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Titlebook: Cold Plasma Waves; Henry G. Booker Book 1984 Martinus Nijhoff Publishers, Dordrecht 1984 Maxwell’s equations.behavior.density.electric cur

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樓主: 果園
11#
發(fā)表于 2025-3-23 11:49:22 | 只看該作者
The hydromagnetic approximation, Section 7.6, and for transverse propagation in Section 9.6. We now proceed to employ the hydromagnetic approximation for propagation in a magnetoplasma in any direction relative to the imposed magnetic field.
12#
發(fā)表于 2025-3-23 16:40:53 | 只看該作者
13#
發(fā)表于 2025-3-23 21:59:52 | 只看該作者
14#
發(fā)表于 2025-3-23 22:30:25 | 只看該作者
Directional behaviour of group velocity in a magnetoplasma,but only for the whistler wave, and then only when the ionization density is sufficiently high to make the plasma frequency substantially greater than the electronic gyrofrequency. It still remains to provide calculations of group velocity in a magnetoplasma in both magnitude and direction that are reasonably comprehensive.
15#
發(fā)表于 2025-3-24 03:06:36 | 只看該作者
16#
發(fā)表于 2025-3-24 08:11:33 | 只看該作者
17#
發(fā)表于 2025-3-24 11:29:07 | 只看該作者
https://doi.org/10.1007/0-387-32227-2y Maxwell’s equations, we will need to know something about the physics of a plasma. Specifically, we will need to be able to relate the electromagnetic field of a wave to the charge and current densities created in the plasma by the wave.
18#
發(fā)表于 2025-3-24 17:53:26 | 只看該作者
Series Approximation Methods in Statistics oscillatory, is uniform in space. We are then considering a homogeneous plasma that is simultaneously subject to a uniform steady magnetic field of flux density .. and to a uniform electric field E that oscillates with angular frequency ω
19#
發(fā)表于 2025-3-24 21:42:04 | 只看該作者
20#
發(fā)表于 2025-3-25 01:40:53 | 只看該作者
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