materials (specific guidelines) and exten-
sive quality control of moisture and density (specific guidelines) during con-
struction are recommended.  At present many samples of hydraulic conductivity
are needed to adequately characterize the potential flux and transport through
the clay.  Because far fewer samples of water content and density are required
to characterize the clay liner compared with the number of samples required to
characterize hydraulic conductivity with the same degree of precision,
increased quality control and use of homogeneous materials at a reasonably
constant water content may help decrease the number of samples needed to
characterize hydraulic conductivity.
                                      13

-------
                                  SECTION 4

                        PRELIMINARY STUDIES  (PHASE II)
DESIGN CRITERIA
     Design criteria and plans for  the liner testing facility and associated
instrumentation included a 10  x 25m elevated platform and a 30cm thick liner.
Figure 4.1  and Plates 4.1  and  4.2 show the schematic plan and different
construction stages of the platform.

     Plate 4.1  shows the reinforced concrete footers,  and in Plate 4.2 we show
the finished (b)  elevated platform.   The open ramps on either side were subse-
quently filled with compacted  soil  and gravel to provide a drive on access to
the platform for  liner construction and removal.  Plates 4.3 and 4.4 give
details of drain  locations and reinforcing grid.  They also show the method of
installation (4.3)  and support (4.4)  for lower access tubes.  In Plate 4.5
lower access tubes  protrude above the just poured concrete floor with spacers
for the upper access tubes in  the sidewall in the background. Plate 4.6
illustrates how density was to be measured after the clay was compacted and
upper access tubes  installed.   The  gamma source was to be placed in the lower
   Figure 4.1.  A platform for testing hydraulic properties of a 30cm thick
                clay liner.
                                      14

-------
access tube and the detector, connected to the scalar (foreground), was to be
placed in the upper access tube.  Density changes were to be computed from
routine measurements at the same locations.  Additional instrumentation was to
include infiltration rings (Plate 4.7) and drain ports (Plate 4.8) equipped
with moisture blocks to detect early arrival of breakthrough front (note wires
hanging from drains), square 10 x 10cm pedestals (several can be seen in Plate
4.7) to monitor swelling, and evaporation pans (same size as infiltration
rings) to correct infiltration and outflow for evaporation.  The instrumenta-
tion at the site was to be installed so as not to interfere with the struc-
tural integrity of the compacted liner.  The clay material was to be trucked
in from an actual commercial facility.  Installation and compaction were to be
carried out according to the USEPA standards (i.e., USEPA, 1988) and also were
to be quality tested during installation.  A special effort was to be made to
take many more moisture samples and make many more measurements of bulk densi-
ty than may strictly be necessary, so as to establish the minimum sampling and
testing criteria needed for adequate quality control.
  Plate 4.1.  Elevated platform construction:  reinforced concrete footers.
                                      15

-------
Plate 4.2.  Elevated platform construction:  finished platform.
                              16

-------
Plate ^.3.   Installation of the lower access tube prior to pouring
            of concrete floor on the platform.
                             16a

-------












Plate 4.4.   The 10m long access tubes were supported by brackets to
            keep them level.
                                 17

-------
Plate M.5.   Location of lower access tubes after concrete floor has
            been poured;  spacers show where upper tubes will go after
            the installation of the clay liner.
                                17 a

-------
Plate 4.6.   Measurement of density in horizontal access tubes
            with dual gamma gauge.
                              18

-------
Plate H.Tt   Distribution of  infiltration rings on compacted  clay  liner, a  few
            pedestals to monitor  swelling can be seen  in the background.
                               18 a

-------
       Plate 4.8.  Distribution of outflow ports equipped with moisture
                   blocks (hanging wires) to indicate early arrival of
                   breakthrough water.                              ' .
     It was anticipated that 30cm diameter infiltration rings (Plate 4.7) and
 complementary network of outflow drains (Plates 4.3 and 4.8) will provide
 sufficiently rapid response to measure infiltration, compute hydraulic
 conductivity and estimate the distribution of macroporosity for a clay liner.
 Because inflow rates were anticipated to be slow, control of evaporation and
 maintaining of relatively constant temperature was thought to be important.
 Many more measurements were to be taken than are necessary, so that enough
 samples were available to estimate the minimum number of samples required to
 characterize variability.  The design called for closing off both ramp ends of
 the liner testing platform and flooding the whole area.  The final output of
 the study was to be a grid of inflow and outflow measurements, calculated
 conductivities and changes in bulk density and porosity over the area with
 depth, and with time.  If areas of high permeability occurred a 1 x 1 m2 grid
 of drains was to intercept the leachate.

     Shrinkage and swelling of the liner system were to be monitored using
 square 10 x 10cm pedestals and a laser beam technique.  Evaporation was to be
 measured with a class A pan and a number of smaller pans the same size as
 infiltration rings.

     Following the ponding stage the clay liner was to be core sampled and
 hydraulic conductivities of cores, evaluated in the laboratory, were to be
 compared with those obtained from field ring and drain measurements and with
overall flow rates through the liner.
                                      19

-------
Clay Liner Materials
     The clay liner material consisted of commercially available B-horizon
subsoil (10" to 60", 25 to 250cm) of Hubblei
the 3 to 8% slopes north of Roaring Springs
Pennsylvania.  Typically, the subsoil exten<
                                            •sburg cherty silt loam found on
                                            and Highway 36 and 164 in central
                                            is to a depth of 60"  (150cm) or
more.  It is yellowish red, friable cherty isilty clay loam, silty clay, and
cherty silty clay to a depth of 35" (90cm).  At a depth of more than 35"
(90cm) it is yellowish red, friable silty clay loam.
     Normally included in this soil (5 to 1
Mertz, Clarksburg, Morrison, and Wharton Va
natural state is considered to be moderate
                                           )$) are small areas of Opequon,
                                            •iant soils.  Permeability in
                                           and available water capacity is
high.  The soil is very strongly acid throughout.  The unified classification
of the subsoil ranges from CL to CH (10" to
less than 5% of fragments > 3" (76mm), with
60-95$ passing #10, 55-95$ passing #40, and
ranges from 35 to 55% and plasticity index
ranges from 20 to 45/5, bulk density from 12DO to 1600 kg/m3 and in place
permeability from 6 to 2 inches per hour (15 to 50mm, 40 to 140 x 10"? m/sec).
Available water is 12 to 16? by volume with
                                            60", 25 to 150cm).  It contains
                                            35 to 100$ passing sieve #4,
                                            55-85$ passing #200.  Liquid limit
                                           from 12 to 30$.  Clay (< 2mm)
                                            pH within 4.5 to 5.5 range.
Shrink swell potential is moderate and erosion potential is quite large.  In
general, organic matter is low (1 to 3$).  Potential for frost action is
moderate and risk of corrosion for steel and concrete is high to moderate,
respectively.  The soil is classified as clayey, illitic, mesic Typic
Hapludult (USDA, 1981), Table 4.1 shows average properties of the B-horizon.
     The site where the soil came from was
own analyses have shown it to be a CL type
                  Liquid Limit:
                  Plastic Limit:
                  Plasticity Index:
                                           mined commercially for clay.
                                           clay with,

                                            water by weight
                                            water by weight
                                            water by weight
Our
which compares reasonably well with values given by supplier.  The material
appears to contain quartz, K-feldspar kaolinite, illite and vermiculite.  It
is 47$ clay, 45$ silt, and 8$ sand as giver
The Standard Proctor test results and 95$ c
                                            by the sedigraph measurements.
                                           ionfidence intervals results are
shown for sieved and unsieved material in Figures 4.2 and 4.3.  The optimum
water content (by weight) was 18$ by weight for both, and the maximum density
is 111.5 pcf (1786 kg/m3) for sieved and 114.5 pcf (1834 kg/m3) for nonsieved
material, respectively.  Comparison with the moisture characteristic curve of
the sieved material (Figure 4.4) shows that the optimum water content (at
least in loose soil) occurred between 2 and 3 bars tension.  What this means
is that when initially water is ponded on the surface of a clay liner a very
high water content gradient will be imposed across the clay-water interface.
                                      20

-------
TABLE 4.1.  AVERAGE PROPERTIES OF THE B-HORIZON OF HUBBLERSBURG CHERTY SILT
        LOAM (TYPIC HAPLUDULT, ILLITIC OR MIXED MESIC) DEVELOPED ON
                       LIMESTONE. FROM PSU GP-10 FILE
Property
Total coarse fragments
Coarse fragments
Less then 2 mm
Bulk density (clod)
Bulk density (< 2 mm)
Cole
Uncor 1 /3 bar core
15 bar, fragment
pH water: soil, field
pH KCL:soil, field
Organic carbon (titratin)
Calcium
Magnesium
Sodium
Potassium
Total bases
Aluminum
CEC:Ex acidity
Base saturation
Fe203
Kaolinite
Illite
Vermiculite
Chloride
Int.
Talc
Unit
% by wt
% by vol
% by wt
kg/m3
kg/m3
cm/ cm
% by wt
% by wt
-
-
% by wt
% by wt
% by wt
% by wt
% by wt
% by wt
% by wt
me/100 g
% by wt
% by wt
% by wt
% by wt
% by wt
% by wt
% by wt
% by wt
Mean Value
14.0
9.5
86.0
1510.9
1488.1
0.017
25.0
17.7
5.1
4.2
0.16
2.1
0.9
0.1
0.2
3.4
4.8
9.9
25.5
5.1
24
52
8
5
5
10
Standard
deviation
10.7
11 .0
10.7
132.0
125.3
0.009
5.4
3.4
0.4
0.4
0.19
1.9
0.7
0.0
0.1
2.2
2.1
2.6
15.7
1.0
18
18
3
-
-
6
                                     21

-------
       I 15.0
        12.5
        10.0
       107.5
     H
     55
     HI
     o
       105.0
       102.5
       100.0
        97.5
        95.0
                                         -i	1
                SIEVED
                 12    14    16    18     20     22


                            MOISTURE (PERCENT)
24    26
Figure U.2.   Standard  Proctor  test on  sieved material.
                             22

-------
CW
c

CD
       BULK DENSITY  PCF
                                     <» r
                                               

-------
        15                 25                35
           WATER CONTENT (WEIGHT PERCENT)
Figure 4.4.  Moisture  characteristic of  the clay liner material.
                            24

-------
Barrel Studies

     Preliminary plans (Rogowski and Richie, 1984) called for installation of
infiltration rings into the compacted clay liner and measurement of infiltra-
tion rate at 250 points over time.  Since clay liner would be ponded, the
procedure was to be essentially an adaptation of a double ring infiltrometer
method and geometry to a large scale study.  To test the procedure clay liner
material was compacted in three 4" (10cm) lifts in large barrels (one-half of
the 40 gallon drum) as shown in Plate 4.9.  The compaction of the three 4"
(10cm) lifts was accomplished using a scaled up version of a Proctor hammer
(Plate 4.10).  Infiltration rings (10", 25cm in diameter and 10" high) were
made of galvanized 14 gauge metal with a rolled lip on top and were installed
to the depth of 3" (8cm) in compacted clay by pounding a solid iron inset
cover with a sledge hammer.  The water was ponded over the surface to the
depth of 2.5" (6cm).   Plate 4.11 shows the experimental set up and Figure 4.5
gives the schematic diagram of the barrel, rings and the inner and outer
constant head devices.  To monitor potential wall flow effects, each barrel
was equipped with a 46cm diameter inner compartment welded to the barrel
bottom (Figure 4.5) which separated the outflow primarily from below the ring
from the outflow percolating through the rest of material and down the walls
of the barrel.  The role of barrel study was two-fold.  A barrel in one sense
was a scaled up version of a Standard Proctor compaction mold.  In another
sense it was a scaled down version of a field facility.

     Figure 4.6 shows the infiltration rate measured in the barrel rings by
weighing the inner constant head device as a function of time.  After the
first 10 days the rate appeared to have settled to a steady 1 x 10~9 m/sec
flow.  For a scaled up version of clay liner we would expect a maximum initial
rate of 100 x 10~9 m/sec would translate to a 75 &/hr (400 gal/day) inflow (on
a 10 x 25m area) at the beginning of experiment which would decrease to about
0.75 l/hr (4 gal/day) inflow after the first 10 days assuming no high perme-
ability zones.  Figures 4.7 and 4.8 show cumulative infiltration and outflow
as a function of time, respectively.  While infiltration stabilized within the
first 10 days, it took about 2 months for outflow to decline.

     Figure 4.7 corroborates, and presents in a different way results of
Figure 4.6.  It appears that during the first week as much as 38mm of water
was likely to infiltrate a clay liner.  Thus, if we were to pond 10cm of water
over the 10 x 25m liner (21,000 I, 5000 gal) we would initially need an addi-
tional 8000 it (1800 gal) to keep the level constant.

     Figure 4.8 illustrates barrel #1 outflow during 100 days of operation.
Results show no outflow during the first 13 days.  Translating this to poten-
tial performance of the full scale facility we expected after the first 10
days an outflow of - 25 mil/drain/day which could drop to as little as 7
m£/drain/day after the first two months.  Figures 4.9 and 4.10 show inflow and
outflow into barrel in terms of pore volumes.  After about three months of
ponding only 0.8 (cm3/cm3) of a pore volume has moved into the compacted clay,
while less than 0.1 (cm3/Cm3) of a pore volume has moved out.
                                       25

-------
Plate 4.9.   To test double ring infiltroraeter  geometry clay liner
            material was compacted  in  barrels  (half  drums).
                                26

-------
Plate 4.10.   Clay liner  material  was compacted using a scaled up version
             of Proctor  compaction mold and drop hammer.
                                   27

-------
Plate 4.11.  An experimental set up to measure infiltration rate
             on compacted clay liner material.
                               28

-------
        Cross Section
                                                       X Rubber
                                                       <  * Stopper
                                                           Glass
                                                           Cylinder
  Ponded
   Water
Compacted
  Clay
Robber
 Stopper
                Rubber
                  Stopper
                    -Glass
                      Bottle
                    -Glass
                      Tube
                                                                  Outer Constant
                                                                    Head  Device
                                                 Collection
                                                 — Drains
                                    Floor
       Figure 4.5.   Permeability  and infiltration measurement:   schematic
                      diagram of  the barrel,  infiltration ring, inner and
                      outer constant head devices.
                                           29

-------
   1000.0
 (ft
o>
b
 UJ
100.0
      10.0
 cc
 5      i.o
       O.I
                                    J.
                                      J.
                       20           40

                               TIME (DAYS)
                                            60
80
   Figure  4.6.  Infiltration rate x 10~9  (m/s) in the inner ring of
               barrel #1 plotted as a function of time (days).
                                29a

-------
I 60
0
+
Monvan
u_
z
UJ
jl 20
-j
C
, , -p j _n_
-^iTj
^rtO CP°
^x«K> °°
/^ffflQVy
.8^
Q
i
•B
— — J 	 L 	 1 	 i | a _^_L_
1 2O 4O 60 «r
                       TIME  (DAYS)
Figure M.7.  Cumulative  infiltration in the inner ring of  the
            Barrel #1 plotted as a function of time (days).
                            30

-------
400
300
i
3 200
u.
1-
o
100
0
0 OO<
0°°° ° "
o
0
o
o
o
•
o
o
~~s~i~0° 1 1 1 1 1 J 	






0 20 40 6O 80
                           TIME  (DAYS)
Figure 4.8.  Cumulative outflow from the inner bottom compartment
            of the Barrel #1  plotted as a function of time  (days)*
                              30a

-------
    0.8
    0.6
 UJ
 O  0.4
 UJ
 ce
 o
 a.
    0.2
    0.0
T	r
                               1 - 1 - 1 - 1
     20         40


           TIME (DAYS)
                                         60
80
Figure 4.9.  Cumulative inflow in the  inner ring of Barrel #1

            as a function of the total pore volume below the

            infiltration ring plotted as a function of time

            (days).
                             31

-------
0.10

^ 0.08
1
E
3 0.06
O
ui
2
0 0.04
>
u
o
Q.
0.02
« />«
i • ' • ' « 6 oo
o
o
m *™
O
o
o
.
o
o
0°
0
J)
§
0
o
	 •_-!-. O 1 1 1 1 1 1
                   20       40        60
                        TIME  (DAYS)
80
Figure  1.10.  Cumulative outflow as a function of the  total
             pore volume above the bottom inner compartment
             plotted as a function of time.
                           3 la

-------
Caisson Prototypes

Caisson #1

     Caisson studies were to test  equipment and methodology.  The first study
initiated towards the end of summer  '84,  was to test a prototype liner,
Construction, and the experimental methods to be used in the full scale liner
facility.  Schematic diagram of  the  caisson set up is shown in Figure 4.11,
Plates 1.12, 4.13 and 4.14.  Four  collection ports (below the liner), three
sets of horizontal dual  access tubes,  four 1  x 1  ft banks of vertical access
tubes, six infiltration  rings and  constant head devices, and square pedestals
to measure swelling were installed in  a compacted 1  ft (30cm) thick clay
material.  The  prototype was compacted by hand in three lifts.  The surface of
each lift was scarified  before a new lift material was applied.  Table 4.2
gives average density and water  content measurements for each lift obtained
with surface and depth nuclear gauges.
                Caisson
                Added Liner
              E
              8

                     Base
                  Crawlspace
Access
 Tubes


 Seal
  Shallow
   Liner
                                                    Collection Ports
                                          Concrete Pad
          Figure 4.11.   Schematic diagram of the first caisson study.
                                       32

-------
Plate 4,12.   A bank of vertical access tubes for measurement of
             moisture and density with depth,  and a ring for
             measuring infiltration rate in flooded caisson.
                               33

-------
Plate 4.13.   Additional details of optocator positioning and of
             the optocator pedestal for measurement of clay
             swelling, infiltration rings and access tubes shown
             in a flooded caisson.
                               34

-------
Plate 4.14.   Constant head devices (cylinders)  for infiltration rings
             and for the caisson itself (carboy)  were placed on the
             outside of the caisson.
           TABLE 4.2.  AVERAGE SURFACE AND DEPTH MOISTURE
                        AND DENSITY READINGS      	
      Lift
               Dry Density
                                                  Water Content
                                   kg/m3
                                     kg/kg
                                         Surface probe
#1
#2
#3
5/31/84
6/1/84
6/4/84
1533 ± 85
1581 ± 39
1500 ± 42
25.5 ± 1.3
23.7 ± 1.2
23.7 ± 1.1
     10 cm
     20 cm
7/13/84
7/13/84
                                          Depth probe
1615 ±71
1504 ± 81
14.5 ± 2.4
23.8 ± 1.4
                                  35

-------
     The first three readings for each one of the three lifts in Table 4.2
were obtained with a surface probe at six locations for each lift.  The last
two readings were made with depth moisture and density probes at 16 locations
and two depths (10 and 20cm).  The 20cm density readings corresponded reason-
ably well to the surface probe readings for lift #1, #2 and #3.   Lift #3
readings on 6/4 appear considerably wetter than the 10cm reading taken with
depth moisture probe on 7/13.  Admittedly, the depth gage reading was taken
six weeks later, however surface gauge readings for lifts in  and #2 show
results similar to depth gage readings at 20cm.  Since lift #1  and #2 soil was
quite wet when compacted, we have allowed lift #3 soil to dry in place with
turning before compacting.  It was considerably easier to compact.  It may be
that surface moisture gauge readings with the surface gauge are in error.  One
probable reasons could be that during compaction liner surface may actually be
somewhat wetter than deeper layers and the neutrons from a surface gauge are
more readily backscattered by this surface layer indicating higher water con-
tent and lower density than actually present.  Following ponding of water over
the compacted surface, underdrains began to flow almost immediately.  There
also appeared some leakage around the perimeter of concrete slab.  The flow
diminished to manageable proportion after a day as the clay begun to swell.

     Liner instrumentation after the clay was compacted took a long time.
Placement of access tubes, rings and optocator pedestals (swelling measurement
by laser beam reflectance) as well as initial measurements before water was
added was very time consuming.  It also appears that some surface drying took
place (i.e., water content for 10cm depth in Table 4.2).  Instrumentation of a
full scale clay liner will also take a long time.  To minimize drying, compact-
ed liner will need to be covered with a surface layer of sand.

     Laser beam (optocator) was switched on as water was added to liner sur-
face to measure swelling of clay in time.  Figure 4.12 shows the results
obtained as percent of liner thickness.  Observed swelling was very rapid
during the first hour following ponding amounting to about \% change of eleva-
tion at the clay surface.  The swelling forced two infiltration rings and a
horizontal access tube (surface) out of the soil.

     Figure 4.13 shows the comparison between cumulative infiltration rate for
the rings in the caisson study and the results previously obtained for the
barrels.  Results suggest that the infiltration are likely to detect differ-
ences in infiltration over the surface of the full scale liner.

     The results also indicated that evaporation rates as measured with class
A pan will be on the order of 1 x 10~9 m/sec.  Consequently, evaporation
losses particularly at the lower rates of infiltration appeared to be
significant and needed to be accounted for in the full scale liner.

     Figure 4.14 shows the distribution of water content in time in one of the
access tubes at 10 and 20cm depth following compaction.  The results for other
access tubes were very similar.  In general, prior to ponding the drier top
layer (10cm) became wetter while the bottom layer (20cm) became drier.  When
caisson was ponded on the 41 st day after compaction water content in both
layers appeared to increase very rapidly.  Subsequent gravimetric sampling
failed to substantiate this apparent increase of water content.   The explana-
tion however may be that water infiltrated preferentially next to the tubes


                                      36

-------
   1.8




   1.5




3  1.2
u
«
ui

£  0.9

UJ
o

<  0.6
X
o


   0.3





   0.0
                 10
    100


TIME (MINUTES)
1000
IOOOO
  Figure 4.12.  Swelling of clay liner  given as percent of liner  thickness

               and plotted as a function of time.
                                  37

-------
U)
~J
pi
  OQ



  CD

  J=r
                                     cr o
                                     JB O
                                     T 3
=tt= co
-» o

OJ
D cr
a a>
  ci-
o s
ft) (D
l-* CD
CO D
CO
O O
                                     D OJ
                                     TO n-
                                     CO >*
                                     «  <
                                       
                                       ct
                                       )-*
                                       O
                                                                 CUMULATIVE  INFILTRATION (mm)

-------
    30
UJ
£20
O
o
(T
HI
     10
                                                    POND
                                                                     • ••
                    10
            20          30
                 DAYS
40
50
       Figure 4.14.
Typical water content with time (access tube  #1),
caisson was flooded 41  days after being compacted.
coating them with a thin sheet of water which the backscattered  neutrons  from
the depth moisture gauge picked up as water content of that layer.   We  have
observed that in the process of swelling two infiltration rings  and  one hori-
zontal access tube were forced out of a soil.   High moisture readings along
the access tubes may be related to disturbance due to swelling.

     Using the depth density gauge which measures density by backscatter  of
photons in a sphere around the source,  the average density of both the  10cm
and 20cm layer was 1831  kg/m3.  After flooding the density in the 10cm  layer
dropped to 1487 kg/m3 and in the 20cm layer remained about the same.  The
drastic decrease in density with a corresponding  increase in total porosity
most probably reflected the swelling of the topmost layer rather than the time
passage of a wetting front.

     While backscatter geometry yields  an average heavily weighted by the
density of material adjacent to the gauge access  tube,  direct transmission
geometry measures the average density in a thin pyramidal wedge  between the
source and the detector.   When density  was measured using direct transmission
gauge there was little or no change at  10 or 20cm depths  when water  was ponded
on the surface.  A slight drop in total pore space (TPS)  and more frequent
fluctuations in apparent  total pore space was  all that  was observed.
                                     38

-------
     At the close of cassion #1 study, direct transmission depth density read-
ings were taken in all pairs of access tubes at 1" intervals.  Results showed
that density near the surface appeared to decrease and IPS appeared to
increase suggesting swelling within the top two inches and little or no change
elsewhere following 16 days of ponding.

     During this preliminary test, access tubes were also placed horizontally,
one at the top and one at the bottom of compacted clay material.  Using dual
gamma gauge, direct measurements of bulk density in 6" (15cm) intervals along
each tube were made.  Total pore space (IPS) values for the horizontal read-
ings appeared higher next to the wall where it was difficult to compact the
clay and lower across the middle where better compaction was achieved.  Marked
response to flooding (41  days) was observed, rapidly reducing the total pore-
space available before ponding.  Differences in density and TPS may also
indicate zones of varying extent of compaction which would be more, or less
permeable than the rest of the compacted area.

     Computed mass balance for water in caisson #1 study showed that about 5%
of water added could not be accounted for.  Results suggested that the full
scale research facility be scrupulously sealed along the sides and bottom
before a liner was installed.  It was decided first to waterproof the side-
walls at the full scale facility, and then apply the foundation coating on the
inside.  Commercially available panels of Vol-Clay (Wyoming Bentonite) were
then to be placed between the liner and the wall to the level above the second
access tube and the sand layer.  In particular, the space around each hori-
zontal access tube would have to be sealed with Vol-Clay.  Vol-Clay has the
property that when wetted it expands to 6 to 14 times the volume thus filling
and closing any open voids at the clay wall interface.

     After ponded water was drained from the caisson #1 prototype study, the
caisson material was sampled on a 6" x 6" grid (15 x 15cm) with a Veihmeier
tube at four depth increments 0 to 3" (8cm), 3" to 6" (15cm), 6" to 9" (23cm),
and 9" to 12" (30cm) in order to verify data obtained with nuclear gauges and
to substantiate hypothesis of leakage next to vertical access tubes.  The
samples were dried immediately in the microwave oven and gravimetric water
contents were determined.  In addition, samples were also taken between access
tubes, to see if water contents were indeed as high as read with nuclear
moisture gauge; next to access tubes to verify the hypothesis of leakage; and
of the first four inches in 1" (2.5cm) increments to see how far the wetting
front has progressed.

     Results are given in Table 4.3 and show that there was essentially no
difference in water content among the access tubes and elsewhere on a 6" x 6"
grid.  The surface 1" (2.5cm) appeared the wettest and most crumbly, probably
because of swelling.  Results for water content next to the access tubes were
not conclusive.  Although the bottom 6" (15cm) were wetter than soil in other
areas the top six inches were not.  However, during sampling the material next
to the tubes appeared considerably wetter.  It should be remembered that a
Veihmeier tube has a bulge; consequently, a vertical sample right next to the
access tube is in reality taken - 0.5cm away, far enough to miss the wettest
zone.  Gravimetric sampling thus failed to substantiate the apparent increase
in water content observed in all access tubes and measured with a nuclear
probe.


                                      39

-------
              TABLE 4.3.  RESULTS OF GRAVIMETRIC MOISTURE SAMPLING
                 	OF THE COMPACTED CLAY LINER IN CAISSON 1
              Depth
             (inches)
Mean Water
 Content
Std. Dev.
                                           % by weight
               0-3
               3-6
               6-9
               9-12
               0-3
               3-6
               6-9
               9-12
               1-6
               6-12
   22.6
   20.0
   21 .0
   19.8
   2.5
   1.8
   1.5
   2.2
                                       Between access tubes
   22.3
   20.1
   21 .8
   19.6
   2.4
   1.4
   1.5
   1.6
                                       Next to access tubes
   22.1
   23.1
   1.7
   0.6
                                             inch depth
0-1
1-2
2-3
3.4
25.2
21.5
20.0
19.8
4.3
1.8
2.5
2.3
Caisson #2

     Based on our experience with Caisson #1 study an improved version (Figure
4.15) of the prototype was designed and tested.  The geometry was that of a
concrete rectangular box contained within the caisson.  The new design
incorporated an inner and outer bottom compartment similar to that used in
barrel studies to separate any outer wall flow from inner flow.  Separate
drains were installed for each area.  The design incorporated inflow and out-
flow pipes to monitor infiltration and mechanized compaction (Plate 4.15),
rather than manual compaction as in cassion 1 to achieve higher levels of
compaction closer to the projected proctor maximum.  The inflow pipe drained
very slowly into a recording rain gauge, while the outflow pipe emptied into
another recording rain gauge, the difference between the two corrected for
evaporation constituted infiltration.  Prior to the addition of clay, the
bottom of the prototype was covered with burlap and on the sides were four
removable wooden wedges (Plate 4.16).  Following compaction (Plate 4.15) the
wedges were lifted out and the space between the soil and the wall was filled
with a 1:1 mixture of fine sand and Vol-Clay, moistened as it was packed.
                                      40

-------
                                                  N
              DRAINS
-HORIZONTAL
 ACCESS TUBE
OUTER  SPACE
INNER SPACE
Im2

      INLET =*
SURFACE
PROBE
LOCATION
              EVAPORATION
              RING


           4= OUTLET
                VERTICAL
                ACCESS TUBES
  -INFILTRATION RINGS
     Figure 4.15.  Improved version of clay liner prototype.
                            41

-------
Plate 4.15.   Prototype liner being installed in caisson #2 study
             using mechanized compaction, neutron surface
             moisture/density gauge was used to monitor compaction.
                              42

-------
Plate 4.16.   The prototype liner concrete box,  just showing,  burlap
             covered bottom,  gypsum blocks located over drains and
             removable wooden wedges on the sides; the bottom
             horizontal access tube is barely visible in the center;
             raised metal ridge separates outer wall flow from flow
             in the inner compartment; constant head devices to be
             used with infiltration rings are shown along the walls.
                                 43

-------
Calibrated gypsum blocks were left in place below the clay (Plate 4.16) with
wires exiting through underdrains.  Following ponding the blocks were to
provide a test of an early warning signal that conditions under the liner were
getting wetter and breakthrough was imminent.  One horizontal set of access
tubes was installed across the box and one cluster of four vertical access
tubes were placed in somewhat larger access holes which were excavated after
the clay was in place.  The space between the access tube and clay was then
packed with dry Vol-Clay to prevent any flow along the walls of access tubes.
The infiltration rings were installed after Caisson #2 was ponded.  Mariotte
type cylinders designed to keep water level constant were placed on the inside
of the caisson to keep the facility nonfreezing during the winter.

     Design of Caisson #2 was an improvement over Caisson #1 and together with
the barrel studies it provided means of testing the concepts, techniques, and
instrumentation to be incorporated in the full scale facility.  Briefly, the
principal results were as follows.  In general, observed swelling (Figure
4.16) was less throughout because of better compaction.  Early arrival of
water at drain locations could be detected with gypsum blocks (Table 4.4).
However, drain outflow was not observed until after the blocks became fully
saturated.  Sufficient flow existed in the clay for block electrical resistiv-
ity to begin changing very shortly (< 1 day) after ponding.

     Several different ways of measuring bulk density of compacted clay were
tested.  They included surface and dual probe measurements and gravimetric
samples with a cork borer and Eley volumeter.  Water content was evaluated
using grab samples, depth and surface nuclear probes as well as previously
mentioned cork borer and Eley volumeter.  Summarized results, given in Tables
4.5 and 4.6, show much scatter depending on the method used.  Microwave drying
of soil gave essentially the same results as conventional oven.  Based on the
results obtained dual gamma probe in the horizontal mode appeared to be a
preferred method to use for extended study in a full scale research facility.
Table 4.7 shows values of wet bulk density (WD) and associated changes in
total available porosity in different parts of the prototype for different
times following ponding.  The method appeared to have sufficient sensitivity
to detect small changes of water content or porosity.  Finally, in Table 4.8,
outflows for different portions of the prototype liner are given.  Results
suggest faster flows next to walls where compaction was less and in general
very low outflow rates near the center.  Infiltration measured with rings had
to be corrected for evaporation since losses due to evaporation were of the
same order of magnitude as inflow.  Infiltration rate reflected outflows
observed in outer drains suggesting that flow was not necessarily vertically
downward.  Based on the results obtained at least 35 evaporation pans, same
size as the rings, were to be used in the large scale facility to provide a
correction for evaporation.  Tracer studies were also to be  incorporated to
evaluate flow pathway, and particular attention was to be focused on outflow
drains to detect first sign of water breakthrough in all of  the 250 drains.
                                       44

-------
     4.5-
     4.0-
               10
   100         1000
TIME (MINUTES)
10000
Figure M.16.   Comparison of observed swelling on prototype
              caisson 1  and 2  studies.
                           45

-------
   TABLE 4.4.   ELECTRICAL RESISTIVITY OF GYMSIUM BLOCKS BURIED BY  RESPECTIVE
     DRAINS (1  TO 6) UNDER THE COMPACTED CLAY PONDED (TIME 0)...QN 10/9/84
Drain Saturated
Value

1 400

2 420
3 390
4 300

5 M20

6 400
Time after ponding
0

4300

4300
4100
3000

5400

4300
1

3200

4000
2700
2700

3600

3700
2
electrical
800

2600
1900
1800

2450

2250
3
resistivity
440*

1850
1500
400*

1950

1625
(days)
6
( ohms )
450
t
460
420*
400*

1000

620

14

380°
0
390
350°
340°

400

320

17

A
360
A
380
A
360
A
360
A
360
A
360
*0utflow (mil) #1(180), #4(130).

^Outflow (mil) #1(2000), #2(25), #3(130), #4(2100).

°0utflow (mil) #1(940), #2(220), #3(360), #4(30), #5(0),  #6(120).

Outflow (mil) #1(910), #2(270), #3(130), #4(30), #5(10),  #6(70).
                                       46

-------
   TABLE 4.5.  WET AND DRY BULK DENSITY (WD AND DD) OF COMPACTED CLAY


    BEFORE PONDING. MEASURED WITH NUCLEAR PROBES AND GRAVIMETRICALLY
Lift
1
2
3
Surface
WD

1910
1984
1973^
1507*
probe
DD

1538
1580
1588
1507
Dual probe
WD

2063
2033
2025
DD


1630
1622
Cork
WD

1770
1728
1633
2195**
borer
DD

1433
1523
1413
1817
    *Surface probe direct transmission from 2" depth.

    £
     Sampled with Eley Volumeter.
  TABLE 4.6.  WATER CONTENT MEASURED GRAVIMETRICALLY AND WITH NUCLEAR


               PROBES ON COMPACTED CLAY PRIOR TO PONDING
Lift Cork
borer

1 17.8
2 14.8
3 15.0
Volumeter Grab
samples1

20.7
18.1
20.9 20.8
Depth
probe

14.7
19.8
-
Surface
probe

24.2
25.6
24.2
1 Conventional oven dried.
                                   47

-------
TABLE 1.7.  WET BULK DENSITY (WD) OF COMPACTED CLAY AS MEASURED WITH HORIZONTAL ACCESS
    TUBES AND COMPUTED VALUES OF TOTAL AVAILABLE PORE SPACE  (TAPS)1 BEFORE  (0) AND
                         FOLLOWING (1.  3. 11 DAYS) PONDING

                                        Days after ponding
Distance from
side2
inches
2
8
20
20
8
2
vjpi
1 iji« prt ^ . ™U _
2650
0
WD
kg/m3
1993
1956
1930
2021
1981
1872


TAPS
-
0.2179
0.2619
0.2717
0.2374
0.2513
0.2936


WD
kg/m3
2066
2087
1971
2075
2090
1969


1
TAPS
-
0.2201
0.2125
0.2562
0.2170
0.2113
0.2570


3
WD
kg/n\3
2075
2051
1989
2086
2086
1970


TAPS
-
0.2170
0.2219
0.2193
0.2128
0.2128
0.2560


11
WD
kg/m3
2089
2097
1991
2109
2106
2060


TAPS
-
0.2116
0.2086
0.2175
0.2012
0.2053
0.2261


      to North across the  prototype (Figure 1.15).
      TABLE  H.8.  OUTFLOW  RATES MEASURED IN INNER  (#5  AND #6)
         AND OUTER (#1.  #2.  *3 AND #4)  COMPARTMENT1  DRAINS
      Days''
  Outer  compartment
#1    #2     #3    #
                                               Inner  Compartment
                                                #5           #6

3

17
200
560

3
11
39
35
27

_
10
12
3
2
	 x 10 ' <
2
16 1
8 1
7 <1
2 «1
3tn/sec 	
-
-
0.02
0.05
0.001

-
0.22
1.40
0.13
0.002
      1See Figure  4.15.

      2After ponding.
                                      48

-------
                                  SECTION 5

                             FIELD SCALE STUDIES
TESTING FACILITY

     Based on the design and preliminary studies in Phase II a field scale
facility was constructed and a clay liner was installed.  After the site was
instrumented inflow, and outflow evaporation changes in density and surface
elevation were continuously monitored for a year.  This constituted Phase III
of the study.  Figure 5.1  shows the field scale facility.  The facility con-
sisted of an elevated bridge-like platform (Plate 4.2) supported by reinforced
concrete beams (Plate 4.1) which rested on compacted level subgrade.  This
arrangement allowed a crawl space under the platform (Plate 4.8) for collec-
tion of percolate which passed through the liner.  A 3' x 3' (0.9 x 0.9m) grid
of collection drains (Plate 4.3) was complemented by a similar grid of 11"
(28cm) diameter buffered infiltration cylinders (Plate 4.7) at the surface.
  Figure 5.1.   Clay liner testing facility,  similar to Figure 4.1  but in SI
               units showing additional detail on horizontal access tubes.
                                      49

-------
       Embedded in the floor of the platform,  horizontally  across  the  facility
  were the lower of the 24 access tubes  (Plate 4.5)  for  the measurement of
  density using the Troxler1 dual gamma  probe, their tops protruding 0.25"
  (0.60cm) above the level of the floor.  Positioned on  top of  the clay and
  situated exactly 1 ' (0.3m) above the lower ones  were the  upper access tubes.
  The attenuation measurements were made with  a gamma source (Cs^37) in the
  lower tube and the detector in the upper tube (Plate 4.6).

       Figure 5.2 shows the measuring grids used in  the  study.  Their  origin
  (0,0) was in the southwest corner of the platform  shown in Figure 5.1.   After
  the liner was compacted the facility was covered with  a building,  and heat and
  light systems were installed.  To account for evaporation from infiltration
  rings 35 small evaporation pans, same  size as the  rings,  were installed
  (Figure 5.2c) in addition to one large class A evaporation pan,  to correct for
  evaporation from water ponded on the liner surface.  In addition,  35  metal
  pedestals and a wooden walkway supported by  access tubes  (Plate  5.1)  were
  placed on the clay surface (Figure 5.2c) to  monitor potential swelling,  to
  keep access tubes from being forced up, and  to provide access to
  instrumentation.
    0123456789
(a)
                              0123456789
 240 DUAL PROBE DENSITY
 READING SITES
                           (b)

•

®

•

®
•
Si







®

.

®

•
®








.

®

•

®
•








®

•

®

•
^








•

®

.

®
•








®

.

®

.
®








•

®

.

®
.








®

•

®

.
®








•

®

•

®
•








®

.

®

.
®



91



 250 INFILTRATION CYLINDERS
 AND UNDERDRAWS
» 35 CYLINDERS STARTED
 INITIALLY
                           (c)
A
B
C
D
E
F
G
H
I
J
K
L
M
N
O
P
Q
R
S
T
U
V
W
X
01 23456789














1


(


(






I






























1


1


1


<


1






>


1

































1


I


(






1

































1


1


(


(






1

































)


1


(


(





























• 35 SITES TO MEASURE SWELUNG
035 SMALL EVAPORATION PANS
O 1 LARGE EVAPORATION PAN
        Figure 5.2.  Experimental measuring grid for  (a) bulk density,  (b)
                     infiltration and drainage, (c) swelling and evaporation.
                                        50

-------
Plate 5.1.  Infiltration rings, a pedestal and a wooden walkway supported
            by access tubes were installed in compacted clay liner.


