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Push In Basal Heave Overall Shear Failure Overall shear failure modesStability Analysis

2 Stability Analysis

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stability in deep excavation push inbasal heaveto help engineer in control of stability of soils

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Page 1: 2 Stability Analysis

Push In

Basal Heave

Overall Shear Failure

Overall shear failure modes:

Stability Analysis

Page 2: 2 Stability Analysis

Overall Shear Failure Mode: PUSH-IN

failure surface

{strut

wall

settlement

wall bottom "kick out"

It is mainly due to the unbalance between passive earth

pressure (inside) and active earth pressure (outside)

Page 3: 2 Stability Analysis

Strut settlement

failure surface

bottom heave

Overall Shear Failure Mode: BASAL HEAVE

It is mainly due to

bearing capacity of the

soil beneath the

excavation bottom

Page 4: 2 Stability Analysis

pp

aL

pL

sM

pP

strut

ap

aP

ANALYSIS OF PUSH-IN

The factor of safety against push-in:

aa

spp

d

rp

LP

MLP

M

MF

+==

Page 5: 2 Stability Analysis

Distribution of earth pressures for cohesive soil:

(4.16)

(4.17)

(4.18)

(4.19)

acava cKK 2-= ss

)1(c

cKK

w

aac+=

pcpvp cKK 2+= ss

)1(c

cKK w

ppc+=

Page 6: 2 Stability Analysis

(5.6)

Cast-in-place pile

API

0.0 0.2 0.4 0.6 0.8 1.00.0

0.2

0.4

0.6

0.8

1.0

1.2

a

vu /s s

FIGURE 4.12 Relation between adhesion and undrained shear

strength of clay

uwsc a=

Page 7: 2 Stability Analysis

Factor of safety

(Diaphragm walls)

(Steel sheet piles)

=1.2~1.3

Cohesionless soil(sandy, gravel)

Distribution of water pressures :

Gross water pressure distribution ?

Net water pressure distribution?

uw sc 67.0=

uw sc 5.0=

pF

Page 8: 2 Stability Analysis

(a) (b)

fu fu

Strut

Strut

id

jd

FIGURE 5.7 Distribution of water pressure due to seepage (a)

distribution of water pressure (b) net water pressure

(note: = water pressure due to seepage)f

u

Page 9: 2 Stability Analysis

Cohesionless soil(sandy, gravel)

Distribution of earth pressures:Caquot-Kerisel's or Coulomb's active earth pressure should be adopted

for the active earth pressure.

Caquot-Kerisel's passive earth pressure should be adopted for the

passive earth pressure. When , Coulomb's passive earth

pressure coefficient is quite close.

Caquot-Kerisel's earth pressure theory's , and have

some relationship. Section 4.5.3 has summarized some findings on

values of .

Clough's research:concluded that between concrete (cast in steel

mold) and sand, is about .

2/fd <

aK pK d

d

d f0.8

Page 10: 2 Stability Analysis

0.0

0.2

0.4

0.6

0.8

1.0

0.8 1.0 1.2 1.4 1.6 1.8

pF

eH(%

)/

eH

FIGURE 5.8 Factors of safety against push-in for excavations in

sand (all cases are safe cases; is assumed)

hm

d

hmd

hmd

fd =

Page 11: 2 Stability Analysis

Conclusion:

Assumption that seems to be reasonable.

For conservative reason, we usually assume

=0.5

=1.2~1.3

=d

pF

d f

f

Page 12: 2 Stability Analysis

(a)

Strut

(b)

anL

pnL

pnP

anP

sM

FIGURE 5 . 9 Analysis of- push in by the net pressure method ( a ) distribution of net earth pressure

( b ) force equilibrium of the retaining wall as a free body

Page 13: 2 Stability Analysis

The analyses of the basal heave failure are only applicable to clayey

soils.

Like Terzaghi, Bjerrum and Eide,

Tschebotarioff, Terzaghi and Peck,

Clough and O'Rourke, etc.

But the most commonly applied of which are Terzaghi's method,

Bjerrum and Eide, and the slip circle method.

