We present a Green's function theory of the rough surface effects on t
he anisotropic BCS states using the formulation developed in the rando
mly rippled wall model. It is shown that the randomly rippled wall for
mulation is general enough to treat rough surface effects from the spe
cular limit to the diffusive limit. We propose a statistical wall conf
iguration such that gives the diffusive limit in the normal state. Wit
hin the weak coupling theory, we give a formal solution of the quasi-c
lassical Green's function in a slab geometry and in a semi-infinite ge
ometry with arbitrarily rough surfaces. The formal solution already sa
tisfies the boundary condition. In the diffusive limit, the present th
eory correctly recovers the linearized gap equation obtained by Kjaldm
an et al. for the p-wave state in a slab geometry.