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Geotechnical Engineering–II [CE-321]
BSc Civil Engineering – 5th Semester
by
Dr. Muhammad Irfan
Assistant Professor
Civil Engg. Dept. – 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
𝐹𝑂𝑆 =
𝑅𝑒𝑠𝑖𝑠𝑡𝑖𝑛𝑔 𝑀𝑜𝑚𝑒𝑛𝑡 (𝑀 𝑅)
𝐷𝑖𝑠𝑡𝑢𝑟𝑏𝑖𝑛𝑔 𝑀𝑜𝑚𝑒𝑛𝑡 (𝑀 𝐷)
4
NSLC
A
B
𝐹𝑂𝑆 =
𝑅𝑒𝑠𝑖𝑠𝑡𝑖𝑛𝑔 𝑀𝑜𝑚𝑒𝑛𝑡 (𝑀 𝑅)
𝐷𝑖𝑠𝑡𝑢𝑟𝑏𝑖𝑛𝑔 𝑀𝑜𝑚𝑒𝑛𝑡 (𝑀 𝐷)
𝐷𝑖𝑠𝑡𝑢𝑟𝑏𝑖𝑛𝑔 𝑀𝑜𝑚𝑒𝑛𝑡
𝑀 𝐷 = 𝑊 ∙ 𝑥
tr = c + sn tan f
For saturated clay under
undrained loading; f=0
 tr = c = su
𝑅𝑒𝑠𝑖𝑠𝑡𝑖𝑛𝑔 𝑀𝑜𝑚𝑒𝑛𝑡
𝑀 𝑅 = 𝜏 𝑟 ∙ 𝐴𝐵 ∙ 𝑅
𝑀 𝑅 = 𝑐 ∙ (𝑅 ∙ 𝜃) ∙ 𝑅
𝑀 𝑅 = 𝑐 ∙ 𝜃 ∙ 𝑅2
𝐹𝑂𝑆 =
𝑀 𝑅
𝑀 𝐷
𝐹𝑂𝑆 =
𝑐 ∙ 𝜃 ∙ 𝑅2
𝑊 ∙ 𝑥
SLOPE STABILITY ANALYSIS
Swedish Slip Circle Method (Cohesive soils (f=0))
Case-I: No Tension Crack
W
x
q
R
𝑊 = (𝐴𝑟𝑒𝑎 𝑜𝑓 𝐴𝐵𝐶𝐴 × 1) × 𝛾
→ q in radians
5
W
x
q
R
NSLC
A
B𝐹𝑂𝑆 =
𝑅𝑒𝑠𝑖𝑠𝑡𝑖𝑛𝑔 𝑀𝑜𝑚𝑒𝑛𝑡 (𝑀 𝑅)
𝐷𝑖𝑠𝑡𝑢𝑟𝑏𝑖𝑛𝑔 𝑀𝑜𝑚𝑒𝑛𝑡 (𝑀 𝐷)
𝑀 𝐷 = 𝑊 ∙ 𝑥
tr = c + sn tan f
For saturated clay under
undrained loading; f=0
 tr = c = su
𝑀 𝑅 = 𝑐 ∙ 𝜃2 ∙ 𝑅2
𝐹𝑂𝑆 =
𝑀 𝑅
𝑀 𝐷
𝐹𝑂𝑆 =
𝑐 ∙ 𝜃2 ∙ 𝑅2
𝑊 ∙ 𝑥
SLOPE STABILITY ANALYSIS
Swedish Slip Circle Method (Cohesive soils (f=0))
Case-II: Development of Tension Crack
ℎ 𝑡 =
2𝑐
𝛾 𝐾𝑎
q2
FOS will reduce after development of tension crack [∵ q2 < q]
𝐷𝑖𝑠𝑡𝑢𝑟𝑏𝑖𝑛𝑔 𝑀𝑜𝑚𝑒𝑛𝑡
𝑅𝑒𝑠𝑖𝑠𝑡𝑖𝑛𝑔 𝑀𝑜𝑚𝑒𝑛𝑡
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
ℎ 𝑡 =
2𝑐
𝛾 𝐾𝑎
q2
𝛾wht
PW
h
2
3
ℎ 𝑡
𝑃 𝑊 =
1
2
𝛾 𝑤 ∙ ℎ 𝑡
2
𝑀 𝐷 = 𝑊 ∙ 𝑥 +
𝑀 𝑅 = 𝑐 ∙ 𝜃2 ∙ 𝑅2
𝐹𝑂𝑆 =
𝑐 ∙ 𝜃2 ∙ 𝑅2
𝑊 ∙ 𝑥 +
1
2
𝛾 𝑤 ∙ ℎ 𝑡
2
ℎ +
2
3
ℎ 𝑡
FOS will reduce further when tension crack is filled with water
𝐹𝑂𝑆 =
𝑅𝑒𝑠𝑖𝑠𝑡𝑖𝑛𝑔 𝑀𝑜𝑚𝑒𝑛𝑡 (𝑀 𝑅)
𝐷𝑖𝑠𝑡𝑢𝑟𝑏𝑖𝑛𝑔 𝑀𝑜𝑚𝑒𝑛𝑡 (𝑀 𝐷)
𝐷𝑖𝑠𝑡𝑢𝑟𝑏𝑖𝑛𝑔 𝑀𝑜𝑚𝑒𝑛𝑡
𝑅𝑒𝑠𝑖𝑠𝑡𝑖𝑛𝑔 𝑀𝑜𝑚𝑒𝑛𝑡
