The self-consistent electron potential in a current-carrying disordered qua
ntum wire is spatially inhomogeneous due to the formation of resistivity di
poles across scattering centres. In this paper it is argued that these inho
mogeneities in the potential result in a suppression of the differential co
nductance of such a wire at finite applied voltage. A semi-classical argume
nt allows this suppression, quadratic in the voltage, to be related directl
y to the amount of intrinsic defect scattering in the wire. This result is
then tested against numerical calculations.