  We calculate analytically the low temperature quasi-particle scattering rate,
the conductivity, and the specific heat in weakly disordered metals close to a
quantum critical point, via the use of a proper fluctuation potential
$V(q,\omega)$ between the quasi-particles. We obtain typical Fermi liquid
results proportional to $T^2$ and $T$ respectively, with prefactors which
diverge as power laws of the control parameter $a$ upon approaching the
critical point. The Kadowaki-Woods ratio is shown to be independent of $a$
(possibly times a logarithmic dependence on $a$) only for the case of
three-dimensional ferromagnetic fluctuations. Our results are consistent with
experiments on the eight materials CeCoIn$_5$, Sr$_3$Ru$_2$O$_7$,
YbRh$_2$Si$_2$, La$_{2-x}$Ce$_x$CuO$_4$, Tl$_2$Ba$_2$CuO$_{6+x}$, CeAuSb$_2$,
YbAlB$_4$, and CeRuSi$_2$.