1
2
𝛾 𝑤 ∙ ℎ 𝑡
2
ℎ +
2
3
ℎ 𝑡
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 = 38°)
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=
40°
R
q2=
35°
D
D’
4m
2m
Area of ABCA
= 90m2
8
SLOPE STABILITY ANALYSIS
Ordinary Method of Slices (OMS) (c-f soils)
 For c-f soils, normal stress would change along slip circle
 Different normal stress means, shear resistance would also be
different (∵ M-C equation)
 Failing slope divided into slices
TR
Guidelines for Slice Selection
 Slices do not have to be of equal
width
 For convenience, base arc of each
slice should pass through one soil
type only
 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
𝑙 =
𝑏
cos 𝛼
𝑙 = 𝑏 sec 𝛼
𝐹𝑂𝑆 =
𝑀 𝑅
𝑀 𝐷 TR = Total shear resistance force acting on slice
𝑇𝑅 = 𝜏 𝑅 × (𝑙 ∙ 1)
𝑇𝑅 = (𝑐′
+ 𝜎 𝑛′ tan 𝜙) × 𝑙
TR
𝑅𝑒𝑠𝑖𝑠𝑡𝑖𝑛𝑔 𝑀𝑜𝑚𝑒𝑛𝑡
tR = Shear resistance (stress) offered by soil
𝑀 𝑅 = 𝑇𝑅 × 𝑟 … (𝐸𝑞. 1)
10
SLOPE STABILITY ANALYSIS
Ordinary Method of Slices (OMS) (c-f soils)
where,
𝜎 𝑛′ =
𝑊𝑡 cos 𝛼
𝑙 × 1
𝑇𝑅 = 𝑐′
𝑙 +
𝑊𝑡 cos 𝛼
𝑙 × 1
𝑙 tan 𝜙
𝑇𝑅 = 𝑐′ 𝑙 + 𝑊𝑡 cos 𝛼 tan 𝜙
𝑀 𝑅 = 𝑟 (𝑐′
𝑏 sec 𝛼 + 𝑊𝑡 cos 𝛼 tan 𝜙)
Wt
a
a
a
TR
l
b
𝑙 =
𝑏
cos 𝛼
𝑙 = 𝑏 sec 𝛼
Wt cos a
Wt sin a
𝑀 𝑅 = 𝑇𝑅 × 𝑟 … (𝐸𝑞. 1)
𝑇𝑅 = 𝜏 𝑅 × (𝑙 ∙ 1)
𝑇𝑅 = (𝑐′ + 𝜎 𝑛′ tan 𝜙) × 𝑙
𝑅𝑒𝑠𝑖𝑠𝑡𝑖𝑛𝑔 𝑀𝑜𝑚𝑒𝑛𝑡
𝐸𝑞. 1
11
SLOPE STABILITY ANALYSIS
Ordinary Method of Slices (OMS) (c-f soils)
Wt
a
a
a
TR
l
b
𝑙 =
𝑏
cos 𝛼
𝑙 = 𝑏 sec 𝛼
Wt cos a
Components of disturbing force (Wt)
1. Wt cos a  Passes through center of rotation, i.e. zero
moment
2. Wt sin a  Tangential component; causing sliding
𝑀 𝐷 = 𝑟 (𝑊𝑡 sin 𝛼)