ANALYSIS OF BASAL HEAVE

Page 14: 2 Stability Analysis

(1) Bearing capacity method (modified Terzaghi’s method)

(a) (b)

(c) (d)

d

a b c

a b c a b c

a b c

d

d d

2/1

BB =2/

1BB =

1BB 1B

1B1B

o45

eH

o45

FIGURE 5.10 Analysis of push-in by bearing capacity method

(a) a wide trial failure surface

(b) a second wide trial failure surface

(c) a third wide trial failure surface

(d) both sides of the excavation produce failure surfaces

1B

1B

1B

Page 15: 2 Stability Analysis

FIGURE 5.11 Excavation profile of the assumed excavation case

X

2.5m

eH

62.19=satg 3

m/kN

Page 16: 2 Stability Analysis

Bearing capacity method

Negative bearing capacity method

Slip circle method (side strength neglected)

Slip circle method (side strength considered)

0 1 2 3 40

1

2

3

eHX

Fb

)/25(2

mKNSu=

FIGURE 5.12 Relations between failure circle sizes and factors of safety against basal heave obtained by the bearing capacity method, negative bearing capacity

method, and the slip circle method

Page 17: 2 Stability Analysis

0 1 2 3 40

1

2

3

eHX

bF

Bearing capacity method

Negative bearing capacity method

Slip circle method (side strength neglected)

Slip circle method (side strength considered)

)3.0/( =vuS s

FIGURE 5 . 13 Relations between failure circle sizes and factors of safety

against basal heave obtained by the bearing capacity method ,

negative bearing capacity method , and the slip circle method

Page 18: 2 Stability Analysis

Terzaghi's method

Stiff soil

B

a b

c

d

1us

2us

2/B 2/B

2/B

sqsq

o45

eH

D

FIGURE 5.14 Analysis of basal heave using Terzaghi's method

2/)( BDa

Page 19: 2 Stability Analysis

When , the formation of a failure surface is not

restrained by the stiff soil.

Vertical plane bc can offer shear resistance and the

factor of safety against basal heave will be:

(5.7)

(5.8)

(5.9)

2/BD

2)()1)(( 1

BqHBqHW sese

+=×+= gg

2)7.5()1(7.5 212

BsBsQ uuu

=×=

euHs

1

euse

u

eu

ub

HsBqH

Bs

HsW

QF

1

2

1 2/)(

2/7.5

-+=

-=

g

Page 20: 2 Stability Analysis

D

D

B

D

1us

2us

sqsq

DeH

2/)( BDb <

Stiff soil

FIGURE 5.14 Analysis of basal heave using Terzaghi's method

2/)( BDb <

Page 21: 2 Stability Analysis

When , the failure surface will be restrained by the stiff soil.

(5.10)

Clough suggested that, Terzaghi's factor of safety should be

greater than or equal to 1.5.

2/BD <

)(b

F

euse

u

eu

ub

HsDqH

Ds

HsW

QF

1

2

1 )(

7.5

-+=

-=

g

Page 22: 2 Stability Analysis

B 1B

(a)

Bd

a b c

(b)

FIGURE 5.15 Relation between the embedded part of the retaining wall and the failure surface

(a) large penetration depth (b) small penetration depth

d

a b

90 °

90 °

eH

e

eH

Page 23: 2 Stability Analysis

(2) Negative bearing capacity method (modified Bjerrem and Eide’s method)

1B1B

B

Assumed failure surface

(a) (b)

(c)

sqsq sqsq

eH

eH

12 B

12 B

sq

eH

sq

FIGURE 5.16 Analysis of basal heave by negative bearing capacity method (a) a wide failure

surface (b) another wide failure surface (c) Failure surface covers the whole

excavation bottom

12B

12B

Page 24: 2 Stability Analysis

FIGURE 5.11 Excavation profile of the assumed excavation case

X

2.5m

eH

62.19=satg 3

m/kN

Page 25: 2 Stability Analysis

Bearing capacity method

Negative bearing capacity method

Slip circle method (side strength neglected)

Slip circle method (side strength considered)

0 1 2 3 40

1

2

3

eHX

F b

FIGURE 5.12 Relations between failure circle sizes and factors of safety against basal heave obtained by the bearing capacity method, negative bearing capacity

method, and the slip circle method )/25(

2

mKNSu=

Page 26: 2 Stability Analysis

0 1 2 3 40

1

2

3

eHX

bF

Bearing capacity method

Negative bearing capacity method

Slip circle method (side strength neglected)

Slip circle method (side strength considered)

)3.0/( =vuS s

FIGURE 5 . 13 Relations between failure circle sizes and factors of safety

against basal heave obtained by the bearing capacity method , negative bearing capacity method , and the slip circle method

Page 27: 2 Stability Analysis

sq

eH

sq

FIGURE 5.16c

Bjerrum and Eide's method

(5.12) se

uc

bqH

sNF

×=

g

Page 28: 2 Stability Analysis

0 1 2 3 4 54

5

6

7

8

9

1=BL

23

BHe

cN

FIGURE 5.17 Skempton's bearing capacity factor

(rectangular) (square)= (5.11) cNcN )16.084.0(

L

B+

Page 29: 2 Stability Analysis

Modified Bjerrum and Eide's method:

