14.330 Effective Stress - Faculty Server...

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Slide 1 of 28 Revised 02/2013 14.330 SOIL MECHANICS Effective Stress EFFECTIVE STRESS CONCEPT NO SEEPAGE Saturated Soil Column (Figure 6.1. Das FGE (2005)) sat A w H H H ) ( from Water from Soil Where: w = Unit Weight of Water sat = Saturated Unit Weight of Soil H = Height of water above Soil H A = Depth of Point A below water table Total Stress () at Point A

Transcript of 14.330 Effective Stress - Faculty Server...

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Slide 1 of 28Revised 02/2013

14.330 SOIL MECHANICSEffective Stress

EFFECTIVE STRESS CONCEPTNO SEEPAGE

Saturated Soil Column (Figure 6.1. Das FGE (2005))

satAw HHH )(

from Water from Soil

Where:w = Unit Weight of Watersat = Saturated Unit Weight of

Soil H = Height of water above SoilHA = Depth of Point A below

water table

Total Stress () at Point A

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Slide 2 of 28Revised 02/2013

14.330 SOIL MECHANICSEffective Stress

1.Portion carried by water in void spaces. THIS IS THE PORE PRESSURE (u).

2. Portion carried by soil solids at points of contact. THIS IS THE EFFECTIVE STRESS (´).

Saturated Soil Column (Figure 6.1. Das FGE (2005))

EFFECTIVE STRESS CONCEPTNO SEEPAGE

Total Stress ()can be divided into 2 Parts:

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Slide 3 of 28Revised 02/2013

14.330 SOIL MECHANICSEffective Stress

Forces acting at Soil Particle Points of Contact at level of Point A (i.e. along Line a-a)

Figure 6.1. Das FGE (2005)

APPPP vnvvv )()(3)(2)(1 ...

Effective Stress (´) alongLine a-a

Saturated Soil Column (Figure 6.1. Das FGE (2005))

EFFECTIVE STRESS CONCEPTNO SEEPAGE

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Slide 4 of 28Revised 02/2013

14.330 SOIL MECHANICSEffective Stress

Forces acting at Soil Particle Points of Contact at level of Point A

(i.e. along Line a-a)Figure 6.1. Das FGE (2005)

APPPP vnvvv )()(3)(2)(1 ...

Effective Stress (´) along Line a-a

Where:P1(v) = Vertical Component of P1

A = Cross-sectional Area of Soil Mass Under Consideration

EFFECTIVE STRESS CONCEPTNO SEEPAGE

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Slide 5 of 28Revised 02/2013

14.330 SOIL MECHANICSEffective Stress

Forces acting at Soil Particle Points of Contact at level of Point A

(i.e. along Line a-a)Figure 6.1. Das FGE (2005).

)1()(

ss au

AaAu

Total Stress () along Line a-a

Where:as = Cross-section Area of Soil

Contacts = a1+a2+a3+…+an

A = Cross-sectional Area of SoilMass Under Consideration

a´s = as/A = Fraction of unit cross-sectional area of soil massoccupied by solid to solidcontacts.

EFFECTIVE STRESS CONCEPTNO SEEPAGE

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Slide 6 of 28Revised 02/2013

14.330 SOIL MECHANICSEffective Stress

)1()(

ss au

AaAu

Total Stress () along Line a-a

a´s ≈ 0 (i.e. very small), so therefore:

uu THE EFFECTIVE STRESS

EQUATION

or

EFFECTIVE STRESS CONCEPTNO SEEPAGE

Figure 6.1. Das FGE (2005)

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Slide 7 of 28Revised 02/2013

14.330 SOIL MECHANICSEffective Stress

wAsatAw HHHHu

)(

THE EFFECTIVE STRESSEQUATION

u = Pore Pressure = Total Stress

)( wsat

))((' wsatA HH

´ = Submerged unitweight of soilHeight of soil column

EFFECTIVE STRESS CONCEPTNO SEEPAGE

Figure 6.1. Das FGE (2005)

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Slide 8 of 28Revised 02/2013

14.330 SOIL MECHANICSEffective Stress

GIVEN SOIL PROFILE (NTS):

SMsat = 115 lb/ft3

CL = 102 lb/ft3sat = 105 lb/ft3

A

B

C

D

5ft9ft

12ft

6ft

FIND:

Total and Effective Stressesat Pts. A, B, C, & D.

EFFECTIVE STRESS CONCEPTNO SEEPAGE: EXAMPLE PROBLEM

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Slide 9 of 28Revised 02/2013

14.330 SOIL MECHANICSEffective Stress

GIVEN SOIL PROFILE (NTS):

SMsat = 115 lb/ft3

CL = 102 lb/ft3sat = 105 lb/ft3

A

B

C

D

5ft9ft

12ft

6ft

FIND:

Total and Effective Stressesat Pts. A, B, C, & D.