Wt sin a
𝐷𝑖𝑠𝑡𝑢𝑟𝑏𝑖𝑛𝑔 𝑀𝑜𝑚𝑒𝑛𝑡
TR
12
SLOPE STABILITY ANALYSIS
Ordinary Method of Slices (OMS) (c-f soils)
Wt
a
a
a
TR
l
b
𝑙 =
𝑏
cos 𝛼
𝑙 = 𝑏 sec 𝛼
Wt cos a
𝐹𝑂𝑆 =
(𝑐′ 𝑏 sec 𝛼 + 𝑊𝑡 cos 𝛼 tan 𝜙)
(𝑊𝑡 sin 𝛼)
Wt sin a
𝐹𝑂𝑆 =
𝑀 𝑅
𝑀 𝐷
𝑀 𝑅 = 𝑟 (𝑐′
𝑏 sec 𝛼 + 𝑊𝑡 cos 𝛼 tan 𝜙)
𝑀 𝐷 = 𝑟 (𝑊𝑡 sin 𝛼)
13
CRITICAL SLIP CIRCLE
NSL
A
B
Many slip circles are possible on any slope
Slip circle having minimum FOS  Critical Slip Circle /
Critical Failure Plane
Design 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
 Plot the configuration according to
scale
 Draw two lines from point A and B
at angles as has been shown in
figure.
 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 60° 29° 40°
1 : 1 45° 28° 38°
1 : 1.5 34° 26° 35°
1 : 2 27° 25° 35°
1 : 3 19° 25° 35°
Empirical values of q1 and q2
15
LOCATION OF CRITICAL SLIP CIRCLE
In Cohesive soils (f=0)
NSL
A
B
 Plot the configuration according to
scale
 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)
 Determine the center by hit and trial
method by comparing the FOS
 Circle with minimum FOS is the
critical circle
Case-II: Base Failure
(Fellenius Method)
𝐻
2
𝐻
2
FOS = 1.65
FOS = 1.10
133.5°
 Angle made by critical circle at the
center is about 133.5°. (Fellenius)
16
NSL
A
B
H
H
 Plot the configuration according to
scale
 Find the intersection point of ‘4.5H’
horizontal and ‘H’ distance vertical
downward from A
 Draw the direction angle q1 and q2
 Join the points of intersection O and
C
 Locate OC by hit and trial. For this
try O1, O2,…… and make circles.
