United States
                   Environmental Protection
                   Agency          	
Robert S. Kerr Environmental
Research Laboratory
Ada, OK 74820
                   Research and Development
EPA/600/S2-89/035 Sept. 1989
&EPA          Project Summary
                    Kinematic  Modeling  of
                    Multiphase  Solute Transport  in
                    the  Vadose  Zone

                    R. J. Charbeneau, J. W. Weaver and V. J. Smith
                     The goal of this research was the
                   development of  a  computationally
                   efficient simulation  model for
                   multiphase flow of organic hazardous
                   waste constituents in the shallow soil
                   environment. Such a  model  is
                   appropriate for investigation of fate
                   and transport of organic chemicals
                   introduced to the soil through spills
                   on the ground surface, leakage from
                   surface  impoundments  or under-
                   ground storage tanks, or land treat-
                   ment of hazardous wastes. During the
                   initial phases of  a site investigation
                   there usually does not exist sufficient
                   data to support  the application of
                   comprehensive,  computationally ex-
                   pensive numerical models. Simplified
                   physically based models which can
                   address the  transport of  an organic
                   constituent experiencing volatiliza-
                   tion, multiphase partitioning, biodeg-
                   radation  and migration  may  be
                   preferred. Two models based  on the
                   kinematic theory  of multiphase flow
                   are developed and presented, along
                   with  a  number of  illustrative
                   examples.  The  Kinematic Oily
                   Pollutant  Transport  (KOPT)  model
                   assumes steady  infiltration  of water
                   based on the  expected annual
                   infiltration rate; the Kinematic Rainfall
                   and Oily Pollutant Transport (KROPT)
                   model  includes transient hydrologic
                   phenomena (evaporation and infiltra-
                   tion) along with a  model of stochastic
                   generation of rainfall. The examples
                   presented suggest that  the KOPT
                   model  may  be  preferred for most
                   applications.
                      This   Project  Summary was
                   developed by EPA's Environmental
Research Laboratory, Ada, Oklahoma,
to announce key  findings  of the
research project  that is  fully
documented  in a separate report of
the same title (see Project Report
ordering information at back).

Introduction
   The focus of this research has been
on the fate and  transport of  organic
hazardous waste constituents  in the
shallow  soil  environment.  Organic
hazardous waste  constituents may be
introduced into the soil by spills on the
ground surface, leakage from  surface
impoundments  or underground  storage
tanks,  or  land  treatment of hazardous
wastes. Oftentimes in  these  circum-
stances,  an "oil"  phase is present in
addition to the water,  air, and soil of the
natural media, and the fate and transport
characteristics  are determined by the
mobility of the water and oil, as well as
by multiphase partitioning of the constit-
uent between  the  air,  water, oil  and soil
matrix. The emphasis of the research has
been on  development  of simplified
models for fate and transport of organic
contaminants which may be appropriate
for the initial screening or investigation of
a site when the available data base does
not warrant the  application of  more
general models.
   The primary objectives of this cooper-
ative  agreement have been to  support
RSKERL  in their  modeling studies of
subsurface contamination from  organic
wastes, including  hazardous waste  land
treatment  operations,  and to investigate
the application of kinematic models for
multiphase processes  including  the flow
of water and oil, as well as multiphase-

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partitioning,  volatilization,  and  bio-
degradation.
   The Kinematic Oily Pollutant Transport
(KOPT) and Kinematic  Rainfall and Oily
Pollutant Transport  (KROPT)  programs
are  implementations  of a  kinematic
multiphase transport  model  that was
developed as a part of this research. The
KOPT  program  is  a  simplified
implementation  of  the  kinematic  multi-
phase  transport model,  intended  to  be
used as a screening tool for hydrocarbon
spills  or  near-surface  releases.  It
addresses the questions  of how far an oil
release  might go  into the soil and how
soon it might get there.  In the  KOPT
implementation, steady  water  infiltration
is  assumed to occur,  and the specified
water saturation  is  taken  as  represen-
tative of climatic conditions. The KROPT
program is the full implementation of the
kinematic  multiphase transport model
and  includes  modeling  of  transient
hydrologic  phenomena (evaporation and
infiltration), along  with a model  for the
stochastic  generation  of  rainfall.  This
model  handles  multiple loadings  or
releases  of oily  wastes at or near the
ground surface, multiple rainfall  events,
potential oil migration, sorption, volatiliza-
tion,  and biodegradation.

