Abstract

Collisionless power dissipation has been calculated analytically taking into account particle trapping in the wave and electron collisions with neutrals. The approximation of analytical calculations for a decrement of nonlinear Landau damping gives, within an error less than $5%$, ${\ensuremath{\gamma}}_{\mathrm{nl}}\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}{\ensuremath{\gamma}}_{l}\mathrm{tanh}(2\ensuremath{\nu}{\ensuremath{\tau}}_{r}),$ where ${\ensuremath{\gamma}}_{l}$ is the linear Landau damping, $\ensuremath{\nu}$ is the total collision frequency, and ${\ensuremath{\tau}}_{r}$ is a bounce time of trapped electrons. The theory is applied to the calculation of collisionless heating in a bounded low-pressure glow discharge plasma. It is shown that the difference with previously published results of linear theory on collisionless power dissipation can be as large as 3 orders of magnitude.

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