 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
 Undrained conditions
 Undrained parameters (cu and fu) to be used for slope stability analysis
 Obtained from UU or CU triaxial tests
 Total unit weight of soil (gb) to be used
 Called as TOTAL STRESS ANALYSIS
 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
 Drained conditions
 Drained parameters (cd (or c’) and fd (f’)) to be used for slope stability analysis
 Obtained from CD triaxial tests, or CU tests with PWP measurements
 Effective unit weight of soil (gsub (or g’)) to be used
 Called as EFFECTIVE STRESS ANALYSIS
 Change in pore water pressure independent of stress change
19
THE END
REFERENCE MATERIAL
Principles of Geotechnical Engineering – (7th Edition)
Braja M. Das
Chapter #13
Essentials of Soil Mechanics and Foundations (7th Edition)
David F. McCarthy
Chapter #17
Geotechnical Engineering – Principles and Practices – (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 Engineering–II [CE-321] BSc Civil Engineering – 5th Semester by Dr. Muhammad Irfan Assistant Professor Civil Engg. Dept. – 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 𝐹𝑂𝑆 = 𝑅𝑒𝑠𝑖𝑠𝑡𝑖𝑛𝑔 𝑀𝑜𝑚𝑒𝑛𝑡 (𝑀 𝑅) 𝐷𝑖𝑠𝑡𝑢𝑟𝑏𝑖𝑛𝑔 𝑀𝑜𝑚𝑒𝑛𝑡 (𝑀 𝐷)
  • 4. 4 NSLC A B 𝐹𝑂𝑆 = 𝑅𝑒𝑠𝑖𝑠𝑡𝑖𝑛𝑔 𝑀𝑜𝑚𝑒𝑛𝑡 (𝑀 𝑅) 𝐷𝑖𝑠𝑡𝑢𝑟𝑏𝑖𝑛𝑔 𝑀𝑜𝑚𝑒𝑛𝑡 (𝑀 𝐷) 𝐷𝑖𝑠𝑡𝑢𝑟𝑏𝑖𝑛𝑔 𝑀𝑜𝑚𝑒𝑛𝑡 𝑀 𝐷 = 𝑊 ∙ 𝑥 tr = c + sn tan f For saturated clay under undrained loading; f=0  tr = c = su 𝑅𝑒𝑠𝑖𝑠𝑡𝑖𝑛𝑔 𝑀𝑜𝑚𝑒𝑛𝑡 𝑀 𝑅 = 𝜏 𝑟 ∙ 𝐴𝐵 ∙ 𝑅 𝑀 𝑅 = 𝑐 ∙ (𝑅 ∙ 𝜃) ∙ 𝑅 𝑀 𝑅 = 𝑐 ∙ 𝜃 ∙ 𝑅2 𝐹𝑂𝑆 = 𝑀 𝑅 𝑀 𝐷 𝐹𝑂𝑆 = 𝑐 ∙ 𝜃 ∙ 𝑅2 𝑊 ∙ 𝑥 SLOPE STABILITY ANALYSIS Swedish Slip Circle Method (Cohesive soils (f=0)) Case-I: No Tension Crack W x q R 𝑊 = (𝐴𝑟𝑒𝑎 𝑜𝑓 𝐴𝐵𝐶𝐴 × 1) × 𝛾 → q in radians
  • 5. 5 W x q R NSLC A B𝐹𝑂𝑆 = 𝑅𝑒𝑠𝑖𝑠𝑡𝑖𝑛𝑔 𝑀𝑜𝑚𝑒𝑛𝑡 (𝑀 𝑅) 𝐷𝑖𝑠𝑡𝑢𝑟𝑏𝑖𝑛𝑔 𝑀𝑜𝑚𝑒𝑛𝑡 (𝑀 𝐷) 𝑀 𝐷 = 𝑊 ∙ 𝑥 tr = c + sn tan f For saturated clay under undrained loading; f=0  tr = c = su 𝑀 𝑅 = 𝑐 ∙ 𝜃2 ∙ 𝑅2 𝐹𝑂𝑆 = 𝑀 𝑅 𝑀 𝐷 𝐹𝑂𝑆 = 𝑐 ∙ 𝜃2 ∙ 𝑅2 𝑊 ∙ 𝑥 SLOPE STABILITY ANALYSIS Swedish Slip Circle Method (Cohesive soils (f=0)) Case-II: Development of Tension Crack ℎ 𝑡 = 2𝑐 𝛾 𝐾𝑎 q2 FOS will reduce after development of tension crack [∵ q2 < q] 𝐷𝑖𝑠𝑡𝑢𝑟𝑏𝑖𝑛𝑔 𝑀𝑜𝑚𝑒𝑛𝑡 𝑅𝑒𝑠𝑖𝑠𝑡𝑖𝑛𝑔 𝑀𝑜𝑚𝑒𝑛𝑡