     Prior to installation of clay, the floor of the platform was sealed with
B/C Cure-Seal1, and a bead of Vol-Clay1  (Wyoming bentonite) was placed 3' away
from the sidewalls (Plate 5.2) on the floor to separate any potential wall
flow from the rest of the leachate.  To minimize wall flow Vol-Clay1  panels
were also placed against sidewalls (Plate 5.3)i which were previously sealed
on the inside and on the outside with Bondex1 waterproof seal, and another
bead of Vol-Clay1  was placed at the junction of sidewall and main deck.  Since
Vol-Clay1  swells on contact with water,  pressure build up between the liner
clay and Vol-Clay1 should have created a leak-proof contact.  The floor of the
platform was first covered with burlap and then a thin layer of coarse sand
was placed on top to just cover the bottom access tubes.  After the liner was
installed another layer of coarse sand was placed on clay surface to minimize
evaporation prior to ponding.
     1The mention of trade names in this publication does not constitute an
endorsement of the product by the U.S.  Department of Agriculture over other
products not mentioned.
                                      51

-------
Plate 5.2.  The floor of the platform was sealed, and the bead
            of the bentonite was placed 3' away from the
            sidewalls, subsequently the floor was covered with
            burlap and a thin layer of sand.
                              52

-------
Plate 5.3.   Bentonite panels are  being placed against sealed platform
            sidewalls,  to  minimize wall effects.
                                  53

-------
     Clay  soil  materials used  for the experimental liner was a B-horizon  of a
commercially available cherty  silt loam  (Typic Hapludult)  from central
Pennsylvania.   Table 5.1 shows some properties of this material as furnished
by the supplier,  as measured by HWERL, and  as determined by us (NWRC).  The
soil is classified as a CL type brown till  with laboratory permeability < 1  x
10~7 cm/sec.  Based on x-ray diffraction procedure the till was found to  be a
mixture of  kaolinite and illite with some smectite.  Prototype studies
suggested  that  some swelling was to be expected after ponding mainly through
enlargement of  capillary films in nonexpanding lattice illite and kaolinite as
well as osmotic imbibition by  the expanding lattice smectite.  Since the
proportion  of smectite was very low, swelling and dispersion were expected to
be minimal.   The till material was purchased from the supplier and trucked to
the site where  the liner was to be constructed.
Soil Materials
     The 180  tons of till brought by truck  (23T/load) to  Klingerstown,  were of
variable quality.  It contained some very large clods (>  6").   Most  seemed dry
(14-1 6% water content by weight), while some got wet (22%)  in transit  since
tarps covering it were not  fastened well enough.  The till  was brought in and
deposited  in  large piles.   These were subsequently sampled  for moisture with a
Veihmeyer  tube,  split into  several (5-6) subsamples dried,  and weighed.   In
addition,  two large samples were also taken for clod size analysis.  The
results are given in Table  5.2.   Average results on delivered material showed
that in general  clods larger than 1" (2.5cm) constituted  more than 25/6 of the
total, while  for sample #2  clods larger than H" (10cm)  constituted almost 10?
of the total.  These large  clods were anticipated to present a problem during
wetting and compaction of the clay.
           TABLE 5.1.  SELECTED PROPERTIES OF THE TILL USED AS LINER MATERIAL AS DETERMINED BY SUPPLIER
             i  ——	OUR (NWRCK AND EPJ CHUFRI 1 onTI Tirei-rur- '""ORATORIES        •"•rruj.nn,
 Property
 Silica
 Alumina
 Titania
 Ferric Oxide
 Sodium Oxide
 Potassium Oxide
 Loss on Ignition

 Mineral Composition

 Attenberg Limits
  Liquid Unit
  Plastic limit
  Plasticity index
  Type

 Hater Content

 Standard Proctor
 Modified Proctor
                 Supplier
                                       NWRC
                                                                HWERL
58.00*
16.06*
0.58*
5. 71 It
0.13*
1.58*
9.56?
36*
20$
16*
CL







quartz , K feldspar , kaol Ini te ,
35*
23*
12*
CL







illite, smectite 	 	 	
36*
19*
17*
CL
13.61*

110 pof at 18* water content
118 pcf at 14* water content
109.5 pcf at 17.8* water content
Permeability Test    1.10 to 1.76 x 10'9 om/seo
                         112.1 pcf at 16.9* water content
                         120.3 pof at 12.9* water content
                                         54

-------
           TABLE 5.2.  CLOD SIZE ANALYSIS OF  TWO LARGE SAMPLES
Sieve
mm
100
-75
50
25
19
10
<10
opening
inches
4
3
2
1
3/4
3/8
<3/8
Sample #1
* -
0
1.5
5.9
11.6
8.0
16.1
56.8
Sample #2
% by wt
9.4
7.5
6.3
12.1
•7.4
14.6
42.6
Average
% by wt
4.7
4.5
6.2
11.8
7.7
15.3
49.7
LINER CONSTRUCTION

    Figure 5.3 shows the Standard Proctor compaction test results for the
material used  in this study.   The maximum bulk density at 17.8$  water content
was found experimentally to be 1754 kg/m3 (110 pcf), about'the value furnished
by supplier and somewhat less than subsequently determined by HWERL (Table
5.1).
            20
        K)
             18
         LU
         O
         m
             16
             14
                                                    SATURATION
                          O
                           i
I I7.8 OPTIMUM
                          10        15        20       25

                          WATER CONTENT  (PERCENT)

    Figure 5.3.  Standard Proctor compaction test on till material used
                in the liner.
                        3O
                                 55

-------
Experimental Procedures

     The contractor arrived on 10/30/84 with a Dratt backhoe, 5-1/2 ton (5Tm)
caterpillar bulldozer tractor, 15 ton truck (14Tra), a 5-2 = 3 (2.7Tm) ton
sheepsfoot roller (empty), Bolag "nervous turtle"—a small vibratory pull type
compactor—and a jackhammer with a 6" x 6" (15 x 15cm) foot.  The original
plan was first to compact a test plot (Plate 5.4).  For that purpose on a 10'
x 10' area (3 x 3m) area about an 8" (20cm) layer of clay was deposited.  It
was underlain in one place by two access tubes horizontally imbedded in a
concrete slab.  Water contents were measured with a microwave (16.5/0,  and an
adequate amount (see example) of water was added with a hose to bring the soil
above the optimum water content.  Application time turned out to be dispropor-
tionately long even for so small a test area although incorporating water into
the soil with a garden rototiller appeared to work well.
     Plate 5.4.  Test plot is being compacted using a sheepsfoot roller,
                                      56

-------
     Example.

     A test plot = 10' x 8' x 6" (3.05 x 2.44 x 0.15m) = 1.133 m3 would
     contain, at Standard Proctor density of 1794 kg/ra3, 2032 kg of soil.
     It needs 386 kg of water to bring it to 19? water content from
     335 kg of water at 16.5? water content.  Therefore, we found we
     needed to apply 51 kg water (~ 14 gallons) to the test plot to bring
     it above the optimum.

     The first lift was installed as follows.  The backhoe operator loaded the
truck with till, perched himself on the side of the platform (Plate 5.5) and
spread the soil from truck on the pad which was covered with burlap and a thin
layer of sand (Plate 5.2).  In this manner several truck loads were spread on
the platform - 6" deep and enough for a 4" finished layer.  As the clay was
spread with a backhoe it was wetted with 183 gallons of water to bring it to a
water content greater than the optimum (19? by wt).  As the operation
progressed two rototillers (Plate 5.6) were used to incorporate the water into
the soil and break layer clods.  When the loose layer appeared ready for
compaction, grab samples were taken at 36 grid locations for moisture, and
Plate 5.5.   Clay material was brought in by trucks and spread on the
            platform with a large backhoe.
                                      57

-------
       Plate 5.6.  After the required amount of water was added, it was
                   incorporated into the clay by rototilling.


clay was rolled first with a bulldozer then smooth with a 7-1/2 (7Tm) ton
roller (rather than with sheepsfoot) to protect access tubes from being dented
(Plate 5.7).  Some access tubes were dented nevertheless, either by stones
falling on them during the spreading of clay, mixing by rototiller process, or
even by tamping with jackhammer along the edges.  However, since cesium-137
source in the dual density probe was relatively small, only the guide geometry
had to be changed (a pie slice was removed) to allow it to slide freely
through the dented tubes.  Following compaction we ended up with about a M"
(10cm) lift quite well compacted near the center, not so well compacted near
the walls, particularly where jackhammer tamper influence ended and smooth
roller compacting influence had not fully begun.  Only 2 passes of the
small—nervous turtle—roller (Plate 5.8) could be used on each side next to
the wall so as not to collapse the access tubes.  To make sure of a flat level
surface elevations were taken at M8 locations, measured from the stretched
string down, and surface probe moisture density (Plate 5.9) readings in the
backscatter mode were made at 36 points.  Prior to spreading the second lift
the smooth surface was roughened (Plate 5.10) by running over it with a
bulldozer.
                                      58

-------
Plate 5.7.   Following several passes with the bulldozer  and
            sheepsfoot roller,  each lift was smoothed out by
            large vibratory roller prior to measurement  of
            density.
                             59

-------
Plate 5.8.   Near the walls clay was compacted using a  "nervous  turtle"
            roller (shown above) and jackhammer  (not shown).
                                 60

-------
Plate 5.9.   Water  content and density were measured using a nuclear
            moisture-density probe.
                                 61

-------
 Plate 5.10.  Prior to installation of the next lift the clay  surface
             was roughened by bulldozer treads.


     Spreading the second layer (lift) was much easier.  The  material  was
 wetted with 151 gallons of water as it was spread by the backhoe from  the
 truck on the platform at about 3 p.m.  It was rototilled and  pushed around
 with the bulldozer.  However, because of the weight of the bulldozer spreading
 the soil simultaneously compacted it, making it hard to rototill and mix the
 water with the entire 8" of loose second lift material.  Subsequently  a sheeps-
 foot roller pulled by the bulldozer made 30 passes over the area (this worked
 out to between 6 and 7 full coverages).  Six "turtle" passes  were made on the
 sides and finally the material was tapped against the walls with a jackhammer.
 Although it would have been preferable to see the sheepsfoot  roller actually
 "walk out" as compaction proceeded, the bulldozer during spreading the slay
 already compacted the soil to a certain extent so that sheepsfoot roller
 appeared1 to "walk out" from the start.  Pre-compaction, grab  samples for water
 content determination were taken at 36 locations also from this layer.

     After the bulldozer-sheepsfoot roller compaction, the surface was rough
with many indentions.  It had to be smoothed with the flat 7-1/2 ton roller
used without vibration before 36 moisture-density readings could be made with
a surface probe in the backscatter mode.  Even then it was difficult to find a
really good smooth surface necessary to make moisture-density measurements
                                      62

-------
with a nuclear gauge.  A number of Eley volumeter samples were also taken
especially close to the walls where it was impractical to use the surface
Troxler1  gauge, and elevations of the clay surface was measured.

     The third lift was spread on the surface of the second lift roughened
with the caterpillar treads and wetted like lift 2.  Soil water readings
(microwave) indicated a somewhat higher initial water content (17.55&) although
the soil did not look any wetter than before.  Consequently, only 92 gallons
of water were added to the clay.  The material was spread as before with the
bulldozer, but again it was difficult to rototill it, especially the eastern
1/3 of the platform which seemed wetter.  The lift was again sampled for
moisture at 36 locations, rolled with the bulldozer and sheepsfoot 28 times
(6-7 passes), rolled on the sides 6 times with "nervous turtle" and tamped
with the jackhammer immediately next to the wall.  Water contents appeared
satisfactory, but density values (taken with nuclear surface probe, in the
backscatter mode) appeared lower, largely because of uneven surface conditions.

     When the liner was trimmed across its entire width and on either side
with a backhoe, all three lifts were well blended and could not be told apart.
The installation was completed by noon of the second day.  The surface again
appeared rough, almost too rough for good surface moisture-density
measurements, and the soil was too hard to attempt any physical smoothing.

     Based on elevation survey, the center of the final lift was about 2"
(5cm) higher than the sides.  To make sure that the horizontal access tubes
were absolutely level and parallel to the lower set they had to be installed
by tapping a solid metal form into the clay on the straight chalkline.  The
clay was so hard that infiltration rings had to be hammered in with a sledge
after a solid metal form was fitted into the ring top.  Pedestals to measure
swelling was tapped in place to provide good contact and a wooden walkway
superstructure resting on the access tubes was constructed to provide access
to installed instrumentation.  After all instrumentation was installed a 1"
(2.5cm) layer of sand was spread on the surface to minimize evaporation.  The
liner had to be periodically moistened to keep the surface from drying out
until the sand layer could be applied.


Summary of Installation

     To summarize, three six inch (15cm) thick layers of clay material were
compacted to four inch (10cm) thick lifts following the procedure developed on
a construction test plot, giving a finished twelve inch (30cm) thick clay
liner.  Although as delivered the clay was wet enough, by the time it was
spread and compacted several weeks later, additional water was needed.  The
clay was, therefore, wetted with a known amount of water necessary to bring it
to wet of optimum, tilled with rototillers to break clods sampled for water
content,  and compacted in place.  Surface gauge readings of water content and
density in 36 locations indicated the level of compaction achieved.

     During the construction phase two problems surfaced:  the bulldozer
tended to compact the clay making it difficult to rototill, and the full scale
compaction equipment could not approach safely any closer than a foot to foot
and a half (30 to 45cm) from the sidewalls.  These problems were addressed by


                                      63

-------
a more intensive but slower rototilling and by  the  use  of  a small  Bomag^
vibrating roller 6" to 12" (15 to 30cm) from  the  sidewall  and an electric
jackhammer with a square 6" x 6" (15 x 15cm)  foot right next to  the wall.
Degree of compaction achieved near the sidewalls  was  judged to be  near  to  that
obtained over the remainder of the area.  However,  detailed analysis of
samples indicated considerably lower density  values near to the  sidewalls.
Figure 5.4 shows the compaction achieved with a sheepsfoot roller  and compares
it with the degree of compaction achieved with  a  small  vibrating roller and
jackhammer next to the sidewalls where it was not possible to operate the  full
scale equipment.  The results suggest considerably  less compaction next to the
sidewalls.  Consequently, for analysis of flow  only an  inner 8 x 23 grid
matrix of rings and drains was to be examined.

     In Figure 5.5 density and water content  values for each of  the three
lifts (sheepsfoot compaction) are compared against  Proctor constants.  The
upper solid line represents the line of saturation  (zero voids), while  the
lower one is the line of maximums for different compactive efforts and  water
contents.  Dashed lines indicate optimum (vertical) water  content  (17.8$)  and
  o>
  X
  X
  Jtt
  to
     18
     16
     14
     12
     10
           Modified
       . • Sheepsfoot
                                                            Saturation
             J
• Jackhammer

o Roller


    _L
              10     15      20     25    30  S      10
                                 Moisture  Content,  percent
           15
                                                                 20
                         25
                                                                              30
    Figure 5.4.   Values  of  water  content and dry density measured with the
                  nuclear surface  probe for the sheepsfoot roller, and with
                  Eleyl volumeter,  gravimetric samples for jackhammer and
                  small vibratory  roller; solid lines represent laboratory
                  measured Standard Proctor compaction and saturation curves,
                  dashed  vertical  lines give optimum moisture content (17.8%)
                  and  dashed horizontal lines represent 90$ of the maximum
                  density (1754  kg/m3).
                                       64

-------
                1700
                1600
                1500
                1400
                1700
                1600
                1500
              s
                1400
                 1700
                 1600
                 1500
                 1400
Opt.
                         LIFT #1
Opt.
                         LIFT #2
                         LIFT
                              _L
                                   _L
                                        _L
                                              _L
                                                   _L
                                                        _L
                                                              06
                                                              00
                                                              94
                                                              88
                                                              106
                                                              100
                                                                 55
                                                               94 8
                                                               88
                                E
                                O
                                                              106
                                                              100
                                                               94
                                                               88
                         16    17   18   19    20    21    22

                               WATER CONTENT % (by weight)
Figure 5.5.   Distribution of water content (by wt)  and dry densities (DD)
              on three  compacted lifts  measured with Troxler1  surface probe
              in the backscatter mode,  shown against the background of
              Proctor density at optimum water content (opt),  lines of
              maximums  and line of saturation (zero  voids).
                                         65

-------
95% Standard Proctor (1754 kg/m3) conditions (horizontal).  The quality of
individual lifts improved markedly from the first to the third.  For lift #1
3Q% of locations had densities below the line of maximums and 15$ had water
contents less than optimum, whereas for lift #3 only 14/6 of locations had
density below the line of maximums and none had the water content less than
optimums.
Site, Scale, and Spatial Relationships

     Water contents and density control data discussed above were collected
during the construction of the liner along with gravimetric water samples,
Eley^ volumeter samples, and a Troxler'' surface moisture density probe.
Following construction bulk density readings were taken vertically with the
dual gamma probe in horizontal position.

     Table 5.3 lists the cross sectional areas and volumes associated with
swelling, flux monitoring, bulk density, and water content measurements.
Figure 5.6. shows the geometry and scale considerations for the different
methods of density measurement.
        TABLE 5.3.  CROSS SECTIONAL AREAS AND VOLUMES ASSOCIATED WITH
                 MONITORING OF WATER FLOW, WATER CONTENT, AND
                   BULK DENSITY IN THE COMPACTED CLAY LINER

                                        Cross sectional        Volume
                                             area
                                              cm^                cm3

                                  Swelling

      Pedestals (36)                             232

                               Flux monitoring

      Infiltration cylinders (250)               613              4,672
      Leachate drains (250)                    8,361            254.952
      Sidewalls                              551,844         16,820,207
      Liner                                2,090,318         63,712,905

                       Moisture and density monitoring

      Volumeter (24)                               6                 10
      Dual gamma probe (240)                       5                 49

      Nuclear surface probe (118)                465             10,619*
                                                                  6,968


      *For moisture at 17.8? water content by weight and backseatter
       density, respectively.

                                      66

-------
                                                     Volumeter
                                                      «-1.1 in-
                     Source
                                           Surface  Probe
                                               (Backscatter)
                                 Source
                               Surface
                                                            Detectors
                                                           ••*.'.!*:'•*

                                                           Photon Paths
       Figure 5.6.  Geometry  and  scale considerations of Troxler^  dual
                    gamma  probe,  Eley^  volumeter, and Troxler^ surface
                    moisture-density probe in backscatter mode.
     On a relative basis,  the  dual gamma probe measures a volume about  5  times
the volume of the volumeter, whereas the nuclear surface probe  in  the back-
scatter mode measures density  and moisture over a volume 100 to 200  times
larger than the volume  measured by the dual gamma probe, and 700 to  1000  times
larger than measured by the volumeter.  The volume of the liner is - 6000 to
9000 times larger than  the volume measured by the surface probe.   Similarly,
the volume of the liner as a whole is 55 times the volume of all the infiltra-
tion rings combined (250), whereas,  the volume assumed associated  with  each
leachate drain (3x3x1  ft)  is - 55 times the volume of each  infiltration
ring*  The sidewall and endwall drains together represent - 1A the  volume of
the whole liner, while  swelling is recorded by a combined (36 locations)
response of less than Q.5% of  the area.
                                       67

-------
Surface Moisture and Density

     Figure 5.7 shows distribution of water contents in the 9 x 23m (30' x
75') liner testing facility for lifts #1,  #2 and #3 based on 36 small gravimet-
ric grab samples taken from each lift before compaction, and Figure 5.8 gives
the distribution of water contents in the same three lifts based on 36 nuclear
surface gauge measurements following compaction.  The differences between the
two reflect primarily differences in methods and sample sizes used.  Gauge
data represent nuclear readings on a larger sample volume.  Small (2 oz, 50g)
grab samples dried in a microwave oven represent point measurements.  Previous
comparisons of surface gauge measurements with samples dried in a microwave
during the prototype study indicated that, at least for our conditions,
                                          MoistureGravimetric
                         (5.1)
                    |    |<9S*OPT
95-105 SORT
                         [>105*OPT
             Figure 5.7.  Distribution of water content in lifts
                          #1, #2 and #3 of the experimental clay
                          liner based on small gravimetric grab
                          samples, optimum (OPT) moisture content
                          is 17.8$ by weight.
                                      68

-------
                  I    I < 95 SOFT
95 -105 H OPT
            Figure 5.8.   Distribution of water content in lifts
                         #1,  #2 and #3 of the experimental clay
                         liner based on nuclear surface moisture
                         gauge, optimum (OPT) moisture content
                         was  17.8$ by weight.
Nearly 9Q% of the water contents measured with a nuclear gauge were greater
than optimum, more than 70/6 were greater than 1 .05 optimum, and only 2% were
less than 0.95 optimum.  Nuclear gauge readings are affected most by the water
content close to or at the soil surface.  In that respect they correspond to
gravimetric point samples.  However, unlike the gravimetric point samples the
overall depth of measurement for the surface gauge varies with the water
content (M) of the soil2,
                        Depth (mm) = 280 - 0.27 M (kg/m3)
                           (5.2)
with M = 178, the depth of measurement is approximately 9".  Consequently,
water content for a much larger and more representative volume of soil is
     Instruction Manual 3^00-B Series surface moisture-density gauges,
Troxler Laboratories, P.O. Box 12057, Research Triangle Park, NC 27709,
USA.
                                      69

-------
averaged in nuclear gauge readings than in grab samples, with a tendency to
smooth out individual lift values.  Table 5.4 shows the actual mean and
standard deviation values of water content for each lift for the two methods.
Point grab samples show considerable variability,  while a smoothing effect of
nuclear gauge readings is quite apparent.

     Figure 5.9 shows the spatial distribution of  dry bulk density for three
lifts of a compacted clay liner and Table 5.5 gives the proportional breakdown
and partitioning of data as a function of Standard Proctor compaction test.
The results show that more than 80% of values for  lift in  and more than 90? of
values for lifts #2 and #3 were within 90 to 95% Standard Proctor or better.
A poorer performance of lift #1  reflects a modified compaction procedure,
whereby the lift was compacted using the dozer and smoothfaced roller only.
      TABLE 5.4.  DISTRIBUTION OF WATER CONTENT (GRAVIMETRIC) IN CLAY
        LINER COMPUTED FROM NUCLEAR GAUGE DATA ANDJ^QINT _GRAB^SAMPLES

      Method                     Lift 1    Lift 2    Lift 3      Average
                                 	 kg/m3 	

      Nuclear

        Mean                       193       192       192         192
        Standard Deviation           111           1

      Point

        Mean                       178       185       180         181
        Standard Deviation          23        17        15          18
                                      70

-------
                   Liftl
        Lift 2
            Lift3
                    I   I <90% Proof.

                        >95% Proof.
                 90-95% Proof.
      Figure  5.9.   Distribution of dry bulk density in lifts
                    #1,  #2 and #3 of compacted clay liner in
                    terms of Standard Proctor (PROCT) density
                    (175*1 kg/m3, 110 PCF).
TABLE 5.5.  DRY BULK  DENSITY OF THE THREE LIFTS OF COMPACTED CLAY
     LINER AS A FUNCTION  OF  STANDARD PROCTOR COMPACTION TEST
Density
Lift 1     Lift 2    Lift 3
                                                           Average
< 90% Proctor
90 to 95$ Proctor
> 9556 Proctor
> 94$ Proctor
  17
  42
  42
  53
percent

   6
  42
  52
  64
 8
53
39
53
10
46
44
57
                                71

-------
EXPERIMENTAL RESULTS

Preponded Stage

Density—

     Collection of  bulk density (wet) data using  dual  gamma probe (WDd) in the
horizontal access tubes begun immediately after the  clay liner was constructed
and the upper  set of  access tubes were installed.  The initial thirteen sets
of density readings were taken across the liner at one foot (30cm) intervals
(rather than at 3'  intervals which would have given  240 values) to give a
total of 720 values for a liner.  Table 5.6 gives the  sample statistics for
the thirteen data sets, taken prior to ponding, as well as their temporal mean
and standard deviation.  The temporal preponding  mean  in Table 5.7, based on
all (9360) observations, differs only by 2 kg/iiP  from  the mean based on
observations taken  at the locations 3' apart as specified in Figure 5.2a.  The
           TABLE 1.6.  STATISTICS Of 13 SULK DENSITY (WET) DATA SETS TAKEN CONTINUOUSLY AND CONSECUTIVELY FOLLOWING



No. of Saaplo*
Hun
Median
T-Mtan
Sta. Deviation
Std. Error of
tin Mean
Max. Value
Hln. Valui
Third Quantll*
First Quantll*


1

720
2185.5
2186.0
2185.2
86.9
3.2

2452.0
1889.0
2238.7
21 3* .2


2 3

720 720
2184.5 2181.6
2188.0 2185.0
2183.7 2181.5
90.
3.

2527.
1900.
223*.
2129.
87.2
3.2

2461.0
1934.0
223*.0
2128.0

Data S«t
» 5 i 7 8
-
720 720 720 720 720
2179.8 2202.2 2182.6 2191.5 2198.5
2186.0 2210.0 2185. 2195.0 2206.0
2180.* 2202.2 2181. 2191.6 2198.7
88.7 90.9 83. 89.1 90.1
3.3 3.4 3. 3.3 3.*

2*28.0 2*78.0 2*48. 2447.0 2462.0
1909.0 1952.0 1971. 1933.0 1533.0
2235.0 2262.7 2233.7 2249.0 2256.7
2126.0 2143.2 2128.2 2129.2 2143.0


9

720
2198.4
2195.0
2190.1
87.4
3.3

2435.0
1934-0
22*6.0
21 34. 0


10

720
2194.4
2201 .0
2194.2
90.3
3.*

2551 .0
1937.0
2250.0
2140.0


11

720
2183.7
2187.0
2184.3
86.5
3.2

2455.0
1939.0
2241 .0
2128.2


12

720
2184.3
2188.5
2184.8
87.1
3.2

2454.0
1914.0
2238.0
2131.2


13

720
2181.5
2184.0
2181.3
87.0
3.2

2466.0
19*0.0
2235.7
2130.0

Mean

9360
2188
2192
2188
88
3

2457
1930
2243
2133

Std. Oevl-
atlon

7
9
7
2
0.1

35
22
9
6
              TABLE 5.7.  PARTICLE DENSITY1  OF GROUND FRACTION OF
                              CLAY LINER  MATERIAL
              Site
 Specific gravity
                 Average
               A6
               06
               K8
               N7
               T2
               W1

              Mean
	 (kg/m3 	

2626          2653
2788          2793
2795          2717
2735          2663
2680          2737
2693          2691
                2640
                2791
                2756
                2699
                2709
                2697
       19
        4
       55
       51
       40
        1
2720 ± 66
2709 ± 52
2714 ± 52
              1 Determined using ASTM C-188-84 procedure at 26°C.

                                       72

-------
difference between the two in standard deviation is somewhat larger but not
alarmingly so (88 vs 83 kg/m3).   Figure 5.10 shows the spatial distribution of
the average preponding bulk density over the liner as a whole.  Highest
density values appear to be in the west central portion of the site.   The
reason for this may be that as the clay was being compacted with rollers
(sheepsfoot and smooth) they would travel back and forth with the central
portion receiving relatively more passes than the side shown on a hypothetical
example in Figure 5.11.


Total available pore space—

     Dual probe density values (WD
-------
      HYPOTHETICAL
     ROLLER  PASSES
  I  5
  I  i
  II
           7 3
f  f  t
                             -SIDE WALLS
           H
          624
Figure 5.11.  An illustration of why the center
            portion of the clay liner may have
            received more passes than the sides.
                     74

-------
                                    a.
                                         N
      (J
      z
      <
      I—
      co
                            8      12
                          DISTANCE
                     16

                     (m)
20
24
        Figure 5.12.
Contours of average density (in kg/m3) adjusted
to surface probe density values (a),  and of
surface probe moisture content (in kg/m3) (b),
before ponding.
the Figure 5.12a-matrix of values we are left with the dry spatial distribu-
tion of bulk density (DD) prior to ponding.   The formulas used are as follows,
           ws + ww   ww _ ws
             vs      vs   vs
                                                                         (5.3)
where WS is the weight of soil (kg),  WW is the weight of water (kg),  and VS is
the volume of soil (m3).   The first term on the left is essentially an expres-
sion for the bulk density of wet material in (kg/m3)f the second term is water
content by volume, and the last term on the right is the expression for dry
bulk density.  Similarly,
                                  WW
                                  vs
               /ws _ ww
              /  vs   ws
                                      75

-------
where the terra on the right is now the water content by weight (kg of water/kg
of soil).  The calculated matrix of dry spatially distributed bulk densities
can now be used in conjunction with measured particle density values for the
liner material (Table 5.7) to compute a 10 x 24 matrix of total available pore
space (TAP) by volume (m3/m3).  Measured water content by volume (kg/m3) can
also be,
                               TAP = (1-DD/27U)
                                                     (5.5)
expressed in the same units as TAP (i.e., 1  kg water/m3 soil = 0.001  m3
water/m3 soil), subtracted from the TAP matrix, multiplied by 1000 (kg/m3) and
expressed as a matrix of the amount of water needed (in kg/mg) to fully satu-
rate the liner.  Figure 5.13 shows such a spatial distribution of the amount
of water needed (kg/irr) to saturate the clay just prior to ponding.  Such a
priori computations may, however, be subject to considerable error for several
reasons.  First, the ratio of surface density to dual probe mean may not truly
represent the extent of local variation.  Second, the water content values
used to correct WD^ to DD may not represent true water contents as perceived
by the dual probe because of differences in geometry.  Finally, particle
density may be varying more than expected for a uniform material since the
                                                                N
          <
          I—
          oo
             18 -
1 1 1 1 1 1 1 1 1 1 1 1
''jS// /in fi n NNN
. y/
.
c


D
. •*
\v 	 ^ 	 40 	 	 40^
!:
ID
D
1 -

-
t).
^_^- $$— 	 	 	 9$ 	 -//'
                      12     24      36     48     60      72
                            DISTANCE,  feet
      Figure ?.13.
Interpolated isopleths of the amount of water needed
to saturate the liner (in kg/m3) at ponding and
associated interpolation variance.
                                       76

-------
statistics given in Table 5.7 are somewhat larger than the ASTM C-188 preci-
sion guidelines call for in case of a uniform material (12 kg/m3).  Soil
particle density is usually taken as 2650 kg/m3.  Larger values observed here
for the clay liner material are probably indicative of high iron content in
the soil (6$).

     The amount of water needed to saturate the clay liner will be discussed
in connection with ponding and compared with a similar matrix derived after
the water is drained.  In the meantime, changes in the amount of water needed
over time may indicate that a part of infiltrating water is diffusing into the
clay and part is passing rapidly through larger pores.
Ponded Stage

Sampling plan—

     After the clay liner was compacted on October 30, 1984 and instrumented,
a walkway resting on the topmost access tubes was constructed and a thin (-
3cm) layer of sand was spread on the surface to minimize evaporation and subse-
quently to help distribute applied water.  The area was ponded on March 26,
1985.  Water was brought in two large tanker trucks on March 26, 1985 and
11,7004 (3080 gal) were applied to the liner through a slotted orifice onto a
plastic sheet covering part of the surface to prevent washout damage to the
clay surface.  This initial water, which was ponded on the liner surface to
the depth of 5.6 cm on the average, was obtained from a nearby farm pond
(Klinger pond).  Subsequent additions as needed were first taken from the
water that remained in the tanker trucks (till 11-7-85), and then from a local
well.  The water level on the liner was maintained with an automatic constant
head tank, and checked daily.  Similarly, each of the infiltration cylinders
and evaporation pans were equipped with a manometer type constant head 1 liter
Mariotte bottle (Figure 5.14) set to the same water level as in the liner.
Initially, leachate was to be collected in ~ 4)1 milk bottles right under the
drains.  This proved impractical and individual drains were routed to the out-
side and leachate was collected in appropriately sized containers on the
volume of outflow.  Simultaneous readings of water level changes in class A
evaporation pan and in a grid of evaporation pans, same size as the rings,
gave the necessary evaporation corrections to be applied to the ring infiltra-
tion data.  Corresponding to each set of ring inflow and drain outflow data
(at 250 locations, Figure 5.2b) a set of wet density readings was taken (at
240 locations, Figure 5.2a) with the Troxler dual gamma probe, and a set of 35
Optocator^ readings (Figure 5.2c) was used to check for any swelling.  The
ultimate purpose of this study was to develop a capability to describe areal
distribution of hydraulic conductivity under field conditions and to  relate
it to tests performed in the laboratory on disturbed samples of clay liner
materials, or on undisturbed cores taken from the liner during construction.
The dilemma was that while the response of the liner as a whole was influenced
by preferential flow pathways, zones of discontinuity and zones of higher
effective porosity (Rogowski, 1988) point laboratory samples generally were
not.
                                      77

-------
                        Bubble Tube Open to Atmosphere

                          Rubber Stopper, removed when refilling

                         Rubber Stopper


                                       Siphon, removed when refilling
                                                             Infiltration Ring

                                                             Water Level

                                                              / Soil Surface
              MARIOTTE BOTTLE AND INFILTRATION RING ASSEMBLY
Figure 5.14.
              Schematic representation of constant head Mariotte bottle
              assemblage.
     Collection of infiltration, leachate and evaporation data (at locations
indicated in Figure 5.2) began immediately after ponding.  Initially, the data
expressed as flux in m/sec x 10~9, were collected on the daily basis with
subsequent transition to weekly and longer intervals.  Soon after the start it
became apparent that the infiltration rings and leachate drains next to the
sidewalls were responsible for much of the infiltration and drainage from the
liner.  Since these rings and drains were situated in a lower density zone,
which was compacted with jackhammer and a small vibratory roller, the higher
rates of flow were not totally unexpected.  The leachate from all drains near
the sidewalls was therefore isolated, combined into one, and measured
separately from the central matrix of 184 individual drains and rings which
represented the area compacted with sheepsfoot roller.  The sampling density
represented by the matrices in Figure 5.2 was on the order of 12,000 samples
per hectare (5,000 samples per acre) with the overall experimental liner area
of 209 m2 (- 0.05 acres).  Particular attention was paid to the scale of
measurement, the number of samples, and the representativeness of the values.


Average values —

     Figure 5.15 shows the changes in average liner bulk density from one
month after it was laid down and compacted (10/30/84) through ponding
(3/26/85) and finally draining of the liner on 7/23/86.  Figure 5.15 also
                                       78

-------
depicts the chronology of events.  A very  rapid  increase  in density after pond-
ing followed by a more gradual rise for  the  next 9  months was indicative of
progressive matrix saturation.  While  at the time of ponding average water
content was 18.1$ by weight, water contents  after the liner was drained and
covered with plastic averaged 18.5$.   Large  fluctuations  in density between
3/85 and 5/85 reflects probe malfunction which necessitated probe repair
(6/85-8/85), subsequently a gradual increase in  density continued through
first half of 3/86 after which the readings  stabilized.  The drains were
vented towards the end of 12/86.  Neither  the venting of  drains nor the addi-
tional measurements affected measured  density.   Fluctuations from 3/86 until
the end were only slightly larger than permissible  experimental error which
allowed standard count to vary within  ±  200  cpm  or  ± 8.7  kg/m3, or less
than 0.4$.  However, each such cycle was on  the  order of  the average change in
water content following ponding.

     Infiltration rings, because of the  their large number, had to be activat-
ed in stages.  Figure 5.16 shows the average infiltration rate during the
study period, and associated chronology  of the events.  Based on results
obtained from the barrel and caisson prototypes  infiltration into the compact-
ed clay was expected to be reasonably  slow - 1 x 10~9 m/sec or - 6 mfc/day for
a 30cm diameter infiltration ring.  Anticipating a  slow infiltration rate to
begin with, measurement using a modified hook gage  principle was tried to
bring and maintain water level inside  the  cylinders at the same level as the
water outside.  This was done as follows.  A sharply pointed metal pin was
inserted into the clay, its point level  with the water outside.  The volume of
water needed to just cover the pin was measured  as  the amount infiltrated
between sequential readings.  Since only a few millimeters change between the
readings was expected, it was felt that  differences in water level (Bower,
1963b) inside and outside the ring would not be  significant.  However, because
of the rapid infiltration in some rings, it  was  not possible to maintain high
    12/84  1/85 2/85 3/85 4/83 5/85  6/85 7/85 8/85 9/85 10/85 11/83 12/83  1/86 2/86 3/86 4/86 5/86  6/86 7/86
                                                                            7/23/88
Figure 5.15.   Average wet density measured with dual gamma probe before and
               after  ponding.
                                       79

-------
 2IOr
                                       (CHEMICAL
                                       INNER (184)
    3/85 4/85 5/85  6/85  7X85  8/85 9/85 10/85 11/85 12/85  1/86  2/86  3/86 4/86  5/86
                                      TIME
Figure 5.16.  Average ring infiltration rate during a one  year  study  period.
enough water level with this method and on 6/18/85 Mariotte  bottles  (Figure
5.14) were installed for all infiltrometers.  The Mariotte bottles maintained
a constant water level and were refilled to mark weekly.  This  procedure
worked fine until very low infiltration rates needed  to be recorded.  It was
difficult to measure accurately the small volumes of  water required  to bring
the bottle level up to mark.  At that time (9/11/85)  weighing of all bottles
was implemented.

     Originally the intention was to start enough rings to see  if hydraulic
conductivity of a clay liner could be calculated using Philip's (1957) method.
Initially, 35 rings were started at ponding, 7 of these were located near
sidewalls (Initial 7 in Figure 5.16) and had a high average  infiltration rate
which increased with time.  For the remaining 28 the  average infiltration rate
first appeared to decrease then to increase.  Subsequently,  a sump was install-
ed (6/85) and all outer drains including "Initial 7"  were allowed to empty
into it together.  By this time all rings had been activated, all were
equipped with Mariotte bottles and all were being measured individually.  The
average infiltration rate for the Inner 184 rings was somewhat  higher than the
average of the Inner 28 rings started initially.  The termination date for
data collection was 4/30/86.  Figure 5.16 shows when  the sump and drain vents
were installed, when chemical samples were taken, underdrains vented, and data
collection ended.  The word "Balance" signifies the time when infiltration
begun to be recorded by weighing.
                                      80

-------
     Figure 5.17 shows the average outflow rate observed  during the study.
The two curves-represent data for the Outer  66 drains along the walls and
Inner 184 drains in the center.  The distinction  between  the two is the extent
of compaction.  The Inner zone was compacted with a crawler tractor and sheeps-
foot roller, while a small vibratory roller  and jackhammer  were used in  the
Outer zone.  Values after 4/30/86 indicate what other studies were conducted
on the liner.  We attempted for example,  to  monitor infiltration rate by bounc-
ing a laser beam off a plate floating in  the ring as a function of time.  This
procedure also involved raising the water level inside the  rings about 10mm to
measure ring area.  Also during that time a  chemical sampling of the 250
drains was carried out to compare results with those obtained in December, and
Br~ tracer was used on selected drains  to evaluate distribution of break-
through time and to check for potential preferential pathways of flow.  Before
the liner was drained, fluorescein was  introduced into all  the rings to check
for leaks and nontoxic fluorescent water  color (Rich Glo3)  was added to mark
preferential flow pathways when the surrounding area was  cored.

