Chapter 5
Basics of Transport of
Pollutant in Aquifers
Amro Elfeki, PhD
Contaminant anything in water that renders
it unsuitable for a particular use
Contaminant (Pollution)
Many Sources and Types of
Contaminants
Various Forms of Pollution in
Groundwater
Classification of Pollutant
• Dissolution in Water: Solutes – Heavy metals
• Density: LNAPLS, DNAPLS
• LNAPLs: light, nonaqueous phase liquid
– lighter than water
– floats on surface of a water table
• DNAPLs: dense, nonaqueous phase liquid
– heavier than water
– sinks to the bottom of a water table
Classification of Pollutant (cont.)
• Reactions with soil: Conservative and non-
conservative
• Organic: Organic (Carbon and Nitrogen) and
Inorganic
• Microbial: Microorganisms, Bacteria and
Viruses
Organics
(gasoline, DDT, detergents)
Volatile organics
(TCE, DCE, Benzene)
Contaminant by Organic
Materials
Inorganics
(chloride, cyanide, nitrate)
Contaminant by Inorganic
Materials
Nitrate concentrations > 10 mg/kg in drinking water pose a health
threat to infants,
Nitrate Pollution
Heavy Metals
(arsenic, cadmium, chromium)
Contaminant by Heavy Metals
Organisms
(Giardia, E. Coli)
Contaminant by Micro-Organisms
Density of Contaminant
LNAPLS(Lighter):“BTEX” Compounds
DNAPL (Denser):Chlorohydrocarbons
Contaminant Transport
Transport Processes
1) Physical :
Advection-Diffusion-Dispersion
2) Chemical:
Adsorption- Ion Exchange- etc.
3) Biological:
Micro-organisms Activity
(Bacteria&Microbes)
4) Decay:
Radioactive Decay-Natural Attenuation.
Physical Processes
1. Advection
2. Molecular Diffusion
3. Mechanical Dispersion
4. Hydrodynamic Dispersion
Advection
• Movement of contaminants with a moving
fluid (e.g., groundwater)
• Controlled by difference in hydraulic head
vs = interstitial velocity or seepage velocity
(L/T)
= Ki/n (Darcy’s law);
K = hydraulic conductivity, L/T;
i = hydraulic gradient, h/L; and
n = porosity.
x
C
v
t
C
s





18
x = vt
Advection (Convection)
adv
J Cq
Advective Solute Mass Flux:
.q = K 
is the advective solute mass flux,
is the solute concentration, and
is the water flux (specific discharge)
given by Darcy's law:
C
q
adv
J
Advection
solute moves
with groundwater
Dispersion/Diffusion
• Molecular Diffusion
– Molecules move from regions of high concentration
to regions of lower concentration
– Length of scale of motion = molecular → slow
• Turbulent Diffusion
– Bulk motion in random directions
• Mechanical Dispersion
– Microscopic velocity variation within the pore space
– Differences in pore sizes along the flow paths
– Mechanical dispersion leads to longitudinal as well
as transverse dispersion, with the former one more
significant than the latter one 20
Diffusion
Diffusive Flux in Bulk: (Fick’s Law of Diffusion)
is the diffusive solute mass flux in bulk,
dif
o oJ =- D C
dif
oJ
is the solute concentration gradient,
C
is the molecular diffusive coefficient in bulk.
oD
Random Particle motion
Time
t1
t2
t3
t4
Diffusion
moving from higher
to lower concentrations
Diffusion
22
A net transport of molecules from a region of higher concentration to one of
lower concentration by random molecular motion
Molecular Diffusion (Dd)
23
L
Lp

Tortuosity factor, ω: the distance a molecule travels to get through porous
media divided by the straight line of the two points
Diffusion in porous media, Dd
*
Dd
* = ωDd
Lp = distance a molecule travels from points A to B
L = straight distance between points A and B
ω=f(1/τ)
=0.01~0.5
Molecular Diffusion
dif
effJ =- D C 

