{"title":"Departure from quasilinear heating in a cross-field ion beam experiment","authors":"R. G. Greaves, P. J. Barrett","doi":"10.1109/PLASMA.1989.166049","DOIUrl":null,"url":null,"abstract":"The heating of an ion beam by the ion acoustic turbulence generated as the beam streams across a weak magnetic field through magnetized electrons was investigated. A quasilinear (QL) relationship between the spatial heating rate delta T/sub i// delta x and the spatially growing noise energy density Psi was sought, as was any departure therefrom as Psi is varied. For the broadband turbulence encountered, QL theory gives delta T/sub i// delta x varies as Psi tau , where tau is the autocorrelation time of the turbulence. If tau remains independent of Psi , then delta T/sub i// delta x varies as Psi /sup beta /, with beta =1 for QL heating. The experiment was carried out in a double-plasma device.<<ETX>>","PeriodicalId":165717,"journal":{"name":"IEEE 1989 International Conference on Plasma Science","volume":"31 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.1989.166049","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
The heating of an ion beam by the ion acoustic turbulence generated as the beam streams across a weak magnetic field through magnetized electrons was investigated. A quasilinear (QL) relationship between the spatial heating rate delta T/sub i// delta x and the spatially growing noise energy density Psi was sought, as was any departure therefrom as Psi is varied. For the broadband turbulence encountered, QL theory gives delta T/sub i// delta x varies as Psi tau , where tau is the autocorrelation time of the turbulence. If tau remains independent of Psi , then delta T/sub i// delta x varies as Psi /sup beta /, with beta =1 for QL heating. The experiment was carried out in a double-plasma device.<>