     Figure 5.18 shows the inflow/outflow balance as a function of time for
the liner as a-whole corrected for evaporation.   The difference between the
two values is on the order of 10 x 10~' m/sec (I80x,/day), or a change in water
level equal to 0.086 cm/day, well within  experimental error of the instruments
used for monitoring inflow and outflow.
—150-
   3/85  4/85 5/85 6/85  7/85  8/85 9/85 10/85  11/85 12/85 1/86 2/86 3/86  4/86 5/86  6/86  7/86
                                      TIME
      Figure 5.17.  Average outflow rate during a one  year  study period.
     3fUch Art Color Co., Inc.1, Lodi, NJ 07644.
                                       81

-------
 220


 2OO
11OO

b
x 80
IU

£ 6O
   20
        k
    0 3/85 4/85' 5/85 ' 6/8S' 7/8S ' 8/85  9/85 10/88  11/85  12/85  1/86  2/86 3/t
Hi
! iii/INFLOW
                                                                       -END
                                                                        4/30/86
Figure 5.18.
      Average infiltration and outflow rates for a ponded liner as
      a  whole during the one year study period.
Gradient—

     In July 1985 (7/12-7/15) clay liner  elevations  in the center of each ring
on top of the sand layer were measured  (z),  the  level  of  ponded water was
taken as h2 and a permanent benchmark,  established  in  one corner of the flat
platform, became the outflow level h-| .  The  gradient i was computed for each
location (250) as,
                       i =  (h2-h1)/L =  (h2-h1)/[z-(a+b)]
                                                                  (5.6)
where a and b were taken as 2.54cm  (1") and  0.635  cm (1/4")  respectively to
correct for the thickness of the sand.  Schematic  representation of parameters
is shown in Figure 5.19 and areal distribution  of  gradient is given in Figure
5.20.
Density—

     Changes in bulk density as shown  in  Figure  5.15  suggest that following
the initial rapid increase in density  at  ponding,  the density increased only
gradually for the next nine months, becoming  essentially constant at about one
year following ponding.  Such changes  may be  due to water moving into and
through the clay since the net gain in density appears to be small compared to
data variability and the magnitude of  experimental errors.
                                      82

-------
     SCALE (cm)


       rSO
        -20
        -10
       L 0
             f
             b
                                             f-. '.''••".
"2
Figure 5.19.  Schematic representation of gradient  parameters

              for  compacted clay liner at Klingerstown,  Pa.
                               83

-------
                                                           N
12
                    24      36       48

                    DISTANCE,  feet
60
72
Figure 5.20.  Interpolated distribution of  hydraulic gradient
             over the study area.
                            83a

-------
     Prior to construction gravimetric soil water content averaged 16.3$
(Table 5.8).  Following compaction and ponding the average water content was
18.6$ by weight, was measured with an Eley volumeter (24 samples from 3
lifts), and an average adjusted (volume basis to weight basis) water content
of 19.2$ was measured radiometrically with a Troxler1  surface probe (108
samples from 3 lifts).  Coincident measurements of the dry density in the
backscatter mode averaged 1655 kg/m3.  Just after the ponded water drained,
gravimetric water content of the clay, based on 55 Veihmeier tube samples was
20.9$.  Subsequently 3" and 2" cores were taken.  Corresponding average water
content and dry density of 3" cores (240 samples) and 2" cores (45 samples)
was very similar to values observed before ponding.  These figures suggest
that values of 1660 kg/m3 and 18.8$ by weight could be taken as the average
dry density and water content, respectively for the compacted clay liner.
When the liner was sampled with the Veihmeier tube just after the ponded water
was drained off the surface, some water still accumulated in the holes left by
the Veihmeier tube, suggesting incomplete drainage from the body of the clay.
This may account for somewhat higher values of water content (20.9$ by weight).
Assuming the figure of 20.9$ is real results (including standard deviations)
in Table 5.8 suggest a possible increase in bulk density due to ponding of at
most [(0.209 + 0.022) - (0.186-0.018)] x 1660 = 105 kg/m3.  Table 5.9 shows
that the differences between "prepond" and "one year" values are indeed less
than that figure (60 kg/m3).
           TABLE 5.8.  AVERAGE VALUES OF DRY BULK DENSITY AND WATER
                               CONTENT BY WEIGHT

                  Time               Dry Density      Water Content


                                        kg/m3            % by wt

           Before construction
             • Veihmeier tube           Loose           16.3 ±0.9*

           After construction
             • Volumeter                                18.6 ±1.8
             • Surface probe           1655±58          19.20±1.21

           After drainage
             •Veihmeier tube                            20.9 ±2.2*
             •3" cores                 1684±73          18.5 ±1.0
             •2" cores                 1643+63          18.7 ±0.6

           Average1                     1660+65          18.8 ±1.2
            Excluding starred *values.
                                      84

-------
THIS PAGE INTENTIONALLY LEFT BLANK

-------
    TABLE  5.9.   SELECTED STATISTICS FOR THE DENSITY DISTRIBUTIONS BEFORE
                     AND AFTER THE CLAY LINER WAS PONDED	
    Time
Mean
SD
Median
                                                        Mode
Range
                                            kg/ra3
Prepond
2 days
10 days
1 month
3 months
6 months
9 months
1 year
2183
2211
2214
2217
2220
2234
2244
2243
83
87
85
85
84
85
84
83
2181
2212
2220
2223
2219
2232
2244
2237
2189
2212
2193
2248
2145
2232
2187
2260
480
496
429
499
432
442
423
387
     The data in Table 5.9 represent average density statistics at specific
times after ponding based on the dual gamma probe readings, while Figure 5.21
shows an example of associated spatial distributions.  The results for
gravimetric samples in Table 5.8 represent water content and density
essentially at a point.  Surface probe samples are based on backscatter and
thermalizing of neutrons by water molecules in the vicinity - 0.4 cu ft (0.01
m3) of emitter.  Dual gamma probe data are based on the degree of attenuation
of gamma radiation between the source placed in the bottom horizontal tube and
the detector placed exactly 30cm (11) above in the second horizontal access
tube at the clay surface.  Density was computed by comparing observed counts
with the standard counts for material of known density.  Figure 5.6 shows the
contrasting geometries and Figure 5.22 gives an example of standard count
distribution.  The dual probe measurements of density were taken continuously
at 240 locations following the clay liner construction, through ponding, until
it was drained.  Tables 5.10 and 5.11 and Figures 5.23 and 5.24 show the type
of data which are given in detail by Appendix B (individual readings) and
Appendix C (statistics).

     Figure 5.23 gives the distribution in time of individual changes in bulk
density for the sites #M4, 14, G4 and J4 between consecutive dates, while the
dashed line shows a range of variability due to differences in the standard
probe counts.  Positive and negative changes in density suggest alternate
filling and draining of pores where the density was being measured.  Values
within the dashed lines could be a result of variation associated with the
standard counts, those which are lower or higher may be a measure of empty
pores or pores filled with percolating water.  Figure 5.24 contains
information, similar to that in Figure 5.23, except that individual changes  in
density are accumulated over time.  Again, the values are for only four (M4,
14, G4, and J4) of the 240 sites.  The dark hatched areas describe net deficit
and the light colored ones suggest surplus.  The figure is similar to Figure
5.15 where average distribution of density over time is shown.  For these four
sites, initial deficit  (because of liner drying) became a surplus after
ponding.  However, the net change in density (relative to 0-line) between
construction and ponding amounted to -2 kg/m3 for M4, and +85, +10 and +36
                                      85

-------
                        12     24     36     48

                               DISTANCE,  feet
        Figure 5.21.
Interpolated contours of density two days (top),
one week (middle), and one month (bottom) after
ponding.
kg/m3 for sites IM, G4 and JU.  Despite the net gain, the pattern among other
sites is quite similar suggesting that draining and filling of pores within
the clay may well be the way water moves in compacted matrix.   Figure 5.25 (a)
through (h) shows spatial distribution of density for the same times as given
in Table 5.8 (i.e., prepond, 2 days, 10 days, etc.).  The density in the
center of the platform appears to increase with little change elsewhere.  In a
gross sense the initial change between "preponded" and "2 days" plots may
represent initial filling up of the larger cracks and conduits with ponded
water.  Subsequent increases would denote the movement of water into the
compacted clay matrix.  It should, however, be emphasized that observed
changes were very small.  Because the dual gamma probe "sees" a relatively
small cross section of the clay matrix, the changes and fluctuations observed
on a daily basis may actually represent alternate filling and draining of the
                                      86

-------
          STANDARD  COUNTS  :   DENSITY
            D I FF
            1000-
                                Probe Repair
-800-
1000-

I

'i ' ' ' ' ' i '"' ' '•' 	 r ' • 	 ' • '" r 	 i 	 ' • ' '
0 go 120 180 240 300 360 420
                      READING DIFFERANCE
           Figure 5.22.
Distribution of standard counts for the
dual  density probe with time.
soil  mass, especially since some results discussed previously suggest that.
little if any change in density and water content of  the liner occurred during
the time it was  ponded.

     A question  may be raised regarding the adequacy  of the standard count
procedure used.  Standard counts were taken at either end of each access tube
pair.  If the results did not agree to within ± 200 counts the entire set of
readings (10) was repeated. Consequently we have a fair amount of confidence
in these values  and think that alternating fluctuations in observed density
are real and represent a realistic picture of transport in the slowly perme-
able  structured  porous media.
                                  87

-------
TABLE 5.10.  INDIVIDUAL VALUES OF BULK DENSITY OBTAINED USING DUAL
         GAMMA PROBE ON 9/25/85 (6 MONTHS AFTER PONDING)
Bulk Density

A
B
C
D
E
F
G
H
I
J
K
L
M
N
0
P
Q
R
S
T
U
V
w
X
0
2099
2182
2248
21 54
2108
2208
2177
2154
2118
2134
2116
2149
2203
2186
2148
2167
2053
2202
2116
2243
2133
2146
2161
2275
1
2158
2218
2322
2228
2148
2349
2390
2223
2334
2243
2232
2232
2296
2291
2258
2259
2087
2255
2244
2347
2229
2287
2241
2414
2
2134
2193
2333
2258
2194
2331
2391
2237
2326
2245
2252
2202
2265
2157
2259
2148
2099
2226
2204
2328
2240
2250
2160
2332
3
2066
2222
2222
2289
2243
2299
2416
2301
2441
2398
2295
2278
2283
2183
2301
2076
2166
2280
2205
2360
2272
2214
2210
2235
4
2128
2235
2229
2273
2223
2337
2458
2307
2440
2411
2343
2270
2276
2238
2337
2118
2232
2316
2257
2265
2316
2221
2276
2201
5
2130
2192
2181
2243
2239
2303
2373
2270
2381
2382
2363
2359
2244
2305
2280
2098
2221
2399
2284
2249
2342
2320
2246
2216
6
2138
2136
2209
2199
2209
2275
2362
2157
2443
2374
2393
2321
2241
2236
2238
2167
2193
2316
2319
2264
2288
2291
2214
2195
7
2123
2104
2177
2154
2082
2183
2267
2156
2318
2386
2349
2188
2217
2185
2207
2214
2212
2299
2314
2188
2282
2235
2167
2205
8
2016
2139
2202
2124
2064
2186
2196
2278
2322
2431
2273
2220
2262
2248
2255
2289
2256
2277
2334
2220
2262
2232
2303
2195
9
2126
2120
2156
2095
2026
2094
2080
2178
2205
2266
2162
2153
2198
2174
2143
2229
2174
2185
2198
2241
2225
2145
2099
2213
                                88

-------
TABLE "5.11.  SUMMARY OF STATISTICS FOR 9/25/85 BULK DENSITY DATA  (6 MONTHS AFTER PONDING)
Moments
Quantiles
(def-4)
Extremes

N
Mean
Std dev
Skewness
USS
oo CV
<£>
T-mean-0
Sgn rank
Hum - 0
240
2231.5
85.7879
0.190179
1200076591
3.83921
103.515
11460
210
Sum wgts
Sum
Variance
Kurtosis
CSS
Std mean
Prob>| T
Prob>| S

240
536280
7359.56
-0.140961
1758931
5.53758
0.0001
0.0001

100} max
79* Q3
50* med
25 % Q1
Q% min
Range
Q3-Q1
Mode
2158
2288.5
2232
2177.25
2016
112
111.25
2232
99*
95?
90$
10*
5*
1*


2442.18
2390.95
2348.8
2124.2
2098.05
2037.07


Lowest
2016
2026
2053
2064
2066


Highest
2431
2440
2411
2443
2458



-------
        >
        Ul
        Q
        in
        UJ
        u
        z
        LJ
        o:
        UJ
        IL
        u_
NET
                FEB MAY  AUG NOV FEB MAY AUG  FEB MAY AUG NOV FEB MAY  AUG

                85  85  85  85  86  86  86   85  85  85  85  86 86  86
                         TIME
                                                  TIME
Figure 5.23.
Net change  in density for  consecutive readings at the
site M#4, G#4,  I#4, and J#4,  plotted as functions of
time,  dashed lines indicate  possible extent  of the
error  of measurement (z 8.7  kg/m3).
                                   90

-------
(/>

I
2
V)
UJ
O
Ul
LJ
             100

             80

             60

             40

             20

              0

            -20

            -40

            -60
          3


          O
                    «  I
                               M4
                                                             t  'M

                                                                '
                                                         14
100
80

60
40
20
0
-20

-40
1 ) "
1 ji
i 1' \
' A • A
I'' nl 1 \ A
1 i / « IAJ ?!i
," / ' y ' "V
!U ' • i '
U/! '
' 1 1! i1
' f J
nr i r
ii Ml l!
ij!'|
*f!
64
i i i i i i i








-
, ! -
) '

| f ji Ijij/iMiM^
yjf/lllll
JJI fl
1 ? J 4

FEB MAY AUG NOV FEB MAY AUG FEB MAY AUG NOV FEB MAY AUG
85 85 85 85 86 86 86 85 85 85 85 86 86 86
                         TIME
                                                   TIME
Figure 5.24.  Cumulative change in density at  the  sites M#4, I#4, G#4,
              and  J#4,  plotted as functions of  time,  each value (•)
              has  an associated uncertainty of  ± 8.7  kg/m3.
                                   91

-------
LESS THAN 20OO


2001 TO 2100
                 I 2101 TO 2200
                                              2201  TO 2300
                                              2301 TO  2400
                            ABOVE 2400
       Figure 5.25.
   Spatial distribution of dual probe density values
   (kg/m3) before ponding (a),  and 2 days (b), 10
   days (c),  1  month (d), 3 months (e), 6 months (f),
   9 months (g),  and 1  yr (h) after ponding.
Inflow and Outflow—

     Inflow rate was measured with a battery of 250 cylinder infiltro--ters
within a ponded liner.   Each galvanized metal ring infiltrometer was hall
covered with a concrete block to minimize evaporation, and a plastic 12,
Mariotte bottle was used to monitor infiltration.   Design specifications
called for 279.4mm diameter infiltration rings (11") to give a ring area of
613.116cm2.  To see how accurate ring areas were,  water level in each ring was
raised by adding a known weight of water and the height of the raise was
measured with laser beam Optocator1 .   The ring area was then calculated for
each ring and appropriate correction was applied to each cylinder
infiltrometer.
                                      92

-------
     The 66 perimeter rings and drains  were routed  separately to a sump and
excluded from consideration because of  the lower  compaction and possible wall
effects discussed earlier.   To check the  integrity  of  the inner 18H rings,
fluorescein was introduced  into the rings at  the  conclusion of the study and
the surrounding ponded water was observed for leaks.   Of the 18M rings that
were checked individually U3 showed no leaks,  31 showed minor or very slight
leaks, and only 10 appeared to have major leaks.  Figure 5.26 shows relative
distributions of rings with leaks.   Under standard  operating conditions in
                     O  I   23456  789
A
B
C
D
E
F
G
H
I
J
K
L
M
N
0
P
Q
R
S
T
U
V
w
X































A



A


X

4

<5
<^

<














X







<£
X



X





^
A

A










<§
X


X

^F













A



A




X







A










A

^

-------
slow flowing rings, and when water in the liner and the ring was maintained at
approximately the same level, effect of small leaks would have been relatively
minor, however, in the fast flowing rings and where large differences in head
between the cylinder and the water outside occur the error could be consider-
able (Bouwer, 1962).  In general, we would expect such rings to overestimate
flows.  Table 5.12 compares average infiltration rates obtained for selected
dates.  There appears to be little difference whether or not a ring area and
leaking ring corrections were included or not.  If leaking rings are omitted
from computations a somewhat higher (rather than lower as expected) average is
obtained (27 vs 23 x 10~9m/sec).  The most significant effect seems to be the
reduction of variance from 9.1 to 2.7 x 10~17 (m/sec2).  Computations of
statistics given in Appendix C are for ring sets from which leaking rings have
and have not been omitted.  In this report only nonleaking rings are used in
computations.

     No such problems existed with outflow data.  However, as a preventative
measure drains next to the wall (66) were excluded from computations to
eliminate possible wall effects.  The outflows from these drains were also
physically separated from the rest by having a bead of Vol-Clay1—a bentonite
material placed between them and remaining drains on. the floor of the struc-
ture (Plate 5.2).  Each column (10) of drains, running south to north, was
separated from the one next to it by a raised portion (- 6mm) of the density
access tube buried in the concrete base of structure.  The drains were assumed
to drain an overlying block of compacted clay 0.9m (3') on the side and 0.3m
(1') thick.  Since however, there were no partitions between such blocks, hori-
zontal and diagonal flows within the clay could have occurred.  Burlap and 3mm
sand covered the level platform under the clay, and preferential flow to some
drains within this layer, although unlikely, cannot be completely ruled out.
The assumption under which the results are analyzed is that infiltration rates
are represented by ring inflow rates and outflow flux for the 3* x 3' blocks
is given by the drain outflow.  Reported variability is assumed to be a func-
tion of soil properties as well as the spatial distribution of the preferen-
tial flow pathways within the experimental structure.
    TABLE 5.12.  AVERAGE INFILTRATION RATES FOR SELECTED TIMES UNCORRECTED
           (ALL) AND CORRECTED FOR RING AREA  (AREA CORRECTION) AND
                       LEAKING RINGS (LEAK RINGS OMIT)	
    Time
    All
Area Correction
Leak Rings Omit
    3 months
    6 months
    9 months
    1 year

    AVG
   15.37
   31.86
   31.29
    5.29

23.56±9.55
    x 10~9 m/sec

     15.51
     31.96
     31.17
      5.31
  24.03±M.17
     16.39
     37.05
     37.2H
      6.41

  27.15±5.22
                                       94

-------
     Initial infiltration — Philip (1957) suggested that when water is ponded
on a deep and homogeneous soil with a uniform initial water content infiltra-
tion (I) in millimeters is given by


                               I = St1/2 + At                           (5.7)


where t is the time in seconds, S is the sorptivity, and A is a parameter
related to the saturated hydraulic conductivity (Ksat)


                                A = 1/3 Ksat                            (5.8)


When equation (5.8) is written as,


                                  2 = S + At1/2                         (5.9)
a linear regression fit gives S as the intercept and A as the slope of the
straight line segment.  This approach has been routinely used, i.e., by Sharma
et al., (1980) for field determination of sorptivity and conductivity values.

     In our study water was ponded on reasonably homogeneous material derived
from the same subsoil horizon which had been brought to a uniform water con-
tent and compacted to a uniform density.  Although the clay layer was not deep
in the strict sense of the word (0.3m), it was assumed to be sufficiently
thick because of low expected values of hydraulic conductivity (1 x 10~9
m/sec).  The initial portion of the infiltration curve following ponding (here
5 hours) was fitted with a linear regression and the values of S, A, and Ksat
were estimated.  The estimated values of Ksat were corrected for the appropri-
ate infiltration ring area and for local gradient and expressed in terms of
flux q for 23 out of the 35 infiltration rings that were started initially.
Figure 5.27 shows the results for the site 11 and Table 5.13 gives the comput-
ed values of sorptivity (S), A-value, and saturated hydraulic conductivity
(Ks) for the 23 rings.  The last two columns give hydraulic conductivities for
the same locations based on the full length of record for the inflow and
outflow, respectively.  Statistical analysis values of Ks estimated using
Philip's method were significantly higher (at better than 1/J) than hydraulic
conductivities based strictly on ring or drain data which were not significant-
ly different from one another (t > 0.5).

     Flow at a point — Figures 5.28 and 5.29 a and b illustrates inflow and
outflow behavior in time at four selected points on a platform along with
associated values of bulk density on either side of a particular ring-drain
location.  Compared to the averages in Figures 5.16 and 5.17, individual
observations in Figures 5.28 and 5.29 show much greater variation.  The flux
in rings and drains at location A3 (Figure 5.28a) was quite different from
that at F1 (Figure 5.29b) varying greatly in time.  At sites N8 and H5 fluxes
were quite similar although both varied extensively in time, while at the site
F1 , a location that also showed a very slight ring leak, there was hardly any
flux at all.  Results illustrate the observed ranges in variability both
spatially and in time.
                                      95

-------
        u
        0
       IO


        ,0


       2
        4-
        X
2.13


   2
           0.61
                   PHILIP (1957) METHOD

                        SITE  No. 11
                                               o.


                                             CP°-
                                                    &>
                                                  cfP
             0L_LJ-
                        	I  I  I I  I I  I
                             1000
                                  2000
                                 tl/2sec
Figure 5.27.  Illustration of Philip's (1957) method for calculation

              of sorptivity S, and A-values.
                                 96

-------
 TABLE 5.13.  SORPTIVITY, A-VALUES, AND SATURATED HYDRAULIC  CONDUCTIVITY  BASED
     ON  INITIAL  (1000  SECS)  INFILTRATION RATES FOR  SELECTED1  DOUBLE  RINGS
                (613 M2 AREA  INFILTRQMETERS USING PHILIP'S  (1957)  METHOD)
Site
        Slope
Intercept
Ks-430I     Ks-4300

C1
C3
C5
C7
C9
FO
F2
F4
F6
F8
11
15
19
LO
L6
L8
01
05
09
RO
R4
R8
U9
cm^/sec i
.00135
.00162
.00116
.00160
.00600
.00530
.00121
.00178
.00185
.00129
.00152
.00216
.00327
.00470
.00145
.00155
.00128
.00169
.00575
.00062
.00042
.00028
.00065
CM3/3eo1/2
1.90
1.60
1.48
2.00
1.00
1.60
1.41
1.05
1.20
1.20
0.61
0.66
1.33
2.48
0.55
0.65
0.58
0.13
0.40
0.96
0.37
0.32
0.05
cm/sec1 /^
.00310
.00261
.00241
.00326
.00163
.00261
.00230
.00171
.00196
.00196
.00099
.00108
.00217
.00404
.0009
.00106
.00095
.00021
.00065
.00157
.0006
.00051
.0008
x 10""9 cm/ sec x 10~9 n/sec
22.02
26.42
18.92
26.10
97.86
86.44
19.74
29.03
30.17
21.04
24.79
35.23
53.33
76.66
23.65
25.28
20.88
27.56
93.78
10.11
6.85
4.485
10.60
66
79
56
78
293
259
59
87
90
63
74
105
160
230
70
75
62
82
281
30
20
13
31
6
4
6
74
-
-
1
67
6
5
8
33
-
-
10
13
4
9
-
-
1
6

11
9
1
83
-
-
6
30
23
14
3
79
-
-
31
24
8
2
-
-
1
32

1 There were insufficient data on sites 13,  17,  L2,  L4,  03,  07,  R2,  R6,  U1,  U3,
 U5, U7, to warrant computation.
                                      97

-------
                            RNG DRAIN A3 DENSTTY AA3 A3
  500

  460

  400

  360

? 300

S 260

J 200

  150

  100

  50
                                                               [2500

                                                                2400

                                                                2300

                                                                2200

                                                                2100

                                                                2000

                                                                1900

                                                                1800

                                                                1700

                                                                1600
         NOV84  FEB86   MAY85  AUQ85  NOV85  FEB86  MAY86   AUG86  NOV86
                                                                1600
                           RING DRAIN N8 DENSITY M8 N8
 500

 450

 400

 360
              //^j^^
2600

2400

2300

2200

2100

2000

1900

1800

1700

1600
        NOV84   FEB85  MAY8S   AUG85  NOV85   FEB86   MAY86  AUG86  NOV86

                                    b
                                                                1600
Figure  5.28.
            Ring  inflow rate  (R),  drain outflow  rate  (D)  and
            associated bulk density distribution to  the  east  (Dg)
            and west  (D^)  of  the ring-drain,  for the  sites A3  (a),
            N8  (b).
                                     98

-------
                          RMQORAM H5 DENSITY GS H5
       600

       460

       400

       360

       300

       260

       200
                                            2600

                                            2400

                                            2300

                                            2200

                                            2100

                                            2000

                                            1900

                                            1600

                                           -1700

                                            1600
                                                            1600
                     MAY86  AUQ66  NOV66   FEB66  MAY86  AUQ6B  NOV86
600
460
400
360
I"
2 260
2 200
«o-
WO
60-
o-
NO
RMQDRAN F1 DENSITY El F1
0E
^ A y^\^"^5^»\/ \$^f*'K!tfi^\f*sr\^





R
V04 FEB66 MAY66 AUQ66 NOV86 FEB66 MAY66 AUQ86 NOV
2600
2400
2300
2200 5
* 2100
2000
- 1900
- «oo z
- 1700
- 1600
- 1600
66









b 	
Figure 5.29.
Ring  inflow rate (R),  drain outflow rate (D)  and
associated bulk density distribution  to the east
(DE)  and west  (Dy) of  the ring-drain,  for the
sites H5 (a),  F1  (b).
                                  99

-------
     In Tables 5.14 and 5.15 selected statistics for particular days after
ponding are given for the raw and log-transformed ring and drain data.

     Figures 5.30 and 5.31 show a comparison of hydraulic conductivity distri-
bution computed from ring and drain flux at 3, 6, 9, and 13 months (1 yr)
after ponding.  Although quite similar at 3 and 6 months, infiltration and
outflow appear different at 9 months and 1  year time, suggesting that reliance
on a one time set of infiltration measurements as a criterion of liner quality
may not be adequate.  However, it is the outflow, the flux out of the lower
bottom that appears to be the best descriptor of clay liner performance
because it shows what actually gets through the liner.  This, of course,
causes a dilemma since under natural conditions 1m (or more) thick liners
should take a long time to equilibrate.

     Finally, Figure 5.32 shows a comparison of hydraulic conductivity distri-
butions computed from time averaged ring infiltration and drain flux.  The
agreement between the two appears considerably better and the distribution of
values are closer to what was observed in practice.  Statistical comparisons
showed that the ring inflow and drain outflow averages were not significantly
different.  However, ring inflows and drain outflows were significantly dif-
ferent at 3, 9, and 12 months following ponding.
       TABLE 5.14.  SELECTED STATISTICS FOR THE HYDRAULIC CONDUCTIVITY
         DISTRIBUTIONS IN TIME COMPUTED FROM NONTRANSFORMED (a) AND
     LOG-TRANSFORMED (bl RING INFILTRATION DATA FOR THE PONDED CLAY LINER
          Time
Mean
 SD
Median
           Mode
           Range
         2 days
        10 days
         1 month
         3 months
         6 months
         9 months
         1 year
         2 days
        10 days
         1 month
         3 months
         6 months
         9 months
         1 year
  30
  19
  37
  13
  30
  29
   5
3.33
2.95
3.14
2.57
2.47
0.70
1.65
                                (a) x 10"? cm/sec
  25
  32
  62
  19
  53
  64
  15
   28
    2
   12
    3
    7
   <1
    0
                               (b)  log-transformed
0.73
 .40
 .43
 .48
 .80
 .74
  3.36
1.95
   .17
   .08
   .89
   .74
 -0.27
  1.90
3,
3.
2.
2,
            0
            0
            0
            0
            0
            0
            0
 1.62
 0.65
 0.36
•3.37
 1.99
•3.39
-2.42
             93
             98
            144
             76
            334
            267
            114
 ,91
 ,93
 ,91
 ,70
8.14
9.03
7.17
                                      100

-------
TABLE 5.15.  SELECTED STATISTICS FOR THE HYDRAULIC CONDUCTIVITY
  DISTRIBUTIONS IN TIME COMPUTED FROM NONTRANSFORMED (a) AND
LOG-TRANSFORMED (b) DRAIN OUTFLOW DATA FOR THE PONDED CLAY LINER
  Time
               Mean
            SD
          Median
Mode
Range
  2 days
 10 days
  1 month
  3 months
  6 months
  9 months
    year
1
                        (a) x 10~9 cm/sec
2 days
10 days
1 month
3 months
6 months
9 months
1 year
2
8
12
11
21
28
17
6
10
21
21
39
38
23
0
5
<1
<1
4
11
9
 0.69
 1.56
-0.48
-1.85
-0.31
-0.43
 1.86
                       (b) log-transformed
                         2.27
                          .38
                          ,89
                          .79
                          ,86
                          ,88
                                                    0
                                                    0
                                                   10
                                                            43
                                                            45
                                                           127
                                                           129
                                                           238
                                                           165
                                                           173
1.66
1.73
1.76
-2.80
-4.75
1.35
2.36
2.05
-2.89
-2.69
-2.81
-4.76
-4.75
- -4.75
2.29
6.68
7.61
7.82
9.79
10.34
9.93
8.83
                          101

-------
              PNG
              ji-
     0.00 TO 1.00
    -rt.oi TO 10.00
     1 IO.OI TO 25.OO
     125.01 TO 50,00
     I5O.O) TO IOO.OO
     lABOVE IOO,OI
                                                    DRAIN
3 MONTHS
                                           6 MONTHS
Figure  5.30.   Comparison of hydraulic  conductivity distributions computed
                from  (ring) inflow and  (drain)  outflow  at 3 months and  6
                months.
                                         102

-------
              RING

                 1
      OOO TO 1.00

   ||t 1,01 TO 10,00

     110.01 TO 25.00

     125,01 TO 50.00

     150.01 TO 100.00

     I ABOVE 100.01

                                                     DRAIN
                             9 MONTHS
                                          I YEAR (13 MONTHS)
Figure  5.31.
Comparison of  hydraulic conductivity distributions computed
from  ring inflow and  drain outflow at  9  months  and 1 yr  (13
months).
                                         103

-------
             SUMMaOHNQ
                                            SJM0430ORAN
                                        la      a

                                         aoo TO i oo

                                        111-01 TO (0.00

                                         110,01 TO 25.00

                                         I25.OI TO 50.0O

                                         150,01 TO lOO.OO

                                              100.01
  Figure 5.32.
Comparison of hydraulic conductivity  distributions computed
from ring inflow and drain outflow  averaged over time
(6/27/85 to 4/30/86).
Tracer Studies—

     Tracer studies were initiated at the conclusion of the main experiment.
To prepare the tracer, 1 gram molecular weight of  KBr (119.0 g)  was dissolved
in 1L of water to give 1M solution of Br~ (79.9  g/L).  Either 50 or 100mS, of
this solution were diluted with ponded water  to  2000mX, and added to 15 rings
(Figure 5.33) in one, two, or three 2000mS,  increments depending  on the
hydraulic flux rate and expected times (Table 5.16).   At the time tracer
solution was applied to rings initial (time =0) samples of leachate from
underlying drain and 8 (or 5) surrounding drains were taken.  Sampling of
leachate was continued at suitable intervals  depending on the volume of
accumulated outflow.  Leachate samples were analyzed for Br~ concentration
using Orion1 Model 9435 bromide electrode,  and Orion1 Model 407A specific ion
meter, and Orion1 double junction reference electrode mode 90-02.  Ion
specific bromide electrode allows simple and  rapid measurement of free Br~
ions in aqueous solutions.  General experimental procedure and detailed
results for each cluster of drains are given  in  Appendix D.  Figure 5.34
illustrates the format of data in Appendix  D  data.  Results are presented as
log-|Q pulses of relative concentration (C/Co) at indicated times in hours
after critical application.  Relative concentration values less than 10"1* are
not reliable and are included here to indicate primarily the first arrival
times at a location, while the pulse  (10~6) at time = 0 denotes the starting
time for each run.
                                      104

-------
                OUTFLOW
                TRACER
Figure 5.33.
Location of 15 infiltration rings and respective
sampling areas (shaded) to which 1M Br~ solution
had been added.
                          105

-------
TABLE 5.16.  AMOUNTS OF 1M BIT1  DILUTED TO
 2000MS, AND APPLIED TO RINGS IN 1 , 2 OR 3
   (USED) INCREMENTS OF 2000MH;  APPLIED
 CONCENTRATION (CO) IN PPM AND GRAMS (G)

Ring     1M Br~     Used          Co

AA7
A3
D7
F1
G5
JO
L3
M?
01
09
05
S1
T5
V8
X3
mi
100
50
100
50
100
100
100
50
100
100
100
100
100
100
50

1
1
2
1
1
1
1
1
1
1
1
1
2
1
3
ppm
4000
2000
4000
2000
4000
4000
1000
2000
4000
4000
4000
4000
4000
4000
2000
g
8.0
4.0
16.0
4.0
8.0
8.0
8.0
4.0
8.0
8.0
8.0
8.0
16.0
8.0
12.0
                    106

-------
             0


            -I


            -2
          o
         u
         H  -3
         o
         O
             -5
             -6
                                                 AA6
                                                JL
                                    J.
                       50     100    150    200    250

                              CUMULATIVE  TIME
                                           3OO
      Figure 5.34.
Logarithm (base 10)  of relative  (C/Co) breakthrough
concentrations of Br~ pulses in  hours at a particular
drain (AA6) and arrival times after  applying Br~
tracer to central ring (AA7).
     Water and tracer breakthrough—Tracer  tests with Br" were carried out
towards the end of the study,  while water breakthrough times, given as first
arrival of water at the respective drains,  were recorded immediately following
ponding.  Bromine was chosen as a tracer because of  its conservative behavior
and low background concentrations. Although anion exclusion and Br~ reactions
with positively charged portions of the clay matrix  may affect tracer
movement, short-circuiting flows through the macropores should be relatively
free of these considerations,  ether because the flow is more rapid, or because
the size of transporting pores is larger then pores  in the clay matrix.

     Tracer breakthrough, given as the first arrival of tracer at the princi-
pal drain or one of the surrounding drains, originated from a centrally
positioned, 600-cm2 infiltration ring.  Water breakthrough, however, was a
result of ponding the entire facility, and  outflow from a 8,000-cm2 area sur-
rounding each drain.   In either case, the clay liner was not fully saturated.
Initial water content distribution corresponded to a 100kPa tension, while
water contents after  the water was drained  were no more than 3% higher
                                      107

-------
throughout.   Under these conditions, observed breakthrough times would most
likely be a result of short-circuiting flow through the macropores.

     Figure 5.35 shows histograms of water and tracer breakthrough data.   The
histogram in Figure 5.35a gives  the distribution of breakthrough times for
water, which is represented by substantial frequencies in all classes.
However, breakthrough times for  tracer (Figure 5.35b) are heavily skewed and
primarily confined to one frequency class.  Figure 5.35 a and b illustrates
relative concentration (%) of Br" in the leachate as a function of cumulative
time (hrs) for drains underlying the rings to which tracer was applied.

     In Figure 5.36 breakthrough times for water and interpolated breakthrough
times for tracer are presented as mosaics of respective distributions.
Numerical values for both fall within a similar range.

     A constant water level was  maintained over the clay following ponding.
Preliminary calculations showed  that, with assumed flux (q) through the clay
matrix on the order of 1  x 10~9  m/sec, water should take as long as 10 years
           o
          O
          O
 10.0

  0.1

0.001
                                          a.
-A7
 A6
                 0    100    200   300    0    100    200
                               CUMULATIVE  TIME (hrs)
                                               300   400
          O
          ~ 0.001
                 0    100
                200   300    0     100   200   300   400
                   CUMULATIVE TIME (hrs)
       Figure 5.35.  Relative concentration of  Br~  in  leachage AA7 and
                     surrounding drains (a),  and from  A3  and surrounding
                     drains (b).
                                      108

-------
                20  -
                       0     200            0      300

                              B-T  TIME, hrs
     Figure 5.36.
Frequency histograms of breakthrough times (B-T time)
for water (a)  and  Br~  (b).
to pass through  the experimental 30-cm-thick clay liner.  Since considerably
faster flow rates  and breakthrough times were observed experimentally at
several locations, it was concluded that short-circuiting flow was taking
place through a  few relatively larger continuous pores in the otherwise slowly
permeable clay matrix.  In contrast, Br" tracer appeared to move only through
that portion of  the profile that was directly influenced by a spiked ring.
The head in each ring was controlled separately.  Tracer would have to diffuse
into the clay matrix if the infiltration ring was not situated directly over,
or close to a macropore.  Consequently, tracer flow would be far less
sensitive to overall hydraulic gradient in ponded water and more sensitive to
local conditions associated with each ring.

    Water breakthrough times on the average appear to be longer than those for
tracer, possibly because of initial radial diffusion of water from macropores
into the adjacent, unsaturated clay matrix.  Actual tracer breakthrough may
                                     109

-------
well be faster still, since Br~ breakthrough distribution was determined in
wet soil.  Under these conditions tracer flow could lag behind due to displace-
ment of tracerless water ahead of the infiltrating solution.

     Effective porosity—In Table 5.17  laboratory values of hydraulic
conductivity measured on selected 9cm diameter cores are given along with
average flux density values based on inflow and outflow.  These cores were
taken within each infiltration ring.  Laboratory hydraulic conductivity was
determined using a flexible wall permeameter,  and with a gradient of about 20.
Results illustrate the extent of discrepancies possible between field and
laboratory determinations.
                    N       DO to 1   fil to 3
                            113 to 7   HMore than 7
                                1U Missing
         Figure 5.37.
Distributions of breakthrough (first arrival)
time (days) for water (a) and Br~ tracer (b)
in compacted, spatially variable clay liner.
                                      110

-------
TABLE 5.17.  LABORATORY VALUES OF HYDRAULIC CONDUCTIVITY1
  COMPARED WITH AVERAGE2 FIELD VALUES OF RING INFLOW AND
                      DRAIN OUTFLOW

                                      Field
 Site          Lab        Ring inflow      Drain ouflow
                                  x 10~9 m/sec
Al
A2
A3
A4
A5
A6
A7
C2
C5
C7
E3
F1*
F3
G2
G5*
G6
H5*
12
J1
K6
N1
N7
S7
T2
V5
W1
Average
1.1
2.2
5.9
1.7
2.6
2.0
0.4
1.7
1.8
2.7
1.5
1.0
0.8
2.6
4.2
2.2
1.2
0.5
1.1
1.2
0.9
1.2
0.8
1.5
2.4
0.8
1.8±1.2
40.1
59.5
235.2
215.5
155.0
85.7
4.0
4.7
6.8
97.8
7.0
0.1
0.4
0.7
43.4
95.9
20.0
0.3
10.8
43.4
19.5
155.4
0.3
1.1
1.7
9.3
50.5±69.2
164.4
99.1
105.7
140.9
149.2
41.8
98.4
0.1
0.6
109.4
0.0
2.2
0.6
0.6
40.8
33.7
30.0
0.3
0.8
39.9
11.8
62.0
4.5
0.4
18.3
12.0
44.9±53.2
1 Laboratory values obtained using flexible membrane
 hydraulic conductivity apparatus.

2Field values are for the "430" data set in which total
 inflow or outflow per unit area for the period of
 6/11/85 to 4/30/86 was divided by total elapsed time.
                            Ill

-------
     Based on laboratory values of hydraulic conductivity breakthrough times
(Table 5.18), for a 30-cm-thick clay layer should be several years.  Even if
larger inflow or outflow rates such as those in column 3 and 4 of Table 5.18
were used in calculations, breakthrough times of 336 and 552 hours,
respectively, would be expected.  Consequently, the considerably shorter break-
through times observed for water and tracer suggest relatively low effective
porosity.  Table 5.18 gives computed values of effective flux density (qe),
observed breakthrough times, and relative amounts of tracer recovered in leach-
ate from selected drains.  Figure 5.38 shows calculated distribution of effec-
tive porosity (Pe).  Results suggest that over 44? of the site, flow took
place through less than 1% of the area.  At a few locations  however, flow may
have occurred through 10? or more of the local cross sectional area despite
the assumed uniform compaction and water content of the clay liner material.
Two such locations, F1 (where flow occurred through less than 1? of the area)
and G5 (where flow occurred through 5 to 10? of the area), will now be
discussed in detail.

     Macropore flow—To illustrate graphically the flow through soils that may
contain macropores, we have chosen two sites that exhibit contrasting
behavior, F1  and G5.  Figure 5.39 shows respective distributions of ring
           TABLE 5.18.  BREAKTHROUGH TIMES (TB) FOR BR" TRACER AND
              WATER, AND CUMULATIVE TRACER CONCENTRATION (C/CO),
              RECOVERED AND COMPUTED EFFECTIVE FLUX DENSITY (qe)
           VALUES FOR SELECTED SITES BASED ON TRACER BREAKTHROUGH
            ,  , ,   TIMES AND AVERAGE 30 CM THICKNESS OF CLAY

                       	IK	
           Site        Tracer     Water     C/Co            qe
                         hrs       hrs        %         10~9 m/sec

           AA7            26        45        5            3,205
           A3             30        22       43            2,778
           D7             29       142       24            2,874
           F1*            25       191        2            3,333
           G5             47       142       84            1,773
           JO            170        46        2              490
           L3           >265       170        2             >314
           M7             53        71       29            1,572
           01             48       311       <1            1,736
           09             48        46       10            1,736
           Q5              7       144        4           11,904
           S1             54       316        2            1,543
           T5            161       195        1              517
           V8            167       144        3              499
           X3             25       144        6            3,333
                                      112

-------
                                             EFFECTIVE POROSITY %
                                          DBAINE50 SUMMITION 4/30/86
   Figure 5.38.
Distribution of effective porosity (Pe) in a compacted and
ponded, spatially variable clay liner given as the percent
of cross sectional area (A), based on first arrival times
of ponded water.
inflow (R), drain outflow (D),  and bulk density east (DE) and west (Dw) of the
flow-monitoring site.  For the site F1  there appears to be some agreement
between lab and field values (Table 5.18), largely because both inflow and
outflow distributions are very low.  This agreement between lab and field
values could be related to rather stable bulk density surrounding the site F1
and to a relatively small effective cross sectional area involved in flow.
The upper curves in Figure 5.39a, which give changes in bulk density with time
adjacent to the ring and drain location, show that except immediately follow-
ing ponding, bulk density both east and west of the site remained essentially
the same for a whole year.  Despite the high uniformity of clay material, a
breakthrough time of 25 hours for Br" at the F1  drain was recorded, although
only 2% of the tracer was subsequently recovered (Table 5.18).  These values
translate to 0.1$ effective porosity with most Br" expected to be retained in
surrounding soil.

