核聚变与等离子体物理
覈聚變與等離子體物理
핵취변여등리자체물리
NUCLEAR FUSION AND PLASMA PHYSICS
2013年
4期
297-303
,共7页
吴娜%王中天%桑超峰%张轶泼%王德真
吳娜%王中天%桑超峰%張軼潑%王德真
오나%왕중천%상초봉%장질발%왕덕진
逃逸电子%环向电场%等离子体破裂%HL-2A装置
逃逸電子%環嚮電場%等離子體破裂%HL-2A裝置
도일전자%배향전장%등리자체파렬%HL-2A장치
Runaway electrons%Toroidal electric field%Plasma disruption%HL-2A tokamak
采用数值模拟方法对托卡马克等离子体破裂期间的逃逸电子(RE)演化行为进行研究。程序所使用的物理模型包含了初级和次级两种RE产生机制,并耦合了麦克斯韦方程组。模拟结果显示:在等离子体破裂开始0.1~0.2ms后感应产生了很强的环向电场,持续约0.1ms之后该环向电场达到最大值,但是在大致2.5ms内逐渐衰减。同时模拟结果也证明了RE产生于等离子体中心处的局部区域,并且在破裂之后约1ms时间内就形成了RE束,实验中等离子体破裂之后出现的几十毫秒的电流平台主要是由RE携带的。从理论模拟与实验的对比中可以得出:HL-2A 15335次放电等离子体破裂期间欧姆电流转化为逃逸电流(RC)的转化率在40%~60%。次级产生机制在RE束的形成过程当中起到了关键作用。
採用數值模擬方法對託卡馬剋等離子體破裂期間的逃逸電子(RE)縯化行為進行研究。程序所使用的物理模型包含瞭初級和次級兩種RE產生機製,併耦閤瞭麥剋斯韋方程組。模擬結果顯示:在等離子體破裂開始0.1~0.2ms後感應產生瞭很彊的環嚮電場,持續約0.1ms之後該環嚮電場達到最大值,但是在大緻2.5ms內逐漸衰減。同時模擬結果也證明瞭RE產生于等離子體中心處的跼部區域,併且在破裂之後約1ms時間內就形成瞭RE束,實驗中等離子體破裂之後齣現的幾十毫秒的電流平檯主要是由RE攜帶的。從理論模擬與實驗的對比中可以得齣:HL-2A 15335次放電等離子體破裂期間歐姆電流轉化為逃逸電流(RC)的轉化率在40%~60%。次級產生機製在RE束的形成過程噹中起到瞭關鍵作用。
채용수치모의방법대탁잡마극등리자체파렬기간적도일전자(RE)연화행위진행연구。정서소사용적물리모형포함료초급화차급량충RE산생궤제,병우합료맥극사위방정조。모의결과현시:재등리자체파렬개시0.1~0.2ms후감응산생료흔강적배향전장,지속약0.1ms지후해배향전장체도최대치,단시재대치2.5ms내축점쇠감。동시모의결과야증명료RE산생우등리자체중심처적국부구역,병차재파렬지후약1ms시간내취형성료RE속,실험중등리자체파렬지후출현적궤십호초적전류평태주요시유RE휴대적。종이론모의여실험적대비중가이득출:HL-2A 15335차방전등리자체파렬기간구모전류전화위도일전류(RC)적전화솔재40%~60%。차급산생궤제재RE속적형성과정당중기도료관건작용。
The simulation of runaway electron (RE) and electric field evolution during HL-2A disruption is presented using a self-consistent model, which is constituted by Maxwell’s equations and generation rate equation. The generation rate equation includes Dreicer and avalanche generation mechanisms of REs. The simulation shows that the electric field increases rapidly from 0.1~0.2ms after the disruption, reaches the maximum about 0.1 ms later, and lasts about 2.5ms. The simulation results also show that REs are produced mostly in the region around the magnetic axis and a RE beam forms at 1ms after disruption, tens of milliseconds steady-state current appearing after disruption is carried mainly by REs. Further, comparing between the simulation and the experimental results, it is found that 40%~60% of the Ohmic current is converted into runaway current (RC) during the disruption (discharge No. 15335) in HL-2A. Although the avalanche generation rate of REs is weaker than Dreicer generation mechanism in HL-2A, it plays a key role because of its larger action time than Dreicer generation mechanism.