Japan Geoscience Union Meeting 2015

Presentation information

Poster

Symbol P (Space and Planetary Sciences) » P-EM Solar-Terrestrial Sciences, Space Electromagnetism & Space Environment

[P-EM26] Space Plasma Physics: Theory and Simulation

Sun. May 24, 2015 6:15 PM - 7:30 PM Convention Hall (2F)

Convener:*Takayuki Umeda(Solar-Terrestrial Environment Laboratory, Nagoya University), Takanobu Amano(Department of Earth and Planetary Science, University of Tokyo), Yasuhiro Nariyuki(Faculty of Human Development, University of Toyama), Tooru Sugiyama(Japan Agency for Marine-Earth Science and Technology Center for Earth Information Science and Technology), Tadas Nakamura(Fukui Prefectural University)

6:15 PM - 7:30 PM

[PEM26-P07] Effects of the alpha-proton drift velocity on alpha firehose instabilities in the solar wind

*Seough JUNGJOON1, Yasuhiro NARIYUKI2, Peter H. YOON3 (1.Faculty of Human Development, University of Toyama / JSPS Postdoctor Fellow, 2.Faculty of Human Development, University of Toyama, 3.IPST, University of Maryland / School of Space Research, Kyung Hee University)

Keywords:firehose instability, solar wind ions, the alpha-proton drift

In situ measurements have shown that the less-abundant alpha particles are characterized by temperature anisotropy which could drive the anisotropy-driven kinetic instabilities in the solar wind. In the collisionless limit, the differential alpha-proton flow velocity usually has finite value of the order of the local Alfven velocity. The presence of such differential flow may affect the properties of dispersion relations for anisotropy-driven instabilities. By making use of linear Vlasov theory, the present study investigates the effects of the alpha-proton drift velocity on firehose instabilities driven by parallel temperature anisotropy of alpha particles. It is found that for parallel firehose mode the dispersion properties are asymmetric in that the maximum growth rate is larger for forward propagating mode than for backward propagating one in the proton rest frame. For both parallel (forward propagating mode) and oblique firehose instabilities overall growth rates increase as the alpha-proton drift velocity increases. Consequently, the firehose instability thresholds are distinctly influenced by the presence of the alpha-proton drift velocity.