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203552 Advanced Soil Mechanics
Dr.Warakorn Mairaing 1
Dr. Warakorn MairaingAssociate Professor
Civil Engineering DepartmentKasetsart University, Bangkok Tel: 02-579-2265Email: [email protected]
Dr. Warakorn MairaingDr. Warakorn MairaingAssociate ProfessorAssociate Professor
Civil Engineering DepartmentCivil Engineering DepartmentKasetsart University, Bangkok Kasetsart University, Bangkok Tel: 02Tel: 02--579579--22652265Email: [email protected]: [email protected]
Lecture No. 2
Soil PermeabilitySoil Permeability
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Soil permeability (k) or Hydraulic conductivity is soil property which allow the seepage of fluid through its interconnected void spaces.
According to Darcy’s law (Laminar’flow)
v=ki If i=1
Then k=v so permeability (k) is the seepage velocity through soil when subjected to the hydraulic gradient of unity (i = 1)
Soil permeability varies on very wide range from 10-10 cm/sec to 10o
cm/sec (10 logarithmic eyeless)
Soil Permeability
Factors affect soil permeability
There an 2 main groups of factors
1. Fluid properties flow through soil (Permeant)2. Pore characters in the soil mass (Porous Media)
Permeability Model
b) Capillary Tubesa) Soil Mass
If total soil x-section = A, Degree of Saturation = S and porosity = n, Then area of water chancels = S.n.A.
Soil Permeability
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- Taylar (1984) using poiseville’s law of flow through. Capillary tubes to formulate permeability as;
( ) ce
eDk s ⋅+
⋅⋅=1
32
μγ
---(1)
- Kazeny – Carman (1927, 1956)
( )eG
skk
+⋅⋅=1.
1 3
20 μ
γ---(2)
Soil Permeability
when
Ds = effective particle diameters, γ = unit wt. of waterμ = viscousity of water, e = void ratioC = shape factor, ko = pore shape and flow path factorSo = specific surface area
,...),,,,,( oo kSSDuvefk =∴ ---(3)
Soil Permeability
Equation (3) is soil permeability model function consisted of
1. Permeant ex. Fresh water, crude oil, contaminant to eliminate the various properties of permeants, the “Absolute Permeability” (k) is proposed as
μγ.kk =
---(4)
For fresh water at 20oc when u and r are known, then
sec)/(1002.1)( 52 cmkcmk ⋅×= −---(5)
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2. Soil or porous media soil, rock, porous stone, sand filter etc.
- Soil larger than coarse gravel
- Soil smaller than coarse gravel
- Cohesive soil
Turbulent flow occurred.? (ND > 1) Darcy’s law invalid.
Darcy’s law is valid Kazeny – Carman and Equation (3) is applied
Permeability model (Eq.3) may not valid due to the influences ofDiffused Double layer or Surface chemical properties of soil particles
Soil Permeability
In general factors influence soil permeabilitics are :
1. Particle size distribution (Pore size distribution)
2. Void ratio (e)
3. Soil mineral (CEC, defuses D.L.)
4. Soil Structure (Flocculation, Dispassion)
5. Degree of Saturation (S)
Soil Permeability
1. Particle Size for sand and silt
Hazen
Land and Washburn
Kane
k ≅ 100 D102
k ≅ (1-40) D102
k ≅ 40 D102
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2. Void ratio
⎟⎟⎠
⎞⎜⎜⎝
⎛+
=e
efk1
3
⎟⎟⎠
⎞⎜⎜⎝
⎛+
=e
efk1
2
( )efk 10=
- Kozeny
Soil Permeability
3. Soil Mineral and Soil Structure for clay
3.1 Defused Double Layer Free water3.2 Dispersed and Flocculated Structures3.3 Anisotropic permeability (kx ≠ ky)
4. Degree of Saturation
High degree of saturation high permeability saturation increase flow area (less are void)
Soil Permeability
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Soil Permeability
Soil Permeability
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Soil Permeability
Soil Permeability
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Soil Permeability
ชวงของคาความซึมน้ําของดินฐานรากชนิดตางๆ
Pore Pressure Development
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PORE PRESSURE DEVELOPMENT
PORE PRESSURE DEVELOPMENT
When partially or fully saturated soils are subjected to external load or change in ground water level, there will be a change in pore water pressure called “Excess pore pressure (Δu)”. This condition occurs temporarily until it reach to stable final pressure.
It is very important to predict Δu since it is related to many soil mechanical behaviors such as strength, consolidation
Pore Pressure Development
Two periods are involved during loading and subsequence times,
1. Undrained loading; When load or excess pore pressure change suddenly
Δu = (P.P.).ΔσσΔΔ
=uPP .. ---(1)
When P.P. = Pore pressure parameterΔu = Pore pressure change.Δσ = Total pressure change.