(5.13)

(5.14)

e

sdscu

bH

ffNsF

g

,1=

L

Bf s 2.01 +=

Page 30: 2 Stability Analysis

D 10

9

8

7

6

5.53

2.62.42.22.01.81.61.41.2

1.00.80.60.40.25.53

5

4

3

2

1

0

0.2

0.3

0.40.5

Nc,s

12 uu ss

12 uu ss

BD /

BD /

Nc,s

112<

uu ss 112>

uu ss

undrained shear strength profile

eH

u1s

u2s

B

1

2

(a) for failure circles passing two soil layersN c,s

Page 31: 2 Stability Analysis

If / exceeds the values in the figure, the failure circle

will be tangent to the top of the lower soil layer.

Nc,s

5

10

20

30

40

50

0.7 0.6 0.5 0.4 0.3 0.2 0.1 0

3.02.5

2.01.45

1.251.2

BD

Nc,s

12 uu ss

(b) for failure circles tangent to the top of the lower soil layer

Page 32: 2 Stability Analysis

DM7.2 suggested that Bjerrum and Eide's factor of safety

should be greater than or equal to 1.5.

FIGURE 5.18 Extended Bjerrum and Eide's method

(a) for failure circles passing two soil layers

(b) for failure circles tangent to the top of the lower soil layer

(c) width modification factorNc,s

df

df

(c)

0 1 2 3 4 5 61.0

1.1

1.2

1.3

1.4

1.5

BH e /

Nc,s

bF

Page 33: 2 Stability Analysis

(3) Slip circle method

O

W

r

us

Lowest level of struts

A

B

FIGURE 5.19 Location of the center of a failure circle for the slip circle method

Page 34: 2 Stability Analysis

(5.15)

X

O

ab

d f

e c

(a)

W

OsM

(b)

Lowest level of struts

N

N

N N

N

N

N

us

us

X

s

g

s

d

a

FIGURE 5.20 Analysis of basal heave by the slip circle method

(a) the failure surface (b) balance of the a free body

2

)(2

0

XW

MdXsX

M

MF

su

d

r

b

×

+

==

+ap

Page 35: 2 Stability Analysis

Bearing capacity method

Negative bearing capacity method

Slip circle method (side strength neglected)

Slip circle method (side strength considered)

0 1 2 3 40

1

2

3

eHX

bF

FIGURE 5.12 Relations between failure circle sizes and factors of safety against basal heave obtained by the bearing capacity method, negative bearing capacity

method, and the slip circle method )/25(

2

mKNSu=

Page 36: 2 Stability Analysis

FIGURE 5.13 Relations between failure circle sizes and factors of safety against basal heave obtained by the bearing capacity method,

negative bearing capacity method, and the slip circle method

)3.0/( =vuS s

0 1 2 3 40

1

2

3

eHX

bF

Bearing capacity method

Negative bearing capacity method

Slip circle method (side strength neglected)

Slip circle method (side strength considered)

Page 37: 2 Stability Analysis

Lowest level

of struts

FIGURE 5.21 Factor of safety increasing due to the failure circle exceeding

the excavation width

Page 38: 2 Stability Analysis

Lowest level of struts

u1s

u2s

u2u1 SS >

FIGURE 5.22 Analysis of basal heave in layered soft soils

Page 39: 2 Stability Analysis

Bearing capacity method

Negative bearing capacity method

Slip circle method (side strength neglected)

Slip circle method (side strength considered)

0 1 2 3 40

1

2

3

eHX

bF

FIGURE 5.12 Relations between failure circle sizes and factors of safety against basal heave obtained by the bearing capacity method, negative bearing capacity

method, and the slip circle method )/25(

2

mKNSu=

Page 40: 2 Stability Analysis

0 1 2 3 40

1

2

3

eHX

bF

Bearing capacity method

Negative bearing capacity method

Slip circle method (side strength neglected)

Slip circle method (side strength considered)

)3.0/( =vuS s

FIGURE 5 . 13 Relations between failure circle sizes and factors of safety

against basal heave obtained by the bearing capacity method , negative bearing capacity method , and the slip circle method

Page 41: 2 Stability Analysis

(5) Applicability to sandy soils

B

a b

c

d

1us

2us

2/B2/B

2/B

sqsq

o45

eH

D

Stiff soil

2/)( BDa

Page 42: 2 Stability Analysis

D

D

B

DStiff soil

1us

2us

sqsq

DeH

FIGURE 5.14 Analysis of basal heave using Terzaghi's method

2/)( BDb <

Page 43: 2 Stability Analysis

X

O

ab

d f

e c

(a)

W

OsM

(b)

Lowest level of struts

N

N

N N

N

N

N

us

us

X

s

g

s

d

a

FIGURE 5.20 Analysis of basal heave by the slip circle method

(a) the failure surface (b) balance of the a free body

Page 44: 2 Stability Analysis

北投自強路 excavation failure case

Page 45: 2 Stability Analysis

5.5.3 Case Study of Overall Shear Failure

The excavation case was located in Taipei. The width of the

excavation was 17.6m; the length was 100.1m ;the depth was

13.45m. The excavation adopted a 70cm thick , 34, deep

diaphragm wall as the retaining wall. There four levels of struts

and the excavation was carried out in 5 stages.