O
eff
D
D 
Diffusive Flux in Porous Medium
is the effective molecular diffusion
coefficient in porous medium,
effD
 is a tortuosity factor ( = 1.4)
0.7eff oD D
Mechanical Dispersion
dis
J =- C .D
Depressive Flux in Porous Media (Fick’s Law):
is the depressive solute mass flux,
is the solute concentration gradient,
is the dispersion tensor,
is the effective porosity
dis
J

C
D
xx xy xz
yx yy yz
zx zy zz
D D D
D D D
D D D
 
 
  
 
 
D
[after Kinzelbach, 1986]
Causes of Mechanical Dispersion
Mechanical Dispersion (Dm)
26
 Function of the shape of the soil particles and the distance between them
Hydrodynamic Dispersion (Dh)
• Hydrodynamic dispersion coe. (Dh) = Mechanical dispersion
coe. (Dm) + Diffusion coe. (Dd)
Dh = Dm + Dd
*
Dh = αv + ωDd
where α = dynamic dispersivity (m) = 0.0175 Lp
1.46 and
Lp = length of the flow path or plum length (m)
α = 0.83 [log Lp]2.414 (Xu and Eckstein, 1995)
• At column scale, dispersivity = 0.01~1.0 cm
• In field experiments, dispersivity = 0.1~2.0 m
27
Hydrodynamic Dispersion
    i j
ij efft ij l t
v v
= |v|+ + -D D
|v|
   
_hydo dis
J =- C .D
Hydrodynamic Depressive Flux in Porous Media (Fick’s Law):
The components of the dispersion tensor in isotropic soil
is given by [Bear, 1972],
is Kronecker delta, =1 for i=j and =0 for i j,ij
are velocity components in two perpendicular directions,
i jv v
is the magnitude of the resultant velocity,v 2 2 2
i j kv v v v  
is the longitudinal pore-(micro-) scale dispersivity, andl
t is the transverse pore-(micro-) scale dispersivity
ij ij
Hydrodynamic Dispersion (Cont.)
In case of flow coincides with the horizontal x-direction
all off-diagonal terms are zeros and one gets,
0 0
0 0
0 0
xx
yy
zz
D
D
D
 
   
  
D
xx effl
yy efft
zz efft
= |v|+D D
= |v|+D D
= |v|+D D



, 0.5
, 0.0157
3.5 Random packing
is the grain diameter
l l p l
t t p t
p
c d c
c d c
d
 
 

 
 

Microscopic Dispersion Simulation
30
Peclet number, Pe
• Ratio of advective flux to diffusive flux
31
d
e
D
vL
P 
v = average linear velocity (L/T);
L = characteristic length (average diameter of grains, d50, in porous
media); and
Dd = molecular diffusion coefficient, L2/T.
 Pe > 1 means diffusive flux is more important than advective flux
 Pe < 1 means diffusive flux is negligible compared to advective flux
Dispersion Regimes at Micro-Scale
D
VL
Pe
eff
cc

Peclet Number:
Advection/Dispersion
Perkins and Johnston, 1963
Chemical Processes
• Sorption & De-sorption.
• Ion Exchange.
• Retardation.
Conservative
do not react with soil / groundwater
Sorbed onto mineral grains
as well as organic matter
Reactive
Conservative and Reactive
Solutes
Adsorption Isotherms
)(CfS 
m
bCS 
CKS d
21 kCkS 
4
3
1 k
Ck
S


Freundlich (1926)
Langmuir (1915, 1918)
Biological Processes
•Biological Degradation
and Natural Attenuation.
•Micro-organisms
Activity.
•Decay.
C
dt
Cd

 )(
 is the decay coefficient
Transport Through Porous Media
Derivation of Transport Equation in
Rectangular Coordinates
Flow In – Flow Out = rate of change within the control volume
Solute Flux in the x-direction
( )
( )
( )
in adv dis
x x x
adv dis
out adv dis x x
x x x
J J J y z
J J
J J J x y z
x


   
 
      
 
Solute Flux in the y-direction
( )
( )
( )
in adv dis
y y y
adv dis
y yout adv dis
y y y
J J J x z
J J
J J J y x z
y


   
 
      
  
