6,0 slope stability_part 1
TRANSCRIPT
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Slope Stability
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Causes of instability
All slopes (natural or manmade) have a tendency to
move. The main force causing movement is gravity.
Causes of instability:
inherent, such as weaknesses in the rock or soilforming the slope;
variable, such as heavy rain and changes in ground-water level;
transient, such as earthquake or volcanic activity;
human activities, such as excavations, removal ofvegetations, etc.
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Types of slope failure
Source: BS6031:1981
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Types of slope failure
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Principles of stability
Disturbing force is generated by self weight of the soil,
surface loadings, and seismic loads.
Tendency to slide is opposed by the shearing resistanceof the soil.
Sliding can be caused by either an increase in thedisturbing force or a decrease in shearing resistance ofthe soil.
Limit equilibrium method is normally used.
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Principles of stability
Limit equilibrium method
Failure is on the point of occurring along an assumedor known failure surface.
The static force and moment equilibrium of the
assumed failed mass is analysed.
A factor of safety is obtained from the ratio of shearstrength of the soil to the mobilised shear stresswhen the slope is on the point of failing.
A search for the critical failure surface is carried outso as to obtain the minimum factor of safety for theslope.
For a slope which has failed, F = 1.
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Principles of stability
Stability analyses may be carried in 2 ways:
Total stress analysis using undrained shear strengthparameters for short term cases
Effective stress analysis using drained shear strengthparameters for long term cases
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Infinite slope analysis
The failure plane is parallel to the surface of the slope
z
En
En+1
N = N' + U
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Infinite slope: effective stress analysis
En+1 and En are equal, opposite and co-linear.
Resolve // failure surface: Wsinb = S = tmob x l
l= b/cosb
tmob = t/F
t = c' + s' tan f'
s' = N'/l
W =g xz x b =g xz x lcosb
F = c' + (N'/l) tan f'
gz sinb cosb
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Infinite slope: effective stress analysis
Resolve perp to failure surface: N = N' + U = WcosbN' = l(gz cos2b u)
F = c' + (gz cos2b u) tan f'gz sinb cosb
which is the general equation of infinite slope in terms ofeffective stress
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Infinite slope: effective stress analysis
Special cases
If c' = 0, F = (1 u/gz cos2b ) tan f'tan b
If c' = 0 and u = 0, F = tan f'tan b
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Infinite slope: effective stress analysis
Special cases
Steady seepage parallel to ground level with groundwater table verticalheight, hw, above failure surface, u =gwhw cos
2b
hw cos2b
b
hw cos b
hw
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Infinite slope: effective stress analysis
If c' = 0 and steady seepage parallel to ground level with groundwatertable vertical height, hw, above failure surface
F = (1 m. gw/g) tan f', where m = hw/z
tan b
If m = 1, F = (g' /g) tan f'
tan b
If m = 1 and F = 1, tan b = (g' /g) tan f', which is approximately = tan f'
2
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Infinite slope: total stress analysis
Saturated soils: fu = 0
F = S = cul = cuW sinb g xz x b gz sinb cosb
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Stability analysis with circular failure surface
d
q
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Stability analysis with circular failure surface
Undrained analysis (fu = 0)
Disturbing moment = W x d
Resisting moment = tmob x r q x r
tmob
= cu
/ F, where F is the factor of safety
F = cu r2q
W d
The critical failure surface is found by searching for theposition of centre of rotation, O, and radius, r, with thelowest F
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Stability analysis with circular failure surface
Undrained/Total stress analysis (fu = 0)
Tension cracks tend in cohesive soils and can be filled with water.
For analysis, refer to Whitlow pages 363 & 364.
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Stability analysis with circular failure surface
Drained/Effective stress analysis (c'f' soil)
Method of slices
The assumed failed mass is divided into a number of slices, theirforce systems are analysed and are then summed up to produce anaverage factor of safety.
The minimum factor of safety is found by analysing many trialcircles.
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Stability analysis with circular failure surface
Method of slices
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Stability analysis with circular failure surface
Method of slices
a
l
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Stability analysis with circular failure surface
Fellenius / Swedish method
It is assumed that
(En En+1) = 0
(Xn Xn+1) = 0
F =
l
= bseca
F =
The Fellenius method underestimates F by 5 to 20%.
S [c'l+ (Wcos a ul)tan f]
S Wsina
S [c'b + (Wcos2a ub)tan f']seca
S Wsina
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Stability analysis with circular failure surface
Bishops simplified method
It is assumed that (Xn Xn+1) = 0, but (En En+1) 0
F =
As F appears on both sides of the equation, F is found by an iterative
process of successive approximations. First, a trial value of F is input
on the right hand side of the equation to obtain a new value of F, which
is substituted back into the right hand side of the equation until F
converges to an acceptable accuracy. The Bishops simplified method
underestimates F by less than 3%.
S Wsina
1S
[c'b + (W ub)tan f']seca
1 + tan a tan f' / F
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Slope stability analysis
Pore pressure ratio, ru
The porewater pressure at a given point in a slope is also given in terms of ru
which is the ratio of the porewater pressure to the weight of the soil per unit
area above the point.
ru
= u/gz
Bishops simplified method
ub/W = ub/gzb = ru
F =
F =
S Wsina1 S [c'b + (W ub)tan f']seca1 + tan a tan f' / F
S Wsina
1S
[c'b + W(1 ru)tan f']seca
1 + tan a tan f' / F
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