A CL ZA 102 lbft3 (5 ft)

A 510 lbft2

A A uA

uA 0

A A 510 lbft2

@ Point A:

EFFECTIVE STRESS CONCEPTNO SEEPAGE: EXAMPLE PROBLEM

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Slide 10 of 28Revised 02/2013

14.330 SOIL MECHANICSEffective Stress

B A ( sat,CLX4 ft)

B 510 lbft3 105 lb

ft3 (4 ft)

B 930 lbft2

B B uB

uB w 4 ft 62.4 lbft3 4 ft 250 lb

ft2

B B uB 930 lbft 2 250 lb

ft2

B 680 lbft2

@ Point B:GIVEN SOIL PROFILE (NTS):

SMsat = 115 lb/ft3

CL = 102 lb/ft3sat = 105 lb/ft3

A

B

C

D

5ft9ft

12ft

6ft

EFFECTIVE STRESS CONCEPTNO SEEPAGE: EXAMPLE PROBLEM

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Slide 11 of 28Revised 02/2013

14.330 SOIL MECHANICSEffective Stress

C B ( sat,SM 6 ft)

C 930 lbft3 115 lb

ft3 (6 ft)

C 1620 lbft2

C C uC

uC w 10 ft 62.4 lbft3 10 ft 624 lb

ft2

C C uC 1620 lbft2 624 lb

ft2

C 996 lbft2

C 1000 lbft2 (round to nearest 5 psf)

@ Point C:GIVEN SOIL PROFILE (NTS):

SMsat = 115 lb/ft3

CL = 102 lb/ft3sat = 105 lb/ft3

A

B

C

D

5ft9ft

12ft

6ft

EFFECTIVE STRESS CONCEPTNO SEEPAGE: EXAMPLE PROBLEM

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14.330 SOIL MECHANICSEffective Stress

D B ( sat,SM 12 ft)

D 930 lbft3 115 lb

ft3 (12 ft)

D 2310 lbft2

D D uD

uD w 16 ft 62.4 lbft3 16 ft 998 lb

ft2

D D uD 2310 lbft2 998 lb

ft2

D 1312 lbft2

D 1310 lbft2 (round to nearest 5 psf)

@ Point D:GIVEN SOIL PROFILE (NTS):

SMsat = 115 lb/ft3

CL = 102 lb/ft3sat = 105 lb/ft3

A

B

C

D

5ft9ft

12ft

6ft

EFFECTIVE STRESS CONCEPTNO SEEPAGE: EXAMPLE PROBLEM

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Slide 13 of 28Revised 02/2013

14.330 SOIL MECHANICSEffective Stress

25

20

15

10

5

0

Dep

th fr

om E

xist

ing

Gro

und

Surf

ace

(ft)

0 2000

TOTAL STRESS()

25

20

15

10

5

0

25

20

15

10

5

0

A

B

C

D

0

510

930

1620

2310

0 200025

20

15

10

5

00 2000

PORE PRESSURE(u)

0 2000

0 2000

EFFECTIVE STRESS(')

0 200025

20

15

10

5

0

25

20

15

10

5

0

25

20

15

10

5

0

25

20

15

10

5

0

Depth

fromExisting

Ground Surface (ft)

0

250

624

998

0

510

680

996

1312

CL = 102 pcfsat = 105 pcf

SMsat = 115 pcf

Use 1310

Use 1000

EFFECTIVE STRESS CONCEPTNO SEEPAGE: EXAMPLE PROBLEM

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Slide 14 of 28Revised 02/2013

14.330 SOIL MECHANICSEffective Stress

Figure 6.3a. Das FGE (2005).

01

1

AAA

wA

wA

uHuH

wB

wwsatB

wsatwB

BBB

wB

satwB

hHhH

hHHHHu

hHHuHH

2

2

2121

21

21

)()()(

)(

Stresses @ Point A:

Stresses @ Point B:

EFFECTIVE STRESS CONCEPTUPWARD SEEPAGE

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Slide 15 of 28Revised 02/2013

14.330 SOIL MECHANICSEffective Stress

Flow Waterof LengthHead in Change

2H

hi

wC

wwsatC

CCC

wC

satwC

zHhz

zHhz

u

zHhzHu

zH

2

2

21

1

)(

)(

Stresses @ Point C:

NOTE:

wC izz Figure 6.3a. Das FGE (2005).

EFFECTIVE STRESS CONCEPTUPWARD SEEPAGE

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14.330 SOIL MECHANICSEffective Stress

0 wcrC ziz

CRITICAL HYDRAULIC GRADIENT(icr)

For Most Soils:icr ranges from 0.9 to 1.1,

with an average of 1

wcri

NO EFFECTIVE STRESS!Known as Boiling or Quick Condition

Figure 6.3a. Das FGE (2005).