Solute Flux in the z-direction
( )
( )
( )
in adv dis
z z z
adv dis
out adv dis z z
z z z
J J J y x
J J
J J J z y x
z


   
 
      
 
From Continuity of Solute Mass
( )solute
in out
M
J J C x y z
t t
 

 
      
Where  is the porosity, and
C is Concentration of the solute.
From Continuity of Solute Mass
( ) ( ) ( )
( )
( )
( )
( )
( )
( )
( )
adv dis adv dis adv dis
x x y y z z
adv dis
adv dis x x
x x
adv dis
y yadv dis
y y
adv dis
adv dis z z
z z
J J y z J J x z J J y x
J J
J J x y z
x
J J
J J y x z
y
J J
J J z y x
z
C x y z
t









          
 
      
 
 
      
  
 
      
 
   
By canceling out terms
( )( ) ( )
adv disadv dis adv dis
y yx x z z
J JJ J J J
z y x
x y z
 
  
  
      
  
(C x y z
t



    )
( )( ) ( )
( )
adv disadv dis adv dis
y yx x z z
J JJ J J J
x y z
C
t
 
  



  
   
  

Assuming Advection and Hydrodynamic
Dispersion
,
,
,
adv dis
x x x xx xx
adv dis
y y y yy yy
adv dis
z z z zz zz
C
J = Cq J = - D C - D
x
C
J = Cq J = - D C - D
y
C
J = Cq J = - D C - D
z
 
 
 

 


 


 

. .
. .
. .
Solute Transport Through Porous Media by
advection and dispersion processes
( )
y yyx xx z zz
CC C
Cq - DCq - D Cq - D
yx z
x y z
C
t
    
  



      
              
 
 
 

.. .
( ) ( ) ( )
Hyperbolic Part
x y z
Parabolic Part
xx yy zz
C
v C v C v C
t x y z
C C C
D D D
x x y y z z
   
   
     
     
   
    
      
    
6 4 4 4 4 44 7 4 4 4 4 4 48
6 4 4 4 4 4 4 4 44 7 4 4 4 4 4 4 4 448
General Form of The Transport Equation
 
}
}
/
( ')
Dispersion Diffusion
Advection Source SinkChemical reaction
Decay
ij i
i j i
C C S C C W
v C + Q CD
t x x x

 


     
    
     
6 44 7 4 48 64 7 48 6 4 7 48
where
C is the concentration field at time t,
Dij is the hydrodynamic dispersion tensor,
Q is the volumetric flow rate per unit volume of the source or sink,
S is solute concentration of species in the source or sink fluid,
i, j are counters,
C’ is the concentration of the dissolved solutes in a source or sink,
W is a general term for source or sink and
vi is the component of the Eulerian interstitial velocity in xi direction
defined as follows,
ij
i
j
K
=-v
x

where
Kij is the hydraulic conductivity tensor, and  is the porosity of the medium.
Schematic Description of Processes
Figure 7. Schematic Description of the Effects of Advection, Dispersion, Adsorption, and Degradation on Pollution
Transport [after Kinzelbach, 1986].
Advection+Dispersion
Advection
Advection+Dispersion+Adsorption
Advection+Dispersion+Adsorption+Degradation
Methods of Solution
1) Analytical Approaches:
2) Numerical Approaches:
i) Eulerian Methods:(FDM,FEM).
ii) Lagrangian Methods:(RWM).
iii) Eulerian-Lagrangian Methods:
(MOC).
Pulse versus Continuous Injection
Concentration Distribution in case of Pulse and Continuous Injections in a 2D Field
[after Kinzelbach, 1986].






tV4
)Y-(y
+
tV4
)tV-X-(x
-
tV4tV4
H)/(M=t)y,C(x,
xt
2
o
xl
2
xo
xtxl
o


exp  
d
tV4
Y-y
+
tV4
tV-X-x
-
tV4
HM=ty,x,C
t
xt
2
o
xl
2
xo
tlx
o
 









0
)(
)(
)(
)((
exp
1)(/
)( 




Flow
t = 0
f
t = Flowing Time
Var(X)
The spread of the front is a measure of the heterogeneity
Random Walk
Transport of a Solute
52
1
0.5
0
Relative
Concentration,C/C0
Distance, x
Concentration Profile at Time t
in One-Dimensional Flow
Advection only
x = vt
Diffusion onlyDispersion only
Mechanical dispersion - caused by motion of the fluid
Longitudinal dispersion – along the streamline
Transverse dispersion – perpendicular to flow path
Flow
Direction

