The transfer equations and Fourier law analogues have been obtained fo
r three types of non-local media: media with heat memory, spatially no
n-local media and media with a discrete structure. The conditions are
specified under which these equations reduce into each other or to fam
iliar transfer equations, such as the classical parabolic-type transpo
rt equation and 'telegraph' equation. It is shown that the type of par
tial differential equations derived from discrete transfer equations i
s governed by the limiting transition law, i.e. by the relationship be
tween the time, tau, and space, h, scales of the medium internal struc
ture. In the case of the 'diffusional' law of limiting transition, whe
n the thermal diffusivity coefficient a = h2/4tau = const for r, h -->
0, the discrete equations yield parabolic-type partial differential e
quations, whereas with the 'wave' law of limiting transition, when the
heat wave speed c = h/2tau = const < infinity for tau, h --> 0, they
yield partial differential equations of hyperbolic type.