     In contrast, at the site G5 (Figure 5.39b)  considerable inflow and out-
flow existed and density increased quickly at ponding and then more slowly
during the remainder of the study.   Such increases, also observed at other
                                     113

-------
500-
450-
400
0 36°
^ 300-
I 250-
m 200-
^ 150
100
50-
o-
NO
•JW







V84 FEB85
RING DRAM PI DENSITY Ft G1
fov*J\f::\$^^






^ 	 D
MAY85 AUG85 NOV85 FEB86 MAY86 AUG86 NOV
2500
-2400
-2300 m
-2200 |
£
- 2100 >
2000 I
1900 jjj
1800 ^
- 1700 3
1600
1500
86
                           RING DRAIN G5 DENSITY F5 H5
        500-


        450



        400
      O 350
      UJ
      U>

      S 300

      o>

      * 250
      *
      o
      C 200-

      III
        wo-


        50
         0<,	

         NOV84
                                              2500



                                              2400



                                              2300 f
                                                  *

                                              2200 §



                                              2100 >



                                              2000 z


                                              1900 uj

                                                  8
                                              1800 g


                                              1700 <

                                                  Q

                                              1600
               FEB85   MAY85  AUG85  NOV85   FEB86   MAY86  AU386  NOV86
  Figure  5.39.
Distribution in time of ring  inflow (R), drain outflow  (D),

and bulk  density in the east  (Dg)  and west  (Dy)  of the  primary

ring and  drain locations  for  the slow-flowing site Fl (a)  and

fast-flowing site G5 (b).
sites, are  probably indicative of surface wetting and inflow  into macropores

at ponding,  with subsequent  movement of water,  either as a wetting front or by

diffusion from macropores  into compacted clay  matrix.
                                      114

-------
     Tracer distributions—Figure 5. MO shows relative cumulative concentration
of tracer in drains under  and  around the infiltration rings F1 and G5, to
which tracer was originally applied.  Although the first breakthrough occurred
after 25 hours from the  drain  F1 (directly under the ring to which tracer was
applied), the largest amount of  tracer (approximately 1$ of that applied) came
from drain FO.

     Effective porosity  calculations generally assume vertical flow.  Results
in Figures 5.MOa and S.MOb suggest that this may not always be the case.  For
example, although 8M? of applied tracer was recovered from the drain G5
(directly under the ring G5 to which tracer has been applied), the first
arrival of Br" tracer occurred at drain H5.  Small amounts of applied tracer
(approximately 0.5%)  came  also from drains G4, G6, and H6.

     At the site H5 (Figure 5.MOb), a relatively rapid (22 hours) breakthrough
of Br", which had been applied to a G5 ring, was observed with a computed
effective flux density (qe) greater than 10,000 x 10~9 m/sec (assuming a
diagonal tracer flux  from  ring G5 to drain H5, over a distance of about 1m in
22 hours).  Since observed water outflow flux (q) at H5 at that time was no
      o°
      o
      _  10.0
        0.001
                                      a.
                               FO  GO
                                                          N
             0    100   200  300    0    100    200   300   400
                            CUMULATIVE TIME (hrs)
       _   10.0

            0.1
        o
       O
       O
         0.001
                                       b.
F4
G4
H4
F5
OS
H5
F6
G6
H6
H5
	 u.'agng* ••
-WS
+ 7" oooo
H6
                                         H4
              0    100    200   300    0     100   200   300  400

                             CUMULATIVE TIME  (hrs)
    Figure 5.MO.  Relative concentration of Br~ as leachate  from site  F1
                  and surrounding drains (a) and site G5  and surrounding
                  drains (b).
                                     115

-------
more than 10 x 10~9 m/sec, effective porosity (Pe) of the area through which
the tracer must have passed could be as little as 0.1$ of the local cross sec-
tional area.  Even at peak water outflow rate of about 125 x 10~9 m/sec the
effective porosity (Pe) values would have been no more than about 1$.

     Such calculations may explain in part the absence of any major changes in
bulk density adjacent to the sites F1  and G5 (Figure 5.39).  In terms of
environmental safety, the flow rate of concern would be the 10,000 x 10~9
m/sec breakthrough time for tracer rather than the very slow (approximately 1
x 10~9 m/sec) matrix flow component.  However, in real-life situations, when
we may wish to evaluate potential impact of pollutant on groundwater, such
high flow rates may need to be considered in terms of cross sectional areas
(effective porosity) that contribute to flow (^ 1$) and the observed concentra-
tion of contaminant in recharge.

     Breakthrough history at sites F1  and G5 and surrounding drains, as well
as order of magnitude differences between lab and field values in Table 5.18,
suggest that even a seemingly uniform clay liner is a highly variable one with
an effective porosity that ranges from as low as 0.155 to more than 5%.
Results suggest that, if potential impacts on groundwater from these sites are
considered, breakthrough times,  delivered concentrations, and contaminant
toxicity should all be carefully evaluated.

     Subsequent coring with a Veihmeier tube of the tracer application area
and surrounding sites on the 0.3m grid and qualitative tests (Goldman and
Byles, 1959) for Br~ corroborated preliminary observations.  On sites such as
F1, where little tracer was lost as leachate, strong evidence of tracer shows
in corings as a tight, well-defined "plume" surrounding the infiltration ring
to which tracer has been added (Figure 5.41 a).  However, for sites such as G5,
where much tracer was lost as leachate, the Br~ distribution plume was quite
extensive but rather diffuse throughout the area of nine drains (Figure 5.4lb).
This shows that the highly mobile tracers (or highly mobile contaminants) may
be more difficult to detect close to the source of application, even though
their impact could be greater and felt sooner further away.  Additional
corroboration of these findings may be found in Br~ plumes for other sites
shown in Figure 5.42, 5.M3, and 5.44.


Swelling—

     A possible source of fluctuations in inflow, outflow, tracer
concentrations, and density could be random swelling of smectite clay minerals
within the liner matrix on wetting and possibly moderate shrinkage as a result
of consolidation and piping in zones of lower compaction.  The mineral composi-
tion of the clay liner material is primarily illite and kaolinite with some
smectite.  Thus, although swelling based on prototype studies could not be
ruled out, little was expected.   It is also conceivable that in pockets of
inadequately compacted clay local consolidation may have occurred.  Figure
5.45 shows the interpolated surface elevation (mm) change as measured with a
Selcom1  Optocator unit.  In general, the changes at nine months amounted to
between 0.5 and 1.50mm.  There were, however, two zones of contrasting
behavior.  On the north side of the liner, about the middle, there appeared a
small zone of consolidation (-1.50 to -2.50mm),  while on the south side to the

                                      116

-------
                      EO              E1              E2
                       o    o    o    o    o    o   o
                       o    o
                       o
             • HIGH

             $ MEDIUM
             © LOW

             O NONE   GO
O
                     o    o   o
                       F4
                       O   O
                       o
• HI6H
® MEDIUM
© LOW
O NONE

0 0
H4

1
O


                               F6
                                O
                                                       O
Figure 5.M1.  Relative distribution of Br~ tracer in soil around the
              sites F1 (a) and G5 (b) to which tracer has been applied.
                                    117

-------
                                               OL6          (017
                                                000
                                                    •   •    •    •/   O   O
                                        • HKH
                                        • MEDIUM
                                        • tow   O    O   O    O    O    O   O
                                        OWME   PO           PI            P2
Figure 5.M2.   Relative distribution of  Br" tracer in soil around  the sites
               D7t  L3,  M7f and 01 to which the tracer has been applied.
                                      118

-------
  • HIGH
  O MEDIUM
  SLOW
  O NONE
  • HIGH
  © MEDIUM
  0 LOW
  O NONE
O
R4
O
R5
O
R6
                                                  S4
                                                  O
                                                      ss
                                                      O
                                                 -»    ss
                                                  O    O
                                  • HIGH
                                  O MEDIUM
                                  e LOW    o
                                  O NONE    W7
                                                      O
                                                      W9
Figure  5.43.   Relative  distribution of Br" tracer  in soil  around the sites
                Q5,  S1, V8,  and 15  to which  the tracer has been applied.
                                         119

-------
  o
  o
                                      08
                                      P8
                                                      O     O    O    O
                                                           O    O    O
                                                                 o    o
  Figure 5.44.
Relative distribution of Br~ tracer in soil around the sites
JO, and 09 to which the tracer has been applied.
left of center, there was a corresponding small zone of expansion (2.00 to
3.50mm).  Although expansion appeared to be associated with a less permeable
zone and consolidation with a more permeable one, no correlation was found
between the degree of expansion and observed conductivity,.
Percolate Quality—

     Percolate quality appeared somewhat related to hydraulic conductivity,
degree of saturation, and number of pore volumes of percolate.  Figure 5.46
shows the spatial distribution of pore volumes leached through the liner at
nine months and the starred points indicate location of monthly leachate
collection.

     Initial changes in water quality as it passed through the clay liner are
given in Table 5.19 for selected locations.  Reported measurements were made
once a month using standard testing procedures on the water supply from the
tanker, ponded water on top of the liner, and percolate collected from the
respective drains.  Following 6/25/85 sampled water was recirculated through
                                      120

-------
to
                    OS
                     C
                     T
                     CD

                     Ul
                     *
                     Jr
              0-32:
              CD O C
              CD 3 3
              3 ct cr
                 3- CD
              CO CO T
              {o -
              B    O
              •o co M)
              M Ct
              CD {B T5
              O. T O
                 T T
              3 CD CD
              O O.
              3    <
              Ct -0 O
              3" O M
              I-1 I-* C
              ^33
              •  Ct CD
                 CO CO
                 3 CD
                 O. 0)
                 1— O
                 o 3-
                 0> CD
                 ct o.
                 CD
                    ct
                 I-1 3"
                 O ~i
                 O O
                 P> C
                 Ct OQ
                 I- 3"
                 O
                 3 ct
                 CO 3"
                    CD
                 CD  I-1
                 T  OJ
                 CD  ^<
                 CD  H-
                 (B  3
                 O  (D
                 3" T
                 O
                 ct {U
                 CD  ct

                 3- 3
                 0)  t-^-
                 CO  3
                    CD
DISTANCE,    feet
                         00
                         c
                                                                                  CO

                                                                                  Ul
                                                                                  Jr-
                                                                                  Ul
                                                                                  CD
                                                            m
                                                            m
                                                         o o
       o o
       o o
       o o
       o o
        i   i
                                                         O Ul
                                                         o o

                                                         ct ct
                                                         o o
                                                         o o
       O Ul
       o o

       ct ct
       o  o

       I   I
       o -»
                   CO

                   CD  3
                   I-1 CD <
                   M T 03
                > 1-    Ct
                >• 3  v£> l-»
                > OQ     O
                >-   S D

                 1330
                (V) CD  ct 3"
                         B>
                         3
                         OQ
                         CD
                         CO
      O Ul  0)  CO
      O O  ct
             ct  ct
             O  O  CD  ct
                                                                          I  CO
                                                                               CD
Ul O
O O

3 3
3 3
Ul O
O O

3 3
3 3
                                                                                                                  ui o cr
                                                                                                                  o o o
                                                                            CO
                                                                            CD
                                                         L

                                                         c-
                                                         tr
       C-<  I—I  SC O 3
       C-,  M  ffi O Q.
       c_,  M  PC O H-
                   O
to ro  ro  —»  —• o p>
	ct
O Ul  O  Ul  O Ul 1—
o o  o  o  o o <
                   CD
ct ct  ct  ct  ct ct
o o  o  o  o  o o
                   >-t>
                                                                                                     LO CO IV)  |\J
                                                         Ul O
                                                         o o
      Ul  O
      o  o
            CO
      Ul O 3"
      O O T
                                                                           OQ
                                                                            CD
O  H-
3  I-1
Q.  H-
H-  >-••
3  3
OQ  CD
..  ct
    CD
•O  T
O  CO
CO
                      CD
                         i-!>
                      CO  O
                      <<  "3

                      cr ct
                      03'
                      (-• CD
                      0)
                         O
                      H- O
                      3  3
                      O.T3
                      H- Cl)
                      O  O
                      tu  ct
                      ct CD
                      CD  a

                         o
                         M
                         (U
                                                                                               35
                                          incioaneic
                                          i m si s> n o o fi	
                                          jggnnngggggggg

                                           §*      s?s
                                           C4        61
                                           s        §
                                           srs    x SB  si
                                           Cl  B 9 68  C
                                           ci  x a a  «
                                                                    B EK a a BE a
                                                                    a a a a a a
                                                                  a a B ai a X a
                                                                  m as B a a a is
                                                                 saaBaaaa
                                                                 szaataaeaaa
                                                                    eaasatra
                                                                                                                                           5    g
                                                      >8§8«
                                                      5§§ss
                                                      i n ci n c
                                                      1 Cl Cl O G
                                                      i ci ci n fi
                                                                                                                         9  a a a
                                                                                                                         a a a a H
                                                                                                                         B a « a a
                                  e- c*

                                M H
                                B a s
                                                                                                               l Cl O C
                                                                                                               l O Cl C
                                                                                                Cl Cl Cl
                                                                                                 §C1 Cl C
                                                                                                 Cl Cl 11
                                                                                                Cl Cl Cl 6
                                                                                               n *«
                                                                                               >5 -^
                                            ci   a B a  ci
                                               §a a a  ci
                                               a a a  ci
                                            n   a B x  n
                                            ci   x a B  «
                                                                                                    ci  B x B a  n

                                                                                                    ci  B x a B a
                                                                                                      3! IB     '-M DJ
                                                       8«ci8
                                                       Cl Cl O
                                                         SSSSc
                                                         gcicinc

                                                         Cl     6
                                                         Cl   Cl C
                                                        no  ci ci t

                                                        il Cl Cl C) Cl «
                                                        n     n c


                                                         aaan
                                                                         j o n
                                                                         j
                                                                          O D
                                                                        33
                                                                                                               B a a a a a
                                                                                                                                                            i ci ci ci  a a
                                                                                                                       B     a a
                                                                                                                       D B  B B B
                                                                                                                       B a B a a
                                                                                                                       B a a a a
                                                                                                                       an  aaa
                                                                                                                                   555
                                                                                                                                   555
                                                      55

                                                 S    ^
                                                 1  ,55
                                                 et  •* "• "'
                                            Cl«ClClClfflClCl<

                                            O 51 SI Cl O s
                                                               a     • ci
                                                               a    a a n
                                                               a n s a a n
                                                               a a B »  a
                                                                                                                                   555
                                                                                                    ClClAClGlClClCl
                                                                                                    ciocinnnnci
                                                                                                    C1C1C1C1G1C1C1C1

                                                                                                   ctciciocifficieaci
                                                                                                   ciciciciciciocici
                                                                                                   cicicicicinncici
                                                                                                                 cici
                                                                                                                 Cict

-------
                      TABLE  5.19.  WATER  QUALITY CHANGES  AS  A RESULT OF PASSING THROUGH EXPERIMENTAL LINER1
Source
pH
El-Garb
                                                  EC
N03-H   NH|»-N
                                                                                 SOi,
                                                                 Na
                                                                                  Ca
                                                                                           Volume
Tanker
Drain (composite]

Tanker
Ponded water-
K-6
0-9
L-6
AA-0

Tanker
Ponded water
AA-0
F-7
K-6
L-6
0-9
P-5
T-3
7.2
) 7.9

5.9
6.9
6.9
6.8
6.8
6.9

6.0
7.3
7.1
7.3
7.2
7.1
7.0
6.8
8.1
(.

1.6(.
3.2
42. 2
32.9
39.1
16.9

2.3(0
1.8(0
8.3(.
7.8(0
6.1
5.6
3.9
6.3
10.4
rax,;

01NH2SOn)
n
tt
n
M
11

.OINHjSOn)
.05NH2SOi,)
01NH2S04)
.05NH2SOi,)
n
it
"
tt
tt
155(27°)
1550(27°)

120
150
985
795
900
110

130(14°)
220(14°)
220(12°)
800(12°)
600(12°)
600(12°)
325(12°)
700(12°)
900(12°)
4-2-85
3.9
8.6
4-25-85
5.2
5.2
3.9
7.6
-
3-7
6-25-85
4.1
2.1
0.3
3.2
0
0.8
0
0.2
0.3
0.02
1.50

0.22
0.02
0.12
0.05
0.08
0.19

0.07
0.08

0.15
0.10
0.08
0.09
0.16
0.07
13
255

17.1
22.7
146.0
139.0
182.0
95.2

14.5
28.1
27.6
139.0
117.0
132.0
22.0
135.0

img/x,; -

7.9
9.4
27.5
18.1
29.0
10.7

8.3
9.2
9.9
18.4
11.4
12.3
8.9
12.3
35.5
3
72

3.4
7.6
22.5
95.3
19.2
19.1

3.6
10.0
11.6
14.4
7.2
7.6
24.8
6.8
64.0
-

5.7 10.2
5.4 15.2
70.4 114.8
32.8 83.2
58.0 116.0
11.5 50.0

11.1
23.6
24.4
103.0
81.0
80.0
35.2
102.0
44.0
(ma)

_
-
5,050
14,200
4,260
6,800

_
-
>50,000
2,450
15,300
8,800
>1 0,000
15,000
400
1 Ponded on 3/26/85.

-------
the system.   Subsequent to 6/25/82 sampling of all the 250 drains was carried
out at 9 months (highest outflow rate)  and again at 12 months when steady
state conditions prevailed at the conclusion of the study.

     Table 5.20 shows the means, standard deviations, and CV's of leachate
quality parameters and Table 5.21  list  correlation matrices for the 9 and 12
month data,  respectively.

     In general, average electrical conductivity (EC), 3014, and Na in leachate
declined substantially in the last three months.  K and Mg remained about the
same, while Ca concentration appeared to decrease.

     Figures 5.47 and 5.48; 5.49 and 5.50; 5.51 and 5.52 show spatial distribu-
tion of leachate quality variables at 9 and 12 months respectively.  The
starred points represent locations of initial sampling sites.  The spatial
distributions suggest a modest decline  in concentrations of Ca and Mg especial-
ly in the western half of the site, much change in K, Na and pH and substan-
tial declines in EC and SOij.  Except for Ca, Mg and 8014 results are quite
similar to those given in Table 5.20 where averages were compared.  Spatial
distribution shows a sharper decline in Mg concentrations than the statistics
in Table 5.20 would lead us to believe.  Ca and SOij although declining
spatially, show substantial increase in variability as evidenced by respective
CV values.  Inspection of contours alone especially for S0jj in Figures 5.47c
and 5.48c would lead us to believe the  contrary.

     Results in Tables 5.19 to 5.21 and Figures 5.4? to 5.52 illustrate
several practical points.  In a commercial facility under field conditions,
effluent from below a clay liner is usually collected by a single drain system.
Such a system tends to average out both the quality and quantity of water over
an area.  Results presented here illustrate how variable are the actual
concentrations over time and in space.   In general, magnitudes of EC, Ca and
        TABLE 5.20.  MEANS AND STANDARD DEVIATIONS, AND COEFFICIENT OF
           VARIATION (CV) OF LEACHATE QUALITY PARAMETERS SAMPLED AT
                         9 AND 12 MONTHS PONDING	
Variable
                          Mean 9 mo
                                         CV
Mean 12 mo
CV
EC (vimhos/cm)
pH
NO 3 (mg/&)
Bi-carb (mfc)
SOij (rng/H)
Ca
K
Mg
Na
630±273
7.9± 0.3
0.047± 0.130
-
32.7±21.0
51.5117.5
26.7+27.5
35.4+13.4
20.2+11 .1
43
4
277

64
34
103
52
55
279±109
7.8+ 0.4
-
5.8± 1.9
9.4±15.6
38.8±25.2
30.4±30.1
29.2+13.9
8.1+ 9.2
34
5

33
166
75
99
48
51
                                      123

-------
      TABLE 5.21.   CORRELATION  MATRIX OF LEACHATE QUALITY PARAMETERS AT
     	9 AND 12 MONTHS FOLLOWING PONDING	
Variables
EC
PH
S04
Ca
K
Mg
Na
   EC
   pH
   N03
   804
   Ca
   K
   Mg
   Na
                                   9 months
1.00
'0.10
0.31
0.38
0.82
0.93
0.97
0.72
1.20
0.19
0.00
-0.21
-0.01
-0.03
0.02

1.00
0.24
0.21
0.3M
0.34
0.16


1.00
0.51
0.31
0.37
-0.01



1.00
0.67
0.74
0.33




1.00
0.91
0.74





1.00
0.69
                                  12 months
                                                          1.00
EC
pH
Bi-carb
SO),
Ca
K
Mg
Na
1.00
0.18
0.74
0.09
0.29
0.65
0.57
0.53
1.00
0.25
0.02
-0.04
0.35
0.32
0.24
1.00
0.06
0.47
0.85
0.80
0.76

1.00
0.14
0.06
0.13
-0.02


1 .00
0.48
0.53
0.39



1.00
0.90 1.00
0.84 0.82





1.00
Mg as well as K and Na in the Figures roughly correspond to their values in
the Tables.  There is little variation between pH values either in space or in
time, and little apparent agreement between SOn values.  This lack of agree-
ment between the time and space averages of 30^ appears to be due to extensive
variation of 30^ concentration.  Since time averages provide a wide range of
values  it may be difficult to select any one value as representative of the
chemistry of the liner.  Closer inspection of hydraulic conductivity values
derived from inflow and outflow suggests that the EC as well as Ca, Mg, K, and
Na concentrations in effluent appear to be inversely correlated with hydraulic
conductivity.  Comparison of the "Storage" and "Ponded" water quality with
that of the effluent indicates that under all circumstances higher concentra-
tions of Ca, Mg, K and Na prevailed in the leachate than in ponded or applied
(storage) water.  Comparisons of values with distribution of pore volumes
suggest that in general average concentrations in leachate were inverse]^
related to the number of solute pore volumes passed through the liner.

     Results to date suggest that considerable variability exists in spatially
distributed properties and leachate chemistry of a compacted clay matrix which
may affect the rate, quality, and pathway of leachate flow through a.clay
liner constructed to industry specifications.  There also appears to be a
discrepancy between the extent of saturation and observed outflow with higher
flows originating in apparently unsaturated areas suggesting an existence of
preferential flow pathways.  Such preferential pathways may potentially pose a
                                      124

-------
grave threat to underlying groundwater quality even in the  presence  of  a  clay
liner.

     Outflow and inflow rates from a liner spanning a range of  two to three
orders of magnitude were observed in this study and chemical concentration in
the leachate appeared inversely related to hydraulic conductivity and number
of pore volumes leached.
                          12      24     36     48      60     72
                          12      24     36     48      60     72
                               DISTANCE,  feet
     Figure 5.47.  Spatial  distribution of electrical conductivity (EC)
                  in  ymhos/cm  (a), pH (b), and SOij mg/X,  (c) in leachate
                  from drains  (250) at 9 months.
                                       125

-------
           24
                         1 - 1 - 1
                                        i - 1 - r
                                                           EC
                    12
24
36
48
60
72
                    12     24     36      48     60      72
                    1E
E4      36     48      60

  DISTANCE, feet
                       72
Figure 5.M8.  Spatial distribution of electrical conductivity (EC)
              in ymhos/cm (a), pH (b), and SOjj mg/fc (c) in leachate
              from drains (250) at 12 months.
                                126

-------
       CD
       0)
                  12     24     36     48     60      72
                       DISTANCE,  feet
Figure 5.49.  Spatial distribution of K (a)  and Na in mg/Jl (b) in
             leachate from drains at 9 months.
                               127

-------
                                                                    OQ
                                                                                                                   DISTANCE,  feet
                                                                     ui
                                                                     o
                                                                     to
oo
                                                                  CD
                                                                  03

                                                                  O
(D
   Q.
i-t> H-
T  CO
O  r+
3  T
   I-"
D. cr
T  C
0)  <-f
I-* H-
3  O
CO  3

SB  o
c-t- •-«>
                                                                  ro
                                                                     y~^
                                                                  3  (u
                                                                  O  ~-s

                                                                  <-f fU

                                                                  CO  O.
                                                                     3
                                                                    OQ
                                                                                                                                O
                                                                                                                                             ru
                                                             ro
                                                                                                                               ru

-------
      CD
      CD
      u
      Q
                  12     24     36     48
72
                      DISTANCE,  feet
Figure 5.51.   Spatial distribution of Ca (a)  and Mg in mg/8,  (b) in
              leachate from drains (250) at 9 months.
                               129

-------
                12
24      36       48
    DISTANCE,  feet
60
Figure 5.52.  Spatial distribution of Ca  (a) and Mg  in mg/S,  (b)  in
              leachate from drains (250)  at 12 months.
                                130

-------
                                   SECTION 6

                              CONCLUDING STUDIES
POSTPONDED STAGE

     After the excess ponded water was siphoned off and the clay liner
drained, several studies were initiated to check or corroborate observations
made during the ponded stage.  Complementing detailed inflow/outflow data for
all ring/drain combinations, 3" (8cm) diameter 12" or 9" (30cm or 23cm) long
cores were removed from the center of each ring infiltrometer (except the ones
to which Br~ had been applied).  The cores were taken using a standard Acker1
split tube sampler.  For each core the central portion, or the most homoge-
neous portion, was trimmed to size (- 4", 10cm) suitable for storing in the
refrigerator for use in subsequent laboratory analysis of saturated hydraulic
conductivity.  Some cores were split into two or even three segments to
provide "replicates."

     In addition, a large number of 2", 3", and 6" (5, 8, and 15cm) diameter
cores were taken for comparison with and calibration of the dual gamma measure-
ments of density; for evaluation of changes in density with depth, and for
assessment of the extent and distribution of coarse fragments within the clay
liner.  Using Troxler^ surface probe, a set of surface moisture as well as
surface and direct transmission density measurements at 2", 4", 6", and 8" was
made to compare with initial surface probe readings and to evaluate the sur-
face probe method as a field method for measurement of density.  When the
water had drained from the liner, a set of vertical access tubes was installed
at each of 45 locations from which 2" cores were previously taken; simulta-
neously 45 gypsum moisture blocks were installed at 3" (8cm) depth.  Monitor-
ing of liner water content change began in the fall of 1986 and continued on a
regular basis until May 19, 1988 when the liner was broken up, inspected, and
removed from the site.  Specific reference samples were saved for further
analysis.  Figure 6.1 shows a schematic distribution of scheduling, and dura-
tion of pertinent additional studies.


LABORATORY HYDRAULIC CONDUCTIVITY

Flexible Membrane Method

     Standard test method for measurement of hydraulic conductivity of saturat-
ed fine grained materials with a flexible wall permeameter11 was used to evalu-
ate hydraulic conductivity of cores taken from the center of each infiltration
ring.  In Table 6.1 summary statistics of the results to date are compared
with hydraulic conductivity values based on ring infiltration and drain
outflow rates, while detailed data for individual samples are given in
Appendix E.
     4Courtesy D.  E.  Daniel,  University of Texas,  Austin.

                                      131

-------
        CLAY LINER DRAINED 7/30/86

      | 1st SET VEIHMEIER SAMPLES FOR MOISTURE (45)
            «—» 2nd  SET VEIHMEIER SAMPLES, SPLIT (45)

       «_»  3* CORES. MOISTURE. DENSITY (24O)
         — 2"CORES. SPLIT (45)
                         «	» 6'POSTHOLE  DATA (240)
                            «-» TRANSECT. I*DEPTH INCREMENTS DUAL PROBE (50)
           ••	»  CORES FOR LAB-K (250)
                  4	*•  SURFACE MOISTURE a DENSITY AT S, 2". 4", 6* S 8" DEPTH (240)
                  I I  I  I  EXCAVATE SITES 2" INCREMENTS (4)
                 A3T6L8R4
                iCORES: L.DOUGLAS  A4.62 a D.NORTON R3, MS (4)
              i CORES DANIEL (12)

                       MOISTURE  BLOCKS (AT 3") (45)
                   DEPTH MOISTURE, NEUTRON (AT 6") (45)
                                                   ^           JCLODS
                                                    SAND CONE (50)
                  _     TRACER a DYE CORES
    JUL AUG SEP  OCT  NOV DEC  JAN FEB  MAR APR MAY JUN JUL  AUG SEP
    	1986	1	1987	
  Figure 6.1.  Chronological distribution of activities after the  clay liner
               was drained.
     The hydraulic conductivity analysis was carried out in 3"  (8cm)  diameter
cores varying in length from 2-7/8"  to 6" (7 to 15cm) depending on  the number
of sections the original core was divided into, and on how well a refrigerated
core segment could be trimmed to fit in the apparatus.  [Because of stones
imbedded in the clay matrix this at  times was very difficult.]   Initially,
only the most homogeneous portion of the original core was selected for
analysis.  The subsequent trimming constituted a further refinement.   The
cores were run using a cell pressure of 25 psi (170 kPa) inflow pressures of
between 21.H and 23.4 psi (1U5 to 165 kPa) and outflow pressures of 20 psi
(140 kPa) giving a gradient of between - 15 and 30 (with most cores at - 25).
Several cores (eight so far) either  broke up during trimming or developed
cracks during storage making them unusable for analysis of K.   If analyzed,
such cores would have abnormally high K-values to the point that some could
not be run at all.
                                       132

-------
TABLE 6.1.  SUMMARY STATISTICS FOR LABORATORY AND FIELD
    EVALUATED HYDRAULIC CONDUCTIVITY (x 10"9 M/SEC)
                 Lab
Drains
Rings

N
Mean
Std Dev
Skewness
CV
T:Mean=0
Variance
Kurtosis
Std Dev
Prob>| T |

100$ max
15% Q8
50% med
25% Q1
0% min
Range
Q3-Q1
Mode
99%
95%
90%
10%
5%
1%

Low




High




Moments
95
7.5
11.9
3.4
159
6.1
142
15.3
1.22
0.0001
Quantiles(Def
79.3 1
7.0
2.6
1.5
0.45

193
19.0
24.8
1.8
130
10.6
6.6
3.7
1.78
0.0001
=4)
29.4
29.4
8.0
1.6
0.03
78.9 129.4
5.5
0.80
79.3 1
33.5
20.48
0.87
0.73
0.45
Extremes
0.45
0.46
0.69
0.72
0.74
33.15
35.2
37.06
51.98
79.35
27.8
0.15
16.4
73.9
50.6
0.40
0.19
0.08

0.03
0.08
0.09
0.09
0.10
84
96
110
115
129

150
19.9
35.6
2.7
178
6.8
1269
8.0
2.90
0.0001

188.152
19.6977
5.27341
1.42623
0.08
188.0
18.2
0.53
181.7
118.3
67.4
0.57
0.27
0.11

0.08
0.13
0.14
0.16
0.22
125
125
168
175
188
                           133

-------
Comparative Analysis

     In Table 6.1 comparative statistics for laboratory and field values of
hydraulic conductivity (derived from ring and drain flux) are given.  Although
the moments of all three distributions are quite similar, comparison of the
respective quantiles and extreme values suggests the laboratory distribution
of K is essentially a nested distribution within a distribution of field
values.  Extreme variability is reflected by high CV values, and particularly
the magnitude of outliers.  It is perhaps worth recalling that more care goes
into selection and preparation of lab cores compared to field data which are
taken at a given site while not being aware how uniform or how variable and
inhomogeneous is the underlying material.  Such inhomogeneities tend to be
avoided on a core scale but are included in analysis on a field scale giving
rise to discrepancies between the lab and field values.  Skewness, kurtosis,
and a very low value of the Prob>| t | suggest (not unexpectedly) that hydraulic
conductivity (whether lab or field) is not likely to be normally distributed.
Surprisingly viewed as a whole laboratory and field distributions are not that
different.  While modes, medians, and lower quantiles are quite low and rather
similar in both the lab and field distributions, the differences arise in the
upper quantiles and outlier values.  It would therefore be expected hydraulic
conductivity to be always larger in the field unless perfectly homogeneous,
and fine materials were used to construct the liner.  Field values of hydrau-
lic conductivity of the defective cores (eight to date) are listed in Table
6.2.  Comparisons with the quantiles of distributions and outlier data in
Table 6.1  suggest that in all but one case (Q8) the defective cores came from
the upper quantile of the drain conductivities and upper half of the ring-K
distribution, suggesting that the cores that broke up came primarily from the
zones of high flow.  Because of the high spatial variability of hydraulic
conductivity, zones of low and high flow could very easily adjoin each other.
                   TABLE 6.2.  FIELD VALUES OF HYDRAULIC
                      CONDUCTIVITY NEAR THE SITES WHERE
                    	DEFECTIVE CORES WERE TAKEN
                    Site          Ring-K          Drain-K
                                      cm/sec
AAM
B8
C8
F5
15
L6
M5
Q8
-
35
9
85
33
10
36
H
-
48
62
63
79
31
68
19
                    Ring and drain K are based on the
                    time averaged flux at each location.
                                      134

-------
     Figures 6.2 and 6.3 represent  scattergraph  comparisons between laboratory
and field derived values.  In Figure  6.2  point to  point comparisons are given.
These comparisons suggest that there  is little if  any relationship between lab
and field derived measurements of hydraulic  conductivity.   When,  however, the
same data are ranked in order and replotted  as was done in Figure 6.3, the
correspondence between the two distributions is  apparent.   The uppermost plots
in Figure 6.3 (also Figure 6.2) represent comparisons between the lab values
and ring or drain derived hydraulic conductivities,  based  on the  final set of
field readings made.  The lower plots give the same  comparison but for the
time averaged values of ring and drain K.  The results suggest a  linear rela-
tionship between the lab and field  distributions.   In our  case, laboratory
values appear to underestimate field  distributions of saturated K when
compared on the distribution to distribution basis.   It is expected that, in
general, laboratory values on cores sampled  from a clay liner will underesti-
mate the field hydraulic conductivity values and that the  point to point
             u
             t-
    I
   8O •

   70

   00

   60
                                LAST DATE
O

3  *
>-  30

>  »1
I-
O  K)

O

o
o
U  90

O  80

0  70
                                                        LAST DATE
                          RINGS
                                                  DRAINS
             CC
             O
             or
             o
             5  30
                                 AVERAGE
                                                         AVERAGE
                      5O     100    160    200  0     60    100    CO

                          HYDRAULIC CONDUCTIVITY (xIO'7cm/sec)
                                                               200
        Figure 6.2.  Point to point comparison of laboratory  hydraulic
                     conductivity (K) with field derived  values  based on
                     last (upper plots) and average  (lower  plots)  observed
                     ring and drain flux.
                                      135

-------

o
41
U
O
T<
5
rDRAULIC CONDUCT
1
cc.
LABORA

80
80
70
80
60
40
30
20
".
00
80-
70^
80
60
40
30
20
n
o
LAST DATE


•

•'
/
•'
RINGS
AVERAGE

•
.•
^•""'
                                           LAST DATE
                                                   DRAINS
                       601001602000    60100160

                          HYDRAULIC CONDUCTIVITY (xlO~7cm/sec)
                                                               200
         Figure 6.3.  Rank to rank comparison of laboratory hydraulic
                      conductivity (K) with field observed values  based
                      on last (upper plots) and average  (lower  plots)
                      observed ring and drain flux.
correspondence is not likely to be observed.  However,  if  sufficient  numbers
of samples are evaluated, field distributions may be  found to  be   linearly
related to laboratory distributions.  For example,  in our  case, field values
would have exceeded laboratory values by a factor of  two to five.   Compared to
two or three orders of magnitude differences in the point  to point
comparisons, distribution to distribution comparisons look more realistic.
Distribution of Bulk Density and Water Content

     We may recall that dual probe density values  (D^) measured prior to pond-
ing did not correspond exactly to the surface probe  values measured during the
liner construction.  To calculate the density for  the evaluation of the
spatial distribution of the available pore space,  dual density readings were
adjusted to the surface probe readings (multiplied by 0.9) and corrected for
the volumetric water content as measured with the  surface  moisture probe
                                       136

-------
during liner construction.  The procedure was not completely satisfactory
because water contents and densities were not measured on the same size grid
(36 vs 240 sites).  At the conclusion of the study and after draining the clay
liner, representative 3" diameter cores (240) were therefore taken at the
exact locations where dual probe densities were measured during the ponded
stage.  Bulk density and water content of cores were determined gravimetric-
ally on these samples in order to provide a calibration for the dual probe
readings at each of the 240 locations.  Since bulk density measurements with
dual probe had been taken continuously (consecutive readings at all locations)
throughout the year of ponded study, changes in the water content of the clay
with time as infiltration proceeded and water moved in and through the clay
could be readily computed provided the correspondence between gravimetric and
nuclear methods could be established for the dual probe and core data.  A
series of studies were therefore initiated to accomplish that purpose.
Veihmeier Tube Samples—

     It was important to know the clay liner water content just after ponded
water was removed from its surface.  Thus, at the conclusion of the study when
the ponded water was no longer visible on the clay the liner was sampled at 45
locations with a Veihmeier tube.  The locations corresponded to the 35 sites
where swelling was previously measured during the ponded stage, and to five
additional sites in similar positions at each (E and W) end of the platform.
At the time of sampling ten of the 45 holes still had water standing in them.
Some of the cores had excess water on the outside (sites A and D) which was
wiped off, and the cores were resampled.  The average water content by weight
was 20.8$ with north and west side of the liner the wettest.  Converted to
water content by volume (34.5$), the results suggested, that on the average,
the clay liner at best was only 90$ saturated after one year of ponding.  This
would constitute an increase of 7.5$ over preponded conditions.  In the fall
(10/86) after the liner was drained, water content began to be monitored on a
regular basis at the 3" depth with gypsum blocks and at the 6" depth with the
neutron probe.  Calibration samples were taken at this time with the Veihmeier
tube to provide a credible starting point for these measurements.  The average
water content at 1" depth was 19.1$ (32.2$ by volume) and 18.4$ (30.9$ by
volume) in the remainder of the core somewhat lower than just after water
disappeared from the liner surface but about the same as the water content of
the liner drained by gravity (18.5$ by weight, 31.1$ by volume).
Core Data—

     The final set of dual probe readings was taken on 8/18/86 just before the
3" diameter cores were removed from the same locations.  The 8/18 dual probe
readings essentially correspond to the reading taken immediately after
(8/1/86) the clay liner was drained on 7/30/86 (Figure 6.4).  Table 6.3 shows
the appropriate statistics of the 3" core data compared to the dual probe
(8/18) values.  The parameters include wet and dry density (WD, DD), core
volume (Vol), water content by weight (9^) and water content by volume (By).
The volume of cores appears to have varied little.  Core data showed moderate
variability in density and water content while dual probe density readings
appeared somewhat less variable.  The water contents measured on cores, on the

                                      137

-------
       2600
    oo
                  2000
22OO
 DUAL 8/1
2400
2600
Figure 6.4.   Comparison between dual  probe  readings on 8/1/86 just
             after the clay liner  was drained  and on  8/18/86 just
             prior to when 3"  core samples  were  taken.
average, were less (18.4$ by wt)  than those  obtained  previously using a
Veihmeier tube (20.8$ by wt).   Since  at  the  time  of Veihmeier sampling when
water was observed standing in the  holes,  the  liner was not  completely drained.
However, when the 3" cores were taken, all gravitational  water would have left
the liner and the values shown represent final moisture content held by the
clay matrix.

