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Water flow
Air flow
THEORY
No suctiongradient but
still flow
Suctiongradient to
the right
Suctiongradient to
the left
Does Suction Gradient
Cause Flow?
Does water content
gradient cause Flow?
Coarse stone
Fine ceramic
Does water flow from A to B?, or B to A?
Permeability is fixed at a particular water content
Childs and Collis-George, 1950
PROOF: Darcy’s Law is valid
kw constant
For a saturated soil,k = k(e) or k(w)
A void of air has the same effect as a void filled with carbowax
SWCC - Soil-Water Characteristic Curve
Deg
ree
ofSa
tura
tion,
S
Soil Suction (kPa)0
1
Residual Saturation
Air-EntryValue
S = 1 1 > S > Sr S = Sr
Water can only flow where there is water
in the voids
Tortuosity dramatically changes permeability
Air entry value is ~ 4 kPa
SWCC - Soil-Water Characteristic Curve
Brooks and Corey 1964
Effective degree of saturation or (Normalized) degree of saturation
Two parameter equation
Assumes there is “no-flow” below residual w%
=
Becomes a straight line on a log-log plot
The Brooks and Corey (1964) equation for SWCC
The Brooks and Corey (1964) equation for Permeability
Becomes linear on a log scale)
Delta is related to the Pore Size Distribution Index
Summary of Brooks and Corey (1964) Equation for the Coefficient of Permeability
Se = (S – Sr ) / ( 1 – Sr )
Se = Measure of amount of water
S = Any degree of saturation
Sr = Residual degree of saturation
λ = Pore size distribution index
( ua – uw)b2+3λ
kw = ks --------------(ua – uw){ }
=
Pore size distribution for SWCC
Constant δ for Permeability
Brooks and Corey is a discontinuous function since it starts at the Air Entry Value of the soil
Gardner’s equation1958
‘a’ parameter bears an inverse relationship to the air entry value
Integration Forms for the SWCC and Permeability Function
• (Childs and Collis-George, 1950); assumed that the soil has a random distribution of pores of various sizes
• Used the summation of a series of terms from the statistical probability of interconnections between the pores
• SWCC was used as an indication of the configuration of the water-filled pores
• Permeability equation was derived based on the Poiseuille equation
Childs and Collis-George
(1950)
Log suction
Measured permeability
Log
Perm
eabi
lity
Childs and Collis-George
(1950)
Based on summation (or integration) along the SWCC
Variable “p” is a power applied to volumetric
water contentAssume p = 2.0
Air entry value= ~ 3 kPa
Log suction
Usual form for Permeability
function
Relationship Between Soil-Water Characteristic Curve
and the Coefficient of Permeability for sand and
a Clayey Silt
• The soil-water characteristic curve defines the amount of water in the soil
– Air entry value initiates a reduction in the coefficient of permeability
– Is possible for a sandy soil to have a lower permeability than a clayey soil
mw2
1
Saturation coefficient ofpermeability (clayey silt)
Matric suction, (ua -uw) (kPa)
Coe
ffici
ent o
f per
mea
bilit
y,k w
(m/s
)
Soil-water characteristic curve
Wat
er c
onte
nt, w
(%)
Start of desaturationfor
a clayey silt
100 200 300 400 500
10-5
10-6
10-7
10-8
10-9
10-10
100 200 300 400 500
0
00
10
20
30
40
50
Saturation coefficient ofpermeability (fine sand)
Matric suction, (ua -uw) (kPa)
desaturationfor a fine sand
Start of
Typical Gardner’s Empirical Permeability Functions Shown for a Sand and a Clayey Silt
• Permeability function is commonly plotted as a function of the logarithm of suction
• Most soils show a straight line as the soil desaturates towards residual conditions
• Gardner’s function is one of the simplest permeability functions with physical meaning to the “a” and “n” parameters
Clayey silt
Fine sand
1 10 100 1000
Clayey silt
kw=ks
1+a(ua- uw)n
10
10-10
Fine sand
Start of desaturation for a
fine sand
Permeability function
203040
50
1 10 100 1000
10-9
10-8
10-7
10-6
10-5
Gardner’s equation n clayey silt
n
Matric suction, (ua -uw) (kPa)
Coe
ffici
ent o
f per
mea
bilit
y,k w
(m/s
)W
ater
con
tent
, w (%
) Start of desaturation for a clayey silt
Matric suction, (ua -uw) (kPa)
sand
Commonly used Permeability Functions• van Genucthen (1980)
– SWCC
– k-functionwhere m = 1-1/n
• Fredlund and Xing (1994)– SWCC
– k-function
m
neS
+
=)(1
1αψ
2
2
1
111
++−
=−−
/mn
mnn
r ])([])([)(k
αψαψαψ
)(C)
A(eln
S
C
Bψ
ψ
+
=1
dy)e(e
)e(
dy)e(e
)uu(f)e(
ky
wln
b)wuauln( ys
yw
yw
ln)wuauln( y
wawy
w
r
θθθ
θθθ
′−
′−−
=
∫ −
∫ −
610
610
10-12
10-10
10-08
10-06
10-04
10-02
10+00
1 10 100Soil suction (kPa)
k r
Brooks and Corey
van Genuchten
0.0
0.1
0.2
0.3
0.4
0.0 0.1 1.0 10.0 100.0 1000.0Soil Suction (kPa)
van Genuchtenlab data
θ
Comparison of van Genuchten (1980) and
Brooks and Corey (1964)
Forms for the Permeability Function Based on the SWCC
• Childs and Collis-George (1950)– Summation
• van Genuchten (1980)• van Genuchten-Burdine (1953, 1980)• van Genuchten-Maulem (1976, 1980)• Fredlund, Xing and Huang (1994)
– Integration form• Rahardjo and Leong (2000)
– Closed form; raised SWCC to a power
Difficulties with Hysteresis of SWCC and Permeability
Is there one Permeability Function for drying and another function for wetting?
Difference at inflection point = 0.2 to 0.5 of a log
cycle
Difference at w% inflection point = 0.2 to 0.5 of a log
cycle
No hysteresis in the water content versus
permeability relationship
Must Live with Hysteresis in SWCC and Permeability
• Generally it is the Drying (or desorption) curve that is measured or estimated
• Sometimes the Wetting (or Adsorption) curve might be measured or estimated
• The Wetting Curve might be estimated as being shifted to the left by approximately (one half) log cycle at the inflection point
• Independent permeability functions can be determined for both the Drying and the Wetting processes
• Some rigorous permeability models have been proposed with scanning curves