DHARM322 GEOTECHNICAL ENGINEERINGThe factor of safety against slippage may be written as:F =^1 −F
HGI
KJ=F −
HGI
KJ= ′γ
γφ
βγγ
γφ
βγ
γφ
βwwtan
tantan
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.zczPurely
cohesive soilLedgetcO sbD( , )stnP(stnf, )fBs = c Strength envelopeAQ(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 shouldlie on a line through origin O inclined at the angle of slope β, sinceτ
σn= tan β. If this point Dlies 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.