Dispersion
DL
2C
x2
- vx
C
 x
=
C
 t
DL = coefficient of longitudinal hydrodynamic dispersion
C = solute concentration in liquid phase
vx = average linear groundwater velocity
t = time
b = bulk density of aquifer
= porosity (saturated aquifer)
C* = amount of solute sorbed per unit weight of solid
-
b

dispersion advection sorption
C*
 t
One Dimension Advection Dispersion
& Sorption
Slows the rate of transport
Retardation and Sorption
Types of Contamination Sources
Continuous Source t1
t4t2 t3
One time release
t2t1
t3
Contaminant Transport
Comparison between Analytical
Solution and RW-method






tV4
)Y-(y
+
tV4
)tV-X-(x
-
tV4tV4
H)/(M=t)y,C(x,
xt
2
o
xl
2
xo
xtxl
o


exp
 
d
tV4
Y-y
+
tV4
tV-X-x
-
tV4
HM=ty,x,C
t
xt
2
o
xl
2
xo
tlx
o
 









0
)(
)(
)(
)((
exp
1)(/
)( 




3D graphical representation of
pollution injection
One-dimensional Pollution
Concentration Profiles in case of
Continuous Injection
2D-Pullotion
Groundwater Restoration
– Dig and remove contamination - Arsenic
– Pump and treat - Nitrate
– Mitigate in ground (in situ)
– Hydrogen Peroxide
- Lower water table
- Seal contamination (Contamination Containment)
- Bioremediation
- Install permeable treatment bed (Permeable
reactive barrier)
National Water Quality Assessment Program
http://water.usgs.gov/nawqa/
Some useful web links for gw contamination:
Superfund Sites in Massachusetts
http://www.epa.gov/superfund/sites/npl/ma.htm
EPA Superfund Homepage
http://www.epa.gov/superfund/index.htm
EPA Major Environmental Laws
http://www.epa.gov/region5/defs/index.html
USGS Toxic Hydrology Program
http://toxics.usgs.gov/
Massachusetts Contingency Plan
http://www.state.ma.us/dep/bwsc/files/mcp/mcptoc.htm
Contaminant Hydrogeology Journals
Water Resources Research
Ground Water
Ground Water Monitoring and Remediation
Environmental Science and Technology
Journal of Contaminant Hydrology

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Basics of Contaminant Transport in Aquifers (Lecture)