Page 46: 2 Stability Analysis

力霸百老匯excavation failure

Page 47: 2 Stability Analysis

力霸百老匯 excavation failure case

Page 48: 2 Stability Analysis

SM

OL-ML

SP-SM

CL

¡E

GL-4.5 m

GL-8.7 m

GL-10.7 m

GL-13.45 m

GL-2.8 m

GL-10.15 m

GL-24.0 m

14.7 2m/kN

FIGURE 5.23 Stability analysis of an excavation case history

(a) excavation and geological profiles

o18=uf

2/7.16 mkNcu

=

3/8.18 mkNt

=g

0=c

3/7.19 mkNt

=g

o10=uf

2/98.0 mkNcu

=

3/6.15 mkNt

=g

o33=f0=c

3/3.20 mkNt

=g

o32=f

Page 49: 2 Stability Analysis

and

will be 1.5

will be 2.3

were the total stress strength parameters of the clay soils,

obtained from the triaxial CU test

adopt by the original designer

We assume the soil below the lowest level of struts (GL-10.15 m)

to be a clayey layer, the adhesion between the retraining wall and

the soil

and the normalized undrained shear strength

(4.16)

(4.18)

pF

bF

3/2 uw sc =

22.0/ =vus s

acava cKK 2-= ss

pcpvp cKK 2+= ss

ucuf

Page 50: 2 Stability Analysis

At the depth of GL-10.15 m

2/5.18545.17.192.46.155.43.20 mkNv

=×+×+×=s

2/1.7281.9)8.215.10( mkNu =×-=

2/3.113 mkNuvv

=-= ss

2/9.243.11322.022.0 mkNs vu

=×== s

2

, /2.1213

21)9.24(25.185)1(2 mkN

s

cKsK

u

wauavah

=+-=+-= ss

Page 51: 2 Stability Analysis

At the depth of GL-13.45 m

Before excavation─

after excavation was started, on the passive side, but

value stayed unchanged.

Thus,

2/0.24875.28.1855.07.195.185 mkNv

=×+×+=s

2/5.10481.9)8.245.13( mkNu =×-=

2/5.143 mkNuvv

=-= ss

2/6.315.14322.022.0 mkNs vu

=×== s

0=vs us

2

, /5.813

21)6.31(20)1(2 mkN

s

cKsK

u

wpupvph

=++=++= ss

Page 52: 2 Stability Analysis

At the depth of GL-24.0 m

The active side─2

/3.44655.108.180.248 mkNv=×+=s

2/0.20881.9)8.224( mkNu =×-=

2/3.238 mkNuvv

=-= ss

2/4.523.23822.022.0 mkNs vu

=×== s

2

, /0.3113

21)4.52(23.446)1(2 mkN

s

cKsK

u

wauavah

=+-=+-=ss

Page 53: 2 Stability Analysis

At the depth of GL-24.0 m

The passive side─

After excavation was start stayed constant,us2

/3.198)45.130.24(8.18 mkNv=-×=s

2

, /6.3333

21)4.52(23.198)1(2 mkN

s

cKsK

u

wpupvph

=++=++= ss

Page 54: 2 Stability Analysis

The factor of safety against push-in as

(b)

81.5

121.2

311.0333.62

mkN

2mkN

2mkN

2mkN

GL-10.15 m

GL-13.45 m

GL-24.0 m

FIGURE 5.23 Stability analysis of an excavation case history

(b) distribution of earth pressure for the push-in analysis

89.03/285.135.085.13)2.1210.311(2/85.1385.132.121

)3.33/255.10(5.055.10)5.816.333()3.32/55.10(55.105.81=

××××-+××

+××××-++××=pF

Page 55: 2 Stability Analysis

Compute the factor of safety against basal heave

according to Slip circle method :Similarly, assuming the soil below the lowest level of

