The adhesive contact between a solid sphere and an elastic half space has b
een treated by Johnson, Kendall, and Roberts (JKR)(1) for zero interfacial
friction (slip boundary condition). The result is the famous JKR theory, wh
ich is now widely used. However, in the real situation, the interfacial fri
ction may not be negligible especially when the contact is adhesive. A solu
tion corresponding to the infinite interfacial friction (stick boundary con
dition) is derived in this paper. The results show that the effect of inter
facial friction depends on the Poisson ratio of the elastic half space. For
an incompressible half space, the two solutions are identical. These two s
olutions can be thought of as the lower and upper bonds for the general cas
e of finite interfacial friction.