We extend our previous theory for the ground state of a disordered ele
ctron solid to calculate its transport properties. The Coulomb interac
tion is taken in the Hartree-Fock approximation and the potential of c
harged impurities in the self-consistent Born approximation. In agreem
ent with recent experiments by Li et al. we find, for strong disorder,
a linear frequency dependence of the in-phase conductivity. We show h
ow the dc conductivity of the system can be determined in our theory.
At strong disorder an algebraic temperature dependence of the conducti
vity results which is consistent with experiments by Goldman et al.