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Fluid Mechanics in Porous Materials BAE 558

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Fluid Mechanics in Porous Materials BAE 558. Solute Transport. Leaching of Organic Chemicals. Adsorption Degradation Ground water contamination is minimal when a chemical is strongly adsorbed, rapidly degraded, and the water table is well below the soil surface - PowerPoint PPT Presentation
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Page 1: Fluid Mechanics in Porous Materials  BAE 558

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Fluid Mechanics in Porous Materials BAE 558

Solute Transport

Page 2: Fluid Mechanics in Porous Materials  BAE 558

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Leaching of Organic Chemicals

• Adsorption

• Degradation

• Ground water contamination is minimal when a chemical is strongly adsorbed, rapidly degraded, and the water table is well below the soil surface

• Reverse: weak adsorption, slow degradation, and high water table

Page 3: Fluid Mechanics in Porous Materials  BAE 558

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Retardation Factor

The retardation factor (R) is a general indication of a chemical’s mobility in the soil compared to the water velocity

• R = u/us

where

• u = mean water velocity (cm yr-1)

• us = mean chemical velocity (cm yr-1)

Page 4: Fluid Mechanics in Porous Materials  BAE 558

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Retardation Factor

• For a nonadsorbed ion such as Cl- or NO3-,

R approaches unity

• For a strongly adsorbed chemical, R will be much greater than 1, and movement through soil will be slow (us << u)

• R can also be taken as the ratio of the total to dissolved chemical in the soil

Page 5: Fluid Mechanics in Porous Materials  BAE 558

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From Selker et al.

CT = cd + cp

• In soil: cd = v Cd

cp = dry Cs

where v is volumetric moisture content (-), dry is dry bulk density (kg m-3)

Page 6: Fluid Mechanics in Porous Materials  BAE 558

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Chemical Displacement

The retardation factor (R) can be used to determine the distance which a chemical moves in t years:

R = ut/ust = Z/X

where

Z = water displacement during time t (cm)

X = chemical displacement during time t (cm)

Page 7: Fluid Mechanics in Porous Materials  BAE 558

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Water Displacement

In unsaturated soil:

In saturated soil:

where• Q = water flow per unit area (cm) fc, s = moisture content at field capacity and

saturation, respectively (cm3 cm-3)

s

QZ

Page 8: Fluid Mechanics in Porous Materials  BAE 558

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Chemical Displacement

• Unsaturated zone:

• Saturated zone:

• X indicates the location of the center of mass after percolation Q

ddrys KQ

X

ddryfc KQ

X

Page 9: Fluid Mechanics in Porous Materials  BAE 558

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Downward Movement of Chemical in Soil

center of mass

X

soil surface

chemical concentration

Page 10: Fluid Mechanics in Porous Materials  BAE 558

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Mean Travel Time

• The time required for the chemical’s center of mass to reach the aquifer, and hence the mean travel time of the chemical through the unsaturated zone is:

• T = 100H/X

• where

• T = mean travel time (yr)

• H = depth to the water table (m)

Page 11: Fluid Mechanics in Porous Materials  BAE 558

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Degradation

• The degree of ground water pollution by an organic chemical is very much influenced by degradation and decay rates

• Assuming a 1st order process:

where

• C(t) = chemical in the soil at time t (g ha-1)

• C(0) = initial chemical at the soil surface (g ha-1)

• ks = decay rate (yr-1)

tske)0(C)t(C

Page 12: Fluid Mechanics in Porous Materials  BAE 558

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Degradation

To calculate the chemical mass entering the water table T years after leaching begins:

where

• C(T) = chemical mass entering water table after T years (g ha-1)

Tske)0(C)T(C

Page 13: Fluid Mechanics in Porous Materials  BAE 558

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Ground Water Loads of Organic Chemicals

Equations are providing “order of magnitude” estimates due to effects of dispersion, uncertainty in decay rates, and the assumption of homogeneous porous media.

