Linear stability and weak nonlinear theories are used to investigate analyt
ically the Coriolis effect on three-dimensional gravity-driven convection i
n a rotating porous layer heated from below. Major differences as well as s
imilarities with the corresponding problem in pure fluids (non-porous domai
ns) are particularly highlighted. As such, it is found that, in contrast to
the problem in pure fluids, overstable convection in porous media is not l
imited to a particular domain of Prandtl number values (in pure fluids the
necessary condition is Pr < 1). Moreover, it is also established that in th
e porous-media problem the critical wavenumber in the plane containing the
streamlines for stationary convection is not identical to the critical wave
number associated with convection without rotation, and is therefore not in
dependent of rotation, a result which is quite distinct from the correspond
ing pure-fluids problem. Nevertheless it is evident that in porous media, j
ust as in the case of pure fluids subject to rotation and heated from below
, the viscosity at high rotation rates has a destabilizing effect on the on
set of stationary convection, i.e. the higher the viscosity the less stable
the fluid. Finite-amplitude results obtained by using a weak nonlinear ana
lysis provide differential equations for the amplitude, corresponding to bo
th stationary and overstable convection. These amplitude equations permit o
ne to identify from the post-transient conditions that the fluid is subject
to a pitchfork bifurcation in the stationary convection case and to a Hopf
bifurcation associated with the overstable convection. Heat transfer resul
ts were evaluated from the amplitude solution and are presented in terms of
Nusselt number for both stationary and overstable convection. They show th
at rotation has in general a retarding effect on convective heat transfer,
except for a narrow region of small values of the parameter containing the
Prandtl number where rotation enhances the heat transfer associated with ov
erstable convection.