The reason for the freezing in of a magnetic field and the reasons for
the disruption of this effect in a collisionless plasma are analyzed.
The concept of a ''freezing-in preserver'' is introduced. In a tokama
k, the role of this preserver may be played by untrapped electrons, wh
ich are not at resonance with turbulence and which thus execute an int
egrable motion. As a result, the poloidal magnetic field is frozen in
the toroidal field. Under these conditions the diffusion of particles
and heat may be governed by turbulence, in agreement with experiment.