Page 14: Fluid Mechanics in Porous Materials  BAE 558

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ExampleNapthalene Leaching from a Waste Storage Site:

50,000 g ha-1 of napthalene is leaching from an abandoned waste disposal site. The site is on a sandy loam with 1% OM. Water table depth is 1.5 m. Mean annual percolation is 40 cm. Kow = 2300 and a half-life of 1700 days

How much napthalene will reach the water table aquifer and what will be the resulting napthalene concentration at the water table surface?

Page 15: Fluid Mechanics in Porous Materials  BAE 558

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Example

Koc = 0.66Kow1.029 = 0.66(2300)1.029 = 1900

%OC = 0.59(%OM) = 0.59(1) = 0.59

Kd = Koc (%OC/100) = 1900(0.59/100) = 11.2

bulk density dry = 1.5 g cm3

moisture at fc: fc = 0.22 cm3cm-3

available water capacity: w = 0.22 - 0.08 = 0.14

Page 16: Fluid Mechanics in Porous Materials  BAE 558

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ExampleAnnual napthalene movement:

Average time to reach the water table aquifer:

• T = 100H/X = 100(1.5)/3.7 = 40.5 yr

yr/cm7.322.0/)2.11(5.11

14.0/40/K1

w/QX

vddry

Page 17: Fluid Mechanics in Porous Materials  BAE 558

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Example• To calculate the napthalene remaining after 40.5

years, use:

• To obtain ks:

Tske)0(C)T(C

sk)365/1700(e5.0 1

s yr149.066.4/)5.0ln(k

Page 18: Fluid Mechanics in Porous Materials  BAE 558

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Example• To calculate the napthalene remaining after 40.5

years, use:Tske)0(C)T(C

1)5.40(149.0 hag120e000,50)T(C

Page 19: Fluid Mechanics in Porous Materials  BAE 558

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Example• To determine the napthalene concentration in

water at the aquifer surface, we need to divide the 120 g ha-1

into dissolved and adsorbed amounts using the retardation factor:

7722.0

)2.11(5.11

K1

CC

Rv

ddry

d

T

1Td hag56.1

77120

RC

C

Page 20: Fluid Mechanics in Porous Materials  BAE 558

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Example

• Assuming the 1.56 g ha-1 is dissolved into one year’s percolation flow, 40 cm = 4000 m3 ha-1, the concentration is:

• 1.56/4000 = 0.00039 g m-3 = 0.39 g L-3

Page 21: Fluid Mechanics in Porous Materials  BAE 558

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Physical Processes

• Convection-dispersion equation (CDE)

• Breakthrough curves

• Piston flow

• Hydrodynamic dispersion, Mechanical dispersion, Molecular diffusion

• Mobile-immobile regions in soils

• Preferential flow

Page 22: Fluid Mechanics in Porous Materials  BAE 558

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Solute Transport in Soils

Applications:

• Design of optimum pesticide and fertilizer application

• Reclamation of saline or sodic soils

• Ground water contamination issues

Page 23: Fluid Mechanics in Porous Materials  BAE 558

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Solute Conservation EquationFor a chemical located in a small volume element of soil V = xyz over a small period t:

mass of solute entering V during t =

mass of solute leaving V during t +

increase in solute mass stored in V during t +

disappearance of solute from V during t by chemical or biological reactions or by plant uptake

z

xy

Page 24: Fluid Mechanics in Porous Materials  BAE 558

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Solute Conservation Equation

z

xy

Js(x,y,z,t)xy

Js(x,y,z+z,t)xy

Js = total solute flux(M/T)

Page 25: Fluid Mechanics in Porous Materials  BAE 558

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Solute Conservation Equation

Js(x,y,z,t+1/2t) xyt =

Js(x,y,z+z,t+1/2t) xyt +

(CT(x,y,z+ 1/2z,t+t)-CT(x,y,z+1/2 z,t)) xyz +

kr(x,y,z+ 1/2z,t+1/2t) xyt

where

CT = dryCs + vCd + (n - v)Cg (M/L3)

kr = reaction rate per volume (loss of solute per soil volume per unit time)

Page 26: Fluid Mechanics in Porous Materials  BAE 558

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Solute Conservation Equation

divide by xyzt and rearranging:

where are the average values of z and t, respectively.

