Observation of Discharge Instability Induced by Shockwave in Self-Sustained High-Pressure Pulsed Glow Discharge

• Published in: IEEE transactions on plasma science Vol. 35; no. 4; pp. 1126 - 1134
• Main Authors: Imada, G., Suzuki, M., Masuda, W.
• Format: Journal Article
• Language: English
• Published: New York, NY IEEE 01.08.2007; Institute of Electrical and Electronics Engineers; The Institute of Electrical and Electronics Engineers, Inc. (IEEE)
• Subjects: Discharge; Disturbances; Electric discharges; Electric shock; Electrodes; Electron tubes; Exact sciences and technology; Excitation; Fluid flow; Gas density; Gas flow; Gas lasers; Glow discharges; Glow; corona; Helium; Holes; Instability; Ionization of plasmas; Laser excitation; Optical pulses; Physics; Physics of gases, plasmas and electric discharges; Physics of plasmas and electric discharges; Plasma properties; Power lasers; Pump lasers; pumping of lasers; shockwaves; Surface waves; transversely excited lasers; Velocity; Preionization; Electric discharges; Helium; transversely excited lasers; High pressure; Gas mixtures; Pulsed discharge; Spatial distribution; pumping of lasers; Gas flow; Shock tubes; Argon; Electron density; Gas lasers; Glow discharges; Mach number; shockwaves
• ISSN: 0093-3813; 1939-9375
• DOI: 10.1109/TPS.2007.901956

Self-sustained high-pressure pulsed glow discharge is applied to excitation discharge on transversely excited atmospheric (TEA) gas lasers. Influence of shockwaves with Mach number M S of 1.1 and 1.35 on the discharge has been investigated. The normal Shockwave, which is normal to gas flow direction in TEA gas lasers, is produced by a shock tube with gas mixture of helium and argon to simulate reflected shockwave in discharge cavity. Discharge instability depends on both the shock Mach number and the position of shockwave in the cavity. The discharge does not collapse by gas density disturbance caused by the shockwave with M S = 1.1, where the gas densities in front of and behind the shockwave are rho 1 = 0.52 kg/m 3 and rho 2 = 0.60 kg/m 3 , respectively. In the two shockwaves with identical M S = 1.35 having rho 2 /rho 1 = 0.83/0.55 or 0.67 kg/m 3 /0.45 kg/m 3 , the recovery of discharge depends on rho 2 , and the gas density disturbance caused by oblique shockwave destroys the discharge even if the cavity is occupied by the gas having suitable density in still gas. The discharge may not be disturbed with spatial distribution of preionization electron density due to the shockwave.