United States
                   Environmental Protection
                   Agency
Robert S. Kerr Environmental
Research Laboratory
Ada OK 74820
                                                                                    ''
                   Research and Development
EPA/600/S2-85/065 Aug. 1985
                                                                                 rn. a? . TI
                                                                                 ^Fi*
&EPA         Project  Summary
                   Plume  2D:  Two-Dimensional
                   Plumes  in  Uniform  Ground
                   Water  Flow

                   Jan Wagner, S. A. Watts, and D. C. Kent
                     A closed-form analytical solution for
                   two dimensional plumes was incorpo-
                   rated in an interactive computer pro-
                   gram. The assumption of an infinite
                   aquifer depth and uniform source mass
                   rate and source location was overcome
                   by using the principal of superposition
                   in space and time. The source code was
                   written in a subset of FORTRAN 77 and
                   can be compiled with FORTRAN IV,
                   FORTRAN 66 as well as FORTRAN 77.
                   As a result, the code is nearly indepen-
                   dent of hardware and  operating sys-
                   tem. The model can be solved for either
                   vertically or horizontally averaged con-
                   ditions.
                    This Project Summary was devel-
                   oped by EPA's Robert S. Kerr Environ-
                   mental Research Laboratory, Ada, OK,
                   to  announce key findings of  the  re-
                   search project that is fully documented
                   in a separate report of the same title
                   (see Project Report ordering informa-
                   tion at back).

                   Introduction
                    Relatively simple analytical methods
                   can often be used to evaluate ground-
                   water contamination problems, de-
                   pending upon the complexity of the sys-
                   tem and the availability of field data.
                   Analytical models can  also serve as
                   valuable tools in developing parame-
                   ters for more sophisticated numerical
                   models. Although the numerical evalua-
                   tion of an analytical  solution to a
                   ground-water problem may be mathe-
                   matically complex,  analytical models
                   are well suited for interactive  use  on
                   digital computers. Many analytical solu-
                   tions to ground-water  contamination
                   problems can  be coded on program-
mable hand-held calculators. In general,
very few input parameters are required
to define a given problem, and numeri-
cal results can be calculated in a few
seconds.
  This report presents analytical solu-
tions to two ground-water pollution
problems—two-dimensional plumes in
uniform ground-water flow. An interac-
tive computer code has been developed
which enables the user to modify the
definition of a  given problem, and thus
gain some insight into the effects of var-
ious parameters on the extent of a con-
taminant plume.

Model Formulation
  The differential equation describing
the conservation of mass of a compo-
nent in a saturated,  homogenous aqui-
fer with uniform, steady flow  in the
x-direction can be written as
rlC

f)X
            = D
                 i>2C
      D;
                            (1)
where
   C = component mass per unit vol-
      ume of fluid phase
  D* =dispersion  coefficient in x-
      direction
  D* =dispersion  coefficient in y-
      direction
  Rd = retardation coefficient
  V* = average interstitial velocity in x-
      direction
  x,y = rectangle coordinates
   \ = first-order decay constant.

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The retardation coefficient accounts for
partitioning of the component between
the fluid and solid phases using a linear
adsorption isotherm and is defined as
= 1 + y Kd
                                  (2)
where
   PB = bulk density of the rock
    0 = effective porosity
   Kd = distribution coefficient for a lin-
       ear adsorption isotherm.

  Closed-form analytical solutions for
the two types of ground-water contami-
nation problems shown in Figure 1 are
included in this report. The first is a
vertically-averaged solution  which de-
scribes a contaminant plume in the x-y,
or horizontal, plane (Figure 1a). The sec-
ond is a horizontally-averaged solution
describing  a contaminant plume in a
vertical plane (Figure 1b).
  The vertically-averaged  solution ap-
plies to an aquifer of infinite areal  extent
and finite depth. The contaminant is as-
sumed to be well mixed over the satu-
rated thickness. The source of contami-
nation is a vertical line source located at
the origin of a coordinate system in the
x-y plane. The conceptual model is sim-
ilarto an injection well which fully pene-
trates the saturated zone or a finite verti-
cal segment of the aquifier. Wilson and
Miller (1978) have also applied this solu-
tion down-gradient from a contaminant
source at the water table. For a rela-
tively thin  saturated zone, vertical dis-
persion  will tend to mix the contami-
nant vertically.  The concentration
distribution can be considered  as being
two-dimensional in a horizontal plane at
distances downstream of the source for
the  concentration distribution to be-
come uniform with depth. For a continu-
ous source of strength MQ at the  origin,
the vertically-averaged solution is
(Hunt, 1978; Wilson and Miller, 1978)
            EXP
     C =
     V
    2D
          4ir8(DxDv)05
       ir-W(U,B)
(3)
where
       U =
                       V*\2
                       vv\
                 4V2t
                     (4)
                          Water    O
                           Table O
      Figure 1 .
                           and
B = i
                                      Coordinate systems for (A) vertically averaged solution and (B) horizontally averaged
                                      solution.
                                             which might fit this conceptual model is
                                             seepage from a trench.
                                               The closed-form  analytical solution
                                             follows directly from the vertically-
                                             averaged solution. Since the water table
                                             represents a no-flow boundary passing
                                             through the origin, the horizontally-
                                             averaged  solution  can  be written  di-
                                             rectly as
                                             Dy \D
                                                            (5)
                          The function W(U,B) is defined as
                                                                          Mi EXP
                                                -€-d?  (6)
                                                                      C =
                                                                                   V*
                                                                               (D*D*)05
                                                                   W(U,B)
                                                                     (8)
                          where 4 is a dummy integration vari-
                          able. This function is often referred to as
                          the  "well function for leaky artesian
                          aquifers" (Hantush, 1956).  The corre-
                          sponding steady-state-solution of Equa-
                          tion 1 is
                                             The steady-state solution is
                                                   C =
                                                       M0 EXP,2D,
                                                        -ire (D*D*
                                                           Ko(B)
                                        (9)
                 i EXP
                                     2TT6
                   Ko(B)
(7)
      where K0(B) is the modified Bessel func-
      tion of the second kind of order zero.
        The horizontally-averaged solution is
      based on the conceptual model shown
      in Figure 1b. A line source is located at
      the water table and normal to the direc-
      tion of ground-water  flow. A problem
Equations 5 and 7 and 8 and 9 can be
used to calculate concentrations in con-
taminant plumes under  the following
assumptions and limitations:
  1.  The ground-water regime is com-
     pletely saturated.
  2.  All aquifer properties are constant
     and uniform throughout the prob-
     lem domain.
  3.  The ground-water flow is horizon-
     tal, continuous, and  uniform
     throughout the aquifer.

