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Transport coefficients of inhomogeneous, magnetized plasmas are derived using the quasilinear approximation. It is shown that mechanisms which allow the motion of ions across the magnetic field, such as ion-neutral collisions, are essential in arriving at divergent-free, finite transport coefficients in unbounded plasmas. The transport coefficients are calculated for both unbounded and bounded plasmas. Although in toroidal plasmas the transport coefficients do not follow the 1/B law, the calculated diffusion coefficients are numerically very close to what is known as the Bohm diffusion coefficients in a number of experimental devices.
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S. Yoshikawa (1970) studied this question.
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