For a moderate level of turbulence, the self-consistent nonuniform profiles
of the turbulent equipartition (TEP) of the density and temperature distri
bution of magnetized electrons in a tokamak were found analytically and num
erically. Only conservation of the adiabatic invariants of the electrons is
needed for the solution of this problem. For passing electrons, the profil
e of the density is determined mainly by the flat radial dependence of the
helicity (AB)(r), in contrast to the pinched profile similar to 1/q of the
trapped electrons determined by the safety factor q(r). The numerically obt
ained, combined profile of the electron density n similar to 1/q(0.58) was
found to be similar to a particular experimental scaling. Also, it was asce
rtained that the high pinching of the temperature profile is mainly determi
ned by the heating of passing electrons in the potential energy well of the
poloidal magnetic field, and depends on the beta(phi) (ratio of the therma
l energy to the magnetic one) value. Large values of beta(phi) give small t
emperature pinching. The TEP distribution also gives one the possibility to
obtain self-consistently the profile and the level of the turbulent fluctu
ations due to the development of quick kinetic instabilities associated wit
h the TEP distribution. The estimation of the time of turbulent mixing of t
he electrons in the tokamak volume gives a realistic value of the order of
10 ms in the central part of tokamak and 0.1 s in the region near the separ
atrix. (C) 1999 American Institute of Physics. [S1070-664X(99)00708-9].