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Geotechnical Engineeringโ€“II [CE-321]
BSc Civil Engineering โ€“ 5th Semester
by
Dr. Muhammad Irfan
Assistant Professor
Civil Engg. Dept. โ€“ UET Lahore
Email: mirfan1@msn.com
Lecture Handouts: https://groups.google.com/d/forum/geotech-ii_2015session
Lecture # 28
20-Dec-2017
2
SLOPE STABILITY ANALYSIS
Finite Slope (Swedish Slip Circle Method)
Assumptions:
1. Material of the slope is homogeneous.
2. Soil is purely cohesive in nature i.e. f = 0.
3. Failure surface has a curved/circular or spoon like surface.
4. Shear strength of the soil is uniformly distributed along
failure plane. (only possible if f = 0)
3
SLOPE STABILITY ANALYSIS
Swedish Slip Circle Method (Cohesive soils (f=0))
NSLC
A
B
๐น๐‘‚๐‘† =
๐‘…๐‘’๐‘ ๐‘–๐‘ ๐‘ก๐‘–๐‘›๐‘” ๐‘€๐‘œ๐‘š๐‘’๐‘›๐‘ก (๐‘€ ๐‘…)
๐ท๐‘–๐‘ ๐‘ก๐‘ข๐‘Ÿ๐‘๐‘–๐‘›๐‘” ๐‘€๐‘œ๐‘š๐‘’๐‘›๐‘ก (๐‘€ ๐ท)
4
NSLC
A
B
๐น๐‘‚๐‘† =
๐‘…๐‘’๐‘ ๐‘–๐‘ ๐‘ก๐‘–๐‘›๐‘” ๐‘€๐‘œ๐‘š๐‘’๐‘›๐‘ก (๐‘€ ๐‘…)
๐ท๐‘–๐‘ ๐‘ก๐‘ข๐‘Ÿ๐‘๐‘–๐‘›๐‘” ๐‘€๐‘œ๐‘š๐‘’๐‘›๐‘ก (๐‘€ ๐ท)
๐ท๐‘–๐‘ ๐‘ก๐‘ข๐‘Ÿ๐‘๐‘–๐‘›๐‘” ๐‘€๐‘œ๐‘š๐‘’๐‘›๐‘ก
๐‘€ ๐ท = ๐‘Š โˆ™ ๐‘ฅ
tr = c + sn tan f
For saturated clay under
undrained loading; f=0
๏œ tr = c = su
๐‘…๐‘’๐‘ ๐‘–๐‘ ๐‘ก๐‘–๐‘›๐‘” ๐‘€๐‘œ๐‘š๐‘’๐‘›๐‘ก
๐‘€ ๐‘… = ๐œ ๐‘Ÿ โˆ™ ๐ด๐ต โˆ™ ๐‘…
๐‘€ ๐‘… = ๐‘ โˆ™ (๐‘… โˆ™ ๐œƒ) โˆ™ ๐‘…
๐‘€ ๐‘… = ๐‘ โˆ™ ๐œƒ โˆ™ ๐‘…2
๐น๐‘‚๐‘† =
๐‘€ ๐‘…
๐‘€ ๐ท
๐น๐‘‚๐‘† =
๐‘ โˆ™ ๐œƒ โˆ™ ๐‘…2
๐‘Š โˆ™ ๐‘ฅ
SLOPE STABILITY ANALYSIS
Swedish Slip Circle Method (Cohesive soils (f=0))
Case-I: No Tension Crack
W
x
q
R
๐‘Š = (๐ด๐‘Ÿ๐‘’๐‘Ž ๐‘œ๐‘“ ๐ด๐ต๐ถ๐ด ร— 1) ร— ๐›พ
โ†’ q in radians
5
W
x
q
R
NSLC
A
B๐น๐‘‚๐‘† =
๐‘…๐‘’๐‘ ๐‘–๐‘ ๐‘ก๐‘–๐‘›๐‘” ๐‘€๐‘œ๐‘š๐‘’๐‘›๐‘ก (๐‘€ ๐‘…)
๐ท๐‘–๐‘ ๐‘ก๐‘ข๐‘Ÿ๐‘๐‘–๐‘›๐‘” ๐‘€๐‘œ๐‘š๐‘’๐‘›๐‘ก (๐‘€ ๐ท)
๐‘€ ๐ท = ๐‘Š โˆ™ ๐‘ฅ
tr = c + sn tan f
For saturated clay under
undrained loading; f=0
๏œ tr = c = su
๐‘€ ๐‘… = ๐‘ โˆ™ ๐œƒ2 โˆ™ ๐‘…2
๐น๐‘‚๐‘† =
๐‘€ ๐‘…
๐‘€ ๐ท
๐น๐‘‚๐‘† =
๐‘ โˆ™ ๐œƒ2 โˆ™ ๐‘…2
๐‘Š โˆ™ ๐‘ฅ
SLOPE STABILITY ANALYSIS
