By
Charchit Jain
Condition for Rotational failure
 Failure is along the line of least resistance through the
slope , observation of various failure suggests that the
failure surface is generally takes the form of a circle
and most of the theories are based on this observation.
 The individual particles in the rockmass are very small
as compared with the size of the slope.
 These particles are not interlocked.
Derivation of Rotational failure
charts
 The following assumptions are made in deriving the
stability charts :
1. Material forming the slope is assumed to be
homogeneous.
2. τe = c + σ tan φ
3. Failure surface passes through the toe of the slope.
4. Location of the tension crack and the failure surface are
such that the FOS of the slope is minimum for the slope
geometry.
5. A range of ground water condition, from dry to fully
saturated condition are considered.
 Factor of safety of the slope is defined as =
and rearranging this equation, we obtain
τe = (c + σ tan φ)/FS
shear stress available to resist sliding depends upon the
distribution of normal stress (σ ) along this surface .
)surface(sliponmequilibriuforrequiredstressshear
)tan(cslidingresisttoavailablestrengthshear
e

FS
 Failure charts are produced depending upon the
ground water condition.
 Location of tension crack and the failure surface is
determined.
Example
 A 50 ft. high slope with the face angle of 40° is to be
excavated In the overburden soil with density ɗ = 100
lb/ft3 ,angle of friction is 30°, cohesive strength of c =
800 lb/ft2 , find the factor of safety of slope assuming it
to be a fully drained slope.
 value of (c/ɗ.H.tanØ) is 0.28 , so the corresponding
tanØ/F value for slope of 40° is 0.28 . Hence , the
Factor of safety is 2.061 .
Location of failure surface and
tension crack
 Charts are used for the construction of drawings of
potential slides.
 Charts are also used for the determination of location
of tension crack.
 Ground water condition is considered while selecting
the chart.
Location of critical failure
surface and tension crack for
drained slope
Location of critical failure surface
and tension crack in the presence
of ground water
Example
 A slope having face angle of 30° in a drained soil with
angle of friction is 20°. Locate the centre of critical
failure surface and tension crack .
 X = 0.2H
Y = 1.85H
b = 0.1H
Short term stability of soils with Ø = 0
 Failure will then occur along the circular arc of radius
R, and soil is assumed to be homogeneous.
F = Resisting moment / disturbing moment
Resisting moment = R2ØCu
Disturbing moment = Wx
Method of slicing
 For soil having Ø ≠ 0 , a more elaborate analysis is
required.
 Dividing the failure mass into number of slices,
preferably more than 5.
Force acting on ith slice
Overturning moment = R W
i=1
n
i i sin 
Restoring moment = R T
i=1
n
i
F
sisting Moment
Overturning Moment
c l N
W
i i i i
i
n
i i
i
n
 
   




Re
[ tan ]
sin
 

1
1
Case of drained slope is considered so Ui = 0
Swedish Method of Slices
This method is based on the assumption that the resultant of
the inter-slice forces acts perpendicular to the
normal force N.
Ei Ei 1
Uii Uii  1
Xi
Xi  1
Ti
Ni
Ui
Wi
Ti
Ni
Ui
Wi
R
N = N + U = Wi i i i i cos 
F =
[ c l + (W - U )
W
i=1
n
i i i i i i
i=1
n
i i


  cos tan ]
sin
 

F =
[ c l + W t
W
i=1
n
ui i i i ui
i=1
n
i i


 cos an ]
sin
 

For effective stress analysis
For total stress (undrained) analysis
Example
Calculations for slice 6
1. Measure l from the figure and width of the slice
6
26 ft
l = 28.5 ft
Embankment
foundation
Example
4. Determine the self-weight of the slice
6
26 ft
embankment
foundation
53.6ft
5 ft
W = A g = 257 pound/ft 3
10.4 ft
 Total resisting force = 640 kips
 Total driving force = 524 kips
Factor of safety = 640 / 524
= 1.22
Bishop’s simplified method
Assumption: The vertical inter-slice forces are equal and opposite. The resultant thus
acts perpendicular to W
Ei Ei 1
Uii Uii  1
Xi
Xi  1
Ti
Ni
Ui
Wi
Ti
Ni
Ui
Wi
R
W = T + N + u xi i i i i i isin cos  
W = T + N + u xi i i i i i isin cos  
T =
c l
F
+
N
F
i
i i i i   tan 








N =
W - u x - (1/ F) c x
1 +
F
i
i i i i i i
i
i i
  tan
cos
tan tan


 
now
hence
Substitution of the expression for N’ into the equation for the factor of safety
F
sisting Moment
Overturning Moment
c l N
W
i i i i
i
n
i i
i
n
 
   




Re
[ tan ]
sin
 

1
1
leads to
F =
( c x + ( W - u x ) )
1
M ( )
W
i=1
n
i i i i i i
i
i=1
n
i i


 





  tan
sin



where
M ( ) = [ 1 +
F
]i i i
i
  

cos tan
tan 
Janbu simplified method of slice
 It is based on the assumption that the failure surface
can be of general shape.
 Analysis of this method is similar to that of bishop’s
method.
The main methods for Rotational failure
analysis
Rotational failure analysis

