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Water vapor cooling when radiation of wavelength λ=2.8 μm is absorbed

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Abstract

Investigations of the processes arising under the influence of electromagnetic radiation on resonantly absorbing gaseous media have now been widely developed. Particular interest is shown in the penetration of a pulse of laser radiation through the atmosphere. The main component absorbing the radiation of both CO2 and HF lasers (wavelengths, respectively, 10.6 and 2.8 μm) in the earth's atmosphere is water vapor [1]. Numerous experimental investigations show that the integrated coefficient of laser radiation absorption by water vapor is fairly large [1–3], while at the same time the energy absorption leads to the heating of the medium in a channel around the beam and, as a consequence, to its defocusing. However, all these investigations were carried out with continuous sources of laser radiation or with pulses of fairly great duration. It will be shown below that gas cooling in the channel around the beam is possible when a pulse of radiation with wavelength λ 2.8 μm whose duration is less than the vibrational-translational (V-T) relaxation time of the