Effects of finite plasma dimension on the whistler wave propagation in a dense plasma (ω 2 p ≫ω 2 c ) are investigated theoretically and experimentally. Dispersion relation for whistler waves in a cylindrical plasma of radius a is solved and compared with the infinite plane wave solution. For \(ωₚa/c{}10\), the finite size effects become so significant that, below half the electron cyclotron frequency ω c , the phase velocity and the damping rate increase in comparison with the infinite case. Measured dispersion and attenuation are well described by the finite plasma theory.
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Sugai et al. (1978) studied this question.
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