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  4. The aquifer is infinite in extent.
  5. The contaminant source is a line
     located at the origin of the coordi-
     nate system.
  6. The mass flow rate of the source is
     constant.
  7. At zero time the concentration  in
     the aquifer is zero.
  The  assumptions of an infinite aqui-
fier and uniform  source  rates can be
overcome by using the principles of su-
perposition in space and time. Superpo-
sition can also be used to include multi-
ple sources.

Computer Program
  The  closed-form analytical solutions
for the two-dimensional plumes as pre-
sented above have been incorporated in
an interactive computer program. The
source code has been written in a sub-
set of FORTRAN 77 and can be compiled
with FORTRAN IV, FORTRAN 66, as well
as FORTRAN 77 compilers. As a result,
the code is almost entirely independent
of hardware and operating systems.
Those  changes which may be required
to implement the code on a given sys-
tem, such as assigning logical devices
are clearly identified.
  The program has been developed for
interactive use and requires input data
under two modes of operation—"Basic
Input Data" and "Edit." The  basic input
data are required to initiate a new prob-
lem. The user is prompted  for the re-
quired data  through  a series of input
commands.
  Once the basic input data have been
entered,  the problem as currently de-
fined is listed and the program  enters
the "edit" mode. The  two character edit
commands listed in Table 1 can be used
to redefine the problem, run the calcula-
tions, and terminate the program.
  The program has been written to re-
quire a minimum of machine resources
and will run on both 8 and 16 bit micro-
computers under CP/M,  MS-DOS,  and
PC-DOS as well as larger minicomput-
ers and mainframe machines.


Summary
  The models and computer codes de-
veloped in this project are intended to
serve as additional tools in the analysis
of ground-water contamination prob-
lems. The user must select the best tool
for  the  problem at hand based on  a
sound  understanding of the principles
of ground-water hydrology,  the  physi-
cal problem, and the  limitations of the
 nathematical model(s). Unfortunately,
Table 1.  Edit Commands

Command     Variable changed/Execution
ST

PO

VX

RD

DE

DX

DY

DZ

RT

OB

XC

YC

ZC

TC

CS

MU

LI

RN

NP

DN
Saturated Thickness

Porosity

New Seepage Velocity

Retardation Coefficient

Decay Constant

X-Dispersion Coefficient

V'-Dispersion Coefficient

Z-Dispersion Coefficient

Source Rate Schedule

Observation Points

X-Coordmates

Y-Coordinates

Z-Coordinates

Observation Times

Change Solution/Sources

Menu of Edit Commands

List input data

Run

New Problem

Done
these computer programs cannot sub-
stitute for an understanding of the pro-
cesses and mechanisms of solute trans-
port in ground-water systems or sound
judgement based on training and expe-
rience.

References
Hantush, M. S., 1956, "Analysis of Data
  from  Pumping  Tests  in  Leaky
  Aquifers," Transitions,  American
  Geophysical Union, Vol. 37, No. 6, pp.
  702-714.
Hunt, B., 1978, "Dispersive  Sources  in
  Uniform Ground-Water Flow," Jour-
  nal of The Hydraulics Division, ASCE,
  Vol. 104, No. HY 1, pp. 75-85.
Wilson,  J. L. and P.  J. Miller, 1978,
  "Two-Dimensional Plume  in Uniform
  Ground-Water Flow," Journal of the
  Hydraulics Division, ASCE, Vol. 104,
  No. HY4, pp. 503-514.

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     Jan Wagner, S. A.  Wans, and Douglas C. Kent are with Oklahoma State
     University, S til/water, OK 74078.
     Carl G. Enfield is the EPA Project Officer (see below).
     The complete report, entitled "PLUME 2D: Two-Dimensional Plumes in Uniform
     Ground Water Flow."(Order No. P8 85-214 450/AS; Cost: $11.50. subject to
     change) will be available only from:
            National Technical Information Service
            5285 Port Royal Road
            Springfield,  VA 22161
            Telephone: 703-487-4650
     The EPA Project Officer can be  contacted at:
            Robert S. Kerr Environmental Research Laboratory
            U.S. Environmental Protection Agency
            P.O. Box 1198
            Ada, OK 74820
United States
Environmental Protection
Agency
Center for Environmental Research
Information
Cincinnati OH 45268
Official Business
Penalty for Private Use $300
EPA/600/S2-85/065
                                           ECTS  SGENCY
                      CHICAGO
                                                                                        U.S. GOVERNMENT PRINTING OFFICE:1985—559-Qlb/27117

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