X-ray observations of tungsten wire array Z-pinch implosions on QiangGuang-1 facility |
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Authors: | Zhang Fa-Qiang Li Zheng-Hong Xu Ze-Ping Xu Rong-Kun Yang Jian-Lun Guo Cun Xia Guang-Xin Chen Jin-Chuan Song Feng-Jun Ning Jia-Min Wang Zhen Xue Fei-Biao Li Lin-Bo Qin Yi Ying Chun-Tong Liu Guang-Jun |
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Affiliation: | Department of Engineering Physics, Tsinghua University, Beijing 100084, China; Institute of Nuclear Physics and Chemistry, Mianyang 621900, China |
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Abstract: | Z-pinch experiments with two arrays consisting, respectively, of 324-μm- and 6-μm-diameter tungsten wires have been carried out onQiangGuang-1 facility with a current rising up to 1.5MA in 80ns. At earlytime of implosion, x-ray framing images show that the initial emission comesfrom the central part of arrays, and double clear emission rings, driftingto the anode and the cathode at 5×106cm/s and 2.4×107cm/s respectively, are often produced near the electrodes. Later,in a 4-μm-diameter tungsten wire array, filamentation caused by ohmicheating is prominent, and more than ten filaments have been observed. Aradial inward shift of arrays starts at about 30,ns earlier than theoccurrence of the x-ray peak power for both kinds of arrays, and theshrinkage rate of emission region is as high as 1.7×107cm/s ina 4-μm-diameter tungsten wire array, which is two times higher thanthat in a 6-μm one. Emission from precursor plasmas is observed inimplosion of 6-μm-diameter tungsten wire arrays, but not in implosionof a 4-μm-diameter tungsten wire array. Whereas, in a 4-μm-diameter tungsten wire array, the soft x-ray emission shows the growth ofm=1 instability in the plasma column, which is caused by current. Thereasons for the discrepancy between implosions of 4-μm- and 6-μm-diameter tungsten wire arrays are explained. |
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Keywords: | Z-pinch x-ray wire array R-T instability |
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