{"title":"Filamentation instability of MHD waves in solar wind plasma","authors":"S. Kuo, M. Whang","doi":"10.1109/PLASMA.1989.166114","DOIUrl":null,"url":null,"abstract":"Summary form only. The ISEE 1 and 2 spacecraft have detected both magnetosonic waves and Alfven waves propagating upstream in the high-speed solar wind. The magnetosonic wave is a hybrid and elliptically polarized mode that can propagate obliquely across the magnetic field. It becomes decoupled from the Alfven wave when the direction of its propagation is exactly perpendicular to the ambient magnetic field. The filamentation instability of the magnetosonic wave that propagates perpendicular to the magnetic field has been analyzed. The authors have extended this analysis to the general case of convective filamentation instabilities of obliquely propagating magnetosonic waves. The dispersion relation of the instability has been derived and solved numerically for the dependence of the threshold field and spatial growth rate on the wave number k of the nonoscillatory mode, the beta of the plasma, and the frequency of the magnetosonic pump.<<ETX>>","PeriodicalId":165717,"journal":{"name":"IEEE 1989 International Conference on Plasma Science","volume":"1 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1989-05-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"IEEE 1989 International Conference on Plasma Science","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/PLASMA.1989.166114","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
Summary form only. The ISEE 1 and 2 spacecraft have detected both magnetosonic waves and Alfven waves propagating upstream in the high-speed solar wind. The magnetosonic wave is a hybrid and elliptically polarized mode that can propagate obliquely across the magnetic field. It becomes decoupled from the Alfven wave when the direction of its propagation is exactly perpendicular to the ambient magnetic field. The filamentation instability of the magnetosonic wave that propagates perpendicular to the magnetic field has been analyzed. The authors have extended this analysis to the general case of convective filamentation instabilities of obliquely propagating magnetosonic waves. The dispersion relation of the instability has been derived and solved numerically for the dependence of the threshold field and spatial growth rate on the wave number k of the nonoscillatory mode, the beta of the plasma, and the frequency of the magnetosonic pump.<>