In a porous or cracked elastic solid, the effective stress (defined in term
s of the loads applied to the solid part of the outer boundary) and effecti
ve strain (defined in terms of the displacements at the solid part of the o
uter boundary) occurring in small-amplitude deformations are connected by a
linear relation along with the pressure within the fluid occupying the por
es and cracks. We derive here a formula of this kind for a static system in
which enough time is allowed for pressure to be equalized throughout the f
luid (on the assumption that all pockets of fluid are connected in some way
). The formula depends on the overall stiffnesses relating stress to strain
for the same material with the fluid removed (dry or empty cracks and pore
s). For undrained conditions where no fluid is allowed to enter or leave th
e body, the pressure is directly related to the effective stress and strain
, and the Gassmann relations are obtained relating the stiffnesses for an i
sotropic material in dry and undrained conditions. For an anisotropic mater
ial, the Brown-Korringa relations are recovered. Externally imposed stresse
s and fluid pressure distort the material structure and influence the wave
speeds of elastic waves. The main way in which this occurs is in changing t
he aspect ratios of flat cracks, the most compliant part of the microstruct
ural geometry. This effect on the wave speeds is studied here both in terms
of crack closure, with corresponding changes in crack number density, and
in variations in crack aspect ratios. The principal way in which the latter
influences the wave speeds is through the fluid incompressibility factor i
n the formula for the properties of materials with connected cracks. An inc
rease in aspect ratio of the cracks is equivalent to a reduction in the bul
k modulus of the fluid. This effect is apparent in the limits of both high
frequencies, when the material behaves as if the cracks were isolated, and
low frequencies, when undrained conditions apply.