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2. Pore Pressure Dissipation; when applied load is rather constant and the excess pore pressure graduately changes until it reaches static pore pressure (us)
Ex. Figure 1 is the typical case of confined compression (typical consolidation test)
Figure 2 is the surface loading on soil layer ---- Field embankment test for SBIA (Suwanabhump Airport)
Figure 3 is the ground water lowering ---- Bangkok ground water pumping and Land subsidence.
Pore Pressure Development
Pore Pressure Development
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Pore Pressure Development
Pore Pressure Development
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Pore Pressure Development
Pore Pressure Development
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Pore Pressure Development
Pore Pressure Development
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ผลที่ตามมาจากความดันน้ําลดลง
( p’ = p – uw )p’ เพิ่มขึ้น
หนวยแรงกดทั้งในแนวดิ่งและแนวราบ เพิ่มขึ้น
การทรุดตัวของชั้นดินเพิ่มขึ้นแรงตานทานของเสาเข็มเพิ่มขึ้นหนวยแรงดันของโครงสรางใตดินเพิ่มขึ้น
อ่ืนๆ
การเปลี่ยนแปลงแรงตานทานตอฐานรากเสาเข็มการเปลี่ยนแปลงแรงตานทานตอฐานรากเสาเข็ม
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0
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0 50 100 150 200 250 300 350 400 450 500 550 600 650 700
Pore Water Pressure (t/m2)
Dep
th (
m.)
Hydrostatic, u0
Pore Pressure, ut
BK
PD
NL
NB
SK
PT
TB
PN
ตัวอยางแรงดันน้ําที่มีการเปลี่ยนแปลงในชั้นน้ําตางๆตัวอยางแรงดันน้ําที่มีการเปลี่ยนแปลงในชั้นน้ําตางๆ
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Skempton’s Pore Pressure Parameters
Prof. Skempton (1954) of Imperial College (London) developed the theory for estimating the excess pore water pressure (Δu) due to increase of total stress in soil mass.
Assuming total stresses (Δσ) changes happen suddenly. (at Δt = 0)
Pore Pressure Development
Skempton’s Pore Pressure =σΔΔu ---(1)
The magnitude of Δu is depended on;1. Compressibility of soil skeleton (Soil = Void) = Csk2. Compressibility of water (pore water) = Cw3. Magnitude of total stress change = Δσ
Then
( )σΔ=Δ ,, wsk CCfu ---(2)
Case study on;
1. Confined Compression
2. Isotropic Compression
3. Uniaxial Stress (Unconfined Compression)
4. Triaxial Compression
Will be considered.
Pore Pressure Development
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1. Confined Compression (1-D Consolidation, Land Reclamation)
Compressibility of soil Skeleton
Compressibility of pore water
KgCmv
v
C esk
26
1
10−≅Δ
Δ
=σ ---(3)
---(4)Kg
Cmu
vv
C ww
2910−≅
Δ
Δ
=
Pore Pressure Development
ΔVw = Change in water volume 0nVuCw ⋅Δ⋅=
01 VCsk ⋅Δ⋅= σΔVsk = Change in soil skeleton volume ---(5)
---(6)
Relationship of total and effective stresses ---(8)uΔ−Δ=Δ 11 σσ
In particular soil mass; change of soil volume = Change in water vol.
