DHARM560 GEOTECHNICAL ENGINEERINGwhere Ppn = normal component of the passive earth pressure on a plane contact face with a
height H,
α = slope angle of the contact face, and
Kpc, Kpq, and Kpγ = coefficients whose values are indpendent of H and γ. In the present case,H =b
2tan φ, α = 180° – φ, δ = φ.Also the total passive earth pressure Pp on the contact face is equal toPpn
cosδ.∴ Pp =Ppn
cosδ=Ppn
cosφ=b
2 cos^2 φ(cKpc + qKpq) +1
242
γ 2φ
φ..tan
cosb. Kpγ ...(Eq. 14.64)
where (cKpc + qKpq) = Ppn is the normal component of the passive earth pressure comprehend-
ing the effect of cohesion and surcharge.
Combining this equation with Eq. 14.58, we haveqult = cKpc
cos
2 tan
φφ+F
HGI
KJ+ qKpq
cos^2 φ+ γb
4tan φKpγ
cos^2 φ− 1F
HGI
KJ...(Eq. 14.65)wherein Kpc, Kpq, and Kpγ are pure numbers whose values are independent of b.
If the soil wedge, ABC, is assumed weightless (γ = 0) (Prandtl, 1920), Eq. (14.65) takes
the formqqultcq+ ult = cKpc
cos
2 tan
φφ+F
HGI
KJ+ q.Kpq
cos^2 φ
= cNc + q. Nq ...(Eq. 14.66)
The factors Nc and Nq are pure numbers whose values depend only on the value φ in
Coulomb’s equation. The value qultcrepresents the bearing capacity of the weightless soil, ifthe surcharge q were equal to zero (γ = 0 and q = 0), and qultqis the bearing capacity exclusively
due to the surcharge q(γ = 0 and c = 0).
On the other hand, if c = 0 and q = 0, γ being greater than zero, the bearing capacity is
given by Eqs. 14.61 and 14.62:
qult =^1
21
4γγφ 2 1
γ φ
bN =−b F Kpγ
HGI
KJtan
cos
(However, it should be noted that the failure surface for this condition is somewhat
above that for γ = 0, and also the exact mathematical shape is not known).
If the values c, Df,and γ are greater than zero,qult = qultc + qultq+ qultr = cNc + γDf Nq +1
2γb Nγ ...(Eq. 14.67)
This is called ‘‘Terzaghi’s general bearing capacity formula’’. (The discrepancy arising
out of the difference in failure surfaces for the two conditions—γ = 0 and γ > 0—is considered
inconsequential).
The coefficients Nc, Nq, and Nγ are called ‘‘bearing capacity factors’’ for shallow continu-
ous footings. Since their values depend only on the angle of shearing resistance φ they can be
computed once and for all.