      Comparison with the initial and the final densities measured with the
Troxler^ surface probe (moisture-density)  (Table  6.4)  suggests that there is
very little difference between the  three sets  of  values.  Similarly, the
average ratio between initial, final  and 3"  core  wet  densities and dual densi-
ty readings was found to be essentially  constant  (0.89),  suggesting that the
ratio may be used to correct the individual  dual  density  values to standard
density.  It is necessary to assume that the 3" core  data represents true
density values.  In Table 6.5 comparisons of wet  density  obtained using cores
of different diameters and excavations (0.77 cu ft, 0.02  m3) from different
parts of the liner are given.   Results basically  agree and support the choice
of 3" core data as a calibration standard for  the dual probe values.
                                      138

-------
        TABLE 6 3.   STATISTICS OF  THE 3"  CORE DATA COMPARED WITH FINAL
       	       DUAL PROBE (8/18)  VALUES	,	:	_
Variable
                        Mean
               Std.  Dev.
               Min
                                                      Max
        Std.  Error
                                                           CV
WDdual (k|/m3)
DD (kg/ciiP)
WD (kg/cra3)
Vol (cm3)
0W (%)
6v W
240
240
240
240
240
240
2233
1683
1995
1125
18.4
31.1
81.6
73
87
33
1.0
2.1
2064
1401
1641
1043
13.5
23.8
2488
1870
2223
1202
21 .0
35.8
5.2
4.7
5.6
2.1
0.06
0.13
3.6
4.3
4.3
2.9
5.4
6.8
   TABLE 6.4.  STATISTICS OF THE WET DENSITY VALUES OBTAINED USING 3" CORES
       AND TROXLER1 SURFACE MOISTURE DENSITY PROBE DURING CONSTRUCTION
              (INITIAL) AND AFTER THE LINER WAS DRAINED (FINAL)
   Method
N
                       Mean
Std. Dev.
                            Min
Max
Ratio1
                                                                        CV
3" cores
Initial
Final
240
240
240
1995
1960
2012
87
66
78
1641
1784
1697
2223
2111
2260
0.89
0.88
0.90
4.3
3.3
3.9
   10ther/dual density, i.e., 3" core density/dual.
 TABLE 6.5.  COMPARATIVE STATISTICS FOR WET DENSITY VALUES (KG/M3) OBTAINED
         USING 3" CORES. 2" CORES. 6" HOLES. EXCAVATIONS AND K-CORES
Method
3" cores
2" cores
6" holes
Excavations
K- cores
Sand cone
N
240
45
240
4
104
49
Mean
1995
1950
2057
2098
2122
1831
Std. Dev.
87
75
104
58
83
123
Min
1641
1760
1782
2025
1869
1448
Max
2223
2143
2354
2161
2272
2097
Ratio1
0.89
0.87
0.92
0.94
0.95
0.82
CV
4.3
3.8
5.1
2.8
3.9
6.7
  10ther/dual density, i.e., 3" core/density/dual density.
                                       139

-------
Consequently,  in Table  6.6  pertinent  statistics of the  3"  core  wet  density/
dual probe 8/18 ratios  are  given  and  its  distribution  is  illustrated  in  Figure
6.5.  Figure 6.6 shows  the  distribution of  dual probe density values  prior to
ponding,  at two days after  ponding and just prior to being drained.   Using the
correction in Figure 6.5  and relationship discussed in  Section  5  (equations
5.4 to 5.6), amounts of water  necessary to  saturate the clay liner  for the
above times were computed and  are shown in  Figure 6.7.  Density contours
 TABLE 6.6.   STATISTICS OF  THE  RATIO;  (V  CORE  DENSITY/DUAL  PROBE  DENSITY)

      Variable        N      Mean       Std.  Dev.      Min      Max       CV
 Ratio:
 3" core

Dual 8/18
240
0.89
0.05
0.74
1 .03
         RATIOTAP
                 LESS  THAN 0 JO
                 0.851  TO 0.900
                 0.951  TO 1.000
                               0.801 TO 0.850
                               0.901 TO 0.950
                               ABOVE 1.00
  Figure 6.5.  Spatial distribution of the 3" core/dual probe density ratio
               on 8/18/86  in the compacted clay liner.
                                      140

-------
       CD
       CD
       t-U
       U
       z
       <
       I—
       CO
                    2     E4      36     48

                            DISTANCE,  feet
60
7P
Figure 6.6.   Contours of density (a)  before  ponding, (b) two days
             after ponding,  and  (c) just  prior to being drained.
                                141

-------
         TO SATURATE CIAYJJNER

    BEFORE PONOiNG
       LESS THAN 20.0

    ;V~...' 20.1 TO 40,0

      I 4OI TO 60 0

      i 6OI TO SG.Q

       8O.I TO 100.0

       ABOVE 100. i
                                        2 DAYS AFTER PONDING
                                        FINAL
  Figure 6.7.  Spatial distribution of  the amount of water needed (in kg/m3)
               to saturate  the  clay liner before ponding, 2 days after
               ponding, and just  before being drained.


plotted in Figure 6.6 show  rearrangement but little change in density with
time, particularly  after the  initial increase (two days) when the liner was
first ponded; amount of water  required  for saturation (Figure 6.7) seem to
corroborate these findings.  The  mosaics plotted in Figure 6.7 show water
needed to saturate the clay in units of X,/m3.  The associated statistics in
Table 6.7 for each time increment suggest that, on the average, the amount of
water required to saturate  the  clay changed about 50 X,/m3.  This corresponds
to average change in density of - 50 kg/m3 (Figure 5.17).  On the average
(Table 6.8) the clay appears to have swelled 2.90mm.  Translated into an
increase in the available pore space, this amount would constitute a
nontrivial - 20% increase in the  available pore space that would account in
part for an apparent lack of change in  the observed density (Figure 6.6).

     When the liner was first  drained,  questions arose as to whether there
could be any differences  in water content and density distribution with depth
and how best should the water  content of the clay liner be monitored with time.
Table 6.9 shows the pertinent  statistics for 2" diameter  cores taken very near
the locations (- 30cm North of the sites) from which Veihmeier samples have
                                       142

-------
              TABLE 6.7.   COMPARATIVE STATISTICS FOR THE AMOUNT
                  OF WATER NEEDED TO SATURATE THE CLAY LINER

              Time               N         Mean       Std. Dev.
                                                   kg/m3
              Prepond           240         79           36
              At 2 days         240         57           48
              At draining       240         29           45
                     TABLE 6.8.  AVERAGE SWELLING OF CLAY
                           Mean    Std. Dev.      Min     Max      CV
Swelling
36 2.90
mm
1.67
-1.56 9.04
%
57.8
been previously removed.  Possibility of water ponding on the surface of lift
1 and 2 could not be completely ruled out.  Results in Table 6.9 suggest that
water content throughout the clay was essentially constant, deviating very
little from the average.  To monitor incipient drying of the surface, the top
layer was instrumented at 3" (8cm) depth with gypsum moisture blocks and
moisture was measured periodically at 6" (15cm) depth with the neutron
moisture probe.  Both the blocks and the probe were corrected to observed 2"
core readings and checked against subsequent Veihmeier sampling.  To correct
the values, moisture block readings at 3" were multiplied by 31.4/38.1  = 0.83,
while neutron probe readings at 6" were multiplied by 31.4/39.2 = 0.80
assuming particle density of 2714 kg/m3 (Table 5.8).  Values in the numerator
are the average water contents in 2" diameter cores at 0 to 3" and 3" to 6"
depth, while the values in the denominator represent total porosity based on
average bulk density at 0 to 3" and 0 to 6" depth.  The respective changes in
the degree of saturation at 3" and water content at 6" are shown in Figure 6.8.
Because of the sand layer over the surface, drying of the clay liner after it
was drained was very slow.  One year after the liner was drained, drying,
particularly in the surface 3" layer, increased dramatically after cores and
other samples of the clay were taken exposing more clay to the air.

     To evaluate the differences among layers of the clay, paired transects
one foot apart of 2" diameter cores were taken (on 3' centers) East to West
through the middle of the clay liner one foot apart.  The cores were sliced
into twelve, 1" increments to evaluate water content, access tubes were placed
in the holes and density was measured using a dual probe in 1" increments of
                                      143

-------
        TABLE  6.9.    STATISTICS  FOR  THE  2"  CORES.  AVERAGE  AND  BY  LAYER

   Variable     N    Mean    Std.  Dev.      Min     Max     Std.  Error      CV
               45     1681        152        1273     1984          27         9.0
               45     1995        181        1519     2355          27         9.0
               45     18.6        1.3        15.4     23.7        0.19         7.0
               45     31.4        3.5        21.0     41.4        0.52        11.1
               45     1649       146        1166     1991          21         8.9
               45     1964       178        1360     2553          26         9.1
               45     19.0       1.1        16.5     22.7        0.17         6.1
               45     31.4       3.6        19.3     39.0        0.54        11.5
               45     1600       136        1213     1862          20        8.5
               45     1905       162        1490     2233          24        8.5
               45     19.0       1.3        14.8     22.8        0.20        7.0
               45     30.4       3.2        22.1     37.1        0.47       10.5
               45    1638       157        1306    2035         23        9.6
               45    1933       184        1533    2395         27        9.5
               45    18.0       1.5        11.8    20.2       0.22        8.5
               45    29.5       3.6        20.4    36.6       0.54       12.3
Avg
DD
WD
ew
ev

45
45
45
45

1642
1949
18.7
30.7

63
75
0.6
1.5

1479
1760
16.9
27.7

1806
2143
20.2
33.7

9
11
0.09
0.23

3.8
3.8
3.3
5.0
depth.  The primary purpose was to determine if any of the layers contained
higher proportions of stones or else exhibited noticeable zones of lower
density.  For example, visitors suggested that a sheepsfoot roller might have
pushed down stones within a clay matrix creating stony layers at the bottom of
each lift.  No evidence for such a layer was found during the excavations of
various cores.  Figure 6.9 shows the wet and dry density, respectively, for
the transect and Figure 6.10 gives the details of the water content by weight
for the north and south positioned access tubes.  The results shown in these
two figures do not suggest any particular layering within the clay; however,
there appear to be several vertical zones of lower bulk density particularly
noticeable in the wet density (upper) plot.  Except for the wetter conditions
at the clay surface, water contents within the liner showed no preferential
orientation, confirming observations made previously when using 2" diameter
cores.
                                      144

-------
<  90
OT
   80

   70

   60

   5O
zo-20
o uj
        T	1	1	1	T
            11/5/86
                                -i	1	1	1	1	1	1	1	r
                                               3" DEPTH
      9/IO/86
      'o—if* o- o   o   0^.0 tf>«o-cP*'*o-o
                                 ,6" DEPTH
                                              8/24/87
                                                                     5/17/88
                   i   i    i	i	1_
                                       I    I	I	I	1	L_
      SEP       DEC
      I	1986	f
                          MAR       JUN       SEP
                          	 1987	
                                                        DEC
 MAR
-1988
     Figure 6.8.  Changes in  the  degree of saturation at 3"  (8cm)  and  water
                  content by  volume  at  6" (25cm) in the drained clay liner
                  with time.
                                        145

-------
               «ET_DUAL'
                           LIT 2100
                           12150 TO 2200
                           (,-SE. 2250
2180 TO 2550
2200 TO 2250
               BRY.DUW.
                          (•IT  1750
                          , tSOO TO 1850
                           GE  1900
1760 TO 1800
1856 10 1900
Figure  6.9.   An east  to west  transect  of wet  (a) and  dry  (b)
               density  in 1"  (2.5cm) depth increments as
               measured with  the dual  gamma probe on 3'  (91cm)
               centers.
                               145a

-------
                      % NORTH TRANSECT
                    Sw% SOUTH TRANSECT
               Q
               35


                                                 ;;::;: If


                    COREIWT
                              i LT 15
                              i 21 TO 24
                         15 T§ 16
                         GE U
                                                        18 "TO 21
     Figure 6.10.
An east to west transect of water contents by weight  in
1" (2.5cm) depth increments measured gravimetrically.
      The  clay  liner  appeared  to contain many  stones.   In order to quantify the
 spatial distribution of  stones relative to density and permeability posthole
 size  holes  (6"  diameter?,  12"  deep) were excavated  7 to 12" (15 to 30cm) from
 where the 3" cores were  previously taken.   Hole  volume (-100 cm3) was
 measured  by inserting a  thin  walled plastic bag  and filling it with water.
 The solid material was weighed, dried,  and weighed again to compute density
 and water content at each location.   Subsequently,  the soil was washed out
 through the #10  (2mm opening) and #6  (3.35mm  opening)  sieves.  The material
 retained  was classified  as "Rocks" and  their  volume and weight were measured.

      Table 6.10 gives the comparative statistics for posthole data.  The data
 show  that the wet and dry density of  the posthole  material,  although somewhat
 larger, are about the same as those for 3"  and 2"  cores.   However,  proportion
 of rocks by volume was much greater than expected  based in the preliminary
 specifications for this material.  (The B-horizon  of the  Hubblersburg cherty
 silt  loam on the average contains 9.5? by  volume of coarse fragments.)   Such a
 large proportion of rocks, even though it  appears  to be  fairly uniformly
distributed throughout the clay matrix, has a definite  influence  on the
                                     146

-------
            TABLE 6.10.  COMPARATIVE STATISTICS FOR POSTHOLE DATA

Variable               Mean    Std. Dev.     Min     Max    Std. Error
Wet density
Dry density
Water (% by
Water (% by
Rocks (% by
Dry density
Dry density
(kg/ra3)
(kg/m3)
wt)
vol)
vol)
(soil)
(rocks)
2057
1729
19.1
33.0
20.8
1555
2389
104
89
3.0
5.0
2.0
108
48
1782
1450
9.0
15.0
15.0
1248
2176
2354
2020
32.0
52.0
28.0
1888
2703
6
5
0
0
0
7
3
.7
.8
.2
.3
.1
.0
.1
5.1
5.2
15.7
15.0
9.7
6.9
2.0
compacted bulk density.  Because of the high density of rock fragments (Table
6.10) soil fraction less than #10 mesh (2mm) when compacted together with
rocks may be of lower density than called for by the specifications.
Conversely, because little water is retained by rock fragments, the water
content of the soil fraction may be correspondingly larger.  These results
suggest that materials used in the construction of clay liners should have a
specified fraction of coarse fragments retained on the #10 sieve.  For
example, if the clay liner material contained only 5% by volume of the rock
fragments the average density of the soil fraction would have been 1694 kg/m3,
a considerable improvement (97% Proctor) over the mean dry density of the clay
liner soil (89$ Proctor).
                                      147

-------
                                  SECTION 7

                                 DATA QUALITY

DATA ACQUISITION

     Clay soil used as the experimental liner material was a subsoil horizon
of a commercially available cherty silt loam from central Pennsylvania.  On
the average, the clay was compacted wet of optimum to better than 90% Standard
Proctor.  The soil is classified as a CL type having a permeability of 1.10 to
1.76 x 10~° cm/sec as determined in the laboratory with a falling head
permeameter at 90% maximum density (Modified Proctor) and a gradient of about
20.  Mineralogically, the soil clay is predominantly a mixture of illite and
kaolinite with some montmorillonite.

     After the liner was constructed, instrumented, and ponded, water level
was maintained with an automatic constant head tank.  Similarly, each of the
infiltration cylinders and evaporation pans were equipped with a Mariotte-type
constant head, one liter bottle set to the same water level as in the liner
outside.  Individual leachate drains were routed to the outside and leachate
was collected in appropriately sized containers.  Simultaneous readings of
water level changes in a grid of evaporation pans gave the necessary
correction which was applied to ring infiltration data.  Corresponding to each
set of ring and drain data, a set of wet density readings was taken with the
Troxler1 dual gamma probe.  Additional details of clay liner construction and
instrumentation are given elsewhere in this report; here the emphasis will be
on data analysis aspects of the study.  The ultimate purpose is to develop a
capability to describe areal distribution of hydraulic conductivity under
field conditions and to relate it to tests performed in the laboratory on
disturbed samples of clay liner materials, or on undisturbed cores taken from
the liner during construction.  The dilemma is that while the response of the
liner as a whole may be influenced by preferential flow pathways, zones of
discontinuity and zones of higher effective porosity, point laboratory samples
generally are not.

     Using surface probe, volumeter and gravimetric samples, moisture and
density control data were collected during the construction of the liner.
Following construction but prior to ponding, 13 sets of density readings with
dual gamma probe were taken and averaged to provide a priori distribution of
density and available porosity.  Following ponding, changes in density with
time were measured and changes in available porosity were evaluated.  After
the clay liner was drained, core samples were taken to calibrate dual probe
density measurements and to evaluate spatial distributions of coarse fragments
and water.

     On a relative basis, dual probe readings are taken over a volume about
five times the volume considered in the volumeter, while surface probe in the
backscatter mode measures density and moisture over a volume 100 to 200 times
larger than the volume considered in dual probe readings, and 700 to 1000
times larger than measured by volumeter.  The volume of the liner is - 6000 to
                                      148

-------
9000 times the volume measured by the surface probe.  Similarly, the volume of
the experimental liner as a whole is 55 times the volume of all the infiltra-
tion rings combined (250), while the volume assumed associated with each leach-
ate drain (3' x 3' x 1') is - 55 times the volume of each infiltration ring.
The sidewall and endwall drains together represent - 1M the volume of the
whole liner.

     The variability of a property can be described by the probability density
function (PDF) which not only contains information about the averages (mean,
mode, median), but also their other moments, and these permit estimation of
confidence limits for that property.  Identifying the appropriate PDF for a
parameter has important implications in computing the number of observations
required to estimate the mean with a specified precision, and in determining
the integrated response of an area.

     In the traditional analysis of variability, properties measured at a
number of sampling points within an area are assumed spatially independent and
are represented by mean, standard deviation, and an assumed (or estimated) PDF.
However, the assumption of spatial independence in soils, at least for
sampling points close together, seldom holds.  Nonparametric techniques can
then be employed to evaluate the extent of spatial dependence.

     Data quality is both the object and subject of this study.  Quality
indicators of the data collected in this research project are documented to
meet the technical goals of this study.  Table 7.1 describes the primary
methods used and shows tentative data quality indicators for each parameter
measured.  Quality indicators for Density and change in surface elevation are
taken from manufacturers specs for the instruments with which measurements are
made (Figure 7.1).  On the other hand, precision of infiltration, evaporation,
and leaching rates measurements depends to a large degree on the volume of
infiltrate, evaporate, or leachate.  We have found gravimetric method superior
to volumetric when measuring infiltrate and evaporate.  Table 7.2 lists
typical volumes of infiltrate and leachate collected by different means.  For
example, HQQl of water is typically added to a liner daily, while drain
outflows range from 50mil to 208, and infiltrate volumes vary between SOmX, or
less to lOOOmfc.  Unfortunately, slow running rings and evaporation pans have
evaporation losses on the order of 100cc or less with possibility of
corresponding large errors.  Current use of balance and gravimetric method
obviates the need for volumetric measurement with graduated cylinders and
improves the degree of attainable precision.

     According to Lumb (1974) if a specimen of, for example, clay is tested
and there exists a true value e and a corresponding test value x, replicate
testing of the same specimen will give different values of x because of lack
of "precision" of the test being used.  The average of several replicates will
likely differ from the true mean because of lack of "accuracy."  For an ith
replication, test value Xj[ is,

                          xi = a . e + 3 + 61                           (7.1)
                                      149

-------
      TABLE 7.1.   METHODS USED AND CLASSICAL DATA QUALITY INDICATORS FOR
       INFILTRATION, EVAPORATION AND LEACHATE RATES,  BULK DENSITY,  AND
                      CHANGE OF SURFACE ELEVATION (CSE)	
Variable
Units
Method
Precision   Accuracy    Completeness
                                                       % bias
Infiltration
Evaporation
Leachate
Density
CSE
cm/ sec
cm/ sec
cm/sec
kg/m3
mm
Gravimetric
Gravimetric
Volumetric
Nuclear probe
Laser beam
± 1
± 1
± 5
± 0.32
± 0.05
± 2
± 2
± 2
± 1
± 1
99
99
99
99
99
        TABLE 7.2.  PERCENT ERROR AS A FUNCTION OF VOLUME OF LEACHATE

        Volume            Error
          20
          15
          10
           5

           5
           4
           3
           2
           1

         0.80
         0.40
         0.20
         0.05

         1.00
         0.80
         0.40
         0.20
         0.05

          100

          400
           3.6
           2.4
           2.1
           1.4

           1.4
           0.7
           0.7
           3.5
           7.1

           2.7
           1.6
          10.0
          10.0

       1.0 to 2.6
           3.3
           1.3
          11.0
          22.0

           9.5

           2.3
              Bucket, drains
              Beaker, drains
              Graduated cylinder, drains
              Graduated cylinder, rings
               Sum,  sidewall  drains

               Liner,  tank
                                      150

-------
       PERFORMANCE  DATA
      MODEL
                                          3862MP8
       WEIGHING RANGE
   I6.500g
       READABILITY
   O.lg
       STANDARD DEVIATION
       (REPRODUC1B1LITY)
   ItO.OSg
       MAXIMUM LINEARITY DEVIATION
   i±O.I5g
       TARRING RANGE (BY SUBTRACTION)
   I6,500g
       MEASURING TIME
   2s
       INTEGRATION TIME
   4 OPTIMIZED DIGITAL FILTERS
       DISPLAY SEQUENCE
   O.I...0.4s (SELECTABLE)
       AMBIENT TEMPERATURE RANGE
       (O°C... + 40°C)
   273K...3I3K
       SENSITIVITY DRIFT (AMBIENT
       TEMPERATURE RANGE (283K...3O3K)     =12-IO~6/K
       LINE VOLTAGE (SELECTABLE)
   IOO/I20/220/240V, -I5%...-HO%
       FREQUENCY
   50-60 Hz
       CONSUMPTION
   15 VA
       DATA OUTPUT (OPTION)
   RS 232/V24-V28/RS 423 V10;
   7 BIT; PARITY EVEN, ODD, MARK,
   SPACE; TRANSFER RATES
   150 TO 9600 BD.
              Figure 7.1.   Gravimetric balance performance data.
where 6 is a random variable of zero mean and with variance V(<5).
of a large number of such tests gives an expected value E(x),
                            E(x)
e +
                            The average
(7.2)
a and $ express bias,  or lack of accuracy,  V(6)  represents  the  lack  of
precision.  In a study such as this one,  it is difficult to determine bias
factors a and & unless an absolute way of measuring e is available.
Occasionally e is inferred from calibration or model tests  but  bias  effects
are mixed since they may be due to a model or to a test.  Changes  from  speci-
fied test conditions may introduce deviations in the results which can  be
interpreted as either  bias or precision factors and which include  such  effects
as machine, operator,  or interaction effects.  The above procedure is diffi-
cult to apply to a study such as ours which attempts to  evaluate distributions
of changes in density  and surface elevation of water as  well as infiltration,
evaporation, and percolation rates both spatially and in time for  a  prototype
clay liner.
                                      151

-------
     Accordingly, novel data quality indicators need to be developed to be
used in the field by field personnel on a large scale, this study's 10 x 24
sampling matrix simulating actual liner conditions.  One objective of this
study was to design acceptable field QA/QC plan.  Thus, even though 250,
1000cc constant head bottles can probably be filled with less than \% error (±
10mX,), this error increases as the volume added decreases, i.e., if only 10mX,
were needed to be added we could easily have a 100% error.  One way to cope
with this problem is to have constant head bottles and leachate drains that
are run slowly being left on for longer time periods so that the total volume
added can be measured with precision 3% or better.

     The second aspect to remember (and this also pertains to Density and CSE
parameters) is that each set of measurements in this study is not an independ-
ent sample but a part of continuous time series distribution, each succeeding
value highly correlated with the preceding ones.  Consequently, QA/QC plan
outlined here will rely heavily on developing appropriate criteria and
methodology of data collection and analysis.

     It should also be remembered that a single point sample in this study
(infiltration, leachate, evaporation, density, or CSE) cannot be replicated
and has no meaning per se.  Replication consists of additional (250) compara-
tive samples taken over an area at approximately the same time assuming spa-
tial stationarity.  To be comparable, such samples need to be easy to obtain
and require a relatively short collection period.  Quality of the data is
dependent on proper equipment operation (density and CSE), or operator's
repetitive ability (infiltration, evaporation, leachate).  We have found, for
example, that our technicians can fill 1000m£ constant head bottles used in
measuring infiltration with better than \% precision and within 2% error
between different operators.  How well could other operators function or be
expected to function under field conditions?  To get answers to some of these
questions, in this study, the sampling is carried out on regular grids.  The
liner, although large, is essentially a prototype of a field scale facility.
Details of procedures used and data reduction are summarized in the following
sections.
Analytical Procedures

Density—

     Use Troxler^ dual gamma probe.  Measure at 2MO locations once a week.
Take standards at the beginning of each new tube, the reading is to agree
within 200 counts with the previous standard reading.
CSE--

     Use optocator equipment, take readings in 36 locations once a month.
Make sure standards are carefully read.  Map (on each pedestal) where the
readings are actually being made.
                                       152

-------
                    or
(This is a one time set of observations)
Leachate Drains—

     Measure individual outlets at 250 locations when needed, report as once a
week cumulative reading (Friday),  for individual drain grid (8 x 23) and for
combined sidewall drains.   Once a  month take samples for chemical analysis
from drains:  AA-0, D-2, F-7, K-6, L-6, 0-9, P-5, T-3, Ponded water, Tanker,
at 9 and at 12 months take samples from all the drains.

     Analyze according to "Standard Methods of Analysis of Water and
Wastewater" for Temp,- EC,  pH and bicarbonate at the site, send to University
Park for analysis of N03,  804, Na, K, Ca, and Mg.


Infiltration Rings-

     Read as needed by adding preweighed water carefully through a small
opening in a stopper with a funnel.  Report combined total weekly (every
Friday).  General procedure:

     a) Remove siphon line, close  it with a nail, and place between two glass
        tubes.

     b) Remove "00" stopper, add measured amount of water through a funnel up
        to one liter mark.

     c) Close carefully the small  "00" stopper, replace line in the ring, make
        sure the system operates properly.  Do not move bottle or large
        stopper unless absolutely  necessary.  Water level to be the same as on
        the outside in liner.  To  check, place tube outside the ring, tilt
        bottle slightly, the bubbler should now engage.  Reweigh containers
        from which water was added.
Liner—

     Measure as needed amounts of water used by liner.
value weekly (every Friday).
                     Report cumulative
Evaporation—

     Measure large pan and small pans on the same schedule as rings.
     P.S.  Place brass pins inside rings level with water, use as a quick
check to see if bubblers are working properly.
                                      153

-------
Data Reduction, Validation and Reporting

     Field data was recorded on field data collection  forms.   Any subsequent
needed transformation or summaries were performed on the  micro- or mainframe
computers.  Data reduction and processing flow chart is shown in Figure 7.2.
                      Density
                    (Transform)
                   Rings/Drain*
                     (Rates)
--.

( START )
\
'
Apple Data
I/O
'

Store Apple
Disk
i

r
Transfer
to PSU
I
1
Variogram
i
t
Krlg
i
1
Individual
Graphics
i
t
Composite
Graphics
i
?
Report
Summaries
1
t


t
\
S
\
\
/
/
/
/
1

Apple
Graphics

Optional
Analysis/Plot

SAS/SUR2/
Custom
Versa:Raster

                                   C STOP )
                    Figure 7.2.   Data processing flow chart.
                                       154

-------
     An Apple lie microcomputer was used to enter the data and create  data
files in a format for transfer to The Pennsylvania State University mainframe
computer.  This was done as soon as possible after the data were taken.

     Density data was transformed on the Apple computer from counts to kg/m3
using the equation

         Density = (1756.0956 + (-625.7235 • loge(count/std))J

where

         Std = average values of standard count.
         Density is computed to an Integer value.

     Inflow/Outflow were computed as rates on The PSU system using the formula

         Rate = volume/(area • time)

where

         Volume was the volume adjusted for evaporation, time, etc.
         as necessary.

         Ring area = 613.1190 cm2 - drain area = 8361.2736 cm2

         Time = seconds between successive measurement.

At the conclusion of the study exact areas of infiltration rings were
evaluated using preweighed water and laser beam optocator for sensing level
changes.  These were the ring areas used in final analysis.  Each ring was
also checked for leaks using fluorescein.  Only those rings which had no leaks
were used in analysis.

     The field facility is a two-dimensional matrix and the data are kept in
formats that allow for printout to screen and hard copy in a two-dimensional
format.   All field forms must have a value in each cell.  Data transfer from
the field site to PSU presents the data in a 24 x 10 or 25 x 10 matrix and
allows for easy edit of data format.

     Due to the nature of this data, outliers were hard to define.   Any value
strongly suspected of being in error was treated as a missing value; however,
this value is carried in computations until sufficient justification is
accumulated to remove it from the data base,  or correct it.

     Statistical analysis was the major editing activity to validate correct
data entry.  Printouts provide maximum, minimum, and variance values.   These
values were expected to be within known limits and to follow similar patterns.
Any deviation from these limits and patterns required checking of the data set.
It is not feasible to check each value at each data step.   Since 250 drain
values were taken daily with a recording step,  Apple data entry step,  a PSU
transfer step,  and data setup step,  i.e., there were 250 x 5 x 4 =  5000
possible data checks during initial data collection of one weekly set of
values.


                                      155

-------
     The software developed for data reduction incorporates known limits to
edit the data during entry and processing.  Programs developed for the Apple
lie check for such items as negative values, non-numeric data, and values
outside upper and lower limits are postulated.


Internal QC Checks

     Density measurements used Troxler^ standards to calibrate and check
instrument operation.  After initial data analysis these standards were
required more frequently.  As a minimum the operator must take a standard at
the beginning of each access tube.

     Inflow measurements required a visual measurement and ten quality samples
have been included on which the technician repeated the same process as on the
data samples.  These samples were routinely checked for accuracy to provide a
percent error expected due to visual measurement volume cutoff.  Evaporation
data was treated similarly to infiltration rings.

     Inflow/outflow flux rates were measured using either volumetric contain-
ers or a balance.  Appropriate equipment checks such as standard weights for
balances and cleanness of graduated cylinders, were used on a regular basis.

     CSE measurements required an internal standard on a fixed rigid stand and
five additional standards permanently mounted to the wall of facility, to
check on the mobile platform performance.

     Chemical analyses were not involved in any significant measurements with-
in this study.  However, in leachate and Br~ tracer analysis, standard methods
and procedures were followed.

     Volumetric devices used to measure flow rates were calibrated using
laboratory volumetric glassware of a grade traceable to National Bureau of
Standards for accuracy.  In some cases weight measurements were used in lieu
of volume to obtain liquid quantities; in these cases a balance of known
accuracy was used.  The balance was regularly calibrated in accordance with
the manufacturer's directions.

     In-house proficiency testing was accomplished by periodic checks of water
volume measurements for uniformity and consistency among inflow and outflow
measurements from the clay liner system.  In addition, different individuals
double checked raw data on a periodic basis.

     The capability and performance of the total measurement systems was
determined by intercomparison of data collected by the several parametric
measurement systems installed within this study.  For example, inflow/outflow
measurements or density evaluation using nuclear probe and core data.

     Technical systems audits were part of the research effort.  In order to
ensure that the best data possible were being collected, newer or better
monitoring apparatus or systems were implemented if it was determined that
better data could be obtained.
                                      156

-------
     A performance evaluation audit was made as part of the ongoing data
interpretations.  Examination of data trends and differences obtained over
time was used to determine whether any changes in data generating systems were
occurring which adversely affected data quality.

     Examination of data collected during the course of this investigation
will provide an opportunity to develop precision and bias information with
respect to variations of flow of water through compacted clay soil over a
large area.  Data completeness is simply defined as obtaining flow measure-
ments from each installed inflow and outlet.  It is possible that at other
locations resource constraints mandate that fewer points be sampled.

     Spatial variability can be systematic or random.  Systematic variability
is a change in clay liner properties as a function of compaction effort,
initial water content, and management.  While, in general, spatial variability
will increase as the size of the area increases, maximum variability of
individual properties may occur within a readily definable and at times small
area.  It thus appears that many soil variables may be considered continuous
at least within a certain size area.

     The data being generated within this research study will be used to
describe the spatial variability of hydraulic conductivity of water over the
experimental area.  This study represents the first known attempt to conduct
such an spatial study, and thus the data generated is specifically representa-
tive only of the soil and construction included within this research project.
Caution must be exercised when applying the ultimate results of this research
to other soils, systems, constructions, and measurement devices.  The results
of this work demonstrate soil hydraulic variability in a way which is useful
to both the USDA and the EPA from the standpoint of better understanding
spatial variation in soil properties.


Final Density Check

     Clay liner dual probe densities were originally recorded by a technician
on field sheets.  This data was entered onto Apple lie diskettes.  The program
used to compute and record the computation to disk contained computer code to
check the input standard counts and dual probe counts for upper and lower
limits.  The standard counts check worked well, as acceptable limits had been
defined.  This also provided a structure that kept the data entry person in
data sequence.  The dual probe counts check had a limit that was larger than
necessary for the upper limit, which allowed values to enter the data sets
that were in error, but detected by data checks during data processing.
During initial computations, outlier values were checked for accuracy, errors
were corrected as found, and new statistical computer runs were processed.

     This initial data checking has removed any gross data errors and provided
good quality data for preliminary and quarterly phase reports.  The final data
base was edited for errors not previously identified.  Prior to this editing
all density values ranged between 1900 and 2500 kg/m3.  Three methods were
used to check the data for entry accuracy, outliers and precision.
                                      157

-------
     Method 1  was to select five of the 80 data sets (Table 7.3) which were
reentered into the Apple lie and new printout of wet density was created.  The
original printout and the new printout were compared and errors were
identified.  The five data sets selected were one from the pre-pond time
period, three from the ponded time period (a random selection from each four
month time interval between March 1985 and April 1986), and the last post-pond
data set.

     At the completion of this method three errors were found in five data
sets.  The error of greatest magnitude was a value of 2111 kg/m3 instead of
2103 kg/m3.  This error was within the measurement error of the instrument.
Another error of concern involved using the wrong standard counts from the
field sheet.   This actually was a field sheet problem and not totally the
fault of the data entry person.  This method indicated that less than 0.5%
data contained errors and that each error was less than 0.5% of data value.

     Method 2 was a statistical/graphical check.  The graphical check allowed
visual inspection of density and ring/drain flow rates.  A plot was made of
each site for the ring/drain inflow and outflow.  The density on the east and
west of each ring/drain site were also plotted on the range plot.  (NOTE:  The
ring/drain on the east and west edge of the platform were matched to the A and
X density rows.)  This produced graphs of the data and identified some
inconsistent data values which were checked and corrected if necessary.  This
procedure identified values that were within the expected range but deviated
from the site trend.  As an example, a site may have generally had a density
value near 2100 kg/m3 and then a value of 2350 kg/m3 would appear.

     This graphical check was then processed as a statistical check.  Each
observation for a site was subtracted from the preceding measurement.  Differ-
ences greater than 99 kg/m3 were flagged.  The need to check the accuracy of
the flagged values was evaluated.  The data were printed in a table by date
and by site (Table 7*4).  A table of differences was also printed.  After
identifying the flagged differences, the associated density values were
flagged in the density table.  The eight values surrounding the value were
then used to evaluate the need to check this value.  If the difference between
this value and the eight values was greater than 99 kg/m3 then this value was
                    TABLE 7.3.  DENSITY DATA SELECTED FOR
                               OC/qA VALIDATION

                                     Data Collection
                    Set        Date Start       Date Stop
1
2
3
4
5
2/ 7/1985
5/17/1985
10/30/1985
3/10/1986
8/ 4/1986
2/13/1985
5/23/1985
11/4/1985
3/12/1986
8/18/1986
                                      158

-------
                       TABLE 7.4.  EXAMPLE OF DENSITY
                                 DATA RECORD

                                            Site
                     Date            024     025     026
85/10/18
85/10/25
85/11 /OH
2185
2203
2244
- Kg/Hi-1
2181
2441
2125
2177
2156
2130
checked.  (NOTE:  One of the eight values was what caused the flag, so the
value was only compared to seven values.)  This procedure checked the data for
consistency to the adjacent measurements and to the preceding and following
observed values.

     Patterns of flagged values were then evaluated for the site.  Any value
that seemed to deviate from a pattern was validated.  An example of a pattern
is a site that has a few values near 2200 then a value near 2300 then a few
values near 2200 then a value near 2300 again.  Data with a pattern such as
the above was accepted as valid.

     During the flagging process, two types of flags were noted.  One type was
a single value where the difference would make a one time change exceeding the
flag limits (99 and -99 kg/m3) and the density would remain consistent
thereafter.  This appeared to be an artifact of the probe count.  The second
type was a pair of values with opposing differences.  The first would be a
change in one direction (99 kg/nP) and the second would be in the opposite
direction (-99 kg/m3) such that the sum of the difference would be about zero.
These values frequently were found as errors or were inconsistent with the
remaining site data.

     The flagged values (Table 7.5, Table 7.6) were classified after identifi-
cation and as expected the calibration and background data collected prior to
ponding are valid and consistent.  The data collected after the second repair
of the Troxler instrument are valid and consistent.  The data collected prior
to the first and second repairs contained most of the flagged data.  Standard
count measurements during these three time intervals reflect the same pattern
and were the quality control measures which the factory used to determine the
need for repair.
                                      159

-------
                         TABLE 7.5.   GROUPING SUMMARY

                                       Count      Errors
Single Flag
Paired Flag
51
21
3
5
            TABLE 7.6.   SUMMARY DENSITY FLAGGED VALIDATION  VALUES
Total Measurements
Flagged Measurements

Errors
  Totals Summary

19200
  100
    8

  Time Summary

   Flag Values
80 data sets at 240 measurements
0.525J of all dual probe
  measurements
0.04? total; 8.00? flagged
                                  10
                                  36
                                  13
                                  32
                                   9
       (11)'
       (9)
          **
                                                   Months
        3
        2
        2
       14
        1
Number Errors
 Identified

      0
      1
      0
      7
      0
Calibration
Pond/1st repair
1st/2nd repair
2nd/postpond
Postpond (2 sets)

 *First week after ponding
  After water removal
                                 Flag Summary

Site  Count  Site  Count  Site  Count   Site  Count  Site  Count  Site  Count
002
003
005
007
017
018
024
025
026
030
031
1
2
2
1
1
1
5
2
2
3
1
033
045
061
080
082
084
087
088
100
118
120
1
1
4
1
1
1
2
1
4
2
1
122
216
128
133
134
138
139
148
150
153
154
1
1
3
2
1
2
1
2
1
1
1
156
158
167
168
176
182
183
188
189
190
197
1
1
3
2
3
3
1
1
1
1
1
198
200
202
203
217
218
222
223
224
225
228
2
1
1
3
2
2
1
2
4
2
1
                                                                   232
                                                                   236
                                                                   237
                                                                   240
                                            1
                                            1
                                            2
                                            1
                                      160

-------
     The method of data collection for this study allowed for only one measure-
ment because of time and technique constraints.  Improved data quality assur-
ance would have been obtained by echo printing to hard copy the input data.
Due to the intensity of data collection, it was not possible for the current
man power to check all data entered at the time of data entry.  However, after
data collection terminated, all the data could have been checked and corrected
in a few weeks.

     Method 3 is related to dual probe precision.  Although no two consecutive
measurements at a point were taken at the same time, sets of 240 measurements
were being continuously taken during the study.  Consequently, comparison of
differences observed for adjacent dates gives an estimate of precision.  Such
comparison was run with the following results:


                                PREPOND

                                                       (kg/m3)

         Mean difference between consecutive dates      -0.21
         Mean standard deviation between consecutive
              dates                                      2.30
         Observed maximum between consecutive dates      8.67
         Observed minimum between consecutive dates     -7.25

                                PONDED

         Mean difference between consecutive dates       0.33
         Standard deviation between consecutive dates    0.68
         Observed maximum between consecutive dates      3.05
         Observed minimum between consecutive dates     -1.44


     Taking the observed average maximum of 7.96 kg/m3 and an average reading
of about 2189 kg/m3 precision error would be on the order of 0.36% compared to
0.32$ given in the probe calibration chart (enclosed).


