Prediction of the thermal properties of CO2, CO, and Xe laser media

Pliński, Edward F.; Witkowski, Jerzy S.

doi:10.1016/s0030-3992(00)00120-1

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Cited by 6 publications

(2 citation statements)

References 18 publications

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“…Edward F. Pliński [24] He recommended a correlation to estimate thermal conductivity of CO 2 , N 2 , He, Xe, CO, O 2 and Ar as a function of temperature.…”

Section: Second Categorymentioning

confidence: 99%

Estimation of thermal conductivity of pure gases by using artificial neural networks

Eslamloueyan

Khademi

2009

International Journal of Thermal Sciences

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“…Edward F. Pliński [24] He recommended a correlation to estimate thermal conductivity of CO 2 , N 2 , He, Xe, CO, O 2 and Ar as a function of temperature.…”

Section: Second Categorymentioning

confidence: 99%

Estimation of thermal conductivity of pure gases by using artificial neural networks

Eslamloueyan

Khademi

2009

International Journal of Thermal Sciences

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“…The PZT moves the laser mirror and in that way it changes the length of the laser resonator -the distance between the laser mirrors. In pulse regime the laser tuning is intrinsically involved [4,5,6]. The explanation is the physical mechanism of pulse developing.…”

Section: Introductionmentioning

confidence: 99%

Acoustic measurement method in investigation of optical phenomena in a modulated CO 2 laser plasma

et al. 2007

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The paper describes the results of investigations of optical phenomena on an RF excited slab-waveguide CO 2 laser. The experiments are performed in two optical arrangements: two-mirror resonator and three-mirror one. The main purpose of the experiments is to check possibilities to observe the optical phenomena using a microphone. The laser plasma is modulated with a self-mixing signal in the three-mirror resonator. The response of the microphone is observed and analyzed. Detection of the laser signature phenomenon with the microphone is experimentally considered. The experiments are done at cw regime of the laser. The investigations are performed at pulse operation of the laser, as well. The response of the microphone is analyzed. It is checked how the laser pulse is reconstructed at a profile of the microphone signal. The output laser pulse with a mapped laser signature in the laser pulse profile is compared to the microphone signal shape. The presence of the laser signature at the acoustic signal is investigated.

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