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REVERSED FIELD PINCH EXPERIMENT ON A NEW LARGE MACHINE, TPE-RX

机译:新型大型机器TPE-RX上的反向磁场挤压实验

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摘要

Reversed field pinch (RFP) experiment on a new large machine, TPE-RX has been started from Marchrn1998. Major and minor radii of TPE-RX are 1.7175m and 0.45m, and the maximum designed plasma currentrn(I_p) and discharge duration are 1MA and 100ms, respectively. TPE-RX is being operated in the medium I_prnregion (I_p < 500kA) with discharge duration about 80ms and RFP discharges with good reproducibility arernroutinely obtained, where the precise compensation of error field at poloidal gap of thick shell is indispensable.rnIn a series of initial phase of experiment, following results are obtained. Non-inductive part of toroidal looprnvoltage (RpI_p) as low as 12 V is obtained at low I_p (~150kA), but it increases with I_p and becomes 22V at I_prn~450kA. However, it is shown that R_pI_p is gradually decreasing as the discharge cleaning has been continued.rnFurther decrease of RpI_p will be expected under the improved wall condition. In almost of all discharges,rnespecially with large I_p (>250kA) the wall and phase locking of the MHD fluctuations is observed. However,rnseveral discharges without this mode locking are found in low I_p and low filling pressure cases. Measurementsrnof electron density () by CO2 laser interferometer, electron temperature (T_e) by soft x-ray pulse heightrnanalysis and ion temperature (T_i) by CV Doppler broadening have been started. Measured values are ~rn5×10~(18)m~(-3), T_e ~1000-1200eV and T_i ~ 130±50eV for the discharge with I_p~ 270kA and reversal/pinchrnparameters ~ -0.1/1.6, although it is possible that this high Te may correspond to high energy part and low T_irnmay correspond to the value near the edge since the radiation profile of CV line is very hollow. An interestingrndependence of plasma rotation on I_p is found in the Doppler shift measurement of CV line.
机译:从1998年3月开始在新的大型机器TPE-RX上进行反向场收缩(RFP)实验。 TPE-RX的主半径和次半径分别为1.7175m和0.45m,最大设计等离子体电流rn(I_p)和放电持续时间分别为1MA和100​​ms。 TPE-RX在中等I_prn区域(I_p <500kA)中工作,放电持续时间约80ms,常规获得具有良好再现性的RFP放电,其中必须精确补偿厚壳的极向间隙处的误差场。实验阶段,获得以下结果。在低I_p(〜150kA)时,可获得低至12 V的环形环路电压(RpI_p)的非感性部分,但随I_p的增加而增大,在I_prn〜450kA时变为22V。然而,已经表明,随着放电清洁的持续进行,R_pI_p逐渐降低。在改善的壁条件下,RpI_p有望进一步降低。在几乎所有放电中,特别是在I_p大(> 250kA)的情况下,都可以观察到MHD波动的壁和相位锁定。但是,在低I_p和低填充压力的情况下,会发现无此锁模的几次放电。已经开始通过CO2激光干涉仪测量电子密度(),通过软X射线脉冲高度分析测量电子温度(T_e)和通过CV多普勒展宽测量离子温度(T_i)。 I_p〜270kA放电和反转/收缩参数〜-0.1 / 1.6的测量值为〜rn5×10〜(18)m〜(-3),T_e〜1000-1200eV和T_i〜130±50eV。由于CV线的辐射轮廓非常空心,因此该高Te可能对应于高能量部分,而低T_irn可能对应于边缘附近的值。在CV线的多普勒频移测量中发现了等离子体旋转对I_p的有趣依赖性。

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  • 来源
    《Fusion energy 1998》|1998年|p.1-8|共8页
  • 会议地点 Yokohama(JP)
  • 作者单位

    Electrotechnical Laboratory, 1-1-4 Umezono, Tsukuba-shi, Ibaraki, Japan 305;

    rnElectrotechnical Laboratory, 1-1-4 Umezono, Tsukuba-shi, Ibaraki, Japan 305;

    rnElectrotechnical Laboratory, 1-1-4 Umezono, Tsukuba-shi, Ibaraki, Japan 305;

    rnElectrotechnical Laboratory, 1-1-4 Umezono, Tsukuba-shi, Ibaraki, Japan 305;

    rnElectrotechnical Laboratory, 1-1-4 Umezono, Tsukuba-shi, Ibaraki, Japan 305;

    rnElectrotechnical Laboratory, 1-1-4 Umezono, Tsukuba-shi, Ibaraki, Japan 305;

    rnElectrotechnical Laboratory, 1-1-4 Umezono, Tsukuba-shi, Ibaraki, Japan 305;

    rnElectrotechnical Laboratory, 1-1-4 Umezono, Tsukuba-shi, Ibaraki, Japan 305;

    rnElectrotechnical Laboratory, 1-1-4 Umezono, Tsukuba-shi, Ibaraki, Japan 305;

    rnElectrotechnical Laboratory, 1-1-4 Umezono, Tsukuba-shi, Ibaraki, Japan 305;

    rnElectrotechnical Laboratory, 1-1-4 Umezono, Tsukuba-shi, Ibaraki, Japan 305;

  • 会议组织
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 受控热核反应(聚变反应理论及实验装置);
  • 关键词

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