Inflow/Outflow Balance

     Table 7.7 gives the difference between total inflow and outflow on days
when both were sampled together.  On the average the difference was 4   7.9%.
Statistical Stability Tests

     Table 7.8 shows an example of a statistical stability test on a surface
probe during the final readings of moisture and density on a drained clay
liner.  Table 7.9 shows an example of a personnel check during inflow
measurements.  Finally in Figure 7.3 distribution of standard counts for the
dual density probe is given for a whole study period.  Following the initial
repair the standard count stayed essentially constant.
                                      161

-------
TABLE 7.7. MASS BALANCE OF INFLOW AND OUTFLOW OF
Date


850620
850627
850702
850711
850718
850725
850801
850808
850815
850822
850829
850905
850912
850919
850926
851003
851010
851017
851 024
851031
851107
851 111
851121
851129
851205
851212
851219
851226
860102
860109
860116
860123
860130
860206
860213
860220
860227
860430
860522
860530
860630
860731


Inner
Inflow
- Rings
Open Ar<


ea Liner


Inner
Outflow
Drains
Outer
CLAY LINER WATER


Liner
,o-7

0.00
15.51
15.03
U.76
17.12
17.76
18.63
19.37
19.93
21.31
22.28
22.92
24.13
25.28
25.76
26.31
26.66
26.38
26.86
27.32
27.09
27.31
27.49
27.94
27.95
28.03
28.22
28.34
27.97
27.46
27.09
26.68
26.31
25.96
25.49
25.04
24.67
20.85
20.01
0.00
0.00
0.00

0.00
34.50
34.65
29.70
30.17
31.01
31.67
33.78
35.20
37.10
38.50
40.18
41.90
43.77
45.19
46.93
48.73
50.02
51.46
52.59
54.53
53.89
54.72
55.68
56.28
56.99
56.96
57.29
57.13
56.76
56.14
55.58
54.98
54.43
53.98
53.66
53.22
49.79
49.44
0.00
0.00
0.00

0.00
32.68
32.79
28.21
28.78
29.59
30.25
32.24
33.58
35.41
36.75
38.34
39.99
41.78
43.12
44.76
46.44
47.60
48.96
50.03
51.80
51.23
52.00
52.91
53.46
54.12
54.11
54.41
54.25
53.88
53.29
52.74
52.18
51.65
51.20
50.88
50.46
48.11
47.73
0.00
0.00
0.00

0.00
13.65
13.16
13.52
13.57
13.73
13.92
14.30
14.66
15.03
15.43
15.78
16.24
16.91
17.53
18.09
18.71
19.19
20.06
20.76
21.39
21.99
22.69
23.34
23.81
24.37
25.17
25.51
25.43
25.25
25.10
24.92
24.78
24.67
24.54
24.41
24.32
23.71
0.00
23.39
23.17
23.09

0.00
96.78
93.31
95.88
96.25
98.58
101.43
104.09
107.77
111.45
114.22
117.32
120.83
123.09
125.82
128.19
130.72
133.28
135.36
136.43
136.56
136.76
136.95
137.72
137.12
135.94
134.41
132.73
130.50
128.05
125.75
123.49
121.14
119.09
117.06
115.04
113.03
100.50
0.00
91.73
88.09
81.36

0.00
35.60
34.32
35.26
35.40
36.13
37.02
38.00
39.24
40.48
41.51
42.58
43.85
44.94
46.12
47.16
48.28
49.31
50.50
51.29
51.79
52.29
52.86
53.54
53.73
53.83
54.01
53.81
53.17
52.39
51.68
50.95
50.22
49.60
48.97
48.34
47.74
43.98
0.00
41.43
40.31
38.47
Average
Difference

*1

- 8.2
- 4.5
-20.0
-18.7
-18.1
-18.3
-15.2
-14.4
-12.5
-11.5
-10.0
- 8.2
- 7.0
- 6.5
- 5.1
- 4.0
- 3.5
- 3.0
- 2.5
+ 0.02
- 2.0
- 1.6
- 1.2
- 0.5
+ 0.5
+ 0.2
+ 1.1
+ 2.0
+ 2.8
+ 3.1
+ 3.5
+ 3.9
+ 4.1
+ 4.6
+ 5.3
+ 5.7
+ 9.4




4.0±7.9
Inflow-Outflow
1 Pernenl
t rHff«r»fl
nr>e •

V 1
nn


.Outflow
         162

-------
TABLE 7.8.  STATISTICAL STABILITY AND DRIFT TEST - SURFACE MOISTURE GUAGE
N/T Moisture
Number Std Cts
m
1
2
3
4
5
6
7
8
9
10
11
12
13
14
15
16
17
18
19
20
n
/T
431
427
415
420
428
431
426
424
424
427
434
427
427
419
426
432
436
430
425
425
= 427.7 I
= 20.66 6
Error
E=(n-n)
4.3
.3
-11.7
- 6.7
1.3
4.3
- .7
- 2.7
- 2.7
.3
7.3
.3
.3
- 7.7
- .7
5.3
9.3
3.3
- 1.7
- 1.7
= 480.20
" /3I-
N/N-1
Ratio = .24
Test
Number
1
2
3
4
5
Avg.
Moisture
Std Cts
428
426
430
424
430
427.6
Difference = 426.7-427
Total

Drift

Avg. = 426.7+427
= 427.15
- ~'9 = -.?!%
427.15








.6 = -.9
.6/2



E^ Density
Std Cts
n
18.49 3199
.09 3186
136.89 3176
44.89 3198
1.69 3183
18.49 3199
.49 3175
7.29 3182
7.29 3170
.09 3175
53.29 3164
.09 3179
.09 3199
59.29 3172
.49 3173
28.09 3202
86.49 3171
10.89 3182
2.89 3186
2.89 3185
n = 3182.8
pr- = 56.42
5.03 >/ n
Ratio = .20
Density
Std Cts
3180
3179
3188
3180
3170
Avg. 3179.4
Difference = 3182
Total Avg. = 3182
= 3181
Drift = 1-7
3181.1
Error
E=(n-n)
16.2
3.2
- 6.8
15.2
.2
16.2
-•7.8
- .8
-12.8
- 7.8
-18.8
- 3.8
16.2
-10.8
- 9.8
19.2
-11.8
- .8
3.2
2.2
I = 2465.
6- nr
x/N-1









.8-3179.4 =
.8+3179.4/2
.1
.05$

£2
262.44
10.24
46.24
231.04
-.04
262.44
60.84
.64
163.84
60.84
353 .M
14.44
262.44
116.64
96.04
368.64
139.24
.64
10.24
4.84
2
= 11.39









1.7




                                     163

-------
       TABLE 7.9.  PERSONNEL CHECK. INFLOW MEASUREMENTS

Site       Wt. Empty                       Wt. Filled to Line
       Technician #1 filled and Technician #2 weighed
                            (Ibs)

  1          0.45                          2.66
  2          0.44                          2.65
  3          0.45                          2.65
  4          0.41                          2.63
  5          0.41                          2.64
  6          0.40                          0.64
  7          0.39                          2.63
  8          0.43                          2.64
  9          0.40                          2.60
 10          0.40                          2.62
             0.418±0.023 (5.5%)            2.636±0.017  (0.

       Technician #1 filled and Technician #2 weighed

  1          0.48                          2.62
  2          0.46                          2.60
  3          0.46                          2.65
  4          0.49                          2.65
  5          0.48                          2.64
  6          0.49                          2.66
  7          0.47                          2.65
  8          0.48                          2.63
  9          0.47                          2.64
 10          0.49                          2.67
             0.477±0.012 (2.5%)            2.641 ±0.020  (0.
                               164

-------
                            STANDARD COUNTS: DENSITY
                                  1200     1600
                                 SAMPLE  NUMBER
                                     2000
2400
2800
 Figuare 7.3.
Distribution of dual density probe standard counts  during the
study period.
Number of Samples

     Figure 7.4 shows the standard error of the estimate as a function of the
number of observations for ring infiltrometers.  For example, approximately
100 samples would need to be taken to keep the standard error below 25 x 10"?
cm/sec, but only 20 to keep it below 5 x 10"? cm/sec.   Table 7.10  and Figure
7.5 shows the comparisons of the relative number of samples required to attain
a given degree of accuracy.  The standard error is expressed here  as a
percentage of the mean for 5, 10,  25, and 50 random samples from a population
of N observations.  Comparisons include density and water content  observations
as well as flux and hydraulic conductivity measurements.   Ring,  drain, and
laboratory values of hydraulic conductivity follow a pattern similar to that
shown in Figure 7.4.  Optimally, to reduce standard error to less  then 25% of
the mean 20 to 25, observations would be needed in our case.  Even if all the
observations are utilized (N), standard error did not  appear to  drop much
below 10$ of the mean at best.  In contrast, both density and water content
would require the same number of samples to keep the relative standard error
in the \% to 2% range for all except the surface probe water content values
(2% to 4$).  Thus, on a field scale clay liner far fewer  (in our case   1/10
as many) samples of density and water content are needed  than hydraulic
conductivity to characterize the system with the same  degree of  precision.

     For infiltration measurements, the cutoff point for  our data  appeared to
be 10 to 20 samples.  The question is:   over what area?  The study represents
2250 ft2 plot of land (5/100 of an acre)  suggesting that  for best  results we
might need to have permeability measurements on the 15'  x 15'  grid.   The soil
material from which the clay liner was constructed,  water content,  and
construction techniques were quite variable,  both spatially and  in time.   It
is possible that with more homogeneous material and water content
distribution,  fewer sampling locations may be necessary.
                                     165

-------
                         40         60

                  NUMBER  OF OBSERVATIONS
100
Figure 7.4.  Standard error of estimate as a function of the number of
           observations for ring infiltrometers.
                             166

-------
    TABLE 7.10.  COMPARISON OF THE RELATIVE VALUES OF STANDARD ERROR"1 FOR
    	DENSITY. MOISTURE. AND HYDRAULIC CONDUCTIVITY MEASUREMENTS
No. of Samples
10
25
50
N
Dual Probe
                                        % of the mean
Wet density
3" Core
Dry density
Wet density
Water by wt
Water by vol
Surface Probe
Dry density
Wet density
Water by wt
Water by vol
Hydraulic Conductivity-K
Drains^
Sum drains3
Sum rings
Laboratory
1.58

2.90
2.71
1.09
1.80

1.63
1.45
3.04
2.66

34.0
54.0
62.0
50.0
0.92

1.76
1.69
0.93
1.53

1.92
1.36
4.90
3.60

25.0
36.0
51.0
36.0
0.57

1.00
1.04
1.10
1.56

1.20
0.80
3.16
2.20

25.0
21.0
29.0
31.0
0.42

0.67
0.68
0.95
1.14

0.78
0.51
2.01
1.37

22.0
20.0
25.0
23.0
0.24/240

0.28/240
0.28/240
0.35/240
0.44/240

0.42/264
0.32/264
0.81/264
0.52/264

9.8/193
9.4/193
13.7/193
16. 3/ 95
1(Standard Error/Mean) x 100.

2Based on drain flux at 1  yr after ponding.

3Based on drain flux averaged over time (9 mos).
                                      167

-------
            LJ
            U
            CC
            LJ
            O.
            O
            O
            < 3
            UJ
            a:
            O
            o:
            IE
            lu
            Q 2
            cc
            <
            o
            z
                                            WATER CONTENT

                                       SURFACE PROBE, WATER BY WT.
                                     v SURFACE PROBE, WATER BY VOL.
                                     • 3" CORES, WATER BY WT.
                                     o 3" CORES, WATER BY VOL.
                                               SURFACE PROBE.
                                               WATER 8Y WT.
                  SURFACE PROBE
                  WATER BY VOL.
   3 CORES, WATER BY VOL   °
                                          3"CORES, WATER BY WT.
                        DENSITY
» DUAL PROBE, WET DENSITY
o 3" CORES, WET DENSITY
• 3" CORES, DRY DENSITY
a SURFACE PROBE, WET DENSITY
v SURFACE PROBE, DRY DENSITY
                                                SURFACE PROBE, DRY
                 SURFACE
                 PROBE, WET
                                           DUAL  PROBE
                 HYDRAULIC CONDUCTIVITY
             50
         * LABORATORY
         a SUM RINGS
         • DRAINS
         0 SUM DRAINS
                  DRAINS
                                                SUM DRAINS
                      10
                                    25
                              NUMBER OF OBSERVATIONS
                                                              50
Figure 1.5.   Relative values  of the standard error as  a function
                of the number of observations  for  density, water
                content, and hydraulic conductivity measurements.
                                      168

-------
                                  LITERATURE

     The literature reviewed (Phase I)  was  divided into six categories.   Each
book or article was first evaluated and classified on a literature review
sheet and subsequently logged on the computer.   The following table shows the
appropriate review categories followed  by the  list of references.


                     	Review Categories       	  	
               Class I       Background Material
                              a)  general  chemistry
                              b)  general  physics,  soil physics
                              c)  soil  chemistry
                              d)  clay

               Class II      Hydraulic  Conductivity Measurements
                              a)  saturated
                              b)  unsaturated
                              c)  laboratory
                              d)  field
                              e)  clay
                              f)  organic  fluids
                              g)  factors  influencing
                              h)  calculated

               Class III     Solid and  Hazardous Waste
                              a)  background
                              b)  case  histories
                              c)  design
                              d)  regulations

               Class IV      Clay  Liners
                              a)  problems
                              b)  suggestions and recommendations

               Class V       Geostatistics

               Class VI      Scaling
                                     169

-------
                                 REFERENCES

Adams, J.E., Kirkham,  D.  and Nielsen, D.R., 1957, A Portable Rainfall
     Simulator Infiltrometer and  Physical Measurements of Soil  in Place,
     SSSAP, Vol 21,  No 5,  p 473-477, Rev  (183), Class  (ID).

Ahmed, S., Lovell Jr., C.W. and Diamond, S.,  1974, Pore  Sizes and Strength of
     Compacted Clay, ASCE:  J of the  Geotech Div, Vol 100, p 407-425, Rev
     (381), Class (Ilg).

Ahuja, L.R., Green,  R.E.,  Chong,  S.K. and Nielsen, D.R., 1980,  A Simplified
     Functions Approach for Determining Soil  Hydraulic Conductivities  and
     Water Characteristics In Situ,  Wat Res Res, Vol 16, No 5,  p 947-953, Rev
     (119), Class (Ilh).

Al-Dhahir, Z.A. and Morgenstern,  N.R.,  1969,  Intake Factors for Piezometer
     Tips, Soil Sci, Vol 107, No  1,  p 17-21,  Rev  (84), Class  (Ilg).

Al-Dhahir, Z.A. and Tan,  S.B., 1968, A  Note on One-Dimensional  Constant-Head
     Permeability Test, Geotechnique, Vol 18, p 499-505, Rev  (67),  Class
      (He).

Aldabagh,  A.S.Y. and Beer, C.E.,  1971,  Field  Measurement of Hydraulic
     Conductivity Above a Water Table with Air Entry  Permeameter,  Trans of
     ASAE, Vol 14, No 1 ,  p 29-31, Rev  (23), Class (lid).

Alemi, M.H., Nielsen, D.R. and Biggar,  J.W.,  1976,  Determining the Hydraulic
     Conductivity of Soil Cores by Centrifugation,  SSSAJ,  Vol 40,  p 212-218,
     Rev  (245), Class (Ilb.c).

Allison,  L.E., 1947, Effect of Microorganisms on Permeability of  Soil  under
      Prolonged Submergence, Soil Sci,  Vol 63, P 439-450, Rev (417), Class
      (Ilg).

Amer,  A.M. and Award, A.A., 1974, Permeability of Cohesionless Soils,  ASCE:
      J of the Geotech Div, Vol 100, No GT12,  Rev (24), Class (Ilg).

Anderson, D., 1982, Does Landfill Leachate Make Clay Liners More Permeable?,
      ASCE-Civil  Engineering, Vol 52.,  No 9, pg 66-69, Rev (12), Class (Ilf).

Anderson, D.C.,  Brown, K.W.  and Green,  J., 1981, Organic Leachate Effects on
      the  Permeability of Clay  Liners,  Nat'l Confer on Management of
      Uncontrolled Hazardous  Waste Sites, Rev  (189), Class (Ilf.a.c).

Anderson, D.M.  and  Low,  P.F.,  1958, The Density of Water Adsorbed by Lithium-,
      Sodium-,  and Potasium-  Bentonite, SSSAP, Vol 22 p 99-103, Rev  (294),
      Class (Id).

 Anderson, J.L.  and  Bouma,  J.,  1973, Relationships Between Saturated  Hydraulic
      Conductivity  and Morphometric  Data of an Argillic  Horizon, SSSAP, Vol
      37,  p 408-413, Rev  (382), Class (Ilg).

 Anonymous, 1981,  Land Disposal Survey, Waste Age, Rev (13), Class  (Ilia).


                                       170

-------
Arya, L.M.,  Farrell,  D.A.  and Blake,  G.R.,  1975,  A  Field  Study  of  Soil Water
     Depletion Patterns in Presence of Growing Soybean Roots: I. Determination
     of Hydraulic Properties of the Soil,  SSSAP,  Vol  39,  p  424-430,  Rev  (383),
     Class (Ib).

Aylmore, L.A.G. and Sills, I.D.,  1978, Pore Stucture  and  Mechanical  Strength
     of Soils in Relation to Their Constitution,  In:   Modification of Soil
     Structure, W.W.  Emerson, R.D. Bond and A.R.  Dexter,  eds.,  John  Wiley and
     Sons,  Ltd.,  New York, New York,  p 69~78,  Rev (423),  Class  (I  ).

Aylmore, L.A.G. and Quirk, J.P.,  1960, Domain  or  Turbostratic Structure  of
     Clays,  Nature, Vol 187, No 4742,  p 1046-1048,  Rev (117), Class  (Id).

Babcock, K.L., 1963,  Theory of Chemical Properties  of Soil  Colloidal Systems
     at Equilibrium,  Hilgardia, Vol 34, no 11, p  417-542, Rev (303), Class
     (Ic).

Baedecker,  M.J. and Back,  W., 1979, Hydrogeologic Processes and
     Chemical Reactions at a Landfill, Groundwater, Vol 17,  No  5,  p
     429-437, Rev (209), Class (Ilia).

Baker, F.G., Veneman, P.L.M. and Bouma, J., 1974, Limitations of the
     Instantaneous Profile Method for Field Measurement of  Unsaturated
     Hydraulic Conductivity, SSSAP, Vol  38, No 6,  p  885-898, Rev  (49),
     Class (II ).

Baker, F.G., 1977, Factors Influencing the Crust  Test for In Situ  Measurement
     of Hydraulic Conductivity, SSSAP, Vol 41, No 6,  p 1029-1032,  Rev (55),
     Class (Ilg).

Baker, J.E.  and Brown, A., 1982,  Geohydrologic Modeling for Industrial Waste
     Disposal Site Evaluation, Fifth Ann..., Rev  (231), Class (III ).

Barber, E.S., 1956, Discussion of Paper by Holtz  and  Gibbs  on Engineering
     Properties of Expansive Clays.  Trans of  ASCE, Vol 121, p  669~673,  Rev
     (308),  Class (Id).

Basak, P.,  1972,  Soil Structure and Its Effect on Hydraulic Conductivity, Soil
     Sci, Vol 114, No 6, p 417-422, Rev (15),  Class (Ilg).

Baver, L.D., Gardner, W.H. and Gardner, W.R.,  1972, Soil  Physics,  John Wiley &
     Sons,  Inc.,  New York, Rev (300),  Class (Ib).

Bear, J., Zaslavsky,  D. and Irmay, S., 1968, Physical Principles of  Water
     Percolation and Seepage, United Nations Educational  Scientific  and
     Cultural Organization, Paris, France,  Rev (299), Class (Ib).

Bear, J., 1972, Dynamics of Fluids in Porous Media, America Elsevier, New
     York,  Rev (260), Class (I ).

Bertrand, A.R., 1965, Rate of Water Intake in  the Field : Methods  of Soil
     Analysis, C.A. Black, ed., Am Soc of Agronomy, Madison, Wise, p 197-208,
     Rev (333), Class (I ).
                                      171

-------
Bianchi, W.C. and Haskell,  E.E.,  1970,  A Strain Gage  Pressure  Cell for Rapid
     Determination of Hydraulic Conductivity of Soil  Cores,  Proceedings of the
     American Society for Testing and Materials,  63:1227-1234, Rev (19), Class
     (Ila.c).

Biggar, J.W.  and Nielsen, D.R., 1967, Miscible Displacement  and Leaching
     Phenomenon : Irrigation of Agricultural Lands, R.M.  Hagen, H.R. Haise and
     T.W. Edminster,  eds.,  Am Soc of Agronomy, Madison, Wise,  p 254-271, Rev
     (324),  Class (Ilia).

Bishop, A.W.  and Henkel,  D.J.,  1957, The Triaxial Test,  Edward Arnold, LTD,
     Rev (29), Class  (lie).

Bjerrum, L.  and Huder, J.,  1957,  Measurement of the Permeability of Compacted
     Clays,  Proceedings,  Fourth International Conference  on  Soil Mechanics and
     Foundations Engineering, London, Vol 1, p 6-8, Rev  (62),  Class (IIo).

Bjerrum, L.,  Nash, J.K.T.L., Kennard, R.M.  and Gibson, R.E., 1972, Hydraulic
     Fracturing in Field Permeability Testing, Geotechnique, Vol 22, No 2, p
     319-332, Rev (48), Class (Ilg,  II  ).

Black, C.A.,  1965, Methods of Soil Analysis, Part I - Physical and
     Mineralogical Properties,  Including Statistics of Measurement and
     Sampling, Am Soc of Agronomy, Madison,  Wise, Rev (326), Class (I ).

Boersma, L.,  1965a, Field Measurement of Hydraulic Conductivity Above a Water
     Table:  Methods of Soil Analysis, C.A.  Black, ed., Am Soc  of Agr, Madison,
     Wisconson, p 222-233,  Rev (21), Class (II ).

Boersma, L.,  1965b, Field Measurement of Hydraulic Conductivity Below a Water
     Table :  Methods of Soil Analysis,  C.A.  Black, ed., Am Soc of Agronomy,
     Madison, Wise, p 222-233,  Rev (331), Class (lid,a).

Bonn, H.L.,  MeNeal, B.L.  and O'Connor,  G.A., 1979, Soil  Chemistry,
     John Wiley & Sons, Rev (11), Class (Ic).

Bond, W.J. and Collis-George, N., 1980, Ponded Infiltration  into Simple Soil
     Samples  :  3.  The Behavior of Infiltration Rate with Time, Soil Sci, Vol
     131, No 6, p 327-333,  Rev (193), Class (Ib).

Bouma, J. and Dekker, L.W., 1981, A Method of Measuring  the  Vertical and
     Horizontal Saturated Hydraulic Conductivity of Clay  Soils with
     Macropores, SSSAJ, Vol 45, p 662-663,  Rev (253), Class  (Ha).

Bouma, J. and Denning, J.L., 1972, Field Measurement  of  Unsaturated Hydraulic
     Conductivity by Infiltration through Gypsum Crusts,  SSSAP, Vol 36, No 5,
     p 846-847, Rev (207),  Class (Ilb.d).

Bouma, J., Beimans, C., Dekker, L.W. and Jeurissen, W.J.M.,  1983, Assessing
     the Suitability of Soils with Macropores for Subsurface Liquid Waste
     Disposal, J. Eviron. Quality, Vol  12,  p 305-311, Rev (202), Class  (lid).
                                      172

-------
Bouma, J.f  Dekker,  L.W.  and Mailwijk,  C.J.,  1981, A Field Method for Measuring
     Short-Circuiting in Clay Soils, J of  Hydrology, Vol 52, p 347-354, Rev
     (90),  Class (II ).

Bouma, J.,  Hillel,  D.I., Hole,  F.D.  and Amerman, C.R., 1971, Field Measurement
     of Unsaturated Hydraulic Conductivity by  Infiltration Through Artificial
     Crusts, SSSAP, Vol  35, No 2,  p  362-364, Rev (204), Class (Ilb.d).

Bouma, J.,  Jongerius, A., Boersma, 0., Jager,  A. and Schoonderbeek, D., 1977,
     The Function of Different Type  of Macropores During Saturated Flow
     Through Four Swelling Soil Horizons,  SSSAJ, Vol 41, No 5, p 945-950, Rev
     (242), Class (Ilg).

Bouma, J.,  Jongerius, A. and Schoonderbeek,  D., 1979, Calculation of
     Satrurated Hydraulic Conductivity of  Some Pedal Clay Soils Using
     Micromorphometric Data, SSSAJ,  Vol 43,  p  261-264, Rev (384),
     Class (Ilh).

Bouma, J.,  1971, Evaluation of the Field Percolation Test and an Alternative
     Procedure to Test Soil Potential  for  Disposal of Septic Tank Effluent,
     SSSAP, Vol 35, No 6, p 871-875, Rev (203), Class (lid).

Boutwell, G.P. and Donald, V.R., 1982, Compacted Clay Liners for Industrial
     Waste Disposal, ASCE National Meeting,  Rev (7), Class (IV ,11 ,111 ).

Bouwer, H.  and Rice, R.C., 1976, A Slug Test for Determining Hydraulic
     Conductivity of Unconfined Aquifers with  Completely or Partially
     Penetrating Wells,  Wat Res Res, Vol 12, No 3, p 423-428, Rev (28),
     Class (IIa,d).

Bouwer, H., 1961, A Double Tube Method for Measuring Hydraulic Conductivity of
     Soils in Situ Above a Water Table,  SSSAP,  Vol 25, No 5, p 334-339, Rev
     (206), Class (lid).

Bouwer, H., 1962, Field  Determination  of Hydraulic Conductivity Above a Water
     Table with the Double Tube Method,  SSSAP,  Vol 26, No 4, p 330-335, Rev
     (205), Class (lid).

Bouwer, H., 1963a,  In-Place Measurement of Soil Hydraulic Conductivity in the
     Absence of a Water  Table,  Proc.,  Intern Soc of Soil Mech and Found Eng,
     2nd Asian Regional  Conference,  Tokyo,  Japan, Vol 1, p 130-133, Rev (139),
     Class (IIb,d).

Bouwer, H., 1963b,  Theoretical Effect  of Unequal Water Levels on the
     Infiltration Rate,  Determined with Buffered Cylindeer Infiltrometers,
     J Hydrol, Vol 1 , p  29-34.

Bouwer, H., 1964, Unsaturated Flow in  Groundwater Hydraulics, ASCE:  J of the
     Hydr Div, Vol 90, No HY5,  p 121-144,  Rev  (137), Class (lib).

Bouwer, H., 1966, Rapid  Field Measurement  of Air Entry Value and Hydraulic
     Conductivity of Soil as Significant Parameters in Flow System Analysis,
     Wat Res Res, Vol 2, No 4,  p 729-738,  Rev  (25), Class (lid).
                                     173

-------
Bouwer,  H.,  1969a,  Infiltration of Water  into Nonuniform Soil, ASCE:  J of the
     Irr and Drain  Div,  Vol 95,  No IR4, p 451-462, Rev  (136), Class  (Ilg).

Bouwer,  H,,  1969b,  Planning and Interpreting Soil  Permeability Measurements,
     ASCE:  J of the Irr  and Drain Div, Vol 95, No  IR3,  p 391-402, Rev (16),
     Class (II ).

Bouwer,  H.,  1976, Infiltration into  Increasingly Permeable Soils, ASCE: J of
     the Irr and Drain Div, Vol 102, No IR1, p 127-137, Rev  (138), Class
     (II ).

Bouwer,  H.,  1979, Soil Water Hysteresis as a Cause of Delayed Yield  from
     Unconfined Aquifers,  Wat Res Res, Vol 15, No  4, p  965-966, Rev  (135),
     Class (Ilg).

Bowles,  J.E., Engineering Properties of Soils and  Their Measurement,
     MaGraw-Hill Book Co,  New York,  Rev (385), Class (I ).

Braids,  D.C. and Gillies,  N.P.,  1978, Groundwater-Literature Review, J of the
     Wat Pol Control Fed,  Vol 50, No 5, p 1406-1414, Rev (158), Class (Illb).

Bresler, E.  and Dagan, G., 1983a, Unsaturated Flow in Spatially Variable
     Fields 2. Application of Water  Flow  Models to Various Fields, Wat Res
     Res, Vol 19, No 2,  p 421-428, Rev  (346), Class  (V  ).

Bresler, E.  and Dagan, G., 1983b, Unsaturated Flow in Spatially Variable
     Fields 3. Solute Transport Models and Their Application to Two  Fields,
     Wat Res Res, Vol 19,  No 2,  p 429-435, Rev (347), Class  (V ).

Bresler, E., Bieloral, H.  and Lanfer, A.,  1979, Field Test of Solution Flow
     Models in a Heterogeneous Irrigated  Crop Soil, Wat Res  Res, Vol 15, p
     643-652, Rev (261), Class (V ).

Brooker, P.I., 1979, Kriging, Engineering Mining Journal, September, p
     148-153, Rev (351), Class (V ).

Brooks,  R.H. and Corey,  A.T., 1964,  Hydraulic Properties of  Porous Media,
     Hydrology Paper No  3, Colorado  State Univ., Fort Collins, Rev (262),
     Class (I ).

Brown, K.W.  and Anderson,  D.C.,  1983, Effects of Organic Solvents on the
     Permeability of Clay Soils, EPA technical report,  Rev  (3), Class (II  ,1,
     III ,IV ).

Brown, K.W.  and Associates, Inc., 1983, Hazardous  Waste Land Treatment, EPA,
     SW-874, Solid  and Hazardous Waste Reasearch Division, Cincinnati, Ohio,
     Rev (376), Class (III ).

Brown, K.W.  and Associates, Inc., 1982, Clay Liner-Hazardous Waste
     Compatibility, EPA  Contract No  68-01-6515, Work Assignment
     HOO-008, Rev (74),  Class (Ilg).
                                      174

-------
Bruce, R.R., 1972, Hydraulic Conductivity Evaluation of the Soil  Profile from
     Soil Water Retention Relations,  SSSAP,  Vol 36,  p 555-561,  Rev (386),
     Class (II ).

Brust, K.J., Van Bavel, C.H.M. and Stirk, G.B., 1968, Hydraulic Properties  of
     a Clay Loam Soil and Field Measurement  of Water Uptake by  Roots.  II.
     Comparison of Field and Laboratory Data on Retention and of  Measurement
     and Calculated Conductivities, SSSAP, Vol 32,  p 322-326, Rev (387),  Class
     (II ).

Brutsaert, W., 1979, Universal Constants for Scaling the Exponential Soil
     Water Diffusivity, Wat Res Res,  Vol 15, No 2,  p 481-483, Rev (149),  Class
     (VI ).

Buckingham, E., 1907, Studies on the Movement of Soil Moisture, U.S.D.A.  Bur.
     Soils Bull., 38. U.S.D.A. Washington, D.C., Rev (130),  Class (Ib).

Burdine, N.T., 1953, Relative Permeability Calculations from Pore Size
     Distribution Data, Trans of the A.I.M.E., Vol  198, p 71-77,  Rev  (147),
     Class (Ilh).

Burgess, T.M. and Webster, R., 1980,  Optimal Interpolation Isarithmic  Mapping
     of Soil Properties :  I. The Semivariogram and  Punctual Kriging, J Soil
     Sci, Vol 13, P 315-331, Rev (263), Class (V ).

Burrows, W.C. and Kirkham, D., 1958,  Measurement of  Field Capacity with  a
     Neutron Meter, SSSAP, Vol 22, p 103-105, Rev (295),  Class  (Ib).

Buss, D.R., Trexler, B.D.  and Knellar,  W.A., 1978, Hydraulic Conductivity
     Measurements Utilizing Heat-Shrinkable  Tubing,  Groundwater,  Vol 16, No 1,
     p 49-50, Rev (92), Class (II ).

Busscher, W.J., 1981, Finite Difference Calculation  of Unsaturated
     Permeability, Soil Sci, Vol 131, No 4,  p 210-214,  Rev (96),  Class (Ilh).

Cameron, Jr., J.D. and Stewart, M.W., 1982,  Leachate Disposal Alternatives  in
     a Sole Source Aquifer Environment, Fifth Ann..., Rev (229),  Class (III ).

Campbell, G.S., 1974, A Simple Method for Determining Unsaturated
     Conductivity from Moisture Retention Data, Soil Sci,  Vol 117,
     p 311-314 Rev (388),  Class (lib).

Canj, A.S., et al., 1943,  Permeability  of Mud Mountain Core Material,  Trans of
     ASCE,  Vol 108, p 719-737, Rev (285),  Class (II  ).

Capper, P.L.  and Cassie, W.  F., 1978, The Mechanics  of Engineering Soils,
     Sixth Edition, E & F.N. Spon, ltd.,  London.

Carvallo, H.O., Cassel, O.K.,  Hammomd,  J.  and Bauer,  A.,  1976,  Spatial
     Variability of In Situ Unsaturated Hydraulic Conductivity  of Maddock
     Sandy Loam,  Soil Sci, Vol 121,  p 1-8, Rev (390),  Class  (V  ).
                                     175

-------
Gary, A.S., Walter,  B.H.  and Harstad,  H.T.,  1943,  Permeability of Mud Mountain
     Core Material,  Trans of ASCE,  Vol 108,  p 719-737.

Gary, J.W. and Taylor,  S.A., 1967,  The Dynamics  of Water,  Part II- Temperature
     and Solute Effects,  R.M. Hagen, H.R.  Haise  and T.W.   Edminster, eds., Am
     Soc of Agronomy,  Madison, Wise, p 245-251,  Rev (323), Class  (Ib).

Cassel, O.K., Warrick,  A.W., Nielsen,  D.R.  and Biggar,  J.W., 1968, Soil Water
     Diffusivity Values Based Upon  Time Dependent  Soil  Water Content
     Distributions,  SSSAP, Vol 32,  p 774-777, Rev  (389), Class (II ).

Cedergren, H.R., 1977,  Seepage, Drainage,  and Flow Nets, John Wiley & Sons,
     Inc., New York, New York, Rev  (391),  Class  (I ).

Chan, H.T. and Kenney,  T.C., 1973i  Laboratory Investigations of Permeability
     Ratio of New Liskeard Vared Soil, Can Geotech J, Vol  10, No  3, P 453-472,
     Rev (31), Class (IIa,c,g).

Cheng, J.D., Black,  T.A.  and Willington, R.P., 1975,  A  Technique  for the  Field
     Determination of the Hydraulic Conductivity of Forrest Soils, Can J  Soil
     Sci, Vol 55, p 79-82, Rev (392),  Class (lid).

Childs, E.G. and Collis-George, N., 1950a,  The Permeability of Porous
     Materials, Proc Roy Soc (London), A201, p 392-405, Rev  (152), Class
     (Hh).

Childs, E.G. and Collis-George, N., 1950b,  The Control  of  Soil Water, Advances
     in Agronomy 2,   p 233-272, Rev (155),  Class (Ib.II ).

Childs, E.C., 1969,  The Physical Basis of Soil Water Phenomena, John Wiley
     Publishing, New York, New York, Rev (393),  Class (Ib).

Chiles, J.P., How to Adapt Kriging to  Non-Classical Problems  :  Three Case
     Studies, Rev (357),  Class (V ).

Chirlin, G.R. and Dagan,  G., 1980,  Theoretical Head Variograms for Steady Flow
     in Statistically Homogeneous Aquifers, Wat  Res Res, Vol  16,  No 6,  p
     1001-1015, Rev (358), Class (V ).

Chirlin, G.R. and Wood, E.F., 1982, On the Relationship Between Kriging and
     State Estimation, Wat Res Res, Vol 18, No 2,  p 432-438,  Rev  (341), Class
     (V ).

Chong, S.K.  and Green, S.K., Application of Field  Measured Sorptivity for
     Simplified Infiltration Prediction, Rev  (129), Class  (II  ).

Chu, S.Y. and Sposito, G., 1976, A Derivation of the Macroscopic  Solute
     Transport Equation for Homogeneous, Saturated, Porous Media, Wat Res Res,
     Vol 16, No 3, P 542-546, Rev  (131), Class (Ilia).

Clark, I., 1979a, The Semivariogram-Part I, Engineering Mining Journal, July,
     p 90-94, Rev (349),  Class (V  ).
                                      176

-------
Clark, I., 1979b, The Semivariogram-Part II,  Engineering Mining Journal,
     August, p 92-97, Rev (350),  Class (V ).

Clark, I., 1982, Practical Geostatistics, Applied Science Publishers,  London,
     Rev (264), Class (V ).

Clerici, J.F. and Collison, G.H., 1982,  Analysis of Underdrain for Waste
     Disposal Leachate Control,  Fifth Ann..., Rev (228),  Class (IIIc).

Clothier, B.E. and White, I.,  1982,  Water Diffusivity of a Field Soil,  SSSAJ,
     46:155-158, Rev (4), Class  (Ilg).

Clothier, B.E. and White, I.,  1981,  Measurements of Sorptivity and Soil Water
     Diffusivity in the Field, SSSAJ, Vol 45, No 2, p 241-245, Rev (194),
     Class (VI ).

Clothier, B.E., Knight, J.H. and White,  I.,  1981 a,  Burger's Equation
     Application to Field Constant-Flux Infiltration, Soil Sci,  Vol 132,
     No 4, p 255-261, Rev (195),  Class (Ib).

Clothier, B.E., White, I. and Hamilton,  G.J., 1981b, Constant-rate Rainfall
     Infiltration : Field Experiments, SSSAJ, Vol 45, No 2,  p 245-249,  Rev
     (191), Class (Ib).

Coleman, J.D. and Marsh, A.D., 1961, An Investigation of the Pressure-Membrane
     Method for Measuring the Suction Properties of Soil, J of Soil Sci,  Vol
     12, p 343-362, Rev (88),  Class  (II ).

Corey, A.T., 1957, Measurement of Water and  Air Permeability in Unsaturated
     Soil, SSSAP, Vol 21, p 7-10, Rev (212),  Class (lib).

Coumoulos, D.G. and Koryalos,  T.P.,  1978, Performance of the Clay Core of a
     Large Embankment Dam During Construction, In:  Clay Fills, Institute  of
     Civil Engineers, London,  p  73~78, Rev (301), Class (Id).

Cox, D.H., 1978, Volume Changes  of Compacted Clay Fills,  In:  Clay Fills,  The
     Institute of Civil Engineers, London, p 79-86, Rev (283), Class (IV  ).

Creutin, J.D. and Obled, C., 1982, Objective Analysis and Mapping Techniques
     for Rainfall Fields : An Objective Comparison, Wat Res Res,  Vol 18,  No 2,
     p 413-431, Rev (342), Class (V  ).

Crites, R.W., Meyer, E.L. and Smith, R.G., 1981,  Process Design Manual Land
     Treatment of Municipal Wastewater,  Env  Prot Agency,  U.S. EPA, Cincinnati,
     Rev (254), Class (Ilia).

Dagan, G. and Bresler, E., 1983,  Unsaturated Flow in Spatially Variable Fields
     1. Derivation of Models of  Infiltration and Redistribution,  Wat Res  Res,
     Vol 19, No 2, p 413-420,  Rev (345), Class (V ).
                                      177

-------
Dagan,  G.,  1982,  Stochastic Modeling of Groundwater Flow by Unconditional and
     Conditional  Probabilities  I. Conditional Simulation and the Direct
     Problem,  Wat Res  Res, Vol  18, No 4,  p 813-833, Rev (339), Class  (V  ).

Dane, J.H.  and Hruska,  S., 1983, In-Situ  Determination of Soil Hydraulic
     Properties during Drainage, SSSAJ, Vol 47, No 4, p 619-624, Rev  (98),
     Class  (Ilh).

Dane, J.H., 1980, Comparison  of Field and Laboratory Determined Hydraulic
     Conductivity Values, SSSAJ, Vol 44,  p 228-231, Rev (235), Class  (lib).

Daniel, D.E.,  Hamilton, J.M.  and Olsen, R.E., 1981, Suitability of
     Thermocouple Psychrometers for Studying Moisture Movement in
     Unsaturated Soils, Permeability and  Groundwater Contaminant
     Transport ASTM STP 746,  T.F. Zimmie  and C.O. Riggs, eds, Am
     Soc for Testing and Materials, p 84-100, Rev (236), Class
     (lib).

Daniel, D.E.,  1987, Hydraulic Conductivity Tests for Clay Liners.   In:   Ninth
     Annual Symp. on Geotechnical and Geohydrological Aspects of Waste
     Management,  Feb.  1-6, Fort Collins,  Colorado, Rev  (1), Class  (II,  IV,
     III).

Daniel, D.E.,  1982, Measurement of Hydraulic Conductivity of Unsaturated Soils
     with Thermocouple Psychrometers, SSSAJ, Vol 46, No 6,  p 1125-1129,  Rev
     (97),  Class (lib).

Daniel, D.E. and Trautwein, S.J., 1986, Field Permeability  Test for Earthen
     Liner.  In:   Proceedings,  In-Situ  1988, ASCE Specialty Conference  on Use
     of In-Situ Tests in Geotechnical Engineering, Virginia Polytechnic
     Institute and State University, Blacksburg, Virginia,  June 22-25.

Davidson, J.M., Stone, L.R.,  Nielsen, D.R. and  LaRue, M.E., 1969a,  Field
     Measurement and Use of Soil Water  Properties, Annual Meeting  of  the
     American Geophysical Union, Rev  (157), Class  (lid).

Davidson, J.M., Stone, L.R.,  Nielsen, D.R. and  LaRue, M.E., 1969b,  Field
     Measurement and Use of Soil Water  Properties, Wat  Resour Res,  Vol  5,
     No. 6, p 1312-1321, Rev  (51), Class  (II  ).

Davis, J.C. and Sampson, R.J.,  Statistics and Data Analysis in Geology, John
     Wiley & Sons, Inc., New  York, Rev  (370), Class  (V  ).

Day, P.R., Bolt, G.H. and Anderson,  D.M., 1967,  Nature  of  Soil Water  :
     Irrigation of Agricultural Lands,  R.M. Hagen, H.R. Haise  and  T.W.
     Edminster, eds., Am Soc  of Agronomy, Madison, Wise,  p 193-207,
     Rev (321), Class  (Ib).

