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冲击压缩下稠密Ar等离子体温度测量 被引量:5

TEMPERATURE MEASUREMENTS OF SHOCK INDUCED ARGON PLASMA
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摘要 测量了稠密氩等离子体温度,并与国外文献报道结果进行了对比。实验时通过对Ar气冲击压缩产生稠密Ar等离子体。Ar样品的初始压力均为0.1MPa,初始温度为293K。五个实验点的压力为0.125~0.163GPa,温度为23400~25900K,等离子体非理想性参数Γ为0.43~0.45。给出了Ar的Hugoniot冲击压缩数据及温度实测数据。理论计算首次考虑了二级电离效应,温度理论计算值明显地偏高于实验值,这说明用Saha加上DebyeH¨uckel修正模型的计算电离度已与实际结果出现了差别,其电离能和能级布居也发生了改变。 Hugoniot data and shock temperatures of the shock generated Ar plasma were measured in this work.Five shots have been done at pressures covering 0.125~0.163GPa and temperatures 2.34×10 4~2.59×10 4K.The non ideality coefficients of plasma Γ are 0.43~0.45.The initial pressure and temperature of Ar sample in all experiments are 0.1MPa and 293K respectively.Using ionization equalibrium model (Saha equation and Debye Hckel correction)and taking into account doubly ionizations as well as singly ionizations,we have calculated the equation of state,degree of ionization,and some other parameters of Ar plasma.In comprarison of the experimental with theoretical results,we find that the shock temperatures are lower than the theoretical.It implys that the theoretical degree of ionization should be lower than that of the experiments due to their lower values of T H,and thus the ionization energies and level populations of the compressed atoms are also changed.
出处 《爆炸与冲击》 EI CAS CSCD 北大核心 1999年第3期204-209,共6页 Explosion and Shock Waves
基金 中国工程物理研究院预研基金
关键词 冲击波 等离子体 电离度 温度测量 冲击压缩 argon plasma,shockwave,equation of state,temperature,ionization equillium
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参考文献4

  • 1陈敬平.冲击压缩下稠密Ar等离子体不透明度及物太方程研究(博士学位论文)[M].成都:中物院流体物理研究所,1998..
  • 2汤文辉.金属冲击温度的理论和实验研究(博士学位论文)[M].长沙:国防科技大学出版社,1994..
  • 3陈敬平,博士学位论文,1998年
  • 4汤文辉,博士学位论文,1994年

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