Research Background and
Scope
   The objective of  this  research was to
apply kinematic modeling  theory to fate
and  transport of  hydrocarbons in the
vadose zone for  oil spills  and  land
treatment sites.  The purpose of the work
was  to  provide a way  to estimate the
gross  movement  of  pollutants  in  a
multiphase system  resulting  from spills,
leaks and at  land treatment sites.  In the
case of land treatment systems, the long-
term behavior of the site is of interest, so
computationally efficient simulations are
needed. This  was the reason for using a
simplified approach.
   When  placed   in  porous media,
immiscible pollutants retain their unique
properties.  Although these pollutants are
largely  immiscible  in  water,  they are
capable of causing ground-water contam-
ination by  their  dissolved constituents.
Immiscibility  leads  to  distinct  bodies of
pollutant in close contact with both  air
and  water, where  present.  Above the
water table, the addition  of an immiscible
pollutant causes the original  two-phase
water/air  system to  become a  three-
phase  water/pollutant/air system.  When
flowing, the transport  and fate  of
immiscible fluids are governed by  a  set
of relationships which  are,  basically,
expanded  forms  of the  single phase
governing equations. The former provides
the theoretical framework  for  solving
immiscible (or multiphase) flow problems
in general. The specific application of the
theory  depends  on  the  initial  and
boundary conditions  imposed during
pollutant  migration  as well  as other
features unique to pollution incidents.
   Currently  available analytic and semi-
analytic multiphase flow models share
the  limitation that  they  rely on  an
assumed shape of the oil profile that is
not based upon solution of the governing
physically based  equations.  After an oil
release ends, the oil is gradually replaced
by  air as it  drains.  A drainage profile,
similar to those observed for  water is
expected, since the same forces that act
on  the water also act  on  the oil. Other
phenomena  outside the scope  of these
models  are  biodegradation,  which  also
causes  variable  oil  saturations,  and
simultaneous unsteady  flow of the water.
The latter is  typical of actual  time-varying
conditions in the field.
   Only a few numeric solutions of  the
multiphase  flow  equations  have  been
presented for the specific  problem of
shallow  aquifer contamination.  A limita-
tion of the numeric approach is  that the
models  are  computationally  very inten-
sive.  To exploit fully  their capacity for
modeling geologic variability,  a  large
amount of data is  required. Because data
is  usually sparse,  the  full capacity  of a
numeric  model may never  be reached
when applied to  specific  site inves-
tigations.
   The analytic and  semi-analytic  flow
models illustrate that if a constant amount
of  water is  present in the pore space,
only the  mass conservation  equation for
the oil needs to  be  solved.  A solution,
that has not been used for this purpose,
is  the kinematic model for soil moisture
transport. In  addition to a solution for the
duration of water  application, this model
gives a solution  for  the unsteady  flow
occurring  in  soils undergoing  drainage
(replacement of soil moisture by air). The
solution is   obtained  by  solving  an
approximate  governing equation for  the
water by  the method  of  characteristics
(MOC). With the proper constitutive
relationships  for  two-phase flow,  the
water solution is  analytic. Adapting  this
solution for  the oil phase gives a  more
realistic  model  than  the analytic  and
semi-analytic models  mentioned above,
since the oil  drainage profile  is deter-
mined by solution  of the  governing
equation. An analytic  solution is  not
possible for the oil because the relative
permeability  function is too  complicated
and depends on the  amount of water in
the pore space. However, a semi-ana
solution for  the  oil  phase can
achieved,  allowing  relatively  low c
putation times to be achieved.
   The  following  assumptions are  i
for the model  formation.  The  m<
equations are  solved for one-dimensi
flow.  This  is  one  of the  neces:
assumptions  to extend kinematic th
to multiphase flow.  Lateral  migra
however,  reduces   the  amount
pollutants   and  water  that  m
downward. The one-dimensional forn
tion is conservative as it  will  deten
the maximum  amount of substances
will  reach  a given  depth. A
component pollutant is assumed.  Th
acts as an inert carrier for the dissc
pollutant. Various transformations, (
than  biodegradation,  that the oil
undergo are  not  modeled.   Adve<
transport is used to model the tran
of the  constituent by oil  and  w
Equilibrium,  linear  partitioning rela
ships  are  used  for sorption,  dissol
into the water  and  for volatilization
the air phase. Volatilization is modele
applying the wet zone/dry zone  m
To extend kinematic modeling to tr
phase, three more assumptions are i
First,  the flow  of the air does not im
the flow of the liquids.  Second, the
phase transport is dominated  by  gr
Lastly, the medium is assumed t
strongly wetted so that water  will r
in the smallest pores,  air  in the  lai
and oil in the intermediate sized pore
   Under the  conditions discussed
kinematic model can be applied 1) I
unsteady flow of both the  oil am
water  and 2) to the fate and transp
the dissolved  constituent.  If onh
advective  motion of  the  constitue
modeled,  the  resulting equation;
compatible with  the numerical app
taken  for the oil equations.
   Two separate implementations
created. The first (KOPT)   was
kinematic  model for   the oil  mig
only,  with a  constant amount of
present in the pore  space. This me
analogous to the simplified analyti
semi-analytic flow models  noted  <
but with  the  capability  to  sin-
degrading oil  and  the  transport  (
dissolved constituent.  In related re:
this model was coupled with  a me
oil spread along the water table, wl
turn supplied input  for a model of
transport in the saturated zone. He
overall model  was  intended
screening tool  for oil spills. A
Guide for  the KOPT model is pre
in Appendix  A  while  the listing
code  is presented in Appendix  B.

