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本工作研究感应磁场压缩下,氢等离子体中的巴耳末系谱线的斯塔克加宽。电容器对围绕在放电管外部的线圈放电,产生交变轴向磁场,使放电管中氢气离化、压缩与加热。放电周期14微秒,放电电压20千伏,最大电流165千安,初始工作气压2.0×10-1毫米汞高。用照相方法研究Hβ和Hγ的轮廓。这些谱线有显著的加宽。在整个发光阶段中,Hβ的平均半宽度为14—16(埃),Hγ为18—19(埃),相应的离子密度为1.7—2.5×1016厘米-3。实验轮廓与Griem,Kolb和Shen的理论较为接近,与Holtsmark理论相差较远。光电测量进一步表明:Hβ的轮廓随着时间而改变,相应的离子密度亦在改变。在放电的第三半周期初级电流极大时,离子密度最大,达到3.2×1O16厘米-3,为初始氢原子密度的2.2倍。The Stark broadening of Balmer lines in a hydrogen plasma produced by induced magnetic field has been investigated. A condenser bank discharging into the coil surrounding the discharge tube, produces an alternating axial magnetic field which ionizes, compresses, and heats the hydrogen in the tube. The working conditions are: initial pressure of hydrogen, 2.0×10-1mm Hg; charging voltage, 20 kV; discharge period, 14 microseconds; maximum current, 165 kA. Profiles of the spectral lines of Hβ and Hγ are studied by the photographic method. These lines are considerably broadened. In the whole luminous stage, the mean half-widths of Hβ and Hγ are 14-16? and 18-19? respectively, corresponding to an ion density of 1.7-2.5×1016cm-3. The experimental profiles agree better with Griem, Kolb, and Shen's theory than with Holtsmark's theory. Photo-electrical measurements show that the profile of Hβ changes with time, accordingly the ion density changes also. At the primary current maximum of the third half-period of discharge, the ion density reaches a peak value of 3.2×1016cm-3 which is 2.2 times the initial density of hydrogen atoms.
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