  We derive the equations of motion of relativistic, resistive, second-order
dissipative magnetohydrodynamics from the Boltzmann-Vlasov equation using the
method of moments. We thus extend our previous work [Phys. Rev. D 98, 076009
(2018)], where we only considered the non-resistive limit, to the case of
finite electric conductivity. This requires keeping terms proportional to the
electric field $E^\mu$ in the equations of motions and leads to new transport
coefficients due to the coupling of the electric field to dissipative
quantities. We also show that the Navier-Stokes limit of the charge-diffusion
current corresponds to Ohm's law, while the coefficients of electrical
conductivity and charge diffusion are related by a type of Wiedemann-Franz law.
