標題: Titlebook: Cold Plasma Waves; Henry G. Booker Book 1984 Martinus Nijhoff Publishers, Dordrecht 1984 Maxwell’s equations.behavior.density.electric cur [打印本頁] 作者: 果園 時間: 2025-3-21 20:06
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)學科排名
書目名稱Cold Plasma Waves網(wǎng)絡公開度
書目名稱Cold Plasma Waves網(wǎng)絡公開度學科排名
書目名稱Cold Plasma Waves被引頻次
書目名稱Cold Plasma Waves被引頻次學科排名
書目名稱Cold Plasma Waves年度引用
書目名稱Cold Plasma Waves年度引用學科排名
書目名稱Cold Plasma Waves讀者反饋
書目名稱Cold Plasma Waves讀者反饋學科排名
作者: CHECK 時間: 2025-3-21 22:44
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.作者: Invigorate 時間: 2025-3-22 04:23 作者: infelicitous 時間: 2025-3-22 08:25
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作者: 形容詞 時間: 2025-3-22 12:05
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.作者: 縫紉 時間: 2025-3-22 13:59 作者: 縫紉 時間: 2025-3-22 18:56
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.作者: Respond 時間: 2025-3-22 22:16
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].作者: Essential 時間: 2025-3-23 04:00
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.作者: 聯(lián)想 時間: 2025-3-23 06:12 作者: 相反放置 時間: 2025-3-23 11:49
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.作者: 猛烈責罵 時間: 2025-3-23 16:40 作者: BATE 時間: 2025-3-23 21:59 作者: ALERT 時間: 2025-3-23 22:30
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.作者: glans-penis 時間: 2025-3-24 03:06 作者: MAOIS 時間: 2025-3-24 08:11 作者: Androgen 時間: 2025-3-24 11:29
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.作者: Nucleate 時間: 2025-3-24 17:53
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作者: 冬眠 時間: 2025-3-24 21:42 作者: thrombosis 時間: 2025-3-25 01:40 作者: radiograph 時間: 2025-3-25 06:50 作者: Saline 時間: 2025-3-25 09:10
https://doi.org/10.1007/978-1-4757-4275-6nstitute a right-handed mutually perpendicular system of directions. For transverse propagation of the . wave, these vectors are linearly polarized as 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作者: 作嘔 時間: 2025-3-25 11:44
Series Approximation Methods in Statisticsc field of the wave back and forth along the imposed magnetic field, together with elliptic polarization of the electric field in a plane perpendicular to the imposed magnetic field. Using the axes indicated in Figure 10.1, the wave is propagating in the . direction and the electric field is . = (.,作者: 內(nèi)閣 時間: 2025-3-25 17:12
Operator Theory: Advances and Applicationsion as described in Chapter 6. It is convenient to begin by supposing that the direction of phase propagation is specified. We are then considering an infinite homogeneous plasma subject to a steady uniform magnetic field, and waves are being launched from an infinite antenna plane whose normal make作者: Antioxidant 時間: 2025-3-26 00:00 作者: 先行 時間: 2025-3-26 00:12
Series of Bessel and Kummer-Type Functionsn has to be replaced by the hydromagnetic approximation (Section 5.7). We have studied the hydromagnetic approximation for longitudinal propagation in Section 7.6, and for transverse propagation in Section 9.6. We now proceed to employ the hydromagnetic approximation for propagation in a magnetoplas作者: URN 時間: 2025-3-26 07:12
https://doi.org/10.1007/978-3-319-74350-9 depends on whether propagation in the direction of interest is roughly like that along the imposed magnetic field or roughly like that transverse to the imposed magnetic field [1, 2]. The concepts of quasi-longitudinal and quasi-transverse propagation apply at both high and low frequencies. They ar作者: Aggrandize 時間: 2025-3-26 09:28
Droop-Based Economical Dispatchh the ionization density is discussed in Sections 13.5, 13.6 and 13.9 using the radio approximation, and in Sections 14.8, 14.9 and 14.12 using the hydromagnetic approximation. The variation of the magnitude of the group velocity with frequency is discussed in Section 8.4 for longitudinal propagatio作者: 幼兒 時間: 2025-3-26 12:42
Droop-Based Economical Dispatchst descent. In this chapter we shall employ the results to study the directional behaviour of the radiated power. We shall plot diagrams to show how the radiated power density varies with the direction of group propagation. In addition, we shall calculate the radiation resistance of the antenna.作者: 子女 時間: 2025-3-26 17:00 作者: fertilizer 時間: 2025-3-26 22:13
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.作者: Indict 時間: 2025-3-27 04:02
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作者: 冬眠 時間: 2025-3-27 07:37 作者: ingenue 時間: 2025-3-27 09:48
Series Approximation Methods in Statisticsc field of the wave back and forth along the imposed magnetic field, together with elliptic polarization of the electric field in a plane perpendicular to the imposed magnetic field. Using the axes indicated in Figure 10.1, the wave is propagating in the . direction and the electric field is . = (., ., 0)作者: cajole 時間: 2025-3-27 17:37
