  We consider a hydrodynamic description of transport for generic two
dimensional electron systems that lack Galilean invariance and do not fall into
the category of Fermi liquids. We study magnetoresistance and show that it is
governed only by the electronic viscosity provided that the wavelength of the
underlying disorder potential is large compared to the microscopic
equilibration length. We also derive the Coulomb drag transresistance for
double-layer non-Fermi liquid systems in the hydrodynamic regime. As an
example, we consider frictional drag between two quantum Hall states with
half-filled lowest Landau levels, each described by a Fermi surface of
composite fermions coupled to a $U(1)$ gauge field. We contrast our results to
prior calculations of drag of Chern-Simons composite particles and place our
findings in the context of available experimental data.
