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Observation of excitation discharge instability induced by shock wave in transversely excited atmospheric gas laser

机译:横向激发大气激光中激波引起的激发放电不稳定性的观察

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Influences of shock waves with Mach number of 1.1-1.35 on excitation discharge in transversely excited atmospheric gas laser have been investigated eliminating the other factors. The shock waves are produced by using a shock tube with the gas mixture of helium and argon. The schlieren photographs of shock wave and direct images of light emitted from the discharge are recorded simultaneously by a streak camera. It is found that the discharge does not collapse with the shock wave of 1.1 in Mach number. The shock waves at Mach number above 1.2 tend to collapse the glow discharge in spite of no halogen gas. If the shock wave does not reach to the center of the electrode, glow discharge occurs only in front of the shock wave. Even if the shock wave passes through the center of the electrode, the glow discharge occurs, however, the discharge concentrates in the tight space between the shock front and the edge of electrode. A streamer exists in the shock front when the shock wave just reaches the edge of electrode. It becomes clear that the discharge characteristics depend on the Mach number of shock wave and the position of shock wave.
机译:消除了其他因素,研究了马赫数为1.1-1.35的冲击波对横向激发大气激光中激发放电的影响。冲击波是通过使用带有氦气和氩气的混合气的激波管产生的。条纹相机同时记录冲击波的震颤照片和放电发出的光的直接图像。发现放电不会因马赫数为1.1的冲击波而崩溃。尽管没有卤素气体,马赫数大于1.2的冲击波仍会使辉光放电崩溃。如果冲击波未到达电极中心,则辉光放电仅在冲击波的前面发生。即使冲击波通过电极的中心,也会发生辉光放电,但是放电会集中在冲击前沿和电极边缘之间的狭窄空间中。当冲击波刚好到达电极边缘时,在冲击前部会存在拖缆。显然,放电特性取决于冲击波的马赫数和冲击波的位置。

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