Sawtooth Activity in Ohmically Heated Plasma on HT-7 Tokamak

来源 :Plasma Science & Technology | 被引量 : 0次 | 上传用户:liqiang20010
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Sawtooth activity on HT-7 tokamak has been investigated experimentally mainly by using soft x-ray diode array and magnetic probes. Their behaviors and occurrences are correlated closely to the discharge conditions: the electron density Ne, the electron temperature Te, the safety factor qa on plasma boundary and wall condition etc. When central line-averaged electron density Ne(0) is over 2.0×1013cm-3 , major sawtooth activity emerges with a period of up to 6.5 ms and a fluctuation amplitude of up to 2-30 % of SXR radiation signal. In some cases such as the safety factor between 4.2-4.7 and Zeff=3.0-6.0, a monster sawtooth activity often emerges without apparent deterioration of plasma confinement and without major disruption. During these events, abundant MHD phenomena are observed including partial sawtooth oscillations. In this paper, the observed sawtooth behaviors and their dependence on the and their dependence density Ne and wall condition in ohmically heated plasma are introduced, the results are discussed and presented. Sawtooth activity on HT-7 tokamak has been investigated experimentally mainly by using soft x-ray diode array and magnetic probes. Their behaviors and occurrences are closely linked to the discharge conditions: the electron density Ne, the electron temperature Te, the safety factor qa on plasma boundary and wall condition etc. when central line-averaged electron density Ne (0) is over 2.0 × 1013 cm-3, major saw tooth activity emerges with a period of up to 6.5 ms and a fluctuation amplitude of up to 2-30% of SXR radiation signal. In some cases such as the safety factor between 4.2-4.7 and Zeff = 3.0-6.0, a monster sawtooth activity often emerges without apparent deterioration of plasma confinement and without major disruption. During these events, abundant MHD phenomena are observed including partial sawtooth oscillations. In this paper, the observed saw tooth smooth and their dependence on the and their dependence density Ne and wall condition in ohmically heated plasma are introduc ed, the results are discussed and presented.
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