EFFECTIVE STRESS CONCEPTUPWARD SEEPAGE

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Slide 17 of 28Revised 02/2013

14.330 SOIL MECHANICSEffective Stress

Figure 6.3b. Das FGE (2005).

EFFECTIVE STRESS CONCEPTUPWARD SEEPAGE

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Slide 18 of 28Revised 02/2013

14.330 SOIL MECHANICSEffective Stress

Figure 6.4a. Das FGE (2005).

01

1

AAA

wA

wA

uHuH

wB

wwsatB

wsatwB

BBB

wB

satwB

hHhH

hHHHHu

hHHuHH

2

2

2121

21

21

)()()(

)(

Stresses @ Point B:

EFFECTIVE STRESS CONCEPTDOWNWARD SEEPAGE

Stresses @ Point A:

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Slide 19 of 28Revised 02/2013

14.330 SOIL MECHANICSEffective Stress

Flow Waterof LengthHead in Change

2H

hi

wC

wsatwC

CCC

wC

satwC

zHhz

zHhzHzH

u

zHhzHu

zH

2

211

21

1

)(

)(

Stresses @ Point C:

wC izz Figure 6.4a. Das FGE (2005).

EFFECTIVE STRESS CONCEPTDOWNWARD SEEPAGE

NOTE:

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Slide 20 of 28Revised 02/2013

14.330 SOIL MECHANICSEffective Stress

EFFECTIVE STRESS CONCEPTDOWNWARD SEEPAGE

Figure 6.4b. Das FGE (2005).

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Slide 21 of 28Revised 02/2013

14.330 SOIL MECHANICSEffective Stress

Figure 6.6. Das FGE (2005).

Where:ua = Pore Air Pressureuw = Pore Water Pressure = Fraction of unit cross-sectional

area of soil occupied by water. = 0 for dry soil; 1 for saturated soil.

depends on degree of saturation (S).Also influenced by soil structure.

)( waa uuu

EFFECTIVE STRESS CONCEPTPARTIALLY SATURATED SOIL

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Slide 22 of 28Revised 02/2013

14.330 SOIL MECHANICSEffective Stress

wc

wc

dTh

dThd

cos4

cos4

2

CAPILLARY RISE IN SOILS

Figure 8.19. Principles of Geotechnical Engineering, Das (2006).

Summing Forces in Vertical Direction

Where:T = Surface Tension = Angle of Contactd = Capillary Tube Diameter

dhc

1

T, , w remain constant

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Slide 23 of 28Revised 02/2013

14.330 SOIL MECHANICSEffective Stress

dhc

1

Figure 8.20. Principles of Geotechnical Engineering, Das (2006).

CAPILLARY RISE IN SOILS

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Slide 24 of 28Revised 02/2013

14.330 SOIL MECHANICSEffective Stress

101 eD

Ch

Where:D10 = Effective Size (mm)e = Void RatioC = Constant (ranging from

10 mm2 to 50 mm2)

Hazen (1930)

CAPILLARY RISE IN SOILS

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Slide 25 of 28Revised 02/2013

14.330 SOIL MECHANICSEffective Stress

whu

Soil TypeRange of Capillary Rise

m ftCoarse Sand 0.1 – 0.2 0.3 – 0.6

Fine Sand 0.3 – 1.2 1 – 4Silt 0.75 – 7.5 2.5 – 25

Clay 7.5 - 23 25 - 75

u

Table 8.2 (Das, PGE 2006). Approximate Range of Capillary Rise in Soils.

EFFECTIVE STRESS IN CAPILLARY ZONE

wShu

100

Saturated:

Partially Saturated:

CAPILLARY RISE IN SOILS

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Slide 26 of 28Revised 02/2013

14.330 SOIL MECHANICSEffective Stress

Figure 6.1. Das FGE (2005).

AzP

z

'

'

1

WITH NO SEEPAGE(i.e. STATIC CONDITIONS)

Effective Stress:

)( wsat

))((' wsatA HH

´ = Submerged unitweight of soil

Height of soil column = z

Effective Force:Where:

A = Area

SEEPAGE FORCE

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Slide 27 of 28Revised 02/2013

14.330 SOIL MECHANICSEffective Stress

z AzP 1AizzP w )('2 wizz

NO SEEPAGE:

EFFECTIVE STRESS EFFECTIVE FORCE

W/ SEEPAGE:

SEEPAGE FORCE PER UNIT VOLUME:

ww i

zAAizPP

Volume) Soil(

21

AizPP w 21

DECREASE OF TOTAL FORCE DUE TO SEEPAGE:

SEEPAGE FORCE: UPWARD SEEPAGE

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Slide 28 of 28Revised 02/2013

14.330 SOIL MECHANICSEffective Stress

NO SEEPAGE

UPWARD SEEPAGE

DOWNWARD SEEPAGE

SEEPAGE FORCE SUMMARY