A linear theory of drift mirror instability accounting for the nonzero elec
tron temperature effects is developed. Generalizing our previous approach t
o the analysis of this instability by accounting for a nonvanishing paralle
l electric field, we have derived the expressions for the mode frequency an
d instability growth rate. The origin of the electric field is due to the e
lectron pressure gradient which builds up in a plasma with nonzero electron
temperature, because the electrons are dragged by mirror-accelerated proto
ns as they pass from regions of high magnetic flux into those of lower magn
etic flux. The electrostatic force drag associated with the parallel electr
ic field provides a substantial reduction of the wave phase velocity and in
creases the drift mirror instability threshold. It is shown that in a plasm
a with nonzero electron temperature the drift mirror mode is accompanied by
the field-aligned current which varies in phase with the compressional cha
nges in the magnetic field. The transition to the cold electron temperature
limit is discussed.