For the mechanical behavior of poroelastic media, the method of homoge
nization has been applied to derive effective equations on the macrosc
ale, for a matrix with a periodic structure on the microscale. In exis
ting theories the resulting effective equations are linear, which not
only confirm the phenomenological theory of Blot [J. Appl, Phys. 12, 1
55-165 (1941)], but also provide a theoretical framework for calculati
ng the constitutive coefficients. We point out that all past authors a
pplied the continuity of displacement and stresses at the initial and
undeformed solid-water interface. this implies that the solid displace
ment, due either to global or local strain, must be much smaller than
the granular or pore size. Here we shall allow the matrix displacement
corresponding to the global strain to be comparable to the granular s
ize, and show that the resulting effective equations are non-linear in
general. The constitutive coefficients of the non-linear terms nevert
heless vanish under two conditions: (i) when the global-scale deformat
ion is also much smaller than the granular size, and (ii) when the glo
bal-scale deformation is comparable to the granular or pore size, but
the microcell geometry is symmetric with respect to three orthogonal p
lanes. The first limit is trivial and is no different from the existin
g theories. The second limit is not trivial and shows the robustness o
f the linearized equations. The result suggests that the linear effect
ive equations may be adequate even for practical problems involving no
t-too-small deformation or loading, as long as the microscale geometry
is isotropic in the statistical sense. (C) 1997 Elsevier Science Ltd.