Swedish Slip Circle Method (Cohesive soils (f=0))
Case-II: Development of Tension Crack
โ„Ž ๐‘ก =
2๐‘
๐›พ ๐พ๐‘Ž
q2
FOS will reduce after development of tension crack [โˆต q2 < q]
๐ท๐‘–๐‘ ๐‘ก๐‘ข๐‘Ÿ๐‘๐‘–๐‘›๐‘” ๐‘€๐‘œ๐‘š๐‘’๐‘›๐‘ก
๐‘…๐‘’๐‘ ๐‘–๐‘ ๐‘ก๐‘–๐‘›๐‘” ๐‘€๐‘œ๐‘š๐‘’๐‘›๐‘ก
6
W
x
R
C
A
tr = c = su
SLOPE STABILITY ANALYSIS
Swedish Slip Circle Method (Cohesive soils (f=0))
Case-III: Tension Crack filled with water
โ„Ž ๐‘ก =
2๐‘
๐›พ ๐พ๐‘Ž
q2
๐›พwht
PW
h
2
3
โ„Ž ๐‘ก
๐‘ƒ ๐‘Š =
1
2
๐›พ ๐‘ค โˆ™ โ„Ž ๐‘ก
2
๐‘€ ๐ท = ๐‘Š โˆ™ ๐‘ฅ +
๐‘€ ๐‘… = ๐‘ โˆ™ ๐œƒ2 โˆ™ ๐‘…2
๐น๐‘‚๐‘† =
๐‘ โˆ™ ๐œƒ2 โˆ™ ๐‘…2
๐‘Š โˆ™ ๐‘ฅ +
1
2
๐›พ ๐‘ค โˆ™ โ„Ž ๐‘ก
2
โ„Ž +
2
3
โ„Ž ๐‘ก
FOS will reduce further when tension crack is filled with water
๐น๐‘‚๐‘† =
๐‘…๐‘’๐‘ ๐‘–๐‘ ๐‘ก๐‘–๐‘›๐‘” ๐‘€๐‘œ๐‘š๐‘’๐‘›๐‘ก (๐‘€ ๐‘…)
๐ท๐‘–๐‘ ๐‘ก๐‘ข๐‘Ÿ๐‘๐‘–๐‘›๐‘” ๐‘€๐‘œ๐‘š๐‘’๐‘›๐‘ก (๐‘€ ๐ท)
๐ท๐‘–๐‘ ๐‘ก๐‘ข๐‘Ÿ๐‘๐‘–๐‘›๐‘” ๐‘€๐‘œ๐‘š๐‘’๐‘›๐‘ก
๐‘…๐‘’๐‘ ๐‘–๐‘ ๐‘ก๐‘–๐‘›๐‘” ๐‘€๐‘œ๐‘š๐‘’๐‘›๐‘ก
1
2
๐›พ ๐‘ค โˆ™ โ„Ž ๐‘ก
2
โ„Ž +
2
3
โ„Ž ๐‘ก
7
Practice Problem #3
Determine the factor of safety of the cohesive slope shown in
the figure for the following two cases;
A. No tension crack
B. 2m deep tension crack filled with water (q1 = 38ยฐ)
NSLC
A
B
gb = 17.75 kN/m3
Cu above line AD = 21.5 kPa
Cu below line AD = 33.5 kPa
W
3.1m
q1=
40ยฐ
R
q2=
35ยฐ
D
Dโ€™
4m
2m
Area of ABCA
= 90m2
8
SLOPE STABILITY ANALYSIS
Ordinary Method of Slices (OMS) (c-f soils)
๏ฑ For c-f soils, normal stress would change along slip circle
๏ฑ Different normal stress means, shear resistance would also be
different (โˆต M-C equation)
๏ฑ Failing slope divided into slices
TR
Guidelines for Slice Selection
๏ฑ Slices do not have to be of equal
width
๏ฑ For convenience, base arc of each
slice should pass through one soil
type only
๏ฑ Slice width should be limited
(curved base approximated as
straight line)
9
SLOPE STABILITY ANALYSIS
Ordinary Method of Slices (OMS) (c-f soils)
Wt
a
a
TR
l
b
๐‘™ =
๐‘
cos ๐›ผ
๐‘™ = ๐‘ sec ๐›ผ
๐น๐‘‚๐‘† =