Rotational failure analysis

  • 1.
  • 2.
    Condition for Rotationalfailure  Failure is along the line of least resistance through the slope , observation of various failure suggests that the failure surface is generally takes the form of a circle and most of the theories are based on this observation.  The individual particles in the rockmass are very small as compared with the size of the slope.  These particles are not interlocked.
  • 3.
    Derivation of Rotationalfailure charts  The following assumptions are made in deriving the stability charts : 1. Material forming the slope is assumed to be homogeneous. 2. τe = c + σ tan φ 3. Failure surface passes through the toe of the slope. 4. Location of the tension crack and the failure surface are such that the FOS of the slope is minimum for the slope geometry. 5. A range of ground water condition, from dry to fully saturated condition are considered.
  • 4.
     Factor ofsafety of the slope is defined as = and rearranging this equation, we obtain τe = (c + σ tan φ)/FS shear stress available to resist sliding depends upon the distribution of normal stress (σ ) along this surface . )surface(sliponmequilibriuforrequiredstressshear )tan(cslidingresisttoavailablestrengthshear e  FS
  • 5.
     Failure chartsare produced depending upon the ground water condition.  Location of tension crack and the failure surface is determined.
  • 12.
    Example  A 50ft. high slope with the face angle of 40° is to be excavated In the overburden soil with density ɗ = 100 lb/ft3 ,angle of friction is 30°, cohesive strength of c = 800 lb/ft2 , find the factor of safety of slope assuming it to be a fully drained slope.  value of (c/ɗ.H.tanØ) is 0.28 , so the corresponding tanØ/F value for slope of 40° is 0.28 . Hence , the Factor of safety is 2.061 .
  • 13.
    Location of failuresurface and tension crack  Charts are used for the construction of drawings of potential slides.  Charts are also used for the determination of location of tension crack.  Ground water condition is considered while selecting the chart.
  • 14.
    Location of criticalfailure surface and tension crack for drained slope
  • 15.
    Location of criticalfailure surface and tension crack in the presence of ground water
  • 16.
    Example  A slopehaving face angle of 30° in a drained soil with angle of friction is 20°. Locate the centre of critical failure surface and tension crack .  X = 0.2H Y = 1.85H b = 0.1H
  • 17.
    Short term stabilityof soils with Ø = 0  Failure will then occur along the circular arc of radius R, and soil is assumed to be homogeneous. F = Resisting moment / disturbing moment Resisting moment = R2ØCu Disturbing moment = Wx
  • 18.
    Method of slicing For soil having Ø ≠ 0 , a more elaborate analysis is required.  Dividing the failure mass into number of slices, preferably more than 5.
  • 19.
    Force acting onith slice
  • 20.
    Overturning moment =R W i=1 n i i sin  Restoring moment = R T i=1 n i F sisting Moment Overturning Moment c l N W i i i i i n i i i n           Re [ tan ] sin    1 1 Case of drained slope is considered so Ui = 0
  • 21.
    Swedish Method ofSlices This method is based on the assumption that the resultant of the inter-slice forces acts perpendicular to the normal force N. Ei Ei 1 Uii Uii  1 Xi Xi  1 Ti Ni Ui Wi Ti Ni Ui Wi R N = N + U = Wi i i i i cos 
  • 22.
    F = [ cl + (W - U ) W i=1 n i i i i i i i=1 n i i     cos tan ] sin    F = [ c l + W t W i=1 n ui i i i ui i=1 n i i    cos an ] sin    For effective stress analysis For total stress (undrained) analysis
  • 23.
  • 24.
    Calculations for slice6 1. Measure l from the figure and width of the slice 6 26 ft l = 28.5 ft Embankment foundation
  • 25.
    Example 4. Determine theself-weight of the slice 6 26 ft embankment foundation 53.6ft 5 ft W = A g = 257 pound/ft 3 10.4 ft
  • 27.
     Total resistingforce = 640 kips  Total driving force = 524 kips Factor of safety = 640 / 524 = 1.22
  • 28.
    Bishop’s simplified method Assumption:The vertical inter-slice forces are equal and opposite. The resultant thus acts perpendicular to W Ei Ei 1 Uii Uii  1 Xi Xi  1 Ti Ni Ui Wi Ti Ni Ui Wi R W = T + N + u xi i i i i i isin cos  
  • 29.
    W = T+ N + u xi i i i i i isin cos   T = c l F + N F i i i i i   tan          N = W - u x - (1/ F) c x 1 + F i i i i i i i i i i   tan cos tan tan     now hence
  • 30.
    Substitution of theexpression for N’ into the equation for the factor of safety F sisting Moment Overturning Moment c l N W i i i i i n i i i n           Re [ tan ] sin    1 1 leads to F = ( c x + ( W - u x ) ) 1 M ( ) W i=1 n i i i i i i i i=1 n i i            tan sin    where M ( ) = [ 1 + F ]i i i i     cos tan tan 
  • 31.
    Janbu simplified methodof slice  It is based on the assumption that the failure surface can be of general shape.  Analysis of this method is similar to that of bishop’s method.
  • 33.
    The main methodsfor Rotational failure analysis