  The confinement mechanism proposed earlier and then applied successfully to
meson spectroscopy by one of the authors is interpreted in classical terms. For
this aim the unique solution of the Maxwell equations, an analog of the
corresponding unique solution of the SU(3)-Yang-Mills equations describing
linear confinement in quantum chromodynamics, is used. Motion of a charged
particle is studied in the field representing magnetic part of the mentioned
solution and it is shown that one deals with the full classical confinement of
the charged particle in such a field: under any initial conditions the particle
motion is accomplished within a finite region of space so that the particle
trajectory is near magnetic field lines while the latter are compact manifolds
(circles). An asymptotical expansion for the trajectory form in the strong
field limit is adduced. The possible application of the obtained results in
thermonuclear plasma physics is also shortly outlined.