๐‘€ ๐‘…
๐‘€ ๐ท TR = Total shear resistance force acting on slice
๐‘‡๐‘… = ๐œ ๐‘… ร— (๐‘™ โˆ™ 1)
๐‘‡๐‘… = (๐‘โ€ฒ
+ ๐œŽ ๐‘›โ€ฒ tan ๐œ™) ร— ๐‘™
TR
๐‘…๐‘’๐‘ ๐‘–๐‘ ๐‘ก๐‘–๐‘›๐‘” ๐‘€๐‘œ๐‘š๐‘’๐‘›๐‘ก
tR = Shear resistance (stress) offered by soil
๐‘€ ๐‘… = ๐‘‡๐‘… ร— ๐‘Ÿ โ€ฆ (๐ธ๐‘ž. 1)
10
SLOPE STABILITY ANALYSIS
Ordinary Method of Slices (OMS) (c-f soils)
where,
๐œŽ ๐‘›โ€ฒ =
๐‘Š๐‘ก cos ๐›ผ
๐‘™ ร— 1
๐‘‡๐‘… = ๐‘โ€ฒ
๐‘™ +
๐‘Š๐‘ก cos ๐›ผ
๐‘™ ร— 1
๐‘™ tan ๐œ™
๐‘‡๐‘… = ๐‘โ€ฒ ๐‘™ + ๐‘Š๐‘ก cos ๐›ผ tan ๐œ™
๐‘€ ๐‘… = ๐‘Ÿ (๐‘โ€ฒ
๐‘ sec ๐›ผ + ๐‘Š๐‘ก cos ๐›ผ tan ๐œ™)
Wt
a
a
a
TR
l
b
๐‘™ =
๐‘
cos ๐›ผ
๐‘™ = ๐‘ sec ๐›ผ
Wt cos a
Wt sin a
๐‘€ ๐‘… = ๐‘‡๐‘… ร— ๐‘Ÿ โ€ฆ (๐ธ๐‘ž. 1)
๐‘‡๐‘… = ๐œ ๐‘… ร— (๐‘™ โˆ™ 1)
๐‘‡๐‘… = (๐‘โ€ฒ + ๐œŽ ๐‘›โ€ฒ tan ๐œ™) ร— ๐‘™
๐‘…๐‘’๐‘ ๐‘–๐‘ ๐‘ก๐‘–๐‘›๐‘” ๐‘€๐‘œ๐‘š๐‘’๐‘›๐‘ก
๐ธ๐‘ž. 1
11
SLOPE STABILITY ANALYSIS
Ordinary Method of Slices (OMS) (c-f soils)
Wt
a
a
a
TR
l
b
๐‘™ =
๐‘
cos ๐›ผ
๐‘™ = ๐‘ sec ๐›ผ
Wt cos a
Components of disturbing force (Wt)
1. Wt cos a ๏ƒ  Passes through center of rotation, i.e. zero
moment
2. Wt sin a ๏ƒ  Tangential component; causing sliding
๐‘€ ๐ท = ๐‘Ÿ (๐‘Š๐‘ก sin ๐›ผ)
Wt sin a
๐ท๐‘–๐‘ ๐‘ก๐‘ข๐‘Ÿ๐‘๐‘–๐‘›๐‘” ๐‘€๐‘œ๐‘š๐‘’๐‘›๐‘ก
TR
12
SLOPE STABILITY ANALYSIS
Ordinary Method of Slices (OMS) (c-f soils)
Wt
a
a
a
TR
l
b
๐‘™ =
๐‘
cos ๐›ผ
๐‘™ = ๐‘ sec ๐›ผ
Wt cos a
๐น๐‘‚๐‘† =
(๐‘โ€ฒ ๐‘ sec ๐›ผ + ๐‘Š๐‘ก cos ๐›ผ tan ๐œ™)
(๐‘Š๐‘ก sin ๐›ผ)
Wt sin a
๐น๐‘‚๐‘† =
๐‘€ ๐‘…
๐‘€ ๐ท
๐‘€ ๐‘… = ๐‘Ÿ (๐‘โ€ฒ
๐‘ sec ๐›ผ + ๐‘Š๐‘ก cos ๐›ผ tan ๐œ™)
๐‘€ ๐ท = ๐‘Ÿ (๐‘Š๐‘ก sin ๐›ผ)
13
CRITICAL SLIP CIRCLE
NSL
A
B
๏ฑMany slip circles are possible on any slope
๏ฑSlip circle having minimum FOS ๏ƒ  Critical Slip Circle /
Critical Failure Plane
๏ฑDesign has to satisfy safety against critical slip circle
FOS = 2.4
1.20
1.79
1.55
14
LOCATION OF CRITICAL SLIP CIRCLE
In Cohesive soils (f=0)
NSL
A
B
๏ฑ Plot the configuration according to
scale
๏ฑ Draw two lines from point A and B
at angles as has been shown in
figure.
