By considering an ensemble of Brownian particles suspended in a heat b
ath as a thermodynamic system with an internal degree of freedom it is
possible to obtain the Fokker-Planck equation for Brownian motion in
a temperature gradient, by applying the scheme of non-equilibrium ther
modynamics. We recover explicitely the equations derived in particular
by Zubarev and Bashkirov using statistical mechanical and kinetic met
hods. In addition when the temperature gradient does not have an exter
nally imposed magnitude we obtain the differential equation for the te
mperature field, which is coupled to the Fokker-Planck equation.