Taking the limit x, y, z, t => 0, we obtaint,z

Page 27: Fluid Mechanics in Porous Materials  BAE 558

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Solute Flux through Soil

The chemical can move in dissolved and vapor phase (sorbed phase is stationary):

Js = Jl + Jg

whereJl = flux of dissolved solute

Jg = flux of solute vapor

Page 28: Fluid Mechanics in Porous Materials  BAE 558

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Dissolved Solute Flux

We will only develop the dissolved solute flux:

• convection of dissolved chemical with flowing solution (bulk transport), Jlc

• diffusive flux of dissolved solute moving by molecular diffusion, Jld

Jl = Jlc + Jld

Page 29: Fluid Mechanics in Porous Materials  BAE 558

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Convection Term

The solute convection term is expressed as:

Jlc = JwCd + Jlh

where

Jw = the water flux

Jlh = hydrodynamic dispersion flux:

where

Dlh = the hydrodynamic dispersion coefficient (cm2day-1)

zC

DJ dlhlh

Page 30: Fluid Mechanics in Porous Materials  BAE 558

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Diffusion Term

The solute diffusion term is expressed as:

where

Dls = the soil liquid diffusion coefficient (cm2 day-1)

zC

DJ dslld

Page 31: Fluid Mechanics in Porous Materials  BAE 558

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Dissolved Solute FluxThe total flux of dissolved solute in a convection-

dispersion model now becomes:

which is commonly written as:

where

De is the effective diffusion-dispersion coefficient

zC

Dz

CDCJJ ds

ld

lhdwl

zC

DCJJ dedwl

Page 32: Fluid Mechanics in Porous Materials  BAE 558

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Convection-Dispersion EquationSubstituting CT, Js (= Jl + Jg) into the solute conservation

equation,

the solute transport equation (without vapor phase):

rd

edwdvsdry kz

CD

zCJ

z)CC(

t

0kzJ

tC

rsT

Page 33: Fluid Mechanics in Porous Materials  BAE 558

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Convection-Dispersion Equation (CDE)

A typical experiment: water is flowing uniformly at steady state through a homogeneous soil column of length L at a constant water content.

For inert, non-adsorbing chemicals (Cs = 0, kr = 0)

where

D = De/v

v = water velocity (Jw/v)

zC

vz

CD

tC d

2d

2d

Page 34: Fluid Mechanics in Porous Materials  BAE 558

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Experiment

At t = 0, we instantaneously switch the water inlet valve of the soil column from its initial solute-free source to a chloride solution at a concentration C0, which continues to flow at Jw through the column

L

inflow rate Jw=Q/A

solute outflow concentration C(L,t)

AC = 0C = C0

Page 35: Fluid Mechanics in Porous Materials  BAE 558

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The Breakthrough Curve

C(L,t)/C0

dimensionless time T = vt/L

1.0

1.0

piston flow D=0

vL/D = 10

vL/D = 30

Plot of outflow concentration versus time, which are mathematical solutions to the convection-dispersion equation

Page 36: Fluid Mechanics in Porous Materials  BAE 558

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Breakthrough Time

The center of each of the solute fronts, for different values of D, arrive at the outflow end of the column at the same time tb = L/v, called the breakthrough time

When dispersion is neglected (D = 0), all solutes move at the same velocity, and the front arrives as one discontinuous jump to the final concentration C0. This is called ‘piston flow’

Page 37: Fluid Mechanics in Porous Materials  BAE 558

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Effect of Dispersion

As can be seen in the breakthrough curves, the effect of dispersion is to cause some early and late arrival of chloride with respect to breakthrough time.