๏ฑ Taking radius equal to OA, draw a
circle passing through the slope
Case-I: Toe Failure
(Fellenius Method)
r
q1
q2
Slope Slope Angle q1 q2
1V : 0.5H 60ยฐ 29ยฐ 40ยฐ
1 : 1 45ยฐ 28ยฐ 38ยฐ
1 : 1.5 34ยฐ 26ยฐ 35ยฐ
1 : 2 27ยฐ 25ยฐ 35ยฐ
1 : 3 19ยฐ 25ยฐ 35ยฐ
Empirical values of q1 and q2
15
LOCATION OF CRITICAL SLIP CIRCLE
In Cohesive soils (f=0)
NSL
A
B
๏ฑ Plot the configuration according to
scale
๏ฑ Draw a vertical line at the mid-point
of slope (the center of critical slip
circle always lies on a vertical line
passing through the mid-point of
slope)
๏ฑ Determine the center by hit and trial
method by comparing the FOS
๏ฑ Circle with minimum FOS is the
critical circle
Case-II: Base Failure
(Fellenius Method)
๐ป
2
๐ป
2
FOS = 1.65
FOS = 1.10
133.5ยฐ
๏ฑ Angle made by critical circle at the
center is about 133.5ยฐ. (Fellenius)
16
NSL
A
B
H
H
๏ฑ Plot the configuration according to
scale
๏ฑ Find the intersection point of โ€˜4.5Hโ€™
horizontal and โ€˜Hโ€™ distance vertical
downward from A
๏ฑ Draw the direction angle q1 and q2
๏ฑ Join the points of intersection O and
C
๏ฑ Locate OC by hit and trial. For this
try O1, O2,โ€ฆโ€ฆ and make circles.
๏ฑ The circle giving minimum FOS is
the critical circle
q2
q1
O1
O2
O3
Omin = Ocr
LOCATION OF CRITICAL SLIP CIRCLE
In c-f soils
O4
4.5H
C
17
SHORT TERM AND LONG TERM
STABILITY
Clay Core
Construction of dam core
- Clay material
- Very low permeability
- Construction in layers with compaction
at OMC
SHORT TERM STABILITY
Stability of slope immediately after construction
๏ฑ Undrained conditions
๏ฑ Undrained parameters (cu and fu) to be used for slope stability analysis
๏ฑ Obtained from UU or CU triaxial tests
๏ฑ Total unit weight of soil (gb) to be used
๏ฑ Called as TOTAL STRESS ANALYSIS
๏ฑ Change in pore water pressure totally dependent upon stress change
18
SHORT TERM AND LONG TERM
STABILITY
Clay Core
Construction of dam core
- Clay material
- Very low permeability
- Construction in layers with compaction
at OMC
LONG TERM STABILITY
Stability of slope long time after construction
๏ฑ Drained conditions
๏ฑ Drained parameters (cd (or cโ€™) and fd (fโ€™)) to be used for slope stability analysis
๏ฑ Obtained from CD triaxial tests, or CU tests with PWP measurements
๏ฑ Effective unit weight of soil (gsub (or gโ€™)) to be used
๏ฑ Called as EFFECTIVE STRESS ANALYSIS
๏ฑ Change in pore water pressure independent of stress change
19
THE END
REFERENCE MATERIAL
Principles of Geotechnical Engineering โ€“ (7th Edition)
Braja M. Das
Chapter #13
Essentials of Soil Mechanics and Foundations (7th Edition)
David F. McCarthy
Chapter #17
Geotechnical Engineering โ€“ Principles and Practices โ€“ (2nd Edition)
Coduto, Yueng, and Kitch
Chapter #17
In fact, this is just the beginning!