struts is clay, the average value of the undrained shear

strengths (the active side) of the soil between GL-10.15 m

and GL-24.0 m would be

The average value of the undrained shear strengths of

the soil between GL-13.45 m and GL-24.0 m would be

2

, /7.382

4.529.24mkNs au

=+

=

2

, /0.422

4.526.31mkNs pu

=+

=

Page 56: 2 Stability Analysis

The radius of the failure circular arc would be

The central angle of the failure circular arc on the active side

would be

The central angle of the failure circular arc on the passive

side would be

The factor of safety against circular arc failure would be

m85.1315.1024 =-

57.12==

p

33.1)85.13

3.3(cos

1 == -

94.023786

22370

2/85.1385.13

85.137.3857.185.1385.130.4233.185.13

)45.13(

==+×

=-GLv

bFs

× × × × ×

××

Page 57: 2 Stability Analysis

Computing the factor of safety against basal heave

following Terzaghi's method:

The width of the excavation , was larger than the

penetration depth (10.55 m). Assumed failure surface will pass below the

bottom of the retaining wall.

Bd

a b c

(b)

90°

eH

FIGURE 5.15 Relation between the embedded part of the retaining wall and the failure surface

(b) small penetration depth

mB 6.17= 2/B

Page 58: 2 Stability Analysis

The average undrained shear strength of soil within the range of

the failure circle can be calculated as follows:

of soil deep below the ground surface--mB 9.252/45.13 =+

2/1.482)45.1390.25(8.180.248 mkNv

=-+=s ×

2/5.25581.9)8.290.25(1.482 mkNuvv

=--=-= ss ×

2/2.565.25522.022.0 mkNs vu

=== s ×

Page 59: 2 Stability Analysis

The average undrained shear strength within the range of the

failure circle would be

As computed earlier, the total stress outside the excavation zone

at the depth equaling the excavation surface would be

2/9.432/)2.566.31( mkNsu

=+=

2/0.248 mkNv

=s

Page 60: 2 Stability Analysis

To simplify the analysis and be conservative, we assume the

soil above the excavation surface is clay and has soil shear

strength expressed as . The average undrained shear

strength of the soil outside the excavation zone and the excavation

surface would be

The factor of safety according to Terzaghi's method would be

22.0/ =vus s

2)45.13(/8.15

2

6.31

2

22.0mkNs

GLv

u==

=

-s

08.12874

3118

45.138.152/6.170.248

2/6.179.437.5

1

==-

=-

=eu

u

bHsW

QF

× ×

× ×

Page 61: 2 Stability Analysis

The factor of safety following Bjerrum and Eide's method would be

10.10.248

2.69.43==

+=

se

cub

qH

NsF

g

×

Page 62: 2 Stability Analysis

Undrained shear strength and the depth:

)(2mkN

Active side ),( uuc f

0.22/ =vus s

Passive side ),(uuc f

(c)

FIGURE 5.23 Stability analysis of an excavation case history

(c) the undrained shear strength used in the analysis

25

2

0

15

10

5

00 50 100 150 200

dept

h(m

)

us

Page 63: 2 Stability Analysis

【Example 5.1】Assume a 9.0 m deep excavation in a sandy

ground and the lowest level of struts is 2.5m above the

excavation surface. The level of groundwater outside the

excavation zone is ground surface high while that within the

excavation zone is as high as the excavation surface. The

unit weight of saturated sandy soils , the

effective cohesion and the effective angle of friction

. Because of the difference between the levels of

groundwater , seepage will occur. Assume that the friction

angles ( ) between the retaining wall and soil on both the

active and passive sides are and the factor of safety

against push-in, . Compute the required penetration

depth( ).

20=satg 3

m/kN

o30=f

0=c

d

f5.05.1=

pF

pH

Page 64: 2 Stability Analysis

jd

id

x

x

a

b

ccu

wjep dHH g)( -+

(a)

bu

(b)

FIGURE 4.22 Simplified analysis method for seepage

(a) distribution of water pressure (b) net water pressure

z

z

wip dH g)( -

eH

pH

Page 65: 2 Stability Analysis

1.determine the coefficient of the earth presure

Compute both the active and passive earth pressures following

Caquot-Kerisel's earth pressure theory. When , the

coefficients of active and passive earth pressure can be found from

Figure 4.9 and Figure 4.10 to be 0.3 and 4.6 separately. Thus, the

coefficients of the horizontal active and passive earth pressure

would be

【Solution】

f=d 5.0

29.05.0cos3.0cos3.0,=== fd

haK

4.45.0cos6.4cos6.4,=== fd

hpK

Page 66: 2 Stability Analysis

2. Compute the effective active active earth pressure on the wall

According to Eq. 4.51the porewater pressure at x away from upstream

water level would be

At the lowest level of strut (z=6.5m, x=6.5m) --

havha K ,,ss = 2

kN/m1305.620 ==vs ×

5.4

77.63

92

81.95.62

2

)(2

+=

+=

--+

-=

p

p

p

p

jiep

wip

H

H

H

H

ddHH

dHxu

g × × ×

5.4

49.187.3729.0)

