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By W. W. Duley
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Extra resources for Co2 Lasers Effects and Applications
Sample text
Typically this may be 200 J/pulse at high output energy. For a prf of 1 kHz, this would correspond to an average power of 200 kW to be dissipated. However, there would seem to be no major problems involved in operating transversely excited lasers of this sort at rates of up to and including 1 kHz. An extensive study by Brown (1973) on repetition rate effects in a fast flow system with an electrode structure similar to that of Dumanchin et al. (1972) showed that the limitation on pulse rate was occasioned by the occurrence of arcing rather than gas heating.
7 % / c m . An output power of 15 kW was obtained in a nearly diffraction-limited beam. McLeary et al. (1974) describe a method of preionization using plasma injection that allows up to 150 kW/liter of power to be dissipated in cw discharges at atmospheric pressure. McLeary and Gibbs (1973) have described cw operation in a linear fastflow system at atmospheric pressure using a flow-conditioning technique. 8 1000 W TGD TGD Tiffany et al. 4 Eckbreth and Davis (1972) Discharge augmented by rf auxiliary source; closed system Closed system; used as multiple- Brown and Davis (1972) pass amplifier; rf augmentation Brandenberg et al.
7 % / c m . An output power of 15 kW was obtained in a nearly diffraction-limited beam. McLeary et al. (1974) describe a method of preionization using plasma injection that allows up to 150 kW/liter of power to be dissipated in cw discharges at atmospheric pressure. McLeary and Gibbs (1973) have described cw operation in a linear fastflow system at atmospheric pressure using a flow-conditioning technique. 8 1000 W TGD TGD Tiffany et al. 4 Eckbreth and Davis (1972) Discharge augmented by rf auxiliary source; closed system Closed system; used as multiple- Brown and Davis (1972) pass amplifier; rf augmentation Brandenberg et al.