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Geotechnical Engineering-II [Lec #28: Finite Slope Stability Analysis]

  • 1. 1 Geotechnical Engineeringโ€“II [CE-321] BSc Civil Engineering โ€“ 5th Semester by Dr. Muhammad Irfan Assistant Professor Civil Engg. Dept. โ€“ UET Lahore Email: mirfan1@msn.com Lecture Handouts: https://groups.google.com/d/forum/geotech-ii_2015session Lecture # 28 20-Dec-2017
  • 2. 2 SLOPE STABILITY ANALYSIS Finite Slope (Swedish Slip Circle Method) Assumptions: 1. Material of the slope is homogeneous. 2. Soil is purely cohesive in nature i.e. f = 0. 3. Failure surface has a curved/circular or spoon like surface. 4. Shear strength of the soil is uniformly distributed along failure plane. (only possible if f = 0)
  • 3. 3 SLOPE STABILITY ANALYSIS Swedish Slip Circle Method (Cohesive soils (f=0)) NSLC A B ๐น๐‘‚๐‘† = ๐‘…๐‘’๐‘ ๐‘–๐‘ ๐‘ก๐‘–๐‘›๐‘” ๐‘€๐‘œ๐‘š๐‘’๐‘›๐‘ก (๐‘€ ๐‘…) ๐ท๐‘–๐‘ ๐‘ก๐‘ข๐‘Ÿ๐‘๐‘–๐‘›๐‘” ๐‘€๐‘œ๐‘š๐‘’๐‘›๐‘ก (๐‘€ ๐ท)
  • 4. 4 NSLC A B ๐น๐‘‚๐‘† = ๐‘…๐‘’๐‘ ๐‘–๐‘ ๐‘ก๐‘–๐‘›๐‘” ๐‘€๐‘œ๐‘š๐‘’๐‘›๐‘ก (๐‘€ ๐‘…) ๐ท๐‘–๐‘ ๐‘ก๐‘ข๐‘Ÿ๐‘๐‘–๐‘›๐‘” ๐‘€๐‘œ๐‘š๐‘’๐‘›๐‘ก (๐‘€ ๐ท) ๐ท๐‘–๐‘ ๐‘ก๐‘ข๐‘Ÿ๐‘๐‘–๐‘›๐‘” ๐‘€๐‘œ๐‘š๐‘’๐‘›๐‘ก ๐‘€ ๐ท = ๐‘Š โˆ™ ๐‘ฅ tr = c + sn tan f For saturated clay under undrained loading; f=0 ๏œ tr = c = su ๐‘…๐‘’๐‘ ๐‘–๐‘ ๐‘ก๐‘–๐‘›๐‘” ๐‘€๐‘œ๐‘š๐‘’๐‘›๐‘ก ๐‘€ ๐‘… = ๐œ ๐‘Ÿ โˆ™ ๐ด๐ต โˆ™ ๐‘… ๐‘€ ๐‘… = ๐‘ โˆ™ (๐‘… โˆ™ ๐œƒ) โˆ™ ๐‘… ๐‘€ ๐‘… = ๐‘ โˆ™ ๐œƒ โˆ™ ๐‘…2 ๐น๐‘‚๐‘† = ๐‘€ ๐‘… ๐‘€ ๐ท ๐น๐‘‚๐‘† = ๐‘ โˆ™ ๐œƒ โˆ™ ๐‘…2 ๐‘Š โˆ™ ๐‘ฅ SLOPE STABILITY ANALYSIS Swedish Slip Circle Method (Cohesive soils (f=0)) Case-I: No Tension Crack W x q R ๐‘Š = (๐ด๐‘Ÿ๐‘’๐‘Ž ๐‘œ๐‘“ ๐ด๐ต๐ถ๐ด ร— 1) ร— ๐›พ โ†’ q in radians
  • 5. 5 W x q R NSLC A B๐น๐‘‚๐‘† = ๐‘…๐‘’๐‘ ๐‘–๐‘ ๐‘ก๐‘–๐‘›๐‘” ๐‘€๐‘œ๐‘š๐‘’๐‘›๐‘ก (๐‘€ ๐‘…) ๐ท๐‘–๐‘ ๐‘ก๐‘ข๐‘Ÿ๐‘๐‘–๐‘›๐‘” ๐‘€๐‘œ๐‘š๐‘’๐‘›๐‘ก (๐‘€ ๐ท) ๐‘€ ๐ท = ๐‘Š โˆ™ ๐‘ฅ tr = c + sn tan f For saturated clay under undrained loading; f=0 ๏œ tr = c = su ๐‘€ ๐‘… = ๐‘ โˆ™ ๐œƒ2 โˆ™ ๐‘…2 ๐น๐‘‚๐‘† = ๐‘€ ๐‘… ๐‘€ ๐ท ๐น๐‘‚๐‘† = ๐‘ โˆ™ ๐œƒ2 โˆ™ ๐‘…2 ๐‘Š โˆ™ ๐‘ฅ SLOPE STABILITY ANALYSIS Swedish Slip Circle Method (Cohesive soils (f=0)) Case-II: Development of Tension Crack โ„Ž ๐‘ก = 2๐‘ ๐›พ ๐พ๐‘Ž q2 FOS will reduce after development of tension crack [โˆต q2 < q] ๐ท๐‘–๐‘ ๐‘ก๐‘ข๐‘Ÿ๐‘๐‘–๐‘›๐‘” ๐‘€๐‘œ๐‘š๐‘’๐‘›๐‘ก ๐‘…๐‘’๐‘ ๐‘–๐‘ ๐‘ก๐‘–๐‘›๐‘” ๐‘€๐‘œ๐‘š๐‘’๐‘›๐‘ก