  • 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 ℎ 𝑡 = 2𝑐 𝛾 𝐾𝑎 q2 𝛾wht PW h 2 3 ℎ 𝑡 𝑃 𝑊 = 1 2 𝛾 𝑤 ∙ ℎ 𝑡 2 𝑀 𝐷 = 𝑊 ∙ 𝑥 + 𝑀 𝑅 = 𝑐 ∙ 𝜃2 ∙ 𝑅2 𝐹𝑂𝑆 = 𝑐 ∙ 𝜃2 ∙ 𝑅2 𝑊 ∙ 𝑥 + 1 2 𝛾 𝑤 ∙ ℎ 𝑡 2 ℎ + 2 3 ℎ 𝑡 FOS will reduce further when tension crack is filled with water 𝐹𝑂𝑆 = 𝑅𝑒𝑠𝑖𝑠𝑡𝑖𝑛𝑔 𝑀𝑜𝑚𝑒𝑛𝑡 (𝑀 𝑅) 𝐷𝑖𝑠𝑡𝑢𝑟𝑏𝑖𝑛𝑔 𝑀𝑜𝑚𝑒𝑛𝑡 (𝑀 𝐷) 𝐷𝑖𝑠𝑡𝑢𝑟𝑏𝑖𝑛𝑔 𝑀𝑜𝑚𝑒𝑛𝑡 𝑅𝑒𝑠𝑖𝑠𝑡𝑖𝑛𝑔 𝑀𝑜𝑚𝑒𝑛𝑡 1 2 𝛾 𝑤 ∙ ℎ 𝑡 2 ℎ + 2 3 ℎ 𝑡
  • 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 = 38°) 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= 40° R q2= 35° D D’ 4m 2m Area of ABCA = 90m2
  • 8. 8 SLOPE STABILITY ANALYSIS Ordinary Method of Slices (OMS) (c-f soils)  For c-f soils, normal stress would change along slip circle  Different normal stress means, shear resistance would also be different (∵ M-C equation)  Failing slope divided into slices TR Guidelines for Slice Selection  Slices do not have to be of equal width  For convenience, base arc of each slice should pass through one soil type only  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 𝑙 = 𝑏 cos 𝛼 𝑙 = 𝑏 sec 𝛼 𝐹𝑂𝑆 = 𝑀 𝑅 𝑀 𝐷 TR = Total shear resistance force acting on slice 𝑇𝑅 = 𝜏 𝑅 × (𝑙 ∙ 1) 𝑇𝑅 = (𝑐′ + 𝜎 𝑛′ tan 𝜙) × 𝑙 TR 𝑅𝑒𝑠𝑖𝑠𝑡𝑖𝑛𝑔 𝑀𝑜𝑚𝑒𝑛𝑡 tR = Shear resistance (stress) offered by soil 𝑀 𝑅 = 𝑇𝑅 × 𝑟 … (𝐸𝑞. 1)
  • 10. 10 SLOPE STABILITY ANALYSIS Ordinary Method of Slices (OMS) (c-f soils) where, 𝜎 𝑛′ = 𝑊𝑡 cos 𝛼 𝑙 × 1 𝑇𝑅 = 𝑐′ 𝑙 + 𝑊𝑡 cos 𝛼 𝑙 × 1 𝑙 tan 𝜙 𝑇𝑅 = 𝑐′ 𝑙 + 𝑊𝑡 cos 𝛼 tan 𝜙 𝑀 𝑅 = 𝑟 (𝑐′ 𝑏 sec 𝛼 + 𝑊𝑡 cos 𝛼 tan 𝜙) Wt a a a TR l b 𝑙 = 𝑏 cos 𝛼 𝑙 = 𝑏 sec 𝛼 Wt cos a Wt sin a 𝑀 𝑅 = 𝑇𝑅 × 𝑟 … (𝐸𝑞. 1) 𝑇𝑅 = 𝜏 𝑅 × (𝑙 ∙ 1) 𝑇𝑅 = (𝑐′ + 𝜎 𝑛′ tan 𝜙) × 𝑙 𝑅𝑒𝑠𝑖𝑠𝑡𝑖𝑛𝑔 𝑀𝑜𝑚𝑒𝑛𝑡 𝐸𝑞. 1
  • 11. 11 SLOPE STABILITY ANALYSIS Ordinary Method of Slices (OMS) (c-f soils) Wt a a a TR l b 𝑙 = 𝑏 cos 𝛼 𝑙 = 𝑏 sec 𝛼 Wt cos a Components of disturbing force (Wt) 1. Wt cos a  Passes through center of rotation, i.e. zero moment 2. Wt sin a  Tangential component; causing sliding 𝑀 𝐷 = 𝑟 (𝑊𝑡 sin 𝛼) Wt sin a 𝐷𝑖𝑠𝑡𝑢𝑟𝑏𝑖𝑛𝑔 𝑀𝑜𝑚𝑒𝑛𝑡 TR
  • 12. 12 SLOPE STABILITY ANALYSIS Ordinary Method of Slices (OMS) (c-f soils) Wt a a a TR l b 𝑙 = 𝑏 cos 𝛼 𝑙 = 𝑏 sec 𝛼 Wt cos a 𝐹𝑂𝑆 = (𝑐′ 𝑏 sec 𝛼 + 𝑊𝑡 cos 𝛼 tan 𝜙) (𝑊𝑡 sin 𝛼) Wt sin a 𝐹𝑂𝑆 = 𝑀 𝑅 𝑀 𝐷 𝑀 𝑅 = 𝑟 (𝑐′ 𝑏 sec 𝛼 + 𝑊𝑡 cos 𝛼 tan 𝜙) 𝑀 𝐷 = 𝑟 (𝑊𝑡 sin 𝛼)
