Electrons can crystallize to form a Wigner crystal. This crystallization is
particularly effective in two dimensions. The effect of disorder on such electronic crystals can be taken
into account using the same techniques and concepts, in particular the notion of Bragg glass
phase, than the one developed to tackle classical disordered elastic systems. We analyze the
properties of such a disordered Wigner crystal and discuss the physical consequences, both for
the thermodynamics (compressibility etc.) and for the transport properties. This approach
allows a good description of the optical conductivity and in particular to obtain correctly the
density and field dependence of the pinning frequency. Relevance to experimental systems is
discussed.