  • 6. 6 W x R C A tr = c = su SLOPE STABILITY ANALYSIS Swedish Slip Circle Method (Cohesive soils (f=0)) Case-III: Tension Crack filled with water โ„Ž ๐‘ก = 2๐‘ ๐›พ ๐พ๐‘Ž q2 ๐›พwht PW h 2 3 โ„Ž ๐‘ก ๐‘ƒ ๐‘Š = 1 2 ๐›พ ๐‘ค โˆ™ โ„Ž ๐‘ก 2 ๐‘€ ๐ท = ๐‘Š โˆ™ ๐‘ฅ + ๐‘€ ๐‘… = ๐‘ โˆ™ ๐œƒ2 โˆ™ ๐‘…2 ๐น๐‘‚๐‘† = ๐‘ โˆ™ ๐œƒ2 โˆ™ ๐‘…2 ๐‘Š โˆ™ ๐‘ฅ + 1 2 ๐›พ ๐‘ค โˆ™ โ„Ž ๐‘ก 2 โ„Ž + 2 3 โ„Ž ๐‘ก FOS will reduce further when tension crack is filled with water ๐น๐‘‚๐‘† = ๐‘…๐‘’๐‘ ๐‘–๐‘ ๐‘ก๐‘–๐‘›๐‘” ๐‘€๐‘œ๐‘š๐‘’๐‘›๐‘ก (๐‘€ ๐‘…) ๐ท๐‘–๐‘ ๐‘ก๐‘ข๐‘Ÿ๐‘๐‘–๐‘›๐‘” ๐‘€๐‘œ๐‘š๐‘’๐‘›๐‘ก (๐‘€ ๐ท) ๐ท๐‘–๐‘ ๐‘ก๐‘ข๐‘Ÿ๐‘๐‘–๐‘›๐‘” ๐‘€๐‘œ๐‘š๐‘’๐‘›๐‘ก ๐‘…๐‘’๐‘ ๐‘–๐‘ ๐‘ก๐‘–๐‘›๐‘” ๐‘€๐‘œ๐‘š๐‘’๐‘›๐‘ก 1 2 ๐›พ ๐‘ค โˆ™ โ„Ž ๐‘ก 2 โ„Ž + 2 3 โ„Ž ๐‘ก
  • 7. 7 Practice Problem #3 Determine the factor of safety of the cohesive slope shown in the figure for the following two cases; A. No tension crack B. 2m deep tension crack filled with water (q1 = 38ยฐ) NSLC A B gb = 17.75 kN/m3 Cu above line AD = 21.5 kPa Cu below line AD = 33.5 kPa W 3.1m q1= 40ยฐ R q2= 35ยฐ D Dโ€™ 4m 2m Area of ABCA = 90m2
  • 8. 8 SLOPE STABILITY ANALYSIS Ordinary Method of Slices (OMS) (c-f soils) ๏ฑ For c-f soils, normal stress would change along slip circle ๏ฑ Different normal stress means, shear resistance would also be different (โˆต M-C equation) ๏ฑ Failing slope divided into slices TR Guidelines for Slice Selection ๏ฑ Slices do not have to be of equal width ๏ฑ For convenience, base arc of each slice should pass through one soil type only ๏ฑ Slice width should be limited (curved base approximated as straight line)
  • 9. 9 SLOPE STABILITY ANALYSIS Ordinary Method of Slices (OMS) (c-f soils) Wt a a TR l b ๐‘™ = ๐‘ cos ๐›ผ ๐‘™ = ๐‘ sec ๐›ผ ๐น๐‘‚๐‘† = ๐‘€ ๐‘… ๐‘€ ๐ท TR = Total shear resistance force acting on slice ๐‘‡๐‘… = ๐œ ๐‘… ร— (๐‘™ โˆ™ 1) ๐‘‡๐‘… = (๐‘โ€ฒ + ๐œŽ ๐‘›โ€ฒ tan ๐œ™) ร— ๐‘™ TR ๐‘…๐‘’๐‘ ๐‘–๐‘ ๐‘ก๐‘–๐‘›๐‘” ๐‘€๐‘œ๐‘š๐‘’๐‘›๐‘ก tR = Shear resistance (stress) offered by soil ๐‘€ ๐‘… = ๐‘‡๐‘… ร— ๐‘Ÿ โ€ฆ (๐ธ๐‘ž. 1)