---(7)0nVuC w ⋅Δ⋅=01 VC sk ⋅Δ⋅= σ)6()5.( EqEq =∴
Pore Pressure Development
Then substitute (8) in (7)
( ) uCwnuCsk Δ⋅⋅=Δ−Δ 1σ ( ) 1.. σΔ=+Δ skskw CCCnu
For saturated soil, when Cw ≈ 10-9 Cm2/kg and Csk ≈ 10-6 Cm2/kg then Eq.(9) become
0.11
1""w
≅
⎟⎟⎠
⎞⎜⎜⎝
⎛−
=
skCCn
C
( ) ""Pr1
CParameteressurePorenCC
Cu
wsk
sk =+
=ΔΔσ
---(9)
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2. Isotropic Compression
Change in Soil Skeleton Volume
330220110 σσσ Δ⋅⋅+Δ⋅⋅+Δ⋅⋅=Δ sksksksk CVCVCVV ---(10)
Pore Pressure Development
Change in Pore Water Volume
uCVnV ww Δ⋅⋅⋅=Δ 0 ---(11)
Eq. (10) = Eq. (11) for the same soil mass
3302201100 σσσ Δ⋅⋅+Δ⋅⋅+Δ⋅⋅=Δ⋅⋅⋅∴ skskskw CVCVCVuCVn
If the applied stresses are truely isotropic compression, then
)(321 uΔ−Δ=Δ=Δ=Δ σσσσ
---(12)
Pore Pressure Development
From Eq.(12) ( )( )321 skskskw CCCuuCn ++Δ−Δ=Δ⋅⋅ σ
""Pr321
321 BParameteressurePoreCCCnC
CCCu
skskskw
sksksk =+++
++=
ΔΔσ
---(13)
---(14)
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13
13
3""+
=+
==ΔΔ
sk
wskw
ski
CnCCnC
CBuσ
If soil is isotropic material, thus Csk1=Csk2=Csk3=Csk.; then
---(15)
Pore Pressure Development
If Soil is saturated normally consolidated clay, then the term
0.1103
4 ≈→≈⋅ − BandCCn
sk
w
But for O.C. and Rock Which are precompressed in the past
B < 1.0 as shown on Table 1
3. Uniaxial Stress (Unconfined Compression)
Where soil mass is compressed in vertical direction, it will expand in other directions. (Swelling Coefficients = Cs2 and Cs3)
Pore Pressure Development
Considering uandu Δ−=Δ=ΔΔ−Δ=Δ 3211 σσσσ ---(16)
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Change in soil-void volume = change in pore water volume
( ) ( ) ( )uCVuCVuCVuCVn ssskw Δ−⋅⋅+Δ−⋅⋅+Δ−Δ⋅⋅=Δ⋅⋅⋅ 30201100 σ
( ) 11321. skssskw CCCCnCu ⋅Δ=+++Δ∴ σ
( )321
1
1 ssskw
sk
CCCnCCu
+++=
ΔΔσ
---(17)
If soil is Isotropic and linear elastic material
Pore Pressure Development
Then ""Pr
3
1
1
DParameteressurePore
CCn
u
sk
w=
+=
ΔΔσ
---(18)
4. Triaxial Compressive Stress
Unconsolidated-Undrained triaxial compression test in consisted of 2-stages of applied stresses as;
1. Stage I Isotropic Compression
When soil sample is applied by all around pressure, Δσ3
2. Stage II Uniaxial Compression (Shearing)
When soil sample is applied by vertical stress of Δσa= (Δσ1 Δσ3)
Pore Pressure Development
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Confining Stage Shearing Stage
Pore Pressure due to Stage 1 : Isotropic compression
Δu2 = D (Δσ1- Δσ2)
Pore Pressure due to Stage 2 : Uniaxial compression
Δu1 = B Δσ3
Pore Pressure Development
+
∴ Overall pore pressure during UU-Triaxial Test
Δu = Δu1 + Δu2 = B Δσ3+ D (Δσ1- Δσ2) ---(19)
Special case for Saturated Soil and Incompressible pore water, then
B ≈ 1.00
From equation (17) when and00.01
≈sk
w
CC
Cs2 = Cs3 = Cs , then
""Pr21
1
1
AParameteressurePore
CC
u
sk
sa=
+=
ΔΔσ
Pore Pressure Development
---(20)
And eq.(19) becomes.
Δu = Δσ3+ A (Δσ1- Δσ3)
As we can see from table 1 that “A-” parameter is depended on it stress history
.)("" OCRfA =∴ ---(21)
When OCR. = Over Consolidation Ration0v
m
σσ
=
For Bangkok Clay and others Sedimentary soil, The Value of “A” can be seen on Figure 9
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Pore Pressure Development
Pore Pressure Development
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Pore Pressure Development
Pore Pressure Development
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Determination of A-Parameter from Stress-path
BDBCu
Afa
ff ⋅
=Δ
=2σ312 σσσ Δ−Δ
Δ=
Δ=
⋅=
uau
xzxyA
Pore Pressure Development
Pore Pressure Development
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อิทธิพลที่มีตอ Pore Pressure Parameter “A” คา Parameter “A” ไมคงที่ ข้ึนอยูกับ
Pore Pressure Development
Pore Pressure Development
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Prediction of Pore Pressure in the Field
Predictions of excess pore pressure in the field are related to stability, bearing capacity and settlement problem
Since effective strength;
and settlement;
φστ tan)( ⋅−+= uc
0
0
0
log1 P
uPHe
CS c Δ+⋅⋅
+=
Pore Pressure Development
Ex.
1. Stability Problem
2. Bearing Capacity – Similar to Stability
Pore Pressure Development
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( )313 .. σσσ Δ−Δ+Δ=Δ ABuExcess P.P.;
Dissipation of Δ u leading to consolidation and settlement of soil layer.
