  We investigate the properties of a three-dimensional homogeneous dipolar Bose
gas in a weak random potential with a Gaussian correlation function at finite
temperature. Using the Bogoliubov theory (beyond the mean field), we calculate
the superfluid and the condensate fractions in terms of the interaction
strength on the one hand and in terms of the width and the strength of the
disorder on the other. The influence of the disordered potential on the second
order correlation function, the ground state energy and the chemical potential
is also analyzed. We find that for fixed strength and correlation length of the
disorder potential, the dipole-dipole interaction leads to modify both the
condensate and the superfluid fractions. We show that for a strong disorder
strength the condensed fraction becomes larger than the superfluid fraction. We
discuss the effect of the trapping potential on a disordered dipolar Bose in
the regime of large number of particles.
