{"title":"高频静电波的跨场电子热输运","authors":"H. Naitou","doi":"10.1143/JPSJ.48.608","DOIUrl":null,"url":null,"abstract":"Cross-field electron heat diffusion due to thermally excited high frequency electrostatic waves propagating almost perpendicular to the magnetic field is studied using a 2–1 /2-dimensional simulation code. It is shown that the electron heat diffusion coefficient D H is an order of magnitude greater than the electron particle diffusion coefficient D p , which is essentially collisional. The characteristic feature of wave transport is observed, namely an increase of D H with increasing values of the characteristic temperature scale length L x . The heat diffusion coefficients D // H and D ⊥ H for the parallel and perpendicular temperatures ( D H ≃ D // H + D ⊥ H ) show quite different magnetic field scalings since D // H is due to ion modes while D ⊥ H arises from electron modes. This is also confirmed by treating the ions as an immobile background.","PeriodicalId":22276,"journal":{"name":"The annual research report","volume":"62 1","pages":"1-29"},"PeriodicalIF":0.0000,"publicationDate":"1979-07-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"3","resultStr":"{\"title\":\"Cross-field Electron Heat Transport due to High Frequency Electrostatic Waves\",\"authors\":\"H. Naitou\",\"doi\":\"10.1143/JPSJ.48.608\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Cross-field electron heat diffusion due to thermally excited high frequency electrostatic waves propagating almost perpendicular to the magnetic field is studied using a 2–1 /2-dimensional simulation code. It is shown that the electron heat diffusion coefficient D H is an order of magnitude greater than the electron particle diffusion coefficient D p , which is essentially collisional. The characteristic feature of wave transport is observed, namely an increase of D H with increasing values of the characteristic temperature scale length L x . The heat diffusion coefficients D // H and D ⊥ H for the parallel and perpendicular temperatures ( D H ≃ D // H + D ⊥ H ) show quite different magnetic field scalings since D // H is due to ion modes while D ⊥ H arises from electron modes. This is also confirmed by treating the ions as an immobile background.\",\"PeriodicalId\":22276,\"journal\":{\"name\":\"The annual research report\",\"volume\":\"62 1\",\"pages\":\"1-29\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1979-07-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"3\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"The annual research report\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1143/JPSJ.48.608\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"The annual research report","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1143/JPSJ.48.608","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Cross-field Electron Heat Transport due to High Frequency Electrostatic Waves
Cross-field electron heat diffusion due to thermally excited high frequency electrostatic waves propagating almost perpendicular to the magnetic field is studied using a 2–1 /2-dimensional simulation code. It is shown that the electron heat diffusion coefficient D H is an order of magnitude greater than the electron particle diffusion coefficient D p , which is essentially collisional. The characteristic feature of wave transport is observed, namely an increase of D H with increasing values of the characteristic temperature scale length L x . The heat diffusion coefficients D // H and D ⊥ H for the parallel and perpendicular temperatures ( D H ≃ D // H + D ⊥ H ) show quite different magnetic field scalings since D // H is due to ion modes while D ⊥ H arises from electron modes. This is also confirmed by treating the ions as an immobile background.