Droop-Based Economical Dispatchst descent. In this chapter we shall employ the results to study the directional behaviour of the radiated power. We shall plot diagrams to show how the radiated power density varies with the direction of group propagation. In addition, we shall calculate the radiation resistance of the antenna.作者: 石墨 時間: 2025-3-27 21:33 作者: 蚊帳 時間: 2025-3-28 00:46
978-94-009-6172-2Martinus Nijhoff Publishers, Dordrecht 1984作者: accessory 時間: 2025-3-28 03:52 作者: Narcissist 時間: 2025-3-28 07:43 作者: mettlesome 時間: 2025-3-28 13:48 作者: single 時間: 2025-3-28 16:41
Energy behaviour of the X wave for transverse propagation,c field of the wave back and forth along the imposed magnetic field, together with elliptic polarization of the electric field in a plane perpendicular to the imposed magnetic field. Using the axes indicated in Figure 10.1, the wave is propagating in the . direction and the electric field is . = (., ., 0)作者: 無意 時間: 2025-3-28 20:47 作者: Ataxia 時間: 2025-3-29 02:48
Series Approximation Methods in StatisticsIn order to discuss the propagation of electromagnetic waves in a plasma, the equations developed in the previous chapter must be combined with Maxwell’s equations. These involve not only the time-varying electromagnetic field of the wave but also the current density . and the charge density . created by the wave in the plasma.作者: BATE 時間: 2025-3-29 05:03 作者: avarice 時間: 2025-3-29 08:00
Series Approximation Methods in StatisticsIn Chapter 3 we saw that the magnitude of the group velocity in an isotropic plasma differs from the magnitude of the phase velocity. In a magnetoplasma we find that, in addition, the direction of group propagation in general differs from the direction of phase propagation.作者: arrhythmic 時間: 2025-3-29 13:55
Conditional Distribution Approximations,In a homogeneous collisionless magnetoplasma let us examine the storage and flow of energy that occurs when a circularly polarized characteristic wave of angular frequency co propagates along the imposed magnetic field. The propagation constant . is given in terms of the refractive index . by (Equation 2.50) .作者: accomplishment 時間: 2025-3-29 16:53
Series-Parallel Converter-Based MicrogridsIn the previous chapter we described the behaviour of the polar diagrams of group velocity for the . and . waves. In Chapter 18 we shall treat the polar diagrams of radiated power. For this purpose we deduce in this chapter expressions for the far field of an antenna located in a homogeneous magnetoplasma.作者: Narrative 時間: 2025-3-29 20:16
,Maxwell’s equations,In order to discuss the propagation of electromagnetic waves in a plasma, the equations developed in the previous chapter must be combined with Maxwell’s equations. These involve not only the time-varying electromagnetic field of the wave but also the current density . and the charge density . created by the wave in the plasma.作者: 勛章 時間: 2025-3-30 00:04 作者: 無可爭辯 時間: 2025-3-30 04:13 作者: 突變 時間: 2025-3-30 08:57
Energy flow and group velocity for longitudinal propagation,In a homogeneous collisionless magnetoplasma let us examine the storage and flow of energy that occurs when a circularly polarized characteristic wave of angular frequency co propagates along the imposed magnetic field. The propagation constant . is given in terms of the refractive index . by (Equation 2.50) .作者: ovation 時間: 2025-3-30 14:52
The field of an antenna in a magnetoplasma,In the previous chapter we described the behaviour of the polar diagrams of group velocity for the . and . waves. In Chapter 18 we shall treat the polar diagrams of radiated power. For this purpose we deduce in this chapter expressions for the far field of an antenna located in a homogeneous magnetoplasma.作者: cuticle 時間: 2025-3-30 20:06 作者: sinoatrial-node 時間: 2025-3-30 23:10
Alternating current in a magnetoplasma, 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作者: 羽飾 時間: 2025-3-31 04:34 作者: 鎮(zhèn)壓 時間: 2025-3-31 07:53
Propagation of phase along the imposed magnetic field,ongitudinal propagation (.. = 0 or π). Because of the axial symmetry round the imposed magnetic field, the direction of group propagation is then the same as the direction of phase propagation (θ. = 0 or π); it may be verified from Equation (6.34) that, when .. = 0, we also have .. = 0. The magnitud作者: 廚房里面 時間: 2025-3-31 09:10 作者: 枕墊 時間: 2025-3-31 15:46
Elliptic polarization of the X wave for transverse propagation,nstitute a right-handed mutually perpendicular system of directions. For transverse propagation of the . wave, these vectors are linearly polarized as 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作者: FRET 時間: 2025-3-31 19:29 作者: FIS 時間: 2025-4-1 01:04 作者: BAIT 時間: 2025-4-1 02:49 作者: dainty 時間: 2025-4-1 08:49
The hydromagnetic approximation,n has to be replaced by the hydromagnetic approximation (Section 5.7). We have studied the hydromagnetic approximation for longitudinal propagation in Section 7.6, and for transverse propagation in Section 9.6. We now proceed to employ the hydromagnetic approximation for propagation in a magnetoplas