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   The second implementation (KROPT)
 vas  a  model   to  investigate  the
 nteractions  between incoming  rainfall
and oil  moving within  the  profile. This
model is suited for studying the effect of
•3 series of rainfall events, irrigations and
cultivations  on  a  land treatment site.
There  are  practical  limitations  to
 ipplication of the KROPT model, and it is
:onsidered a research code at this time.
Discussion
  This work has shown that  kinematic
heory can be applied to multiphase flow
)roblems. Kinematic models  have  an
idvantage over traditional numeric mod-
»ls in that the kinematic models are well-
tiited  for studying  the hyperbolic  or
/ave  behavior  of the  multiphase flow
iquations. Inclusion  of  sharp  fronts is
 atural to the  kinematic models, while
inite difference or finite  element  models
 ncounter difficulties  when derivatives in
he governing equations  tend to become
 ndefined.  Solution  of the kinematic
 lodel shows how the oil and water fronts
nteract. Thus,  by  simplifying  the  gov-
 rning  equations, some of the  funda-
 lental behavior of the solution  is clearly
evealed. The  effect of  the  neglected
 apillary pressure  gradients  are  to
 crease  the infiltration  capacity  of  the
 oil and  smear the  fronts.  Much of the
mportant physics is retained, however, in
he kinematic model.
  Computationally,  by reducing  the
 nginal  system of  coupled  partial
 ifferential  equations to a system  of
 rdinary differential  equations,  the
 ifficulty of finding a numerical solution is
 educed  greatly. Resulting  computer
^odes are well  suited  to solving  problems
where  there is  a  constant amount of
water in the  pore space. Such a situation
corresponds to a soil at the so-called field
:apacity and  can  represent  typical
:onditions of the profile. The  best per-
ormance of  the KOPT model is obtained
 vhen the oil is  nondegrading and the oil
 iharacteristics  are straight. Curving char-
 ictenstics,  due to  biodegradation, in-
 rease the computational effort.
  The  implementation of the more
 eneral  model  (KROPT)  reveals  the
 iteractions  between  the oil and water
 onts.  The model is  limited to  situations
 'here the initial water profile is uniform.
 ince again the best   performance is
 btained  when the oil characteristics are
 raight,  since  the characteristic equa-
 Dns  are not  solved  explicitly.  Per-
 imance is degraded  where rainfalls
 cceed the kinematic capacity of the soil.
 ince the infiltration  capacity  is infinite
initially,  very  large water  fluxes are
possible  until runoff is produced. During
this period small time steps are required.
   This  modeling  work  enhances
understanding of multiphase flow through
the results obtained from the  example
problems presented. Most  important  is
the material concerning  the oil  banks. If
incoming rainfalls displace  oil,  then the
banks  are  created. Although  this is a
result of  simplified modeling, the  notion
that incoming water displaces oil  into a
bank moving ahead of the water front is a
more  general result.  In  situations  where
the flow  of  the  fluids is not kinematic,
banks will also exist. In certain cases, the
banks may  be very pronounced, although
short-lived.  In others,  the banks may
persist for  longer periods but would  be
virtually  undetectable in  the  laboratory
and the  field or by  numerical  methods
that are  not based upon the kinematic
model.
   The kinematic model  results indicate
that the water displaces  all of the mobile
oil. This  result was contrary to what was
expected but was established through
conservation of  mass.  Some  displace-
ment of oil would be expected, along with
the creation of an oil bank, but the model
result may  or may not  be confirmed by
experiment.
   The value of the residual oil saturation
is critical  for the results obtained from the
model. This parameter  could  be  easily
manipulated  to  show  that  oil  would
spread over a smaller depth.
   Biodegradation of the oil has only a
small  effect upon  the  ultimate  depth
attained  by  the  oil.  It  does  affect the
mobility  of the  oil  (reducing it).  An
interesting  effect on the constituent  is
caused  by  biodegradation  of the oil.
Concentrations  increase  as  the  oil
degrades because of the loss of solvent.
If the constituent is also biodegradable,
the shorter  half  life determines  if the
concentration will increase or not.
   As in  field  cases where constituent
concentrations in water are measured, a
large  mass of  constituent may  reside  in
the oil phase and not be  detected.  In one
of  the examples,  concentrations  in  the oil
are 50 times greater than in the water. If
only the  water phase concentrations are
measured,  most of mass in  the  soil  is
missed. This is particularly a problem if
the oil is  immobilized, since the  oil
cannot flow into an  observation well
(phenomena akin  to end  effects may
prevent oil flow into wells even  at  higher
saturations).  The  presence  of the  oil
material is  not  detected  by  the
observation wells; the core material itself
must be analyzed.
   Using a differential equation  solver is
well  suited to solving  the  kinematic
model, since the model equations can be
written  as  a  system  of  ordinary
differential  equations.  The speed  of  the
solver  is degraded as more  and  more
equations  are  added.  For these
situations, it might  be advantageous  to
solve  the  method  of characteristics
portion of the solution  by  finite difference
techniques instead  of tracking the
characteristics. The overhead  associated
with  using the  Runge-Kutta-Fehlberg
solver may be comparable to  that for the
discretization  methods.   Also, the
necessity  to  track sets  of oil  bank
characteristics makes the program  ex-
ceedingly  complex   Extension of the
model  may not be  practical  because of
this.

