{"title":"强非线性对等离子体中哨子稳态自聚焦和成丝影响的数学分析","authors":"G. Rai","doi":"10.21013/JTE.V5.N1.P4","DOIUrl":null,"url":null,"abstract":"A high-power Gaussian Whistler propagating in a magnatoplasma becomes self-focused because of (i) ponderomotive force and (ii) nonuniform heating nonlinearities (i) being dominant for t t E . On short time scale (t t E ) only high frequency whistlers (ω> /2) are focused. At very high powers the plasma is depleted almost completely from the axial region and self-focusing does not occur, rather, defocusing takes place. A plane uniform whistler of high intensity is seen to be unstable for small scale fluctuations, i.e., it must break up into filaments in course of it propagation. The growth rate increases with decreasing scale length of perturbation and is seen to be a saturating function of power density of the beam.","PeriodicalId":269688,"journal":{"name":"IRA-International Journal of Technology & Engineering","volume":"18 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2016-11-09","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"The Mathematical Analysis On The Effect Of Strong Nonlinearity On Steady-State Self-Focusing And Filamentation Of Whistlers In A Plasma\",\"authors\":\"G. Rai\",\"doi\":\"10.21013/JTE.V5.N1.P4\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"A high-power Gaussian Whistler propagating in a magnatoplasma becomes self-focused because of (i) ponderomotive force and (ii) nonuniform heating nonlinearities (i) being dominant for t t E . On short time scale (t t E ) only high frequency whistlers (ω> /2) are focused. At very high powers the plasma is depleted almost completely from the axial region and self-focusing does not occur, rather, defocusing takes place. A plane uniform whistler of high intensity is seen to be unstable for small scale fluctuations, i.e., it must break up into filaments in course of it propagation. The growth rate increases with decreasing scale length of perturbation and is seen to be a saturating function of power density of the beam.\",\"PeriodicalId\":269688,\"journal\":{\"name\":\"IRA-International Journal of Technology & Engineering\",\"volume\":\"18 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2016-11-09\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"IRA-International Journal of Technology & Engineering\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.21013/JTE.V5.N1.P4\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"IRA-International Journal of Technology & Engineering","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.21013/JTE.V5.N1.P4","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
摘要
在磁等离子体中传播的高功率高斯惠斯勒变得自聚焦,因为(i)有质动势和(ii)非均匀加热非线性(i)在t t E中占主导地位。在短时间尺度(t t E)上,只有高频哨子(ω> /2)被聚焦。在非常高的功率下,等离子体几乎完全从轴向区域耗尽,并且不会发生自聚焦,而是发生散焦。高强度的平面均匀哨子在小尺度波动时是不稳定的,即它在传播过程中必须断裂成细丝。生长速率随微扰尺度长度的减小而增大,是光束功率密度的饱和函数。
The Mathematical Analysis On The Effect Of Strong Nonlinearity On Steady-State Self-Focusing And Filamentation Of Whistlers In A Plasma
A high-power Gaussian Whistler propagating in a magnatoplasma becomes self-focused because of (i) ponderomotive force and (ii) nonuniform heating nonlinearities (i) being dominant for t t E . On short time scale (t t E ) only high frequency whistlers (ω> /2) are focused. At very high powers the plasma is depleted almost completely from the axial region and self-focusing does not occur, rather, defocusing takes place. A plane uniform whistler of high intensity is seen to be unstable for small scale fluctuations, i.e., it must break up into filaments in course of it propagation. The growth rate increases with decreasing scale length of perturbation and is seen to be a saturating function of power density of the beam.