De Bruijn, C.A., Collins, L.E.  and Williams,  A.A.B.,  1956,  The Specific
     Surface, Water Affinity  and Potential Expansiveness  of Clay,  Clay
     Minerals Bulletin, Vol  3,  No  17,  p 120-128,  Rev (305), Class  (Id).
                                      178

-------
Delfiner, P. and Delhomme, J.P.,  1973,  Optimum Interpolation by  Kriging,  In:
     Display & Analysis of Spatial Data,  NATO Advanced Study Institute, J.C.
     Davis and M.J.  McCullagh,  eds.,  John Wiley & Sons,  New York,  Rev  (359),
     Class (V ).

Delfiner, P., 1976,  Linear Estimation of  Non Stationary Spatial  Phenomena,  In:
     Advanced Geostatistics in the Mining Industry,  M. Guarascio,  et al.,
     eds., D. Reidel Publishing Co.,  Dordrecht, Holland,  Rev (364),
     Class (V ).

Delhomme, J.P., 1979b, Spatial Variability and Uncertainty in Groundwater Flow
     Parameters: A Geostatistical Approach, Wat Resour Res,  Vol  15, No 2, p
     269-280, Rev (340), Class (V ).

Delhomme, J.P., 1979a, Kriging in the Design of Streamflow Sampling Networks,
     Wat Resour Res, Vol 15, No 6, p  1833-1840, Rev  (368),  Class (V ).

Derr, B.D., Matelski, R.P. and Petersen,  G.W., 1969,  Soil Factors  Influencing
     Percolation Test Performance, SSSAP, Vol 33, No 6,  p 942-946, Rev (208),
     Class (Ilg).

Diamond, S., 1970, Pore Size Distributions in Clays,  Clays and Clay
     Minerals, Vol 18, p 7-23,  Rev (394), Class (Id).

Dietzler, D.P., 1983, Structural Design of Landfill  Leachate Collection
     Systems, 6th Ann..., Madison, Wise,  Rev (172),  Class (IIIc).

Doering, E.J., 1965, Soil-Water Diffusivity by the One-Step Method, Soil Sci,
     Vol 99, No 5, p 322-326, Rev (40), Class (He).

Dovichi, M.D. and Miller, D.L., 1982, Baling : An Alternative to Conventional
     Landfilling, Fifth Ann..., Rev (222), Class (III  ).

Dovichi, M.D. and Miller, D.L., 1983, A Landfill Siting and Approval
     Guideline-A First Approximation, 6th Ann..., Madison,  Wise, Rev (165),
     Class (III ).

Duvel,  D.A., Practical Interpretation of  Groundwater Monitoring
     Results, Geohydrology, Rev (201),  Class (V ).

Elrick, D.E., Scandrett, J.H. and Miller, E.E., 1959,  Tests of Capillary Flow
     Scaling, SSSAP, Vol 28, No 5, p  329-332,  Rev (102),  Class (VI ).

Emerson, W.W., Bond, R.D. and Dexter, A.R., 1978, Modification of  Soil
     Structure, John Wiley and Sons,  Ltd., New York,  New York, Rev (418),
     Class (I ).

Ferguson, H. and Gardner, W.H., 1962, Water Content  Measurement  in Soil
     Columns by Gamma Ray Absorption, SSSAP,  Vol 26,  No 1,  p 11-14, Rev (216),
     Class (Ib).
                                      179

-------
Fok, Y.S.,  1975,  A Comparison of  the  Green-Ampt  and  Philip Two Term
     Infiltration Equations,  Trans of ASAE,  Vol  18,  No 6, p 1073-1075, Rev
     (162), Class (Ib).

Folkes, D.J.,  1982, Fifth Canadian Geotechnical  Colloquium :  Control of
     Contaminant Migration by the use of  Liners,  Can Geotech J, Vol 19, p
     320-344,  Rev (218),  Class (IV ).

Forsyth, P., Marcelja,  S., Mitchell,  D.J.  and  Ninham, B.W., 1978, Stability of
     Clay Dispersions,  In: Modification of Soil  Structure, W.W. Emerson, R.D.
     Bond and A.R. Dexter, eds.,  John Wiley and  Sons, Ltd., New York, New
     York,  p 17-26, Rev (420), Class  (Id).

Freeze, R.A. and Cherry,  J.A., 1979,  Groundwater,  Prentice-Hall, Inc.,
     Englewood Cliffs,  N.J.,  Rev  (286), Class  (I ).

Freeze, R.A.,  1980, A Stochastic-Conceptual Analysis of  Rainfall-Runoff
     Processes on a Hillslope, Wat Res Res,  Vol  16,  No 2, p 391-408, Rev
     (289), Class (V ).

Frenkel, H. and Rhoades,  J.D., 1978,  Effects of  Dispersion and Swelling on
     Soil Hydraulic Conductivity, J of Testing and Evaluation, JTEVA, Vol 6,
     No 1 ,  p 60-65, Rev (257), Class  (Id).

Frenkel, H., Goertzen,  J.O. and Rhoades,  J.D., 1978, Effect of Clay Type and
     Content,  Exchangeable Sodium Percentage and Electrolyte Concentration on
     Clay Dispersion and Soil Hydraulic Conductivity, SSSAJ, Vol 42, No 1,
     p 32-39,  Rev (180),  Class (Ilg).

Gairon, S.  and Swartzendruber, D., 1975,  Water Flux and  Electrical Potentials
     in Water Saturated Bentonite, SSSAP, Vol  35, No 9,  p 811-817, Rev  (34),
     Class (Ilg,a).

Garcia-Bengochea, I. and Lovell Jr.,  C.W., 1981, Correlative Measurements of
     Pore Size Distribution and Permeability in Soils,  Permeability and
     Groundwater Cont aninant Transport,  ASTM  STP 746,  T.F. Zimmie and C.O.
     Riggs, eds., Am Soc for Testing and  Materials,  Philadelphia, PA, Rev
     (239), Class (Ilg).

Gardner, W.H., 1965, Water Content :  Methods of Soil Analysis, C.A. Black,
     ed., Am Soc of Agronomy, Madison, Wise, p 82-125,  Rev  (327), Class  (Ib).

Gardner, W.R., 1956, Calculation of Capillary Conductivity  from  Pressure  Plate
     Outflow Data, SSSAP, Vol 20, p 317-320, Rev (213),  Class  (II  ).

Gardner, W.R., 1970, Field Measurement of Soil Water Diffusivity, SSSAP,  Vol
     34, No 5, p 832-833, Rev (53), Class (II  ).

Gee, J.R., 1983, Leachate Generation in Landfills : A New Method,
     6th Ann..., Madison, Wise, Rev (168), Class (III ).
                                      180

-------
Geswein, A.J., Landreth, R.E. and Haxo, Jr., H.,  1978, Use of Liner Materials
     for Land Disposal Facilities, 71st Ann Meet of the Am Inst of Chem Eng,
     Rev (175), Class (Ilia).

Ghassemi, M., Haxo, M., Metzger, J., Powers, M.,  Quinlivan, S., Scinto, L.  and
     White, H., 1983, Assessment of Technology for Constructing and Installing
     Cover and Bottom Liner Systems for Hazardous Waste Facilities, EPA
     Contract No 68-02-3174, Rev (248), Class (IV ).

Gibson, R.E., 1966, A Note on the Constant Head Test to Measure Soil
     Permeability In Situ, Geotechnique, Vol 16,  p 256-259, Rev (47),  Class
     (Hg,II ).

Gibson, R.E., 1970, An Extension to the Theory of the Constant Head In Situ
     Permeability Test, Geotechnique,  Vol 20, No 2,  p 193-197, Rev (80),
     Class (Ilg).

Gibson,R.E., 1963, An Analysis of System Flexibility and its Effect on Time
     Lag in Pore-Water Pressure Measurements, Geotechnique, Vol 13, p  1-11,
     Rev (46), Class (Ilg,II ).

Gillham, R.W., Klute, A. and Heerman,  D.F., 1976, Hydraulic Properties of a
     Porous Medium: Measurement and Empirical Representation,  SSSAJ, Vol  40,
     p 203-207, Rev (395), Class (II ).

Glaub, J.C., Savage, G.M., Tuck, J.K.  and Henderson, T.M.,  1983,  Waste
     Characteristics for North Santa Clara County California,  6th Ann	
     Madison, Wise, Rev (167),  Class (Ilia).

Goodall, D.C. and Quigley, R.M., 1977,  Pollutant  Migration  from Two Sanitary
     Landfill Sites near Sarnia, Ontario, Can Geotech J,  Vol 14,  No 2,  p
     223-236, Rev (76),  Class (Illb).

Goodman, R.E., 1980, Permeability and  Piping in Fractured Rook,  ASCE:  J of  the
     Geotech Div, Vol 1066,  No GT5,  p  485-498,  Rev (148), Class (Ilg).

Gordon, B.B. and Forrest, M.,  1981,  Permeability  of  Soils Using Contaminated
     Permeant, Permeability and Groundwater Contaminant Transport,  ASTM STP
     746, T.F. Zimmie and C.O.  Riggs,  eds., Am Soc of Testing  and Materials,
     Philadelphia, PA,  Rev (237),  Class (Ilg,II ).

Gordon, M.E.  and Huebner, P.M.,  1983,  An Evaluation  of the  Performance  of Zone
     of Saturation Landfills in Wisconsin,  6th Ann	  Madison,  Wise,  Rev
     (166),  Class (III  ).

Green,  R.E.  and Corey,  J.C.,  1971,  Calculation of Hydraulic Conductivity: A
     Further Evaluation of Predictive  Methods,  SSSAP,  Vol 35,  p 3-8, Rev
     (265),  Class (Ilh).
                                     181

-------
Green,  R.S.B.,  Posner,  A.M.  and  Quirk,  J.P., 1978, A Study of the Coagulation
     of Montmorillonite and  Illite  Suspensions by Calcium Chloride using the
     Electron Microscope,  In:  Modification of Soil Structure, W.W. Emerson,
     R.D.  Bond and A.R. Dexter,  eds., John Wiley and Sons, Ltd., New York, New
     York, p 35-40,  Rev (421), Class  (Id).

Green,  W.H. and Ampt,  G.A.,  1911, Studies on Soil Physics. Part I, The J of
     Agriculural Sci,  Vol  IV,  p  1-24, Rev  (151), Class  (Ib).

Green,  W.J., Lee, G.F., and  Jones,  R.A., 1981, Clay Soils Permeability and
     Hazardous Waste Storage,  J  Wat Pol Control Fed, Vol 53, No 8, p.
     1347-1354, Rev (9), Class (Ilf.e.g, IV  ).

Green,  W.J., Lee, G.F.  and Jones, R.A., 1979, Impact of Organic Solvents on
     the Integrity of Clay Liners for Industrial Waste  Disposal Pits  :
     Implication for Groundwater Contamination, Final Report, Project No R-804
     549 010-02-0, Department  of Civil  Engineering, Fort Collins, CO, Rev
     (68), Class (II ,111  ).

Greenland, D.J., Lindstrom,  G.R. and  Quirk,  J.P., 1961, Role of
     Polysaccharides in Stabilization of Natural Soil Aggregates,
     Nature, Vol 191,  No 4795, p 1283-1284,  Rev  (118),  Class  (Id).

Griffin, Jr., D.M.,  Zavoral, P.  and Wagner,  R.E., 1982, An Investigation of
     Some Aspects of a Completed Landfill,  Fifth Ann..., Rev  (223), Class
     (III ).

Groenevelt, P.H. and Bolt, G.H., 1971,  Water Retention  in Soil, Soil  Sci, Vol
     113, No 4, p 238-245, Rev (145), Class (Id).

Gumbs, F.A. and Warkentin, B.P., 1972,  The  Effect of Bulk Density and Initial
     Water Content on Infiltration  in Clay  Soil  Samples, SSSAP, Vol 36, p
     720-724, Rev (312), Class (Ilg).

Gupta, S.C. and Larson, W.E.,  1979, Estimating  Soil Water Retention
     Characteristics from Particle  Size Distribution, Organic Matter  Percent,
     and Bulk Density, Wat Res Res, Vol 15,  No  6,  p 1633-1635,  Rev  (146),
     Class  (Ib).

Hagan, R.M., Raise, H.R. and Edminster, T.W.,  1967, Irrigation  of Agricultural
     Lands, Am Soc of Agr, Madison, Wisconsin,  Rev  (320), Class (I  ).

Haines, W.B., 1925, Studies in the  Physical Properties  of Soils.  II. A Note
     on the Cohesion Developed by  Capillary Forces  in  an  Ideal  Soil,  J of
     Agricultural Sci, Vol 15, p 529-535,  Rev  (125), Class  (Ib).

Haines, W.B., 1930, Studies in the  Physical Properties  of Soil.   V.   The
     Hysteresis  Effect  in Capillary Properties and  the  Modes of Moisture
     Distribution Associated Therewith, J  of Agricultural Sci,  Vol  20,  p
     97-116, Rev  (153), Class (Ib).
                                      182

-------
Haji-Djafari,  S and Wright,  Jr.,  J.C.,  1982,  Determining the Long-Term Effects
     of Interactions Between Waste Permeants  and  Porous Media, ASTM 2nd
     Symposium on Testing of Hazardous  and  Industrial Soild Wastes, Rev  (176),
     Class (II ).

Hamilton, J.M., Daniel,  D.E. and  Olsen,  R.E.,  1981, Measurement of Hydraulic
     Conductivity of Partially Saturated Soils, Permeability and Groundwater
     Contaminant Transport,  ASTM  STP  746, T.F. Zimmie and C.O. Riggs, eds.,
     Amer Soc for Testing and Materials,  Philidelphia, PA, p 182-196, Rev
     (396), Class (lib).

Hannoura, A.A. and McCorquodale,  J.A.,  1978,  Air-Water Flow in Coarse Granular
     Media, ASCE: J of the Hydr Div,  Vol 104,  No  HY7, p 1001-1010, Rev (134),
     Class (Ilg).

Haridasan, M.  and Jensen, R.D., 1972, Effect  of Temperature on Pressure
     Head-Water Content Relationship  and Conductivity of Two Soils, SSSAP,
     Vol 36, No 5, p 703-708, Rev (39),  Class (Ilg.c).

Harris, A.E.,  1931, Effect of Replaceable Sodium  on Soil Permeability, Soil
     Sci, Vol 32, p 435-446, Rev  (57),  Class  (Ilg).

Haxo, Jr., H.E., 1981, Testing of Materials for Use in the Lining  of Waste
     Disposal Facilities, Hazardous Solid Waste Testing : First Conference,
     ASTM STP 760, R.A.  Conway and B.C.  Malley, eds., Am Soc of Testing  and
     Materials, p 269-292, Rev (250), Class (Ilia).

Healy, K.A. and Laak, R., 1973, Factors Affecting the Percolation Test,  J Wat
     Pol Control Fed, Vol 45, No   7,  P  1508-1516,  Rev (22), Class (lid).

Hendry, M.J.,  1982, Hydraulic Conductivity  of a Glacial Till in Alberta,
     Groundwater, Vol 20, No 2, p 162-169,  Rev (220), Class (lid).

Higgins, G.H., 1959, Evaluation of the  Ground-Water Contamination Hazard from
     Underground Nuclear Explosions,  J  of Geophysical Res, Vol 64, No 10,
     p 1509-1519, Rev (120), Class (Illb).

Hill, R.L. and King, L.D., 1982,  A Permeameter which Eliminates Boundary Flow
     Errors in Saturated Hydraulic Conductivity Measurements, SSSAJ, Vol 46,
     p 877-880, Rev (100), Class  (Ila).

Hillel, D. and Gardner,  W.R., 1970, Measurement of Unsaturated Conductivity
     and Diffusivity by Infiltration  Through  an Impending Layer, Soil Sci, Vol
     109, No 3, Rev (54), Class (II ).

Hillel, D., Krentos, V.D. and Stylianou,  Y.,  1972, Procedure and Test of an
     Internal Drainage Method for Measuring Soil  Hydraulic Characteristics In
     Situ, Soil Sci, Vol 114, No   5,  p  395-400, Rev (52), Class (II ).

Hillel, D.I.,  1971, Soil and Water :  Physical Principles and Processes,
     Academic Press, New York,  New York,  Rev  (397), Class (Ib).
                                     183

-------
Hillel,  D.I.,  1980,  Fundamentals  of  Soil  Physics, Academic Press, New York,
     New York, Rev (398),  Class  (Ib).

Hoeks, J. and  Agelink,  G.J.,  Hydrological Aspects of Sealing Waste Tips with
     Liners and Soil Covers,  Institute  for Land  and Water Management Research,
     Wageningen, The Netherlands,  Rev  (73)t  Class (lid).

Holmes,  J.W.,  Taylor, S.A. and Richards,  S.J., 1967, Measurement of Soil
     Water : Irrigation of Agricultural Lands, R.M. Hagen, H.R. Haise and T.W.
     Edminster, eds., Am Soc  of  Agronomy, Madison, Wise, p 275-298, Rev (325),
     Class (II ).

Holtz, W.G. and Gibbs,  H.J.,  1956, Engineering Properties of Expansive Clays,
     Trans of  ASCE,  Vol 121,  p 641-663, Rev (304), Class (Id).

Holtz, W.G., 1959, Expansive  Clays Properties and Problems, Soil Mechanics
     Conference, Golden, Colorado, Colorado School of  Mines Quarterly, Rev
     (307), Class (Id).

Hoover,  J., 1983, Evaluation  of  Flow Pathways in a Sloping Soil Cross-Section,
     Annual Meeting, ASAE, Rev (20), Class (lid).

Horn, M.E., 1971, Estimating  Soil Permeability Rates,  ASCE: J  of the Irr and
     Drain Div, Vol 97, No IR2,  p 263-274, Rev  (17), Class  (Ilg).

Hughes,  J.P. and Lettenmaier, D.P.,  1981, Data Requirements for Kriging:
     Estimation and Network Design,  Wat Res Res, Vol 17, No 6, p 1641-1650,
     Rev (343), Class (V  ).

Jackson, M. and Marechal, A., Recoverable Reserves Estimated  by Disjunctive
     Kriging  : A Case Study,  Rev  (362), Class (V ).

Jackson, R.D., Reginato,  R.J. and Van Bavel, C.H.M., 1965, Comparison of
     Measured  and Calculated Hydraulic Conductivities  of Unsaturated Soils,
     Wat Resour Res, Vol  1, p 375-380,  Rev (400),  Class (lib).

Jackson, R.D., 1963, Porosity and Soil-Water Diffusivity Relations, SSSAP, Vol
     27, p 123-126, Rev (399), Class (Ilg).

James,  P.M.,  1970, The Behavior of a Soft Recent Sediment  Under  Embankment
     Loadings,  Quarterly  Journal  of Engineering Geology, Vol  3,  No 1 ,  p  41-53,
     Rev (77), Class (II  ).

Jaynes,  D.  and Rogowski,  A.S., 1983, Applicability of  Pick's  Law to Gas
     Diffusion,  SSSAJ, Vol 47, No 3, P 425-439,  Rev (312),  Class (Ilia).

Jennings,  J.E.  and Burland, J.B., 1962,  Limitations to the use of  Effective
      Stresses in Partly Saturated Soils, Geotechnique, Vol 12, p 125-144,
      Rev (314),  Class  (Id).

Johnson, Jr.,  V.R.,  1983, Overview of  Hazardous Waste Disposal Technology,
      Pollution Equipment  News, Vol. 16,  No. 5,  p 61-63, Rev (27),  Class
      (Ilia).
                                      184

-------
 Journel,  A.G. and Huijbregts, C.J., 1978, Mining Geostatistics, Academic
      Press, New York, Rev (266), Class (V ).

 Journel,  A.G., 1979, Geostatistical Simulation : Methods for Exploration and
      Mine Planning, Engineering Mining Journal, December, p 86-91, Rev (352),
      Class (V ).

 Jumikis,  A.R., 1965, Soil Mehcanics, D. Van Nostrand Co., Inc., Princeton,
      N.J.,  Rev (284), Class (Ib).

 Kemper, W.D. and Evans, N.A., 1963, Movement of Water as Effected by Free
      Energy and Pressure Gradients III. Restriction of Solutes by Membranes,
      SSSAP, Vol 27, P 485-490, Rev (433), Class (Id).

 Kemper, W.D. and Letey, J.,  1970,  Solute and Solvent Flow as Influenced and
      Coupled by Surface Reactions, Trans 9th International Congress of Soil
      Sci,  Vol 1, p 233-261,  Rev (428), Class (Id).

 Kemper, W.D. and Maasland, D.E.L., 1964b, Reduction in Salt Content of
      Solution on Passing Through Thin Films Adjacent to Charged Surfaces,
      SSSAP, Vol 28, p 318-323, Rev (432), Class (Id).

 Kemper, W.D. and Quirk, J.P., 1972, Ion Mobilities and Electric Charge of
      External Clay Surfaces Inferred from Potential Differences and Osmotic
      Flow, SSSAP, Vol 36, p 426-433,  Rev (429), Class (Id).

 Kemper, W.D. and Rollins, J.B.,  1966a, Osmotic Efficiency Coefficients Across
      Compacted Clays, SSSAP, Vol 30,  No 5,  p 529-534, Rev (430),  Class (Id).

 Kemper, W.D. and Van Schaik, J.C., 1966b, Diffusion of Salts in Clay- Water
      Systems, SSSAP, Vol 30, p 535-540, Rev (431),  Class (Id).

 Kemper, W.D., Maasland, D.E.L. and Porter,  L.K.,  1964a,  Mobility of Water
      Adjacent to Mineral Surfaces, SSSAP, Vol 28,  p 164-167,  Rev (434),  Class
      (Id).

 Kemper, W.D., 1960,  Water and Ion Movement  in Thin Films as  Influenced by the
      Electrostatic Charge and Diffuse Layer  of Cations Associated with Clay
     Mineral Surfaces,  SSSAP,  Vol 24,  p 10-16,  Rev (437),  Class (Id).

 Kemper, W.D.,  1961 a, Movement of Water as Effected by Free Energy and Pressure
     Gradients:   I.   Application of Classic  Equations for  Viscous and
     Diffusive Movements to  the  Liquid Phase in Finely Porous Media,  SSSAP,
     Vol 25, p 255-260,  Rev  (436),  Class  (Id).

Kemper, W.D.,  1961b, Movement  of Water as Effected by Free Energy and Pressure
     Gradients:  II.  Experiemental Analysis of Porous Systems  in Which Free
     Energy and  Pressure Gradients Act in Opposite  Directions,  SSSAP,  Vol 25,
     p 260-265,  Rev  (435), Class (Id)

Kenney, T.C. and  Chan,  H.T., 1973,  Field  Investigation of  Permeability Ratio
     of New Liskeard Varved  Soil,  Can  Geotech J, Vol 10, p 473-488,  Rev  (401)
     Class (lid).
                                     185

-------
Kesler, K.A.,  Johnson,  T.M.,  Griffin, R.A.  and Sehgal, S.B., 1983,
     Hydrogeologic Investigations  of Organic Contaminant Migration
     at Uncontrolled Hazardous Waste Disposal Sites, 6th Ann...,
     Madison,  Wise,  Rev (174), Class (Ilia).

Kirkham, D. and Affleck,  S.B., 1977, Solute Travel Times to Wells,
     Groundwater,  Vol 15,  No  3,  P  231-242,  Rev (184), Class (Ilia).

Kirkham, D. and Feng, C.L., 1949,  Some  Tests of  the Diffusion Theory, And Laws
     of Capillary  Flow,  in Soils,  Soil  Sci, Vol  67, P 29-40, Rev  (187), Class
     (Ib).

Kirkham, D. and Powers,  W.L., 1972, Advanced Soil Physics, Wiley  Interscience,
     A Division of John Wiley &  Sons, Inc., New  York, Rev  (298),  Class  (Ib).

Kirkham, D. and Van Bavel, C.H.M., 1948,  Theory  of Seepage into Auger Holes,
     SSSAP, Vol 13,  P 75-82,  Rev (215), Class  (Ila.d).

Kirkham, D., 1963, Some Physical Processes  Causing Movement of Ions  and other
     Matter Through Soil,  Journal  Paper No  J 4748 of the Iowa Agricultural  and
     Home Economics Station,  Ames, Iowa,  Rev  (182), Class  (Ib).

Kitanidis, P.K., Statistical  Estimation of  Polynomial Generalized Covariance
     Functions and Hydrologic Applications, Wat  Res Res, Vol 19,  No  4,  p
     909-921,  Rev (356),  Class  (V  ).

Klute, A. and Wilkinson,  G.E.,  1958, Some Tests  of  the Similar Media Concept
     of Capillary Flow :  I.  Reduced Capillary  Conductivity and Characteristic
     Data, SSSAP,  Vol 22,  No  4,  p 278-281,  Rev  (105), Class  (VI  ).

Klute, A., 1965, Water Capacity :  Methods of Soil Analysis, C.A.  Black, ed.,
     Am Soc of Agr, Madison,  Wise, p 273-278,  Rev  (335), Class  (Ib).

Klute, A., 1965a,  Laboratory Measurement  of Hydraulic Conductivity of
     Saturated Soil  : Methods of Soil  Analysis,  C.A. Black,  ed.,  Am  Soc of
     Agronomy, Madison, Wise, p210-220, Rev (252),  Class  (IIa,c).

Klute, A., 1965b,  Laboratory Measurement  of Hydraulic Conductivity of
     Unsaturated Soil : Methods of Soil Analysis, C.A. Black,  ed., Am  Soc  of
     Agronomy, Madison, Wise, p 253-261,  Rev  (332), Class  (Ilb.c).

Klute, A., 1965c,  Water Diffusivity  :  Methods  of Soil Analysis,  C.A.  Black,
     ed.,  Am Soc of Agronomy, Madison,  Wise,  p 262-272,  Rev  (334), Class
     (II  ).

Klute, A., 1972, The Determination of  Hydraulic Conductivity of  Unsaturated
     Soils, Soil Sci, Vol 113,  P 264-276, Rev (402),  Class (lib).

Kmet,  P.  and McGinley, P.M.,  1982, Chemical Characteristics  of Leachate from
     Municipal Solid Waste Landfills in Wisconsin,  Ann..., Rev (227),  Class
     (Ilia).
                                      186

-------
Kmet, P., Quinn, K.J. and Slavik, C.,  1981,  Analysis of Design Parameters
     Affecting the Collection Efficiency of  Clay Lined Landfills,  Fourth
     Ann..., Rev (244), Class (IV ).

Knight, S.K., Molsather, L.R. and Bonnell, M.D., 1983,  Retrofitting an
     Existing Landfill with a Leachate Collection System:  A Case
     History, 6th Ann..., Madison, Wise, Rev (173),  Class  (IIIb,c).

Kuno, G., Shinoki, R., Kondo, T.  and  Tsuchiya,  C., 1978, On the Construction
     Methods of a Motorway Embankment by a Sensitive Volcanic Clay,  In:  Clay
     Fills, The Institute of Civil Engineers,  London,  p 149-156,  Rev (318),
     Class (Id).

Kunze, R.J. and Kirkham, D., 1964, Capillary Diffusion and Self-diffusion of
     Soil Water, Soil Sci, Vol 97, No 3, P 145-151,  Rev (185),  Class (Ilia).

Kunze, R.J. and Nielsen, D.R., 1983,  Comparison of Soil Water Infiltration
     Profiles Obtained Experimentally and by Solution of Richard's Equation,
     Soil Sci, Vol 135, No 6, p 3^2-349, Rev (128),  Class  (Ib).

Kunze, R.J., Uehara, G. and Graham, K.,  1968,  Factors Important in the
     Calculation of Hydraulic Conductivity,  SSSAP, Vol 32, p 760-765,  Rev
     (93), Class (Ilh).

Lagerwerff, J.V., Nakayama, F.S.  and  Frere,  M.H., 1969, Hydrailic  Conductivity
     Related to Porosity and Swelling of Soils,  SSSAP,  Vol 33,  p 3-11, Rev
     (95), Class (Ilg).

Lambe, T.W. and Whitman, R.V., 1979,  Soil Mechanics, John  Wiley and  Sons.,
     Inc., New York, New York, Rev (403), Class (Ib).

Lambe, T.W., 1955, The Permeability of Fine-Grained Soils, In : Symposium on
     Permeability of Soils. ASTM STP  163, Am 890 of Testing and Materials,
     Rev (240), Class (Ilg).

Lascano, R.J. and Van Bavel, C.H.M.,  1982, Spatial Variability  of  Soil
     Hydraulics and Remotely Sensed Soil Parameters, SSSAP,  Vol 46,  No 2,
     p 223-228, Rev (112), Class (VI  ).

Lee, I.K., ed., 1974, Mechanics New Horizons,  American Elsevier Publ.  Co., New
     York, NY, 286 p.

Libardi, P.L., Reichardt, K., Nielsen, D.P.  and Biggar, J.W.,  1980,  Simple
     Field Methods for Estimating Soil Hydraulic Conductivity SSSAJ,  Vol  44
     P 3-7, Rev (234), Class (IIh,d,V  ).

Lieszkowszky, I.P., 1978, Fort Creek  Dam-Impervious Clay Core,  In: Clay Fills,
     The Institute of Civil Engineers, London,  p 157-164,  Rev (319),  Class
     (Id).

Lorenzen, D., 1983, Personal Communication,  Div of Hazardous Waste Management,
     Dept of Env Resources, Harrisburg,  PA,  Rev (427) Class  (III ).
                                      187

-------
Loveday,  J. and Pyle,  J.,  1973i  The  Emerson Dispersion  Test  and  its
     Relationship to Hydraulic Conductivity,  Div of  Soils, Tech  Paper No 15,
     Commonwealth Scientific and Industrial Research Organization, Australia,
     Rev (241), Class (Ilg).

Lumb, P.  and Holt, J.K.,  1968, The Undrained Shear Strength  of a Soft Marine
     Clay from Hong Kong,  Geotechnique,  Vol 18,  p 25-36, Rev (83), Class
     (II  ).

Luthy, R.G. and McMichael, F.C.,  1983, The  Effect of Electrical  Gradients on
     Movement of Organic  Chemical Pollutants in  Saturated Flow Through Soils,
     proposal submitted to Raymond W.  Regan,  PSU, Office of  Hazardous and
     Toxic Waste Management, University  Park,  PA, Rev (188),  Class (Ilg).

Lutton, R.J.,  1982, Evaluating Cover Systems for Solid  and Hazardous
     Waste, EPA, SW-867,  Solid and Hazardous Waste Research  Division,
     Cincinnati, Ohio, Rev (378), Class  (Ilia).

Luxmoore, R.J. and Sharma, M.L.,  1980, Runoff Responses to Soil
     Heterogeneity: Experimental and Simulation  Comparisons  for  Two
     Contrasting Watersheds, Wat Res Res, Vol 16, p  675-684,  Rev
     (267), Class (V ).

Luxmoore, R.J., Spalding,  B.P. and Munro, 1981,  Areal Variation  and Chemical
     Modification of Weathered Shale Infiltration Characteristics, SSSAJ, Vol
     45,  p 687-691, Rev (404), Class (V  ).

Macey, H.H., 1942, Clay-Water Relationships and  the  Internal Mechanisms of
     Drying, Trans of the British Ceramic Society, Vol  41, p 73-121, Rev (64),
     Class (Ilg).

Makeig, K.S.,  1982, Natural Buffers  for  Sludge Leachate Stabilization, Fifth
     Ann..., Rev (233), Class (III ).

Marbeau,  J.P.  and Marechal, A.,  1979,  Geostatistical Estimation  of Uranium Ore
     Reserves, Colloque International Sur Les Techniques D1Evaluation Et
     D1Exploitation Des Gisements D'Uranium,  Rev (361), Class (V ).

Marechal, A. and Shrivastava, P., 1977,  Geostatistical  Study of  a Lower
     Proterozoic Iron Orebody in the Pilbara Region  of  Western Australia,
     15th APCOM Symposium, Brisbane, Australia,  Rev  (360), Class (V  ).

Marshall, T.J. and Holmes, J.M.,  1979, Soil Physics, Cambridge University
     Press, Cambridge, Great Britain,  Rev  (259), Class  (Ib).

Marshall, T.J., 1957,  Permeability and the  Size  Distribution of  Pores, Nature,
     Vol 180,  p 664-665,  Rev (113),  Class  (IIg,h).

Marshall, T.J., 1958,  A Relationship between Permeability and Size
     Distribution of Pores, J of Soil Sci,  Vol 9, No 1, p 1-8, Rev
     (114), Class (Ilg.h).
                                     188

-------
Marthaler, H.P.,  Vogelsanger,  W.,  Richard,  F.  and Wierenga, P.J., 1983, A
     Pressure Transducer for Field Tensiometers, SSSAJ, Vol 47, p 624-627,
     Rev (99), Class (Ilb.d).

Matheron, G. and  De Marsily, G., 1980,  Is Transport  in  Porous Media Always
     Diffusive? A Counterexample,  Wat Res Res,  Vol 16,  No 3, P 901-917, Rev
     (363), Class (Ilia).

Matheron, G., 1963, Principles of  Geostatistics, Economic Geology, Vol 58,
     p 1246-1266, Rev (369), Class (V ).

Matrecon, Inc., 1983, Lining of Waste Impoundment and Disposal Facilities,
     EPA, SW-870, Solid and Hazardous Waste Research Division, Cincinnati,
     Ohio, Rev (248), Class (IV ).

Matyas and Radhakrishna, 1968, Volume Change Characteristics of Partially
     Saturated Soils, Geotechnique,  Vol 18,  No 4, p  432-448, Rev  (315),
     Class (Id).

McBratney, A.B. and Webster, R., 1981,  The  Design of Optimal Sampling Schemes
     for Local Estimation and Mapping of Regionalized Variables-II Program and
     Examples, Computers and Geosciences, Vol 7, No  4,  p 335~365, Rev (367),
     Class (V ).

McBratney, A.B.,  Webster, R. and Burgess, T.M.,  1981, The Design of Optimal
     Sampling Schemes for Local Estimation  and Mapping  of Regionalized
     Variables-I  Theory and Method,  Computers and Geosciences, Vol 7, No 4,
     P 331-33M, Rev (366), Class (V ).

McDowell, C., 1959, The Relation of Laboratory Testing  to Design for Pavements
     and Structures on Expansive Soils, Quart.  Journal  of the Colorado School
     of Mines, Vol 54, No 4, p 122,  Rev (306),  Class (Id).

Molntyre, D.S., Cunningham, R.B.,  Vatanakal, V.  and  Stewart, G.A., 1979,
     Measuring Hydraulic Conductivity in Clay Soils  : Methods, Techniques
     and Errors,  Soil Sci, Vol 128,  No 3, P 171-183, Rev (89), Class (lie).

MoNeill, J.D., Electromagnetic Resistivity  Mapping of Contaminant Plumes,
     Rev (190), Class (II ).

McWhorter, D.B. and Nelson, J.D.,  1978a, Drainage of Earthen Lined Tailing
     Impoundments, Symposium on Uranium Mill Tailings Management, Fort
     Collins, Colorado, Rev (71),  Class (Ilh).

McWhorter, D.B. and Nelson, J.D.,  1978b, Seepage in  the Partially Saturated
     Zone Beneath Tailing Impoundments, Preprint No  78-AG-306, Soc of Mining
     Eng, AIME, Fall Meeting,  Lake Buena Vista,  FL,  Rev (70), Class (Ilh).

McWhorter, D.B. and Nelson, J.D.,  1979, Unsaturated  Flow Beneath Tailing
     Impoundments, ASCE: J of the  Geotech Div,  Vol 105, No GT11, p 1317-1334,
     Rev (69), Class (Ilh).
                                     189

-------
Mesri, G.  and Olsen,  R.E.,  1971,  Mechanisms Controlling the Permeability of
     Clays,  Clay and  Clay Minerals, Vol  19, p  151-158, Rev (60), Class (Ilg).

Michaels,  A.S. and Lin,  C.S.,  1955, Permeablity of Kaolinite, Industial and
     Engineering Chemistry,  Vol  46, p  1239-1246, Rev  (63), Class (Ilg).

Miller, E.E. and Klute,  A.,  1967,  The  Dynamics of Water, Part I-Mechanical
     Forces : Irrigation Irrigation of Agricultural Lands, R.M. Hagen, H.R.
     Raise and T.W. Edminster, eds., Am  Sod of Agronomy, Madison, Wise, p
     209-240, Rev (322), Class (Ib).

Miller, E.E. and Miller, R.D., 1955, Theory of Capillary Flow :  I. Practical
     Implications, SSSAP, Vol  19,  No 3,  P  267-271, Rev (107), Class (VI ).

Miller, E.E. and Miller, R.D., 1956, Physical  Theory  for Capillary
      Flow Phenomena, J  of  Applied Physics, Vol 27, No 4, p 324-332,
      Rev (103), Class (VI  ).

Miller, E.E., 1980, Similitude and Scaling of  Soil Water Phenomena,
     In D. Hillel (ed),  Applications of  Soil Physics, Academic
     Press,  New York, p  300-318,  Rev  (101), Class  (VI ).

Miller, R.D. and Miller, E.E., 1955, Theory of Capillary Flow : II.
     Experimental Information, SSSAP,  Vol  19,  No 3, p 271-275, Rev
     (108),  Class (VI ).

Millington,  R.J. and  Quirk,  J.P.,  1959,  Permeability  of Porous Media, Nature
     (London), Vol 183,  P 387-388, Rev (268),  Class (II ).

Mitchell,  J.K., Hooper,  D.R. and Campanella, R.G., 1965, Permeability of
     Compacted Clays, ASCE:  J  of the Soil  Mech and Found Div, Vol 91,
     No SM4, p 41-65, Rev (65),  Class  (Ilg).

Mitchell,  J.K., 1976, Fundamentals of  Soil Behavior,  John Wiley and
     Sons, Inc., New  York,  New York, Rev (405), Class (Ib).

Montague,  P., 1982, Hazardous  Waste Landfills  : Some  Lessons from New Jersey,
     ASCE-Civil Engineering, Vol. 52,  No.  9, pg 53-56, Rev  (8), Class  (III  ).

Moore, C.A., 1983, Landfill and  Surface  Impoundment Performance Evaluation,
     EPA,  SW-869, Solid  and Hazardous  Waste Research  Division, Cincinnati,
     Ohio, Rev  (380), Class (III ).

Mualem, Y. and Dagan, G., 1978,  Hydraulic  Conductivity of Soils:  Unified
     Approach to the  Statistical Models, SSSAJ, Vol 42, p 392-395, Rev  (94),
     Class  (Ilh).

Mualem, Y., 1978, Hydraulic Conductivity of Unsaturated Porous Media  :
     Generalized Macroscopic Approach, Wat Res Res, Vol 14, No 2,
     p 325-334, Rev  (91), Class  (Ilh).

Murray, D.E., 1982,  Case Study of Leachate and Gas Management at a Sanitary
     Landfill, Fifth Ann..., Rev (221),  Class  (Illb).


                                      190

-------
Nagpal, N.K. and DeVries,  J.,  1976,  An Evaluation  of  the Instantaneous Profile
     Method for In Situ Determination of Hydrologic Properties of Layered
     Soil, Can J Soil Sci, Vol 56,  p 453-461,  Rev  (406), Class (lib).

Nichols, D.G., 1982,  Field Investigation of  a  Superfund Site, Fifth Ann...,
     Rev (232), Class (Illb).

Nielsen, D.R. and Biggar,  J.W., 1961,  Measuring Capillary Conductivity, Soil
     Sci, Vol 92, p 192-193,  Rev (85), Class (Ilb.c).

Nielsen, D.R., Biggar, J.W. and Ehr, K.T., 1973, Spatial Variability of Field
     Measured Soil-Water Properties, Hilgardia,  Vol  42, p 215-259, Rev (26,
     Class (V ).

Nielsen, D.R., Davidson, J.M., Biggar, J.W.  and Miller, R.J., 1964, Water
     Movement Through Panoche Clay  Loam Soil,  Hilgardia, Vol 35, No 17, p
     491-505, Rev (86), Class (IIh,g).

Nielsen, D.R., Jackson, R.D.,  Gary,  J.W. and Evans, D.D., 1972, Soil Water, Am
     Soc of Agronomy and Soil Sci Soc of Am, Madison,  Wise, Rev (426), Class
     (Ib).