3. Consolidation and Settlement
Pore Pressure Development
ตัวอยาง Preloading Area
Pore Pressure Development
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Pore Pressure Development
Henkel’s Pore Pressure Parameters.
In case of plan-strain stress condition when stresses on x,y and z directions are all different. Henkel (1960) proposed that intermediate principal stress (Δσ2) should be included in pore pressure calculation.
octoct au τσ Δ⋅+Δ=Δ .3
when
and
( )32131 σσσσ Δ+Δ+Δ=Δ oct
213
232
221 )()()(
31 σσσσσστ Δ−Δ+Δ−Δ+Δ−Δ=Δ oct
---(22)
---(23)
---(24)
Special case for triaxial loading when Δσ2 = Δσ3, then from eq. (22), (23) and (24)
( ) ( )3131 2
32 σσσσ
Δ−Δ+Δ+Δ
=Δ au ---(25)
Pore Pressure Development
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Special case for uniaxial loading when Δσ1-Δσ3 = Δσ1 and Δσ2 = Δσ3 = 0, then
⎟⎠⎞
⎜⎝⎛ +Δ=Δ 231
1 au σ
From eq.(20), Skempton’s parameter for uniaxial loading
)(0 1σΔ+=Δ Au
Equate eq (26) = (27), then
231
⋅+= aA or ⎟⎠⎞
⎜⎝⎛ −=
31
21 Aa
When A = Skempton pore pressure parametera = Henkel pore pressure parameter
---(28)
---(26)
---(27)
Pore Pressure Development
ตัวอยาง
ถนนบนดินเหนียวออน มีคันถนนสูงจากผิวดิน 2.00 เมตร กวาง 25 เมตร ดินบดอัดคันถนนมีความหนาแนน 2.0 ตันตอลบ.ม. จากการทดสอบ Triaxial Test ของดินฐานราก ทราบวาดินมีคุณสมบัติดังนี้
“A” parameter = 0.90 , υ = 0.45
จงหาวา ที่จุด A, B และ C ในดินฐานรากจะมีความดันน้ําสวนเกินเกิดขึ้นเทาใด โดยใหถือวาการกอสรางเกิดขึ้นเร็วมาก
- Surcharge load
ที่ผิวดิน = 2x2 = 4 ตัน/ตร.ม.
- จากตารางที่ 3.4
“Advanced Soil Mechanics” By B.M. Das page 182
B = 12.5 , z = 6.25 m.
Pore Pressure Development
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1.1980.29961.3890.34721.9880.49690.51.0C
0.5100.12741.5680.39203.6110.90280.50.5B
001.7990. 44983.8380.95940.50A
σxzσxz /qσxσx /qσzσz /qσxzσxσzz/bx/bตําแหนง
Pore Pressure Development
จาก Mohr’s Diagram
22
1 22⎟⎠⎞
⎜⎝⎛ =
+++
= xzxz
zx σσδσσσ
22
3 22⎟⎠⎞
⎜⎝⎛ =
+−+
= xzxz
zx σσδσσσ
( ) ( )31312 45.0 σσσσνσ +=+=
1.5200.4542.9231.1981.9881.389C
2.3311.4483.7310.5103.6111.568B
2.5371.7993.8380.03.8381.799A
σ2σ3σ1σxzσzσxตําแหนง
---(1)
---(2)
---(3)
Pore Pressure Development
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Henkel’s pore pressure
⎟⎠⎞
⎜⎝⎛ −=
31
21 Aa 400.0
319.0
21
=⎟⎠⎞
⎜⎝⎛ −=a
( ) ( ) ( )2132
322
21321
3σσσσσσσσσ
Δ−Δ+Δ−Δ+Δ−Δ+++
=Δ∴ au
ที่ตําแหนง A Pore Pressure ΔμA = 3.55 ตัน / ตร.ม.B Pore Pressure ΔμB = 3.43 ตัน / ตร.ม.C Pore Pressure ΔμC = 2.62 ตัน / ตร.ม.
Pore Pressure Development
Pore Pressure Development
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Pore Pressure Development
4.07E-073.66E-06CL3
1.00E-081.00E-08Slurry4
3.30E-091.00E-08Dam5
1.00E-031.00E-03Relief Well6
6.35E-066.35E-06SP-SM7
1.73E-071.56E-06SC2
1.00E-101.00E-10Rock1
Kv
Cm/sec
Kh
Cm/sec
Soil TypeMaterial No.
Pore Pressure Development
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Pore Pressure Development
Pore Pressure Development
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Pore Pressure Development
Pore Pressure Development
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Pore Pressure Development
Pore Pressure Development
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Pore Pressure Development
Pore Pressure Development
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Pore Pressure Development
Pore Pressure Development
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Pore Pressure Development
Pore Pressure Development