  • 10. 10 SLOPE STABILITY ANALYSIS Ordinary Method of Slices (OMS) (c-f soils) where, ๐œŽ ๐‘›โ€ฒ = ๐‘Š๐‘ก cos ๐›ผ ๐‘™ ร— 1 ๐‘‡๐‘… = ๐‘โ€ฒ ๐‘™ + ๐‘Š๐‘ก cos ๐›ผ ๐‘™ ร— 1 ๐‘™ tan ๐œ™ ๐‘‡๐‘… = ๐‘โ€ฒ ๐‘™ + ๐‘Š๐‘ก cos ๐›ผ tan ๐œ™ ๐‘€ ๐‘… = ๐‘Ÿ (๐‘โ€ฒ ๐‘ sec ๐›ผ + ๐‘Š๐‘ก cos ๐›ผ tan ๐œ™) Wt a a a TR l b ๐‘™ = ๐‘ cos ๐›ผ ๐‘™ = ๐‘ sec ๐›ผ Wt cos a Wt sin a ๐‘€ ๐‘… = ๐‘‡๐‘… ร— ๐‘Ÿ โ€ฆ (๐ธ๐‘ž. 1) ๐‘‡๐‘… = ๐œ ๐‘… ร— (๐‘™ โˆ™ 1) ๐‘‡๐‘… = (๐‘โ€ฒ + ๐œŽ ๐‘›โ€ฒ tan ๐œ™) ร— ๐‘™ ๐‘…๐‘’๐‘ ๐‘–๐‘ ๐‘ก๐‘–๐‘›๐‘” ๐‘€๐‘œ๐‘š๐‘’๐‘›๐‘ก ๐ธ๐‘ž. 1
  • 11. 11 SLOPE STABILITY ANALYSIS Ordinary Method of Slices (OMS) (c-f soils) Wt a a a TR l b ๐‘™ = ๐‘ cos ๐›ผ ๐‘™ = ๐‘ sec ๐›ผ Wt cos a Components of disturbing force (Wt) 1. Wt cos a ๏ƒ  Passes through center of rotation, i.e. zero moment 2. Wt sin a ๏ƒ  Tangential component; causing sliding ๐‘€ ๐ท = ๐‘Ÿ (๐‘Š๐‘ก sin ๐›ผ) Wt sin a ๐ท๐‘–๐‘ ๐‘ก๐‘ข๐‘Ÿ๐‘๐‘–๐‘›๐‘” ๐‘€๐‘œ๐‘š๐‘’๐‘›๐‘ก TR
  • 12. 12 SLOPE STABILITY ANALYSIS Ordinary Method of Slices (OMS) (c-f soils) Wt a a a TR l b ๐‘™ = ๐‘ cos ๐›ผ ๐‘™ = ๐‘ sec ๐›ผ Wt cos a ๐น๐‘‚๐‘† = (๐‘โ€ฒ ๐‘ sec ๐›ผ + ๐‘Š๐‘ก cos ๐›ผ tan ๐œ™) (๐‘Š๐‘ก sin ๐›ผ) Wt sin a ๐น๐‘‚๐‘† = ๐‘€ ๐‘… ๐‘€ ๐ท ๐‘€ ๐‘… = ๐‘Ÿ (๐‘โ€ฒ ๐‘ sec ๐›ผ + ๐‘Š๐‘ก cos ๐›ผ tan ๐œ™) ๐‘€ ๐ท = ๐‘Ÿ (๐‘Š๐‘ก sin ๐›ผ)
  • 13. 13 CRITICAL SLIP CIRCLE NSL A B ๏ฑMany slip circles are possible on any slope ๏ฑSlip circle having minimum FOS ๏ƒ  Critical Slip Circle / Critical Failure Plane ๏ฑDesign has to satisfy safety against critical slip circle FOS = 2.4 1.20 1.79 1.55
  • 14. 14 LOCATION OF CRITICAL SLIP CIRCLE In Cohesive soils (f=0) NSL A B ๏ฑ Plot the configuration according to scale ๏ฑ Draw two lines from point A and B at angles as has been shown in figure. ๏ฑ Taking radius equal to OA, draw a circle passing through the slope Case-I: Toe Failure (Fellenius Method) r q1 q2 Slope Slope Angle q1 q2 1V : 0.5H 60ยฐ 29ยฐ 40ยฐ 1 : 1 45ยฐ 28ยฐ 38ยฐ 1 : 1.5 34ยฐ 26ยฐ 35ยฐ 1 : 2 27ยฐ 25ยฐ 35ยฐ 1 : 3 19ยฐ 25ยฐ 35ยฐ Empirical values of q1 and q2
  • 15. 15 LOCATION OF CRITICAL SLIP CIRCLE In Cohesive soils (f=0) NSL A B ๏ฑ Plot the configuration according to scale ๏ฑ Draw a vertical line at the mid-point of slope (the center of critical slip circle always lies on a vertical line passing through the mid-point of slope) ๏ฑ Determine the center by hit and trial method by comparing the FOS ๏ฑ Circle with minimum FOS is the critical circle Case-II: Base Failure (Fellenius Method) ๐ป 2 ๐ป 2 FOS = 1.65 FOS = 1.10 133.5ยฐ ๏ฑ Angle made by critical circle at the center is about 133.5ยฐ. (Fellenius)