Nielsen, D.R., Kirkham, D. and Perrier, E.R.,  1960, Soil Capillary
     Conductivity : Comparison of Measured and Calculated Values,
     SSSAP, Vol 24, No 3,  P 157-160, Rev (37), Class  (IIb,c,h).

Nightingale, H.I. and Bianchi, W.C., 1970, Rapid Measurement of Hydraulic
     Conductivity Changes in Slowly Permeable  Soils,  Soil Sci, Vol 110,
     No 4, p 221-228, Rev (18), Class (Ha,c).

Ogata, G. and Richards, L.A.,  1957,  Water Content  Changes Following Irrigation
     of Bare-Field Soil That is Protected from Evaporation, SSSAP, Vol 21, No
     4, p 355-359, Rev (59),  Class  (II ).

Olsen, H.W., 1965, Deviations from  Darcy's Law in  Saturated Clay, SSSAP, Vol
     29, No 2, p 135-140,  Rev (32),  Class (Ila.c.e)

Olsen, R.E. and Daniel, D.E.,  1979,  Field and  Laboratory Measurement of the
     Permeability of Saturated and  Partially Saturated Fine-Grained Soils,
     Permeability and Groundwater Contaminant  Transport, ASTM STP 746, T.F.
     Zimmie and C.O.  Riggs, eds., Am Soc of  Testing and Materials,
     Philadelphia, PA, Rev (26), Class (II  ).

Olsen, R.E. and Langfelder, L.J., 1965, Pore Water Pressures in Unsaturated
     Soils, ASCE: J of the Soil Mech and Found Div, Vol 91, No SM4, p 127-150,
     Rev (66), Class (He).

Olsen, T.C. and Swartzendruber, D.,  1968, Velocity-Gradient Relationships for
     Steady-state Unsaturated Flow  of Water  in Nonswelling Artificial Soils,
     SSSAP, Vol 32, No 4,  p 457-462, Rev (43), Class  (Ilg).
                                      191

-------
Ortiz, N.V.,  McWhorter,  D.B.,  Sanada,  O.K.  and  Duke, H.R., 1978, Growth of
     Groundwater Mounds  Affected by  In-Transit  Water, Wat Res Res, Vol 14,
     No 6,  p 1084-1088,  Rev (72),  Class  (Ilia).

Oster, J.D.  and Rhoades, J.D.,  1976, Various  Indices for Evaluating the
     Effective Salinity  and Sodicity of  Irrigation Waters, Proc Inter Salinity
     Confer,  Texas Tech  University,  Lubbock,  Texas, p 1-14, Rev (181), Class
     (Ilia).

Page, L.M.,  Raila, S.J.  and Woliner, W.R.,  1982,  Investigations of Leachate
     Contamination of Ground and Surface Waters at the  Fresh Kills Landfill,
     Fifth Ann..., Rev (226),  Class  (Illb).

Parker, H.,  1979, The Volume-Variance  Relationship : A  Useful Tool for Mine
     Planning, Engineering Mining Journal,  October, p 106-119, Rev (355),
     Class (V ).

Parker, J.C., Amos, D.F. and Sture,  S.f  1980, Measurement of Swelling
     Hydraulic Conductivity, and Shear Strength in a Multistage Triaxial
     Test,  SSSAP, Vol 44,  p 1133-1138, Rev  (217), Class (He).

Parlange, J., 1973, Horizontal Infiltration of  Water in Soils:  A Theoretical
     Interpretation of Recent Experiments,  SSSAP, Vol 37, p 329-330, Rev
     (292),  Class (Ib).

Parry, R.H.G., 1971, A Simple Driven Piezometer,  Geotechnique, Vol 21, No 2, p
     163-167, Rev (79),  Class (lid).

Peck, A.J.,  Luxmoore, R.J. and Stolzy, J.L.,  1977, Effects of Spatial
     Variability of Soil Hydraulic Properties in Water  Budget Modeling, Wat
     Res Res, Vol 13, No 2, p 348-354, Rev  (110), Class (VI ).

Peck, A.J.,  1982, Field  Variability  of Soil Physical Properties, In: D.
     Hillel,  ed., Advances in Irrigation, Vol 2,  p 189-221, Academic Press,
     New York, Rev (270),  Class (V ).

Perrier, E.R. and Evans, D.D.,  1961, Soil Moisture Evaluation by Tensiometers,
     SSSAP,  Vol 25, No 3,  P 173-175, Rev (36),  Class (Ilb.Va).

Perrier, E.R. and Gibson,  A.C., 1982,  Hydrologic Simulation on Solid Waste
     Disposal Sites, EPA,  SW-868,  Solid  and Hazardous Waste Research Division,
     Cincinnati, Ohio, Rev (377),  Class  (Ilia).

Perroux, P.M., Raats, P.A.C. and Smiles, D.E.,  1982, Wetting Moisture
     Characteristic Curves Derived from  Constant-rate Infiltration into Thin
     Soil Samples, SSSAJ,  Vol 46,  No 2,  p 231-234, Rev  (197), Class  (Hh).

Peters, D.B., 1965, Water Availability : Methods of Soil Analysis, C.A. Black,
     ed., Am Soc of Agronomy, Madison, Wise,  p  279-285, Rev (336), Class  (Ib).

Philip, J.R.  and Smiles, D.E.,  1982, Macroscopic Analysis of the Behavior of
     Colloidal Suspensions, Advances in  Colloid and Interface Sci, Vol 17,
     p 83-103, Rev (198),  Class (Id).
                                      192

-------
Philip,  J.R.,  1954a,  An Infiltration Equation with Physical Significance, Soil
     Sci,  Vol  77,  No  2,  p  153-157, Rev  (293), Class (Ib).

Philip,  J.R.,  1954b,  The Concept of Diffusion Applied to Soil Water, Proc
     Nat'l Acad Sci,  India, Vol A24, p  93-104, Rev (150), Class (Ib).

Philip,  J.R.,  1957, The Theory of Infiltration : 4. Sorptivity and Algebraic
     Infiltration  Equations, Soil Sci,  Vol 84, No 3, P 257-264, Rev  (161),
     Class (Ib).

Philip,  J.R.,  1964, Similarity Hypothesis for Capillary Hysteresis in Porous
     Materials, J  of  Geophysical Res, Vol 69, No 8, p 1553*1562, Rev (124),
     Class (Ib).

Philip,  J.R.,  1967, Sorption and Infiltration in Heterogeneous Media, Aust J
     Soil Res, Vol 5,  P 1-10, Rev (288), Class (II ).

Philip,  J.R.,  1968, Moisture Equilibrium in the Vertical in Swelling Soils I.
     Basic Theory, Aust J  of Soil Res,  Vol 7, p 99-120, Rev (127), Class (Id).

Philip,  J.R.,  1969a,  Hydrostatics and Hydrodynamics in Swelling Soils, Wat Res
     Res,  Vol  5, No 5,  p 1070-1077, Rev (126), Class (Id).

Philip,  J.R.,  1969b,  Moisture Equilibrium in the Vertical in Swelling Soils
     II. Application,  Aust J of Soil Res, Vol 7, p 121-141, Rev (140), Class
     (Id).

Philip,  J.R.,  1970a,  Addendum to Three  Papers on Hydrostatics in Swelling
     Soils, Rev (246),  Class (Id).

Philip,  J.R.,  1970b,  Hydrostatics in Swelling Soils and Soil Suspensions :
     Unification of Concepts, Soil Sci, Vol 109, No 5, p 294-298, Rev (123),
     Class (Id).

Philip,  J.R.,  1970c,  Reply, Wat Res Res, Vol 6, No 4, p 1248-1251, Rev (310),
     Class (Id).

Philip,  J.R.,  1972, Future Problems of  Soil Water Research, Soil Sci, Vol 113,
     No  4, p 294-300,  Rev  (122), Class  (Ib).

Philip,  J.R.,  1974, Fifty  years Progress in Soil Physics, Geoderma,
     Vol 12, p 265-280,  Rev (121), Class (Ib).

Philip,  J.R.,  1980, Field  Heterogeneity : Some Basic Issues, Wat Res Res, Vol
     16, No 2, p 443-448,  Rev (141), Class (Id).

Prudic,  D.E.,  1982, Hydraulic Conductivity of a Fine-Grained Till, Cattaraugus
     County, New York,  Groundwater, Vol 20, No 2, p 194-204, Rev (219), Class
     (II ).

Quinn, K.J., 1983, Numerical Simulation of Typical Zone of Saturation Landfill
     Designs,  6th  Ann...,  Madison, Wise, Rev (169), Class (Ilia).
                                     193

-------
Quirk,  J.P.  and Aylmore, L.A.G., 1960, Swelling and Shrinkage of Clay-Water
     Systems,  Transactions of the 7th International Congress of Soil Science,
     Madison,  Wise.,  Rev (116), Class (Id).

Quirk,  J.P., 1955,  Significance of Surface Areas Calculated from Water Vapor
     Sorption Isotherms by use  of the B.E.T.  Equation, Soil Sci, Vol 80, No
     6, p 423-429,  Rev (115), Class  (Id).

Quirk,  J.P., 1978,  Some Physio-Chemical Aspects of Soil Structural Stability-A
     Review, In: Modification of Soil Structure, W.W.  Emerson, R.D. Bond  and
     A.R. Dexter, eds., John Wiley and Sons,  Ltd., New York, New York, p  3-16,
     Rev (419), Class (Ib).

Rakoczynski, R.W.,  1982, Advanced Secure  Landfill Design,  Fifth Ann..., Rev
     (225), Class (IIIc).

Rao, P.S.C., Rao, P.Y. and Davidson, J.M., 1977, Estimation of the Spatial
     Variablility of the Soil Water  Flux,  SSSAJ, Vol  41,  p 1208-1209, Rev
     (271), Class (V ).

Rawlins, S.L. and Gardner, W.H., 1963, A  Test of the  Validity of the Diffusion
     Equation for Unsaturated Flow of Soil Water, SSSAP,  Vol 27, No 5, p
     507-511, Rev (41),  Class  (Ilc.g).

Rawls, W.J., Brakensiek,  D.J. and Saxton,  K.E., 1982,  Estimation of Soil  Water
     Properties, Trans of  ASAE, Vol  25,  p 1316-1320,  1328, Rev  (272), Class
     (Ib).

Reeve, R.C., 1965, Hydraulic Head  :  Methods  of  Soil  Analysis, C.A. Black, ed.,
     Am  Soc of  Agronomy,  Madison, Wise,  p 180-196,  Rev (330), Class  (Ib).

Reeves,  M.  and  Miller, E.E., 1975,  Estimating Infiltration for  Erratic
     Rainfall,  Wat Res Res,  Vol 11,  No  1, p  102-110,  Rev (290),  Class  (Ib).

Regan, R.W., 1982, Summary of the  Hazardous  Wastes  Handled by  Commercial
     Facilities in Pennsylvania during 1981, Institute for Research on Land
     and Water  Resources,  Rev (6),  Class (Ilia).

Reginato,  R.J.  and Jackson,  R.D.,  1971,  Field Measurement of Soil-Water
     Content  by Gamma-Ray Transmission Compensated for Temperature
     Fluctuations, SSSAP,  Vol 35,  P 529-533, Rev (287),  Class (II  ).

Reichardt,  K.  and Libardi,  P.L., 1974,  A New Equation to Estimate Soil-Water
     Diffusivity, Proceedings of a Symposium Isotope and Radiation Techniques
      in  Soil  Physics nd Irrigation Studies,  Vienna, Rev (291),  Class (II ).

Reichardt,  K.,  Libardi, P.L. and Nielsen, D.R., 1975, Unsaturated Hydraulic
     Conductivity  by a Scaling Technique, Soil Sci, Vol. 120,  No.  3,  P
     165-168,  Rev  (14), Class  (VI ,IIh).

Reichardt,  K.,  Nielsen, D.R. and Biggar, J.W., 1972, Scaling of Horizontal
      Infiltration  into Homogeneous Soils, SSSAP, Vol 36, No 2,  p 241-245,
     Rev (104), Class (VI ).


                                      194

-------
Remy, J.P., 1973,  The Measurement of Small  Permeabilities  in  the Laboratory,
     Geotechnique, Vol 23,  No 23, p 454-458,  Rev (30),  Class  (Ila.b.c).

Rendu, J.M.,  1980, A Case Study : Kriging for Ore Valuation and Mine Planning,
     Engineering Mining Journal,  January, p 114-120,  Rev (353), Class  (V  ).

Rhoades, J.D., 1971, Quality of Water for Irrigation,  Soil Sci, Vol 113,  No 4,
     p 277-284, Rev (177),  Class (Ib).

Richards, L.A., 1941, A Pressure-Membrane Extraction  Apparatus for Soil
     Solution, Soil Sci, Vol 51,  p 377~386, Rev (87),  Class (IIb,c).

Richards, L.A., 1965, Physical Conditions of Water in a Soil  : Methods of Soil
     Analysis, C.A. Black,  ed., Am Soc of Agronomy, Madison,  Wise, p 128-151,
     Rev (328), Class (Ib).

Richards, S.J., 1965, Soil  Suction Measurements with  Tensiometers  : Methods of
     Soil Analysis, C.A. Black, ed., Am Soc of Agronomy, Madison, Wise, p
     153-163, Rev (329), Class (II ).

Ritchie, J.T., Kissel, D.E. and Burnett, E.,  1972, Water Movement in
     Undisturbed Swelling Clay Soils, SSSAP,  Vol  36,  No 6, p 874-879, Rev
     (56), Class (Ilg).

Robins, J.S., 1965, Evapotranspiration : Methods of Soil Analysis, C.A. Black,
     ed., Am Soc of Agronomy, Madison,  Wise,  p 286-297, Rev (337), Class  (Ib).

Rogowski, A.S. and Weinrich, B.E., 1981, Modeling Water Flux  on Stripmined
     Land, Trans of ASAE, Vol 24, p 935-940,  Rev (296), Class (Ib).

Rogowski, A.S., 1971, Watershed Physics: Model of the Soil Moisture
     Characteristic, Wat Res Res, Vol 7, p 1575-1582,  Rev  (273),
     Class (V ).

Rogowski, A.S., 1972, Watershed Physics: Soil Variability  Criteria,
     Wat Res Res,  Vol 8, p 1015-1023, Rev (274), Class (V  ).

Rose, C.W. and Krishnan, A., 1967, A Method of Determining Hydraulic
     Conductivity Characteristics for Non-Swelling Soils In Situ, and of
     Calculating Evaporation from Bare Soil,  Soil Sci,  Vol 103, No 6,
     p 369-373, Rev (50), Class (II ).

Rose, C.W., Stern, W.R. and Drummond, J.E., 1965, Determination of Hydraulic
     Conductivity as a Function of Depth and Water Content for Soil In Situ,
     Aust J of Soil Res, Vol 3, P 1-9,  Rev (407), Class (Ilh).

Roulier, M. and Otte, A., 1983, Performance of Clay Caps and  Liners for
     Disposal Facilities, EPA Contract No.  68-03-3149,  Rev (251),
     Class (IV ).

Roulier, M.H., Stolzy, L.H., Letey, J.  and Weeks, L.V., 1972, Approximation of
     Field Hydraulic Conductivity by Laboratory Procedures on Intact Cores,
     SSSAP, Vol 36, p 387-393, Rev (408), Class (lie).


                                     195

-------
Roulier, M.H.,  1983,  Prepare Technical  Resource  Document  on Maintenance, and
     Evaluation of Clay Liners for Hazardous Waste Facilities, EPA contract
     No. 68-03-3149-1-2,  Rev (211),  Class (IV ).

Rowe, P.W. and Barden,  L.,  1966,  A New  Consolidation  Cell, Geotechnique, Vol
     16, No 2,  p 162-170,  Rev (82),  Class (II ).

Royle, A.G., 1979, Why  Geostatistics?,  Engineering Mining Journal, May, p
     92-99, Rev (348),  Class (V ).

Runyon, K., Slade, R.C. and Leitzell, C.R.,  1982,  Red Hill Disposal Site : A
     Case Study, Fifth  Ann..., Rev (224),  Class  (Illb).

Russo, D. and Bresler,  E.,  1980,  Scaling Soil Hydraulic Properties of a
     Heterogeneous Field,  SSSAJ,  Vol 44,  p 681-684, Rev (275), Class
     (VI ).

Sandefur, R.L.  and Grant,  D.C., 1980, Applying Geostatistics  to Roll Front
     Uranium in Wyoming,  Engineering Mining Journal,  February, p 90-96, Rev
     (354), Class (V  ).

Sanders, T.G. and Adrian,  D.D., 1978, Sampling Frequency  for  River Quality
     Monitoring, Wat  Res Res, Vol 14, No 4,  p 569-576, Rev (156), Class (V ).

Scheidegger, A.E., 1974,  The Physics of Flow Through  Porous Media, University
     of Toronto Press,  Toronto, Rev (409),  Class (Ib).

Schraugge, T.J., Jackson,  T.J. and McKim,  H.L, 1980, Survey of Methods for Soil
     Moisture Determination, Wat Res Res,  Vol 16,  No  6, p 961-979, Rev (160),
     Class (II ).

Schofield, R.K., 1 938, Pore-Size Distribution as  Revealed by the Dependence
     of Suction on Moisture Content, Trans of the  First Commission of the
     International Society of Soil Sci, Vol A, Rev (159), Class (Ilg).

Shainberg, I.,  Rhoades, J.D. and Prather,  R.J.,  1981 a, Effect of Low
     Electrolyte Concentration on Clay  Dispersion  and Hydraulic Conductivity
     of a Sodic Soil, SSSAJ, Vol 45, No 2,  p 273-277, Hev (179), Class (Ilg).

Shainberg, I.,  Rhoades, J.D., Suarez, D.L.  and Prather, R.J., 198lb, Effect of
     Mineral Weathering on Clay Dispersion and Hydraulic  Conductivity of Sodic
     Soils, SSSAJ, Vol  45,  No 2,  p 287-291,  Rev  (178), Class  (Ilg).

Sharma, M.L. and Luxmoore,  R.J.,  1979,  Soil Spatial Variability and Its
     Consequences on  Simulated Water Balance, Wat  Res Res, Vol 15, p
     1567-2573, Rev (276),  Class (V ).

Sharma, M.L., Gander, G.A.  and Hunt, C.G.,  1980, Spatial  Variability of
     Infiltration in  a  Watershed, J Hydrology, Vol 45, -p  101-122, Rev  (277),
     Class (V ).
                                      196

-------
Sharma, M.L., 1983,  Field Variability and Its Hydrological  Consequences  -  A
     Synthesis.  A Conference on Hydrology and Water Resources,  Institute  of
     Engineers, Hobart, Australia (In press), Rev (278),  Class  (V  ).

Shiraek, S.J., 1983,  Landfill Development in Shallow Saturated Soils  :  A  Case
     History, 6th Ann..., Madison,  Wise, Rev (170),  Class (Illb).

Shuckrow, A.J., Pajak,  A.P.  and Touhill, C.J., 1982,  Management  of Hazardous
     Waste Leachate, EPA, SW-871, Solid and Hazardous Waste Research Division,
     Cincinnati, Ohio,  Rev (379), Class (Ilia).

Sienko, M. J. and Plane, R.A., 1966,   Chemistry Principles  and Properties,
     McGraw-Hill Book Co., Rev (10),  Class (la).

Silva, A.J., Hetherman, J.R. and Culnan, D.I., 1981,  Low-Gradient Permeability
     Testing of Fine-Grained Marine Sediments, Permeability and  Groundwater
     Contaminant Transport,  ASTM STP 746, T.F. Zimmie and C.O. Riggs,  eds., Am
     Soc of Testing and Materials,  Philadelphia,  PA,  Rev  (238),  Class  (II  ).

Sisk, S.W., 1981, NEIC  Manual for Groundwater/Subsurface  Investigations  at
     Hazardous Waste Sites,  EPA-330/9-81-002, PB  82-103 755,  Rev (164),
     Class (Ilia).

Smalley, I.J., 1978, Mineralogy,  Interparticle Forces and Soil Structures  of
     the Leda/Champlain Clays of Eastern Canada,  In:  Modification of Soil
     Structure, W.W. Emerson, R.D.  Bond and A.R.  Dexter,  eds., John Wiley  and
     Sons, Ltd., New York, New York,  p 59~68, Rev (422),  Class  (Id).

Smiles, D.E. and Gardiner, B.N.,  1982,  Hydrodynamic Dispersion During
     Unsteady, Unsaturated Water Flow in a Clay Soil,  SSSAJ,  Vol 46,
     p 9-14, Rev (196), Class (Ib).

Smiles, D.E. and Philip, J.R., 1978,  Solute Transport During Adsorption  of
     Water by Soil : Laboratory Studies and Their Practical Implications,
     SSSAP, Vol 42,  No  4, p 537-544,  Rev (111), Class (VI ).

Smiles, D.E. and Young, E.G., 1965, Hydraulic Conductivity  Determinations  by
     Several Field Methods in a Sand Tank,  Soil Sci,  Vol  99,  No  2, p 83-87,
     Rev (45), Class (II ).

Smiles, D.E., Knight, J.H. and Perroux, K.M., 1982,  Adsorption of Water  by
     Soil : The Effect  of a Surface Crust,  SSSAJ, Vol 46, p 476-481, Rev
     (199), Class (Ilg).

Smiles, D.E., Perroux,  K.M., Zegelin,  S.J.  and Raats,  P.A.C., 1981,
     Hydrodynamic Dispersion During Constant Rate Absorption of
     Water by Soil,  SSSAJ, Vol 45,  No 3, P 453-458,  Rev (192),
     Class (Ib).

Smiles, D.E., Raats, P.A.C.  and Knight, J.H., 1982,  Constant Pressure
     Filtration : The Effect of a Filter Membrane,  Chem Eng Sci,
     Vol 37, No 5, p 707-714, Rev (200), Class (Ib).
                                      197

-------
Smiles, D.E.,  1978,  Constant  Rate  Filtration of Bentonite, Chera Eng Sci, Vol
     33, P 1355-1361,  Rev (143), Class  (Id).

Smith,  L.  and  Schwartz,  F.W.,  1981, Mass Transport 3. Role of Hydraulic
     Conductivity Data in Prediction, Wat Res Res, Vol 17, No 5,
     p 1463-1479, Rev  (344),  Class (II  ).

Smith,  R.M.  and Browning, D.R., 1942, Persistant Water-Unsaturation of Natural
     Soil in Relation  to Various Soil and Plant Factors, SSSAP, Vol 7, p
     114-119,  Rev (58),  Class (Ilg).

Sposito, G., Giraldez, J.V. and Reginato, R.J., 1976, The Theoretical
     Interpretation  of Field  Observations of Soil Swelling Through a Material
     Coordinate Transformation, SSSAJ,  Vol 40, p 208-211, Rev (244), Class
     (Id).

Sposito, G., 1972, Thermodynamics  of Swelling Clay-Water Systems, Soil Sci,
     Vol 114,  No 4,  p  243-249, Rev (311), Class (Id).

Sposito, G., 1973, Volume Changes  in Swelling Clays, Soil Sci, Vol 115, No 4,
     p 315-320, Rev  (313), Class (Id).

Sposito, G., 1975a,  A  Thermodynamic Integral Equation for the Equilibrium
     Moisture  Profile  in Swelling  Soil, Wat Res Res, Vol 11, No 3, p 449-450,
     Rev (256), Class  (Id).

Sposito, G., 1975b,  On the Differential Equation for the Equilibrium Moisture
     Profile in Swelling Soil, SSSAP, Vol 39, p 1053-1056, Rev (317), Class
     (Id).

Sposito, G., 1975c,  Steady Vertical Flows in Swelling Soils, Wat Res Res,
     Vol 11, No 3, P 464, Rev (316), Class (Id).

Sposito, G., 1978, The Statistical Mechanical Theory of Water Transport
     Through Unsaturated Soil 1. The Conservation Laws, Wat Res Res,
     Vol 14, No 3, P 474-484,  Rev  (302), Class (Id).

Stecker, P.P.  and Garvin, J.W., 1983, Control and Prevention of Landfill
     Leachate  Seeps, 6th Ann..., Madison, Wise, Rev (171), Class (Illb).

Swartzendruber, D.,  De Boodt,  M.F.  and  Kirkham, D., 1954, Capillary Intake
     Rate of Water and Soil Structure,  SSSAP, Vol 18, No 1 , p 1-7, Rev (186),
     Class (Ib).

Swartzendruber, D.,  1968, The Applicability of Darcy's Law, SSSAP, Vol 32,
     No 1, p 11-18,  Rev (33),  Class (Ilg).

Swartzendruber, D.,  1963, Non-Darcy Behavior and the Flow of Water in
     Unsaturated Soils,  SSSAP, Vol 27,  No 5, p 491-495, Rev (42),
     Class (Ilg).
                                     198

-------
Swartzendruber, D.,  1987, Rigorous Deviation and Interpretation  of  the  Green
     and Ampt Equation,  In:  Infiltration Development and  Application, Yu-Si
     Fok, ed.,  Univ. of  Hawaii,  Honolulu,  Hawaii.

Sykes, J.F., Pahwa,  S.B., Lantz, R.B.  and Ward,  D.S.,  1982, Numerical
     Simulation of  Flow  and  Contaminant Migration at an Extensively Monitored
     Landfill,  Wat  Res Res,  Vol  18,  No 6,  p 1687-1704,  Rev  (210), Class
     (IHb).

Talsma, T. and Flint, S.E.,  1958, Some Factors Determining  the Hydraulic
     Conductivity of Subsoils with Special Reference to Tile  Drainage
     Problems,  Soil Sci, Vol 85, p 198-206,  Rev (416),  Class  (Ilg).

Talsma, T. and Van  Der Lelij, A., 1976, Infiltration and  Water Movement in an
     In Situ Swelling Soil During Prolonged Ponding,  Aust J Soil Res, Vol 14,
     P 337-349, Rev (414), Class (Id).

Talsma, T., 1974, Moisture Profiles in Swelling Soils,  Aust J Soil  Res, Vol
     12, p 71-75, Rev (415), Class (Id).

Talsma, T., 1977a,  A Note on the Shrinkage Behavior  of a  Clay Paste under
     Various Loads,  Aust J Soil  Res, Vol 15,  p 275-277, Rev (133),  Class (Id).

Talsma, T., 1977b,  Measurement of the  Overburden Component of Total Potential
     in Swelling Field Soils, Aust J Soil Res, Vol 15,  p  95-102, Rev (258),
     Class (Id).

Tchobanoglous,  G.,  Theisen,  H. and Eliassen,  R.,  1977,  Solid  Wastes
     Engineering Principles  and  Management Issues, McGraw-Hill Book
     Company, New York,  Rev  (375), Class (Ilia).

Terzaghi, C., 1925,  Principles of Soil Mechanics : III  Determination of
     Permeability of Clay, Engineering News Record,  Vol 95, No   5,  p 832-836,
     Rev (61 ),  Class (Ilg).

Terzaghi, Karl and  Peck, Ralph,  1948,   Soil Mechanics  in  Engineering Practice,
     John Wiley & Sons,  Inc., Rev (2), Class (Ib).

Topp, G.C. and Binns, M.R.,  1976, Field Measurements of Hydraulic Conductivity
     with a Modified Air Entry Permeameter,  Can J Soil  Sci, Vol  56, p 139-147,
     Rev (255), Class (lid).

Topp, G.C., Zebchuk, W.D. and Dumanski, J.,  ?, In Situ Measurement  of Soil
     Water Properties for Differentiation of Soil Map  Units,  Handout, ?,
     Rev (154), Class (Ia,d).

Townsend, M.A., 1982, Impact of  Sewage Irrigation on the  Chemistry  of Ground
     and Surface Waters, Fifth Ann..., Rev (230),  Class (Illb).

U.S. Environmental  Protection Agency,  1988,  Design Construction  and Evaluation
     of Clay Liners  for  Waste Management Facilities, EPA/530/SW86/007F,
     Washington, DC.
                                      199

-------
U.S. Geological Survey,  1977,  National Handbook  of Recommended Methods for
     Water-Data Acquisition, Office  of Water  Data Coordination, Geological
     Survey,  U.S.  Department of  the  Interior,  Reston, Virginia, Rev  (297),
     Class (Ib).

Vachaud,  G.,  1967, Determination of  the  Hydraulic Conductivity of Unsaturated
     Soils from an Analysis of Transient Flow Data, Wat Res Res, Vol 3,
     p 697-705, Rev (410),  Class (Ilh).

Van Bavel, C.H.M.  and Kirkham, D., 1948,  Field Measurement of Soil
     Permeability Using  Auger  Holes,  SSSAP, Vol  13, p 90-96, Rev
     (214),  Class (Ila.d).

Van Bavel, C.H.M., Stirk,  G.B. and Brust,  K.J.,  1968, Hydraulic Properties of
     a Clay Loam Soil and the  Field  Measurement  of Water Uptake by Roots I.
     Interpretation of Water Content and Pressure Profiles, SSSAP, Vol 32,
     p 310-317, Rev (411),  Class (Id).

Van Zelst, T.W., 1948, An Investigation  of the Factors Affecting Laboratory
     Consolidation of Clay, Proceedings,  Second  International Conference on
     Soil Mechanics and  Foundations  Engineering, Rotterdam, Vol 7, p 52-61,
     Rev (75),  Class (Ilg).

Vaughan,  P.R.,  1969, A Note on Sealing Piezometers in Boreholes, Geotechnique,
     Vol 19,  No 3, P 405-413,  Rev 78), Class  (Ilg).

Vieira, S.R., Nielsen, D.R. and  Biggar,  J.W.,  1982, Spatial Variability of
     Field Measured Infiltration Rate, SSSAJ,  Vol 45, p 1040-1048, Rev (279),
     Class (V ).

Vomocil,  J.A.,  1965, Porosity  :  Methods  of Soil  Analysis, C.A. Black, ed., Am
     Soc of Agronomy, Madison, Wise,  p 299~314,  Rev (338), Class (Ib).

Wang, M.C.,  1983, Permeability Behavior  of Compacted Soil Liners for Hazardous
     Waste Disposal, Research  Proposal,  Rev (5), Class  (IIe,g,c,d).

Ware, S.A. and Jackson,  G.S.,  1978,  Liners for Sanitary Landfills and Chemical
     and Hazardous Waste Disposal Sites, EPA-600/9-78-005, PB-293 335, Rev
     (163),  Class (Ilia,c,IV  )

Warrick,  A.W. and Amoozegar-Fard, 1979,  Infiltration and Drainage Calculations
     Using Spatially Scaled Hydraulic Properties, Wat Res Res, Vol 15, p
     1116-1120, Rev (280),  Class (V  ).

Warrick,  A.W. and Nielsen,  D.R., 1980, Spatial Variability of Soil Physical
     Properties in the Field,  In: D. Hillel,  ed., Applications of Soil
     Physics, p 319-344, Academic Press, New  York, Rev  (281), Class  (V ).

Warrick,  A.W.,  Mullen, G.J. and  Nielsen, D.R., 1977, Scaling Field-Measured
     Soil Hydraulic Properties Using a Similar Media Concept, Wat Res Res,
     Vol 13, No 2, p 355-362,  Rev (109), Class (VI  ).
                                      200

-------
Watson, K.K. ,  1967, The Measurement of the Hydraulic  Conductivity  of
     Unsaturated Porous Materials Using a Zone of  Entrapped  Air,
     SSSAP, Vol 31, p 716-721,  Rev (ill 2),  Class (II  ).

Webster, R. and Cuanalo De La C., H.E.,  1975,  Soil Transect  Correlograms of
     North Oxfordshire and Their Interpretation, J of Soil Sci, Vol 26, No 2,
     p 176-194, Rev (372), Class (V ).

Webster, R. , 1973> Automatic Soil-Boundary Location  from Transect  Data,
     Mathematical Geology, Vol 5, No 1,  p 27-37, Rev  (371),  Class  (V  ).

Webster, R., 1978, Optimally Partitioning Soil Transects, J  of Soil Sci, Vol
     29, p 388-402, Rev (373),  Class (V ).

Weeks, L.V. and Richards,  S.J., 1967,  Soil Water Properties  Computed  from
     Transient Flow Data,  SSSAP, Vol  31,  No 6,  p  721-725, Rev (38),  Class
     (lib).

White, I., Smiles, D.E. and Perroux, K.M. , 1979, Absorption  of Water  by Soil  :
     The Constant Flux Boundary Condition, SSSAJ,  Vol 43, No 4, p  659-664, Rev
     (142), Class (Ib).

Whittle, P., On Stationary Processes in the Plane, Applied Mathematics
     Laboratory, New Zealand Department of Scientific and Industrial
     Research, Rev (374),  Class (V ).

Wilkes, P.F.,  1970, The Installation of Piezometers  in  Small Diameter
     Boreholes, Geotechnique, Vol 20,  No 3,  p  330-333,  Rev (81),
     Class (II ).

Wilkinson, G.E. and Klute, A.,  1959, Some Tests of the  Similar Media  Concept  :
     II. Flow Systems Data, SSSAP, Vol.  23,  No 6,  p 434-437,  Rev (106), Class
     (VI ).

Wilkinson, W.B., 1968, Constant Head in Situ Permeability Tests in Clay
     Strata, Geotechnique, Vol 1 1 , No 2,  p 172-194, Rev (44), Class
Wu, T.H., Chang,  N.Y.  and Elfatih,  M.A.,  1978,  Consolidation and Strength
     Properties of a Clay,  ASCE:  J  of  the Geotech  Eng  Div, Vol 104, No GT7,
     p 899-905, Rev (35), Class (Ilg).

Young, R.A. and Onstad,  C.A.,  1978,  Characterization of Rill and Interrill
     Eroded Soil, Trans  of ASAE,  Vol 21,  No  6,  p 1126-1130, Rev (144),
     Class (Ib).

Young, R.N. and Warkentin,  B.P.,  1975,  Soil  Properties and Behavior, Elsevier
     Scientific Publishing Co,  New  York,  Rev (243), Class (Ib).

Youngs, E.G.  and Price,  R.I.,  1981,  Scaling  of  Filtration Behavior in
     Dissimilar Porous Media,  Wat Res  Res ,  Vol 17, p  1065-1070, Rev
     (282), Class (VI  ).
                                     201

-------
Youngs, E.G. and Towner,  G.D.,  1976,  Comments  on  'Hydrostatics  and
     Hydrodynamics in Swelling  Soils'  by J.R.  Philip, Wat Res Res,
     Vol 6, No 4, p 1246-1247,  Rev (309),  Class  (Id).

Yule, G.E. and Kendall, M.G., 1968,  Introduction  to  the Theory  of Statistics,
     Charles Griffin and  Company Limited,  London,  Rev  (424), Class  (V  ).

Zimmie, T.F., 1981, Geotechnical Testing Considerations in  the  Determination
     of Laboratory Permeability for  Hazardous  Waste  Disposal Siting, Hazardous
     Solid Waste Testing: First Conference,  ASTM  STP 760, R.A.  Conway  and B.C.
     Malloy, eds., Am Soc for Test and Mater,  p 293-304, Rev (413), Class
     (He).

Zimmie, T.F. and Riggs, C.O.  (Ed.),  1981,  Permeability and  Groundwater
     Contaminant Transport,  Am. Soc.  for Testing  Materials, Philadelphia,
     PA, USA.
                                      202

-------
                          PUBLICATIONS - CLAY LINER
                               A. S. Rogowski


0.  Rogowski, A. S.  1984.  Clay liner facility construction logbook.  EPA
    Munic. Environ. Res. Lab., EPA-DW12930303-01-0, 33 p.

1.  Rogowski, A. S.  1984.  Relationship of laboratory and field determined
    hydraulic conductivity in compacted clay liner.  Phase I Progress Report.
    EPA Munic. Environ. Res. Lab., EPA-DW12930303-01-0, 72 p.

2.  Rogowski, A. S.  1984.  Relationship of laboratory and field determined
    hydraulic conductivity in compacted clay liner.  Phase II Progress Report.
    EPA Munic. Environ. Res. Lab., EPA-DW12930303-01-0, 54 p.

3.  Rogowski, A. S. and E. B. Richie.  1984.  Relationship of laboratory and
    field determined hydraulic conductivity in compacted clay soils.
    Proceedings, 16th Mid-Atlantic Industrial Waste Conference on Toxic and
    Hazardous Wastes, June 24-26, University Park, Pennsylvania, pp. 520-533.

4.  Rogowski, A. S.  1985.  Effectiveness of a compacted clay liner in
    preventing ground water contamination.  Iri Proceedings, 5th National
    Symposium and Exposition on Aquifer Restoration and Ground Water
    Monitoring, May 21-24, Columbus, Ohio, National Water Well Association,
    Worthington, Ohio, pp. 412-429.

5.  Rogowski, A. S., B. E. Weinrich, and D. E. Simmons,  1985.  Permeability
    assessment in a compacted clay liner.  Eighth Annual Madison Waste
    Conference, Municipal and Industrial Waste, September 18-19, Department
    Engineering, Univ. of Wisconsin, Madison, pp. 315-336.

6.  Rogowski, A. S., E. L. Jacoby, Jr., D. E. Simmons,  W. M. Yazujian, and
    P. J. Dockey.  1985.  Relationship of laboratory and field determined
    hydraulic conductivity in compacted clay liner.  Phase 111(1) Progress
    Report.  EPA-DW12930303-01-0, June 1985, 17 p.

7.  Rogowski, A. S., E. L. Jacoby, Jr., D. E. Simmons,  W. M. Yazujian, and
    P. J. Dockey.  1985.  Relationship of laboratory and field determined
    hydraulic conductivity in compacted clay liner.  Phase 111(2) Progress
    Report.  EPA-DW12930303-01-0, September 1985, 41  p.

8.  Rogowski, A. S.  1986.  Degree of saturation, hydraulic conductivity, and
    leachate quality in a compacted clay liner.  Iri Ground Water Hydrology,
    Contamination,  and Remediation,  R. M. Khanbilvardi  and J. Fillos (eds.),
    Scientific Publications Co.,  Washington, D.C., pp.  339-362.

9.  Rogowski, A. S.  1986.  Hydraulic conductivity of compacted  clay soils.
    Proceedings, 12th Annual Research Symposium,  "Land  Disposal, Remedial
    Action, Incineration and Treatment of Hazardous Waste," April 21-23,
    Cincinnati,  Ohio,  EPA/600/9-86/022,  pp.  29-39.
                                      203

-------
  10.   Rogowski,  A.  S.,  E.  L.  Jacoby,  Jr.,  D.  E. Simmons, W. M. Yazujian, D.
       Gedon,  and P.  J.  Dockey.   1986.  Relationship of laboratory and field
       determined hydraulic conductivity in compacted clay liner.  Phase 111(3)
       Progress Report.   EPA-DW12930303-01-0,  November 1986, 133 p.

  11.   Rogowski,  A.  S.   1987.   Distribution of flow rates and tracer breakthrough
       times in field soil.  Proceedings, 2nd International Conference on New
       Frontiers for Hazardous Waste Management, September 27-30, Pittsburgh,
       Pennsylvania,  EPA/600/9-87/018F,  pp. 219-230.

  12.   Rogowski,  A.  S.   1987.   Probability kriging approach to risk assessment of
       environmental problems.  Iri Pollution,  Risk Assessment and Remediation in
       Groundwater Systems, Reza M. Khanbilvardi and John Fillos (eds.), Third
       Annual  Conference on Groundwater Tech., The City Univ. of New York, NY,
       pp.  353-370.

  13.   Rogowski,  A.  S.,  D.  E.  Simmons, and B.  E. Weinrich.  1987.  Variability of
       infiltration in a clay layer of a Typic Hapludult.  Proceedings,
       International Conference on Infiltration Development and Application,
       Yu-Si Fok (ed.),  January 6-9, Honolulu, Hawaii, pp. 502-525.

  14.   Rogowski, A.  S.  and  D.  E.  Simmons.  1988.  Geostatistical analysis of
       field hydraulic conductivity in compacted clay.  Mathematical Geology
       20(4)-.423-446.

  15.   Rogowski, A.  S.   1988.   Flux density and breakthrough times for water and
       tracer in a spatially variable compacted clay soil.  J. Contam. Hydrol.
       3:327-348.

  16.   Rogowski, A.  S.,  J.  K.  Wolf, and D. E. Simmons.  Conditional simulation of
       flow and transport through a spatially variable compacted clay soil layer.
       J. Contam. Hydrol.  (Under Review).

  17.   Rogowski, A.  S.  Relationship of laboratory and field determined hydraulic
       conductivity in compacted clay liner.  U.S. Environmental Protection
       Agency Series, Final Report, EPA-DW12930303-01-0.  (Under Review).
                                          204

-------