  In this paper I report a pedagogical derivation of the unconventional
electronic hydrodynamics in graphene on the basis of the kinetic theory. While
formally valid in the weak coupling limit, this approach allows one to derive
the unconventional hydrodynamics in the system which is neither Galilean- nor
Lorentz-invariant, such that hydrodynamic equations can not be inferred from
symmetry arguments. I generalize earlier work to include external magnetic
fields and give explicit expressions for dissipative coefficients, the shear
viscosity and electrical conductivity. I also compare the resulting theory with
relativistic hydrodynamics.