  • 1. Chapter 5 Basics of Transport of Pollutant in Aquifers Amro Elfeki, PhD
  • 2. Contaminant anything in water that renders it unsuitable for a particular use Contaminant (Pollution)
  • 3. Many Sources and Types of Contaminants
  • 4. Various Forms of Pollution in Groundwater
  • 5. Classification of Pollutant • Dissolution in Water: Solutes – Heavy metals • Density: LNAPLS, DNAPLS • LNAPLs: light, nonaqueous phase liquid – lighter than water – floats on surface of a water table • DNAPLs: dense, nonaqueous phase liquid – heavier than water – sinks to the bottom of a water table
  • 6. Classification of Pollutant (cont.) • Reactions with soil: Conservative and non- conservative • Organic: Organic (Carbon and Nitrogen) and Inorganic • Microbial: Microorganisms, Bacteria and Viruses
  • 7. Organics (gasoline, DDT, detergents) Volatile organics (TCE, DCE, Benzene) Contaminant by Organic Materials
  • 9. Nitrate concentrations > 10 mg/kg in drinking water pose a health threat to infants, Nitrate Pollution
  • 10. Heavy Metals (arsenic, cadmium, chromium) Contaminant by Heavy Metals
  • 16. Transport Processes 1) Physical : Advection-Diffusion-Dispersion 2) Chemical: Adsorption- Ion Exchange- etc. 3) Biological: Micro-organisms Activity (Bacteria&Microbes) 4) Decay: Radioactive Decay-Natural Attenuation.
  • 17. Physical Processes 1. Advection 2. Molecular Diffusion 3. Mechanical Dispersion 4. Hydrodynamic Dispersion
  • 18. Advection • Movement of contaminants with a moving fluid (e.g., groundwater) • Controlled by difference in hydraulic head vs = interstitial velocity or seepage velocity (L/T) = Ki/n (Darcy’s law); K = hydraulic conductivity, L/T; i = hydraulic gradient, h/L; and n = porosity. x C v t C s      18 x = vt
  • 19. Advection (Convection) adv J Cq Advective Solute Mass Flux: .q = K  is the advective solute mass flux, is the solute concentration, and is the water flux (specific discharge) given by Darcy's law: C q adv J Advection solute moves with groundwater
  • 20. Dispersion/Diffusion • Molecular Diffusion – Molecules move from regions of high concentration to regions of lower concentration – Length of scale of motion = molecular → slow • Turbulent Diffusion – Bulk motion in random directions • Mechanical Dispersion – Microscopic velocity variation within the pore space – Differences in pore sizes along the flow paths – Mechanical dispersion leads to longitudinal as well as transverse dispersion, with the former one more significant than the latter one 20
  • 21. Diffusion Diffusive Flux in Bulk: (Fick’s Law of Diffusion) is the diffusive solute mass flux in bulk, dif o oJ =- D C dif oJ is the solute concentration gradient, C is the molecular diffusive coefficient in bulk. oD Random Particle motion Time t1 t2 t3 t4 Diffusion moving from higher to lower concentrations
  • 22. Diffusion 22 A net transport of molecules from a region of higher concentration to one of lower concentration by random molecular motion
  • 23. Molecular Diffusion (Dd) 23 L Lp  Tortuosity factor, ω: the distance a molecule travels to get through porous media divided by the straight line of the two points Diffusion in porous media, Dd * Dd * = ωDd Lp = distance a molecule travels from points A to B L = straight distance between points A and B ω=f(1/τ) =0.01~0.5
  • 24. Molecular Diffusion dif effJ =- D C   O eff D D  Diffusive Flux in Porous Medium is the effective molecular diffusion coefficient in porous medium, effD  is a tortuosity factor ( = 1.4) 0.7eff oD D
  • 25. Mechanical Dispersion dis J =- C .D Depressive Flux in Porous Media (Fick’s Law): is the depressive solute mass flux, is the solute concentration gradient, is the dispersion tensor, is the effective porosity dis J  C D xx xy xz yx yy yz zx zy zz D D D D D D D D D            D [after Kinzelbach, 1986] Causes of Mechanical Dispersion
  • 26. Mechanical Dispersion (Dm) 26  Function of the shape of the soil particles and the distance between them
