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Dispersion Equation of Low-Frequency Waves Driven by Temperature Anisotropy

Dispersion Equation of Low-Frequency Waves Driven by Temperature Anisotropy
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摘要 The plasma temperature (or the kinetic pressure) anisotropy is an intrinsic characteristic of a collisionless magnetized plasma. In this paper, based on the two-fluid model, a dispersion equation of low-frequency (ω〈〈ωci, ωci the ion gyrofrequency) waves, including the plasma temperature anisotropy effect, is presented. We investigate the properties of low-frequency waves when the parallel temperature exceeds the perpendicular temperature, and especially their dependence on the propagation angle, pressure anisotropy, and energy closures. The results show that both the instable Alfven and slow modes are purely growing. The growth rate of the Alfven wave is not affected by the propagation angle or energy closures, while that of the slow wave depends sensitively on the propagation angle and energy closures as well as pressure anisotropy. The fast wave is always stable. We also show how to elaborate the symbolic calculation of the dispersion equation performed using Mathematica Notebook. The plasma temperature (or the kinetic pressure) anisotropy is an intrinsic characteristic of a collisionless magnetized plasma. In this paper, based on the two-fluid model, a dispersion equation of low-frequency (ω〈〈ωci, ωci the ion gyrofrequency) waves, including the plasma temperature anisotropy effect, is presented. We investigate the properties of low-frequency waves when the parallel temperature exceeds the perpendicular temperature, and especially their dependence on the propagation angle, pressure anisotropy, and energy closures. The results show that both the instable Alfven and slow modes are purely growing. The growth rate of the Alfven wave is not affected by the propagation angle or energy closures, while that of the slow wave depends sensitively on the propagation angle and energy closures as well as pressure anisotropy. The fast wave is always stable. We also show how to elaborate the symbolic calculation of the dispersion equation performed using Mathematica Notebook.
作者 陈玲 吴德金
出处 《Plasma Science and Technology》 SCIE EI CAS CSCD 2012年第10期880-885,共6页 等离子体科学和技术(英文版)
基金 supported by National Natural Science Foundation of China(Nos.10973043,41074107) Ministry of Science and Technology of China(No.2011CB811402)
关键词 dispersion equation low-frequency waves temperature anisotropy dispersion equation low-frequency waves temperature anisotropy
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  • 1Vedenov A A, Sagdeev R Z. 1959, Some properties of a plssma with an anisotropic ion velocity distribu- tion in a magnetic field, in Plasma Physics and the Problem of Controlled Thermonuclear Reactions, III. Pergamon, New York.
  • 2Ichimaru S. 1973, Basic Principles of Plasma Physics. Benjamin, New York.
  • 3Hasegawa A. 1975, Plasma Instabilities and Nonlinear Effects. Springer-Verlag, New York.
  • 4Hau L N, Sonnerup B U O. 1993, Geophys. Res. Lett. 20:1763.
  • 5Wu D J, Chao J K. 2000, Commun. Theor. Phys., 33: 125.
  • 6Wang B J, Hau L N. 2003, J. Geophys. Res., 108:1463.
  • 7Hellinger P, Matsumoto H. 2000, J. Geophys. Res., 105:10519.
  • 8Hau L N, Wang B J, Teh W L. 2005, Phys. Plasmas, 12:122904.
  • 9Hau L N, Wang B J. 2007, Nonlin. Processes Geophys.,14:557.
  • 10Wang B J, Hau L N. 2010, J. Geophys. Res., 115: A04105.

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