5.4

77.63130()( ,,

+-=

+-=-=

p

p

P

p

hahaH

H

H

HKuss ×

Page 67: 2 Stability Analysis

At the bottom of the retaining wall( , )─pHz +=9 pHx +=9

)5.4

60.2584.28.52.52(

29.0)5.4

29.8881.920180(

2

2

,

+

+-+=

×+

+-+=

p

pp

p

p

pp

pha

H

HHH

H

HHHs

ppv HH 20180)9(20 +=+=s ×

5.4

29.8881.9

92

81.9)9(2

2

)(22

+

+=

+

+=

--+

-=

p

pp

p

pp

jiep

wip

H

HH

H

HH

ddHH

dHxu

g × × ×

Page 68: 2 Stability Analysis

3. Compute the lateral effective passive earth pressure on the wall

At the bottom of the retaining wall( )─pHz =

ppv HH 2020 =×=s

5.4

29.8881.92

+

+=

p

pp

H

HHu

5.4

48.38816.4388

4.4)5.4

29.8881.920(

2

2

,

+

+-=

×+

+-=

p

pp

p

p

pp

php

H

HHH

H

HHHs

Page 69: 2 Stability Analysis

4. Compute the maximum net water pressure (at the

excavation surface)

According to Eq. 4.53, the maximum net water pressure

would be

5.4

29.88

92

81.992

2

))((2

+=

+

×××

=--+

--+=

p

p

p

p

jiep

wipjie

bH

H

H

H

ddHH

dHddHu

g

Page 70: 2 Stability Analysis

5. The effective earth pressure on both sides of the wall and the

distribution of the net water pressure are as shown in Figure

5.24

Lowest level

of struts

FIGURE 5.24 Distribution of lateral earth pressure

o

b

2.5

9

pH

bu9

5.6 bu

netu

hp ,s

ha,s

5.4

48.38816.4388

2

+

+-

p

pp

pH

HHH

5.4

60.2584.28.52.52

2

+

+-+

p

pp

pH

HHH

5.4

49.187.37

+-

p

p

H

H

Page 71: 2 Stability Analysis

6. Compute the driving moment ( ) and the resistant moment

( ) for the free body below the lowest level of strutsrM

dM

bppp

p

pp

p

bbppb

p

p

pp

p

p

p

p

ahad

uHHHH

HHH

uuHHu

H

H

HHH

H

H

H

LPM

]84.225.117.0[)5.2)(5.4

62.1195.093.168.23(

32

5.22

9

5.2

2

5.2

9

5.6)

35.2(

2

32

)5.2(2)

5.4

11.784.28.55.14(

2

)5.2()

5.4

49.187.37(

22

2

22

222

,

+++++

+-+=

×

××+×++×+

×

+

+-++

+-=

=

bppp

p

pp

p

bbppb

p

p

pp

p

p

p

p

ahad

uHHHH

HHH

uuHHu

H

H

HHH

H

H

H

LPM

]84.225.117.0[)5.2)(5.4

62.1195.093.168.23(

32

5.22

9

5.2

2

5.2

9

5.6)

35.2(

2

32

)5.2(2)

5.4

11.784.28.55.14(

2

)5.2()

5.4

49.187.37(

22

2

22

222

,

+++++

+-+=

×

××+×++×+

×

+

+-++

+-=

=

Page 72: 2 Stability Analysis

)3

25.2)(

5.4

24.19458.2144(

)3

25.2(

2)

5.4

48.38816.4388(

23

2

2

,

p

p

pp

p

pp

p

pp

p

phpr

H

H

HHH

HH

H

HHH

LPM

++

+-=

+××

+

+-=

=

Page 73: 2 Stability Analysis

7. determine the penetration depth

Then we have m

pH

5.1==

d

rp

M

MF

25.7=pH

Page 74: 2 Stability Analysis

【Example 5.2】An excavation in clay goes 9.0m in to the

ground . The groundwater outside the

excavation zone is at the ground surface level while

that within the excavation zone is at the level of the

excavation surface. . The

undrained shear strength .

Suppose the excavation width B =10m and the

excavation length L =30m. Compute the factor of

safety against basal heave according to Terzaghi's

method and Bjerrum and Eide's method,

respectively.