  • 27. Hydrodynamic Dispersion (Dh) • Hydrodynamic dispersion coe. (Dh) = Mechanical dispersion coe. (Dm) + Diffusion coe. (Dd) Dh = Dm + Dd * Dh = αv + ωDd where α = dynamic dispersivity (m) = 0.0175 Lp 1.46 and Lp = length of the flow path or plum length (m) α = 0.83 [log Lp]2.414 (Xu and Eckstein, 1995) • At column scale, dispersivity = 0.01~1.0 cm • In field experiments, dispersivity = 0.1~2.0 m 27
  • 28. Hydrodynamic Dispersion     i j ij efft ij l t v v = |v|+ + -D D |v|     _hydo dis J =- C .D Hydrodynamic Depressive Flux in Porous Media (Fick’s Law): The components of the dispersion tensor in isotropic soil is given by [Bear, 1972], is Kronecker delta, =1 for i=j and =0 for i j,ij are velocity components in two perpendicular directions, i jv v is the magnitude of the resultant velocity,v 2 2 2 i j kv v v v   is the longitudinal pore-(micro-) scale dispersivity, andl t is the transverse pore-(micro-) scale dispersivity ij ij
  • 29. Hydrodynamic Dispersion (Cont.) In case of flow coincides with the horizontal x-direction all off-diagonal terms are zeros and one gets, 0 0 0 0 0 0 xx yy zz D D D          D xx effl yy efft zz efft = |v|+D D = |v|+D D = |v|+D D    , 0.5 , 0.0157 3.5 Random packing is the grain diameter l l p l t t p t p c d c c d c d          
  • 31. Peclet number, Pe • Ratio of advective flux to diffusive flux 31 d e D vL P  v = average linear velocity (L/T); L = characteristic length (average diameter of grains, d50, in porous media); and Dd = molecular diffusion coefficient, L2/T.  Pe > 1 means diffusive flux is more important than advective flux  Pe < 1 means diffusive flux is negligible compared to advective flux
  • 32. Dispersion Regimes at Micro-Scale D VL Pe eff cc  Peclet Number: Advection/Dispersion Perkins and Johnston, 1963
  • 33. Chemical Processes • Sorption & De-sorption. • Ion Exchange. • Retardation.
  • 34. Conservative do not react with soil / groundwater Sorbed onto mineral grains as well as organic matter Reactive Conservative and Reactive Solutes
  • 35. Adsorption Isotherms )(CfS  m bCS  CKS d 21 kCkS  4 3 1 k Ck S   Freundlich (1926) Langmuir (1915, 1918)
  • 36. Biological Processes •Biological Degradation and Natural Attenuation. •Micro-organisms Activity. •Decay. C dt Cd   )(  is the decay coefficient
  • 38. Derivation of Transport Equation in Rectangular Coordinates Flow In – Flow Out = rate of change within the control volume
  • 39. Solute Flux in the x-direction ( ) ( ) ( ) in adv dis x x x adv dis out adv dis x x x x x J J J y z J J J J J x y z x                 
  • 40. Solute Flux in the y-direction ( ) ( ) ( ) in adv dis y y y adv dis y yout adv dis y y y J J J x z J J J J J y x z y                  
  • 41. Solute Flux in the z-direction ( ) ( ) ( ) in adv dis z z z adv dis out adv dis z z z z z J J J y x J J J J J z y x z                 
  • 42. From Continuity of Solute Mass ( )solute in out M J J C x y z t t             Where  is the porosity, and C is Concentration of the solute.
  • 43. From Continuity of Solute Mass ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) adv dis adv dis adv dis x x y y z z adv dis adv dis x x x x adv dis y yadv dis y y adv dis adv dis z z z z J J y z J J x z J J y x J J J J x y z x J J J J y x z y J J J J z y x z C x y z t                                                          
  • 44. By canceling out terms ( )( ) ( ) adv disadv dis adv dis y yx x z z J JJ J J J z y x x y z                   (C x y z t        ) ( )( ) ( ) ( ) adv disadv dis adv dis y yx x z z J JJ J J J x y z C t                   
  • 45. Assuming Advection and Hydrodynamic Dispersion , , , adv dis x x x xx xx adv dis y y y yy yy adv dis z z z zz zz C J = Cq J = - D C - D x C J = Cq J = - D C - D y C J = Cq J = - D C - D z                   . . . . . .
  • 46. Solute Transport Through Porous Media by advection and dispersion processes ( ) y yyx xx z zz CC C Cq - DCq - D Cq - D yx z x y z C t                                         .. . ( ) ( ) ( ) Hyperbolic Part x y z Parabolic Part xx yy zz C v C v C v C t x y z C C C D D D x x y y z z                                          6 4 4 4 4 44 7 4 4 4 4 4 48 6 4 4 4 4 4 4 4 44 7 4 4 4 4 4 4 4 448
