The stability of a planar slab of electron plasma confined in the tran
sverse direction by a longitudinal magnetic field is investigated nume
rically. The plasma slab can be created by using either a nonequipoten
tial of equipotential cathode that. in the general case, makes it nece
ssary to take into account the nonuniformity of the longitudinal and t
ransverse electron velocities. If the magnitude and direction of the m
agnetic field at the cathode are chosen properly, the plasma frequency
can be higher than the cyclotron frequency. It is shown that, in this
cast, an instability inevitably arises in the system; this instabilit
y leads to the growth of disturbances that are similar to Taylor's vor
tex cells. This fact indicates a similarity between this instability a
nd the Rayleigh-Taylor instability, which is known from conventional h
ydrodynamics.