Abstract

The effects of finite geometry on the frequency spectrum and mode structure of ion-acoustic oscillations in an equilibrium (Te=Ti) plasma are investigated. Numerical and analytical results for one-dimensional models of collisionless plasmas with both absorbing and reflecting boundaries show that these modes are strongly damped. With absorbing boundaries the fluctuations are damped in an ion-transit time. For reflecting boundaries the frequency spectrum is identical to the heavily Landau-damped spectrum for an unbounded plasma. These theoretical calculations suggest that the weakly damped, low-frequency density fluctuations recently observed in incandescent cavities are not ion-acoustic waves.

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