The process of magnetic field influence on the movement of a viscous,
conducting liquid was described by using a Maxwell-Navier-Stokes syste
m of equations. By introducing vector potentials psi, xi, A and elemen
ts of dimensional analysis there was educed a non-linear Poisson equat
ion for a function describing pressure distribution in a flat channel.
For a Poiseulle flow there was formulated a Neuman boundary condition
in a generalised form as an integral identity. To solve the above pro
blem, finite element approximation method was used. Appropriate numeri
cal experiments were conducted. The calculation results were presented
as a family of constant pressure lines and as lines of pressure value
on the channel boundaries. All the experiments were performed for dif
ferent values of criterion numbers: Reynolds (R-e), Reynolds magnetic
(R-m) and Hartman (H-a).