  • 47. General Form of The Transport Equation   } } / ( ') Dispersion Diffusion Advection Source SinkChemical reaction Decay ij i i j i C C S C C W v C + Q CD t x x x                       6 44 7 4 48 64 7 48 6 4 7 48 where C is the concentration field at time t, Dij is the hydrodynamic dispersion tensor, Q is the volumetric flow rate per unit volume of the source or sink, S is solute concentration of species in the source or sink fluid, i, j are counters, C’ is the concentration of the dissolved solutes in a source or sink, W is a general term for source or sink and vi is the component of the Eulerian interstitial velocity in xi direction defined as follows, ij i j K =-v x  where Kij is the hydraulic conductivity tensor, and  is the porosity of the medium.
  • 48. Schematic Description of Processes Figure 7. Schematic Description of the Effects of Advection, Dispersion, Adsorption, and Degradation on Pollution Transport [after Kinzelbach, 1986]. Advection+Dispersion Advection Advection+Dispersion+Adsorption Advection+Dispersion+Adsorption+Degradation
  • 49. Methods of Solution 1) Analytical Approaches: 2) Numerical Approaches: i) Eulerian Methods:(FDM,FEM). ii) Lagrangian Methods:(RWM). iii) Eulerian-Lagrangian Methods: (MOC).
  • 50. Pulse versus Continuous Injection Concentration Distribution in case of Pulse and Continuous Injections in a 2D Field [after Kinzelbach, 1986].       tV4 )Y-(y + tV4 )tV-X-(x - tV4tV4 H)/(M=t)y,C(x, xt 2 o xl 2 xo xtxl o   exp   d tV4 Y-y + tV4 tV-X-x - tV4 HM=ty,x,C t xt 2 o xl 2 xo tlx o            0 )( )( )( )(( exp 1)(/ )(     
  • 51. Flow t = 0 f t = Flowing Time Var(X) The spread of the front is a measure of the heterogeneity Random Walk
  • 52. Transport of a Solute 52 1 0.5 0 Relative Concentration,C/C0 Distance, x Concentration Profile at Time t in One-Dimensional Flow Advection only x = vt Diffusion onlyDispersion only
  • 53. Mechanical dispersion - caused by motion of the fluid Longitudinal dispersion – along the streamline Transverse dispersion – perpendicular to flow path Flow Direction  Dispersion
  • 54. DL 2C x2 - vx C  x = C  t DL = coefficient of longitudinal hydrodynamic dispersion C = solute concentration in liquid phase vx = average linear groundwater velocity t = time b = bulk density of aquifer = porosity (saturated aquifer) C* = amount of solute sorbed per unit weight of solid - b  dispersion advection sorption C*  t One Dimension Advection Dispersion & Sorption
  • 55. Slows the rate of transport Retardation and Sorption
  • 56. Types of Contamination Sources Continuous Source t1 t4t2 t3 One time release t2t1 t3 Contaminant Transport
  • 57. Comparison between Analytical Solution and RW-method       tV4 )Y-(y + tV4 )tV-X-(x - tV4tV4 H)/(M=t)y,C(x, xt 2 o xl 2 xo xtxl o   exp   d tV4 Y-y + tV4 tV-X-x - tV4 HM=ty,x,C t xt 2 o xl 2 xo tlx o            0 )( )( )( )(( exp 1)(/ )(     
  • 58. 3D graphical representation of pollution injection
  • 60. Concentration Profiles in case of Continuous Injection
  • 62. Groundwater Restoration – Dig and remove contamination - Arsenic – Pump and treat - Nitrate – Mitigate in ground (in situ) – Hydrogen Peroxide - Lower water table - Seal contamination (Contamination Containment) - Bioremediation - Install permeable treatment bed (Permeable reactive barrier)
  • 63. National Water Quality Assessment Program http://water.usgs.gov/nawqa/ Some useful web links for gw contamination: Superfund Sites in Massachusetts http://www.epa.gov/superfund/sites/npl/ma.htm EPA Superfund Homepage http://www.epa.gov/superfund/index.htm EPA Major Environmental Laws http://www.epa.gov/region5/defs/index.html USGS Toxic Hydrology Program http://toxics.usgs.gov/ Massachusetts Contingency Plan http://www.state.ma.us/dep/bwsc/files/mcp/mcptoc.htm
  • 64. Contaminant Hydrogeology Journals Water Resources Research Ground Water Ground Water Monitoring and Remediation Environmental Science and Technology Journal of Contaminant Hydrology