=17.0

=45

9.0m)( =e

H

satg 3

m/kN

2m/kNus

Page 75: 2 Stability Analysis

【Solution】

In this example, the surcharge

According to Terzahi's method,

0=sq

7.2

107.0

4517

457.5

9

1

7.0

7.51=

×-

×=

-

××=

B

s

s

HF

u

u

e

b

g

Page 76: 2 Stability Analysis

According to Bjerrum and Eide's method,

According to Figure 5.17, we have

0.310

30==

B

L

9.010

9==

B

He

1.7=cN

09.2917

1.745=

×

×==

et

cub

H

NsF

g

Page 77: 2 Stability Analysis

Upheaval

Impermeable layer

Permeable layerw

HWater pressure

1h

2h

1tg

2tg

The factor of safety against upheaval should be larger than or equal to 1.2

FIGURE 5.31 Analysis of upheaval

(5.17)

ww

iiti

upH

h

Fg

g

×

×

=

upF

Page 78: 2 Stability Analysis

(CL)

(ML)

(SM)

GL-0.0m

GL-8.0m

GL-25.0m

GL-32.5m

GL-36.0m

GL-40.5m

Grouting

Gravel

2.9m -Stage 1

5.9m -Stage 2

8.8m -Stage 311.9m -Stage 4

14.4m -Stage 5

17.5m -Stage 6

20.0m -Stage 722.5m -Stage 825.1m -Stage 9

27.55m -Stage 10

30.6m -Stage 11

(SF)

GL-58.5m GL-58.0m

GL-63.0m

33.7m -Stage 12

36.75m -Stage 13

40.5m -Stage 14

GL-10.0m(CL)

(SP-SM)GL-15.0m

(CL)

(SM)GL-43.0m

Case Study

ww

iiti

upH

h

Fg

g

×

×

=

ww

i

iti

upH

h

Fg

g

=

Upheaval failure:

Page 79: 2 Stability Analysis

1H

2H

z

Upward water flow

u

0

Saturated soil

A

C

B

2H

hzh

FIGURE 5.32 Total stresses, effective stresses, and change of porewater pressure in

sandy soils acted on by an upward water flow

wH g1 wH g

1

satw HH gg21

+whHH g)( 21

++whH gg -

2

s s

Sand Boiling --- Factor of safety and failure mechanism

Page 80: 2 Stability Analysis

The critical hydraulic gradient is then

Besides, according to the phase relationship of soil, the

submerged unit weight is

(5.24)

(5.25)

-w

s

e

Ggg |

+

=1

1

e

Gi

s

cr+

-=

1

1

)max(exit

crs

i

iF = (5.26)

Page 81: 2 Stability Analysis

(5.26)

A

wHD

pH

FIGURE 5.33 Seepage in soil below sheetpiles

Impermeable layer

Wall

Sand boiling zone

)max(exit

cr

si

iF =

Page 82: 2 Stability Analysis

Terzaghi's method:

=(the volume of the soil column)

The factor of safety is

(5.27)

(5.28)

(5.29)

wavgpwaviHi gg 2

2

1)( =×

ggg =-= 22

2

1)(

2

1pwsatp HHW

wavg

siU

WF

g

g =

=

U

Page 83: 2 Stability Analysis

Provided the computed factor of safety is too small, we can

consider placing filters at the exits of seepage. Assuming the

weight of filters is Q, the factor of safety will be

(5.30)

In general, the required for the above equation should

be greater than of equal to 1.5sF

U

QWFs

+=

Page 84: 2 Stability Analysis

Marsland's method:

DM7.1 suggested that the reasonable factor of safety against piping

in an excavation be around 1.5 to 2.0.

Retaining wall

2.0

1.5

1.0

0.5

00.5 1.0 1.5 2.0

2.0

1.5

2.0

1.5

1.0

1.0sF

Loose sandDense sand

wH

PH

B

(a)

)2/(w

HB

wp

HH

/

FIGURE 5.34 Relations between wall penetration depths and factors of safety against sand boiling

(a) dense and loose sands with the impermeable layer located at the infinite depth

Page 85: 2 Stability Analysis

FIGURE 5.34 Relations between wall penetration depths and factors of safety against sand boiling

(b) dense sand with the impermeable layer located at a finite depth

2.0

1.5

1.0

0.5

00.5 1.0 1.5 2.0

2.0

1.5

1.01.0

2.0

1.5

wH

B

D

Impermeable layer

(b)

sF

PH

)2/( wHB

2=wHD

1=wHD

wp

HH

/

Page 86: 2 Stability Analysis

One dimension seepage method:

id

FIGURE 5.35 Analysis of sand boiling

wH

Sandy soil

a

bc

d

pH

eH

jd

D

Page 87: 2 Stability Analysis

The total head at the upstream elevation (point a) will be

The difference of the total heads between upstream and

downstream levels will be

If we assume the datum is at the downstream level, the total

head at the elevation of downstream (point d) will be

(5.31)