  • 13. 13 CRITICAL SLIP CIRCLE NSL A B Many slip circles are possible on any slope Slip circle having minimum FOS  Critical Slip Circle / Critical Failure Plane Design 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  Plot the configuration according to scale  Draw two lines from point A and B at angles as has been shown in figure.  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 60° 29° 40° 1 : 1 45° 28° 38° 1 : 1.5 34° 26° 35° 1 : 2 27° 25° 35° 1 : 3 19° 25° 35° Empirical values of q1 and q2
  • 15. 15 LOCATION OF CRITICAL SLIP CIRCLE In Cohesive soils (f=0) NSL A B  Plot the configuration according to scale  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)  Determine the center by hit and trial method by comparing the FOS  Circle with minimum FOS is the critical circle Case-II: Base Failure (Fellenius Method) 𝐻 2 𝐻 2 FOS = 1.65 FOS = 1.10 133.5°  Angle made by critical circle at the center is about 133.5°. (Fellenius)
  • 16. 16 NSL A B H H  Plot the configuration according to scale  Find the intersection point of ‘4.5H’ horizontal and ‘H’ distance vertical downward from A  Draw the direction angle q1 and q2  Join the points of intersection O and C  Locate OC by hit and trial. For this try O1, O2,…… and make circles.  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  Undrained conditions  Undrained parameters (cu and fu) to be used for slope stability analysis  Obtained from UU or CU triaxial tests  Total unit weight of soil (gb) to be used  Called as TOTAL STRESS ANALYSIS  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  Drained conditions  Drained parameters (cd (or c’) and fd (f’)) to be used for slope stability analysis  Obtained from CD triaxial tests, or CU tests with PWP measurements  Effective unit weight of soil (gsub (or g’)) to be used  Called as EFFECTIVE STRESS ANALYSIS  Change in pore water pressure independent of stress change
  • 19. 19 THE END REFERENCE MATERIAL Principles of Geotechnical Engineering – (7th Edition) Braja M. Das Chapter #13 Essentials of Soil Mechanics and Foundations (7th Edition) David F. McCarthy Chapter #17 Geotechnical Engineering – Principles and Practices – (2nd Edition) Coduto, Yueng, and Kitch Chapter #17 In fact, this is just the beginning!