We present calculations of the temperature-dependent electrostatic and
chemical potential distributions in disordered normal metal-supercond
uctor structures. We show that they differ appreciably in the presence
of a superconducting terminal and propose an experiment to measure th
ese two different potential distributions. We also compute the resista
nce change in these structures due to a recently proposed mechanism wh
ich causes a finite effect at zero temperature. The relative resistanc
e change due to this effect is of the order of the interaction paramet
er in the normal metal. Finally a detailed calculation of the resistan
ce change due to the temperature dependence of Andreev reflection in d
iffusive systems is presented. We find that the maximal magnitude due
to this thermal effect is in general much larger than the magnitude of
the interaction effect.