  Since nearly 4 decades, various theoretical behaviours have been found for
the thermopower in the variable range hopping regime. In 1969, Cutler and Mott
have predicted a linear variation with temperature T of the thermopower: S =
const.T. In the seventies, it has beenfound by Zvyagin, Overhof and Mott that S
= const.T(1/2). In 1986, Triberis and Friedman have found S = const.T^(-1/4) .
But there is up to now no theoretical formulation of the thermopower when this
one is T-independent. By choosing a specific distribution for the density of
states, we show in this paper that all behaviours above can be unified in a
unique thermopower formula. We find in addition with this formula, a
T-independent expression given by: S=(L/xi)(k/e), in which xi is the wave
function decay length and L is a characteristic length, depending on the form
of the density of states.
