Fast potential change during sawteeth in JIPP T-IIU tokamak plasmas
Fast potential change during sawteeth in JIPP T-IIU tokamak plasmas
复制标题
JIPP T-IIU 托卡马克等离子体中锯齿期间的快速电势变化
DOI:
10.1088/0029-5515/36/4/i11
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发表时间:
1994
期刊:
影响因子:
3.3
通讯作者:
T. Watari
中科院分区:
文献类型:
--
作者:
Y. Hamada;A. Nishizawa;Y. Kawasumi;K. Kawahata;K. Itoh;A. Ejiri;K. Toi;K. Narihara;K. Sato;T. Seki;H. Iguchi;A. Fujisawa;K. Adachi;S. Hidekuma;S. Hirokura;K. Ida;M. Kojima;J. Koong;R. Kumazawa;H. Kuramoto;R. Liang;T. Minami;H. Sakakita;M. Sasao;K. Sato;T. Tsuzuki;J. Xu;I. Yamada;T. Watari
Fast changes of electric potential with different polarities are observed during sawtooth oscil- lations in the core region of a tokamak plasma using a heavy ion beam probe. Near the inversion radius the polarity of the observed change of the potential is found to be dependent on the swift movement of the hot core at the crash and is consistent with the prediction of one- fluid MHD theory. Near the magnetic axis the change of the potentials is positive and outside the inversion radius the change is negative. This is in contradiction with the MHD prediction. A periodic crash of the central electron tempera- ture called a sawtooth oscillation is a common fea- ture of tokamak plasmas (l-61. After the crash, a flattening of the pressure throughout the q = 1 sur- face is observed. Kadomtsev proposed a theoretical model of the resistive reconnection (7). The theory predicted the flattening of the q profile as well as the pressure profile inside the q = 1 surface. The predic- tion was, however, found to be in contradiction with recent measurements of the current density in toka- mak plasmas (8). In addition, experiments in large machines such as JET and TFTR showed much faster crashes than those predicted by resistive reconnection (2-61. More refined theories, which take account of the kinetic effect and ergodicity on the reconnections, have now been proposed (9-121. The present Letter reports the first measurement of potential changes during sawtooth oscillations and discusses the impli- cations of the results. The experiment is performed with the JIPP T-IIU tokamak (13). Its major radius is 93 cm and the maximum toroidal field is 3 T. The experiment is conducted at a relatively low electron density of about 2 x 1013 cm3, so that good beam penetra- tion into the centre of the plasma could be obtained. A 450 keV singly ionized thallium beam is injected
影响因子:
3.3
作者:
A. Gibson;T. Sekiguchi;K. Lackner;S. Bodner;R. Hancox
通讯作者:
A. Gibson;T. Sekiguchi;K. Lackner;S. Bodner;R. Hancox