(5.32)

(5.33)

000,=+=+=

pedt hhh

jiejiepeat ddHddHhhh -+=+-+=+= 0,

jiedtatw ddHhhH -+=-=,,

D

Page 88: 2 Stability Analysis

Suppose the seepage is one dimensional and the hydraulic

gradients for each depth along the flow path abcd are equal. the

hydraulic gradient will be

The factor of safety against boiling will be

The required for the above equation should be greater than

or equal to 1.5.

jipe

w

ipije

wavg

ddHH

H

dHddH

Hi

--+=

-++-=

2)(2

DD

ww

jipe

avg

cs

H

ddHH

i

iF

Dg

g )2( --+==

sF

Page 89: 2 Stability Analysis

Case Study

FIGURE 5.36 Excavation of Siemen Station of Taipei Rapid Transit System

(a) excavation and geological profiles

SM

CL

SM

CL

SM

EL.+72.5m

EL.+69.4m

EL.+63.4m

EL.+59.6m

EL.+56.4m

Sungshan III formation

Sungshan II formation

. . .. . . .. . . .. . . . . ... .. . .. .... .. .... .

EL.+81.8m

EL.+87.2m

EL.+95.0m

EL.+104.5m

Sungshan IV formation

Sungshan VI formation

Groundwater level EL.+98.0mEL.+98.0m

CL

SM

CL

Chingmei formation

EL.+88.0m

EL.+80.0m

Sand boiling

23.25m

(a)

Sungshan V formation

Sungshan I formation

Page 90: 2 Stability Analysis

FIGURE 5.36 Excavation of Siemen Station of Taipei Rapid Transit System

(b) plan view

6.2m

5.0m

23.25m

sump

bore

Diaphragm wall

N

(b)

Page 91: 2 Stability Analysis

SM

CL

SM

CL

SM

EL.+80.0m

EL.+72.5m

EL.+69.4m

EL.+63.4m

EL.+59.6m

EL.+56.4m

Casing

5m 6m

4m

Sump

8m9m

. . . . . .

. .

. . . . . . . .. .. .. . . . .. . . . .

. .

. . . . .. . . .

(c)

. . . .

. .

FIGURE 5.36 Excavation of Siemen Station of Taipei Rapid Transit System

(c) process of sand boiling

Sungshan III

Sungshan I

Sungshan II

Page 92: 2 Stability Analysis

Marsland’s method {Fig. 5.34,1.5}(1, 5)

Terzaghi’s method {Eq. 5.30

assuming Ms=0}(1)

Overall shear failure

Push-in Basal heave

Gross pressure method

{Eq. 5.5, }(1)

Short term behaviors can

be ignored while long

term behaviors may need

consideration. The

analysis methods are the

same as those for sand

and gravel.

Sand boiling Upheaval

San

d o

r g

rav

e A

lter

nat

ed l

ayer

s of

sand

(or

gra

vel

) an

d c

lay

Cla

y ˍˍ

ˍˍ ˍˍ

ˍˍ

TABLE 5.2 Stability analysis methods for strutted walls and the required minimum factors of safety

Gross pressure method

{Eq.5.5, 1.2,

Harza’s method {Eq. 5.26,

2.0}(4)

1.5~2.0}(4)

}(1, 5)

Simplified 1-D seepage

method {Eq. 5.35,

Terzaghi’s method

Bjerrum and Eide’s

Slip circle method {Eq. 5.15,

}(1)

Gross pressure method

{Eq. 5.5, }(1)

assuming Ms=0}(1)

assuming Ms=0}(1)

Terzaghi’s method {Eq. 5.9 or

5.10, }(1,2,3)

Bjerrum and Eide’s method{Eq.

5.12 or 5.13, }(4,3)

Slip circle method {Eq. 5.15,

}(1,3)

{Eq. 5.17, Fup≧1.2}(1)

pF

sF

sF

sF

0.2sF

2.1bF

2.1pF

2.1pF

5.1bF

2.1bF

2.1bF

Page 93: 2 Stability Analysis

NOTE:

(1) The methods and factors of safety are suggested by TGS (2001)

and JSA (1988)

(2) The factor of safety is suggested by Mana and Clough (1981)

(3) It is only when clay is the dominant soil layer that the analysis of

basal heave is required

(4) The factor of safety is suggested by NAVFAC DM 7.1 (1982)

(5) TGS (2001) and JSA (1988) suggest the conservative value

obtained by Terzaghi's method or the simplified 1-D seepage be

adopted for design.