  • 16. 16 NSL A B H H ๏ฑ Plot the configuration according to scale ๏ฑ Find the intersection point of โ€˜4.5Hโ€™ horizontal and โ€˜Hโ€™ distance vertical downward from A ๏ฑ Draw the direction angle q1 and q2 ๏ฑ Join the points of intersection O and C ๏ฑ Locate OC by hit and trial. For this try O1, O2,โ€ฆโ€ฆ and make circles. ๏ฑ The circle giving minimum FOS is the critical circle q2 q1 O1 O2 O3 Omin = Ocr LOCATION OF CRITICAL SLIP CIRCLE In c-f soils O4 4.5H C
  • 17. 17 SHORT TERM AND LONG TERM STABILITY Clay Core Construction of dam core - Clay material - Very low permeability - Construction in layers with compaction at OMC SHORT TERM STABILITY Stability of slope immediately after construction ๏ฑ Undrained conditions ๏ฑ Undrained parameters (cu and fu) to be used for slope stability analysis ๏ฑ Obtained from UU or CU triaxial tests ๏ฑ Total unit weight of soil (gb) to be used ๏ฑ Called as TOTAL STRESS ANALYSIS ๏ฑ Change in pore water pressure totally dependent upon stress change
  • 18. 18 SHORT TERM AND LONG TERM STABILITY Clay Core Construction of dam core - Clay material - Very low permeability - Construction in layers with compaction at OMC LONG TERM STABILITY Stability of slope long time after construction ๏ฑ Drained conditions ๏ฑ Drained parameters (cd (or cโ€™) and fd (fโ€™)) to be used for slope stability analysis ๏ฑ Obtained from CD triaxial tests, or CU tests with PWP measurements ๏ฑ Effective unit weight of soil (gsub (or gโ€™)) to be used ๏ฑ Called as EFFECTIVE STRESS ANALYSIS ๏ฑ Change in pore water pressure independent of stress change
  • 19. 19 THE END REFERENCE MATERIAL Principles of Geotechnical Engineering โ€“ (7th Edition) Braja M. Das Chapter #13 Essentials of Soil Mechanics and Foundations (7th Edition) David F. McCarthy Chapter #17 Geotechnical Engineering โ€“ Principles and Practices โ€“ (2nd Edition) Coduto, Yueng, and Kitch Chapter #17 In fact, this is just the beginning!