Conclusions and
Recommendations
   The results  of this research found that
kinematic theory  was  successfully ap-
plied to multiphase flow of water and oil.
Kinematic  models  have  an  advantage
over traditional numeric  models in that
the kinematic models  are well-suited foi
studying the hyperbolic or wave behavioi
of the  multiphase  flow  equations.
Inclusion of sharp fronts is natural  to the
kinematic models,  while finite difference
or finite  element  models  encounter
difficulties  when  derivatives  in the
governing  equations  tend to  become
undefined.  The kinematic model simpli-
fies  the  governing  equations revealing
some of the fundamental  behavior  of the
solution and  showing  how the oil and
water  fronts  interact. Solution of  the
kinematic  model  indicates that the
incoming water must  displace all   of the
mobile  oil  for mass  to  be  conserved.
Another important result is that oil  banks
are formed when the incoming  water
displaces the oil that is present. The main
limitation to the  kinematic model is that
displacement of oil  by  water  may be
unstable depending on the  fluid  prop-
erties of the oil and  the speed of  the
incoming water.
   The  two computer  codes  written  to
implement  two versions of the kinematic
model,  KOPT  and KROPT, run  in  a
computationally  efficient manner and
may be used to estimate the vertical
migration  of  oil  and  a dissolved con-
stituent within the soil profile,  including
the  effects  of  volatilization   and
biodegradation.  Running these codes
showed that the amount of  residual  oil
saturation strongly affects the total  depth
over which the oil  will be predicted  to
spread.

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   In light of the success of kinematic
models  for multiphase flow problems,
further  development of the  KOPT and
KROPT  programs  is  recommended.
Specifically,  the  following recommenda-
tions are suggested:
•  Generalize KOPT  and KROPT models
   for use  in  simulation of facilitated
   transport.  Such an  application  could
   look at the  use of solvents  (such  as
   heptane) for flushing a soil  profile to
   remove  low mobility  organic
   hazardous wastes and then model the
   much  more rapid volatilization and
   degradation of the solvent.
            Development and  implementation  of
            user-friendly versions  of  the KOPT
            and KROPT programs.
            Expand KROPT program to handle
            unstable  displacements  of oil by
            water, thereby  eliminating the  main
            limitation  of the model  and enabling
            the use  of randomly  generated
            rainfalls that may  exceed the  kine-
            matic rate. This program enhancement
            would also handle cases where oil is
            the displacing fluid, instead  of water,
            such  as for when the oil loading rate
            exceeds  the kinematic capacity  of an
            initially nonuniform water profile.
Expand KROPT  to  handle lay
systems,  where  the  effects of
fluids crossing into media of diff<
intrinsic permeabilities and pore
distributions can  have an  impo
effect on their migration.
Modify KROPT to have the optk
use  other  oil  relative permea!
models, in addition  to  the Br<
Corey approach.
Modify KROPT to handle depth
time  variability  in oil  resi
saturations.
   R. J. Charbeneau, J. W. Weaver, and V. J. Smith are with the University of Texas
   at Austin,  Austin, TX 78712.
   John E. Matthews is the EPA Project Officer (see below).
   The  complete  report,  entitled  "Kinematic  Modeling  of  Multiphase  Solute
         Transport in the Vadose Zone," (Order No. PB 89-207 948/AS; Cos?:
         527.95, subject to change) will be available only from:
             National Technical Information Service
             5285 Port Royal Road
             Springfield, VA22161
             Telephone: 703-487-4650
   The EPA Project Officer can be contacted at:
             Robert S. Kerr Environmental Research Laboratory
             U.S. Environmental Protection Agency
             Ada,  OK 74820
 United States
 Environmental Protection
 Agency
Center for Environmental Research
Information
Cincinnati OH 45268
 Official Business
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