DHARM
322 GEOTECHNICAL ENGINEERING
The factor of safety against slippage may be written as:
F =^1 −
F
HG
I
KJ
=
F −
HG
I
KJ
= ′
γ
γ
φ
β
γγ
γ
φ
β
γ
γ
φ
β
wwtan
tan
tan
tan
.tan
sat tan ...(Eq. 9.7)
9.2.2 Infinite Slope in a Purely Cohesive Soil
Let us consider an infinite slope in purely cohesive soil as shown in Fig. 9.5.
zc
z
Purely
cohesive soil
Ledge
t
c
O s
b
D( , )stn
P(stnf, )f
Bs = c Strength envelope
A
Q
(a) Infinite slope in purely cohesive
soil-critical depth
(b) Relation between strength envelope
and angle of slope
Fig. 9.5 Infinite slope in a purely cohesive soil
For a particular depth z, the values of the normal and shear stresses at the base of the
element are given by Eqs. 9.2 and 9.3, i.e.,
σn = γ. z cos^2 β
and τ = γ. z sin β. cos β
If these are represented as co-ordinates on a σ – τ plot, point D is obtained. This should
lie on a line through origin O inclined at the angle of slope β, since
τ
σn
= tan β. If this point D
lies below the Coulomb strength envelope, s = c for the purely cohesive soil, the slope will be
stable.
The factor of safety against slippage will be AB
AD
, at a depth z from the surface.
∴ F = c/τ =
c
γββzsin cos
...(Eq. 9.8)
If the line OD is extended it will meet the horizontal strength envelope at a point, say P,
the foot of the perpendicular from P on to σ-axis being Q. The point P represents a stress
condition for a different depth, greater than z. At this point the shearing stress at the base of
the element equals the shearing strength of the soil; that is to say, failure is incipient at this
depth. In other words, the slope will be stable only up to a maximum depth zc, called the
critical depth, at which the shearing stress reaches the value of the shearing strength of the
soil, which is merely c in this case, as it is a purely cohesive soil. A ledge or some other material
with a sufficiently large strength exists below the soil of critical depth.
The critical depth zc can be evaluated by equating F to unity.