This deviation is due to diffusion and small-scale convection ahead of and behind the front moving at v, and becomes more pronounced as D becomes larger

Page 38: Fluid Mechanics in Porous Materials  BAE 558

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Pore Volumes

Instead of plotting outflow concentration as a function of time, concentration can be plotted against cumulative water drainage dw passing through the outflow end of the column. At steady state: dw = Jwt

At breakthrough time, dwb = Jwtb = JwL/v = Lv

L v is called a ‘pore volume’, so it requires approximately one pore volume of water to move a mobile solute through a soil column

Page 39: Fluid Mechanics in Porous Materials  BAE 558

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Transport of Pulses through Soil

In many cases, a narrow pulse of solute, rather than a front, might be added to the inlet at t=0

A solution to the CDE is then:

As D becomes larger, the pulse becomes more spread out

Dt4

2)vtL(

30 eDt2

LC)t,L(C

Page 40: Fluid Mechanics in Porous Materials  BAE 558

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The Breakthrough Curve

C(L,t)/C0

dimensionless time T = vt/L

1.0

1.0

vL/D = 10

vL/D = 30

Plots of outflow concentration versus time, which are mathematical solutions to the convective-dispersion equation

Page 41: Fluid Mechanics in Porous Materials  BAE 558

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Inert, Adsorbing Chemicals

• For chemicals that partition between solid phase and dissolved phase, the transport equation is written as:

• Using a linear partition coefficient, Kd:

zC

vz

CD

tC

tC d

2d

2ds

v

dry

tC

Kt

C dd

s

Page 42: Fluid Mechanics in Porous Materials  BAE 558

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Inert, Adsorbing Chemicals

• Combining previous two equations:

• where the retardation factor R is:

zC

vz

CD

tCK

1 d2d

2d

v

ddry

v

ddryK1R

Page 43: Fluid Mechanics in Porous Materials  BAE 558

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Inert, Adsorbing Chemicals

• If we divide through by R:

where DR = D/R, and vR = v/R

• Breakthrough time, tbR = L/vR = RL/v = Rtb

• Dispersion is greater than for non-adsorbing chemical because while the dispersion coefficient is reduced by R, travel time is increased

zC

vz

CD

tC d

R2d

2

Rd

Page 44: Fluid Mechanics in Porous Materials  BAE 558

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Effect of Soil Structure on Transport• Soil structure can create preferential flow

channels for water and dissolved solutes

C(L,t)/C0

dimensionless time T = vt/L

1.0

1.0

undisturbed column

repacked column

Page 45: Fluid Mechanics in Porous Materials  BAE 558

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Preferential Flow Effects

• The early arrival of solute may be attributed to preferential flow of water through the larger channels of the wetted pore space (large channels and wetted regions between finer pores in an aggregated soil)

• Water in the finer pores is more stagnant and do not contribute to solute transport, except for diffusion exchange, explaining the later arrival

Page 46: Fluid Mechanics in Porous Materials  BAE 558

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Mobile-immobile Water Model

• A model that represents the wetted pore space with two water contents:

• a mobile water content, m, through which water is flowing

• an immobile water content, im, which contains stagnant water

im = v - m

Page 47: Fluid Mechanics in Porous Materials  BAE 558

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Mobile-immobile Water Model

• Solute concentration is divided into an average concentration Cm in the mobile region and a second Cim in the immobile region

• In the mobile region, solute is transported by a convective-dispersive process

• In the immobile region, a rate-limited diffusion process exchanges solute with the mobile region

Page 48: Fluid Mechanics in Porous Materials  BAE 558

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Mobile-immobile Water Model

• For an inert, non-reactive solute, the conservation equation is now written as:

• where

• CT = mCm + imCim

zC

Jz

CD

tC

tC m

w2m

2

eim

imm

m

Page 49: Fluid Mechanics in Porous Materials  BAE 558

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Preferential Flow

• Macropores

• Funnel flow

• Fingering