The process of steady heat conduction in a composite in which equal spheric
al inclusions are distributed according to a non-uniform probability distri
bution is studied numerically. While the standard results are recovered in
the uniform case, the nonuniformity introduces a non-local correction in th
e form of a difference between the average temperatures in the two phases.
As a consequence, the relation between the mean heat flux and the phase tem
peratures must be expressed in terms of two effective conductivities rather
than only one as in the uniform case. In other words. contrary to the situ
ation encountered with a uniform composite, an effective Fourier law of con
duction of the standard form does not hold for a non-uniform composite. In
addition to an equation expressing the overall energy balance, closure of t
he system of. averaged equations requires a second relation that reveals th
e non-local origin of the difference between the phase temperatures. This s
econd equation involves two coefficients, dependent on the particle volume
fraction. The method used in this paper establishes a relation between the
two, but does not determine them individually.
The technique developed for the heat-conduction problem studied here can be
adapted to the modelling of other disperse physical systems such as non-un
iform suspensions.