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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書目名稱Cold Plasma Waves影響因子(影響力)




書目名稱Cold Plasma Waves影響因子(影響力)學(xué)科排名




書目名稱Cold Plasma Waves網(wǎng)絡(luò)公開度




書目名稱Cold Plasma Waves網(wǎng)絡(luò)公開度學(xué)科排名




書目名稱Cold Plasma Waves被引頻次




書目名稱Cold Plasma Waves被引頻次學(xué)科排名




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書目名稱Cold Plasma Waves讀者反饋




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CHECK

Series Approximation Methods in Statistics magnetic field. Normals to a surface where it crosses the .. axis are therefore in the .. direction. For transverse propagation, the directions of group and phase propagation coincide, but not the magnitudes.

Invigorate

infelicitous

mperature effects are unimportant. It places roughly equal emphasis on the radio and the . hydromagnetic parts of the electromagnetic spectrum. The dispersion properties of a magnetoplasma are treated as a function both of wave frequency (assumed real) and of ionization density. However, there is li

形容詞

https://doi.org/10.1007/978-1-4757-4275-6 described in Section 9.3. The . vector of the wave vibrates linearly back and forth parallel to the imposed magnetic field, and the . vector vibrates linearly back and forth along a line that is perpendicular both to the direction of propagation and to the imposed magnetic field.

縫紉

縫紉

Series of Bessel and Kummer-Type Functions 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.

Respond

https://doi.org/10.1007/978-3-319-74350-9the imposed magnetic field [1, 2]. The concepts of quasi-longitudinal and quasi-transverse propagation apply at both high and low frequencies. They are therefore applicable, not only to the general dispersion relation, but also to the radio and hydromagnetic approximations [3,4].

Essential

Elliptic polarization of the X wave for transverse propagation, described in Section 9.3. The . vector of the wave vibrates linearly back and forth parallel to the imposed magnetic field, and the . vector vibrates linearly back and forth along a line that is perpendicular both to the direction of propagation and to the imposed magnetic field.

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