  We study the density of states and magnetotransport properties of disordered
Weyl semimetals, focusing on the case of a strong long-range disorder. To
calculate the disorder-averaged density of states close to nodal points, we
treat exactly the long-range random potential fluctuations produced by charged
impurities, while the short-range component of disorder potential is included
systematically and controllably with the help of a diagram technique. We find
that for energies close to the degeneracy point, long-range potential
fluctuations lead to a finite density of states. In the context of transport,
we discuss that a self-consistent theory of screening in magnetic field may
conceivably lead to non-monotonic low-field magnetoresistance.
