期刊文献+

ITER条件下高能量粒子对一种新型离散阿尔芬本征模的影响

EFFECTS ONαTAE BY ENERGETIC PARTICLES IN ITER OPERATION
下载PDF
导出
摘要 离散阿尔芬本征模是托克马克中存在的一种模式,它具有准边缘不稳定性,能被高能量粒子激发成不稳定模式.国际热核实验反应堆(International Thermonuclear Experimental Reactor,ITER)的设计运行有感应方案、稳态方案和混合方案,文中将在稳态方案下结合电流驱动方式来探讨αTAE的不稳定性.本文主要介绍ITER实验设计运行条件,并据此探究ITER中的αTAE(α-induced toroidal Alfvén eigenmode,α是表示等离子体压强梯度大小的一个参数)及其由高能量粒子激发的不稳定性,结果表明在ITER中能够存在这种αTAE,且能够被高能量粒子激发成为不稳定模式. The discrete Alfv6n eigenmodes existing in Tokamak reactor, are quasi-marginally stable and can be destabilized by energetic particles easily. Design of international thermonu- clear experimental reactor (ITER) include three possible scenarios. They are inductive operation, steady state operation, and hybrid operation, respectively. In this work, the instability feature of a-induced toroidal Alfv6n eigenmode (aTAEs) are investigated in the steady state operation with both positive and negative magnetic share. This paper is to present the ITER operations and to study ingtability features of the ~TAE and their kinetic excitations by ener- getic particles in the designed operate conditions of ITER experiments. The results show that aTAE indeed exists in ITER operation and can be destabilized by energetic particles.
出处 《物理与工程》 2015年第2期60-65,共6页 Physics and Engineering
基金 国家自然科学基金(11264006) 国家自然科学基金项目(11275053)
关键词 磁约束聚变 运行模式 阿尔芬波 高能量粒子 不稳定性 magnetic confinement fusion operation scenario Alfvfn wave energetic particles plasma instability
  • 相关文献

参考文献18

  • 1Shimada M,Campbell D J,Mukhovatov V,et al.Chapter 1:Overview and summary[J].Nuclear Fusion,2007,47(6):1-17.
  • 2张一鸣,曾丽萍,沈欣媛,张利,丁亚清,肖成馨,康卫红,王海.ITER计划与聚变能发展战略[J].核聚变与等离子体物理,2013,33(4):359-365. 被引量:25
  • 3冯开明.可控核聚变与ITER计划[J].现代电力,2006,23(5):82-88. 被引量:19
  • 4冯开明.ITER实验包层计划综述[J].核聚变与等离子体物理,2006,26(3):161-169. 被引量:52
  • 5Alfvén H.Existence of electronmagnetic-hydrodynamic waves[J].Nature,1942,150(3805):405-406.
  • 6Jephcott D F.Alfvén waves in a gas discharge[J].Nature,1959,183(4676):1652-1654.
  • 7Rosenbluth M N,Rutherford P H.Excitation of Alfvén waves by high-energy ions in a tokamak[J].Physical Review Lettres,1975,34(23):1428-1431.
  • 8Cheng C Z,Chen L,Chance M S.High-n ideal and resistive shear Alfvén waves in tokamaks[J].Annals of Physics,1985,(161):21-47.
  • 9Hu S H,Chen L.Discrete Alfvén eigenmodes in high-βtoroidal plasmas[J].Physics of Plasmas,2004,11(1):1-4.
  • 10Hu S H,Chen L.Discrete Alfvén eigenmodes excited by energetic particles in high-βtoroidal plasmas[J].Plasma Physics and Controlled Fusion,2005,47(8):1251-1269.

二级参考文献95

  • 1冯开明.ITER实验包层计划综述[J].核聚变与等离子体物理,2006,26(3):161-169. 被引量:52
  • 2冯开明.可控核聚变与ITER计划[J].现代电力,2006,23(5):82-88. 被引量:19
  • 3Alfvén H.Existence of Electromagnetic-Hydrodynamic waves[J].Nature,1942,150:405-406.
  • 4Wong K L,Fonck R J,Paul S F,et al.Excitation of ToroidalAlfvén Eigenmodes in TFTR[J].Phys Rev Lett,1991,66(14):1874-1877.
  • 5Cheng C Z,Chen L,Chance M S.High-n Ideal and ResistiveShear Alfvén Waves in Tokamak[J].Ann Phys(N.Y),1985,161:21-46.
  • 6Chen L.Theory of magnetohydrodynamic instabilities excited by ener-getic particles in tokamaks[J].Phys Plasmas,1994,1:1519-1522.
  • 7Hu S,Chen L.Discrete Alfvén eigenmodes in high-βtoroidalplasmas[J].Phys Plasmas,2004,11(1):1-4.
  • 8Lee Y C,Van Dam J W.Kinetic Theory of Balloning Instabilities[C]//B Coppi,W Sadowski.Proceedings of the Finite Beta TheoryWorkshop.Washington,D.C.:U.S.Department of Energy,1977:93-101.
  • 9Connor J W,Hastie R J,Taylor J B.High Mode Number Stabilityof an Axisymmetric Toroidal Plasma[J].Proc R Soc London,Ser.A,1979,365:1-17.
  • 10Connor J W,Hastie R J,Taylor J B.Shear,Periodicity,andPlasma Ballooning Modes[J].Phys Rev Lett,1978,40:396-399.

共引文献101

相关作者

内容加载中请稍等...

相关机构

内容加载中请稍等...

相关主题

内容加载中请稍等...

浏览历史

内容加载中请稍等...
;
使用帮助 返回顶部