  Here we derive the relativistic resistive dissipative second-order
magnetohydrodynamic evolution equations using the Boltzmann equation, thus
extending our work from the previous paper
\href{https://link.springer.com/article/10.1007/JHEP03(2021)216}{JHEP 03 (2021)
216} where we considered the non-resistive limit. We solve the Boltzmann
equation for a system of particles and antiparticles using the relaxation time
approximation and the Chapman-Enskog like gradient expansion for the
off-equilibrium distribution function, truncating beyond second-order. In the
first order, the bulk and shear stress are independent of the electromagnetic
field, however, the diffusion current, shows a dependence on the electric
field. In the first order, the transport coefficients~(shear and bulk stress)
are shown to be independent of the electromagnetic field. The diffusion
current, however, shows a dependence on the electric field. In the
second-order, the new transport coefficients that couple electromagnetic field
with the dissipative quantities appear, which are different from those obtained
in the 14-moment approximation~\cite{Denicol:2019iyh} in the presence of the
electromagnetic field. Also we found out the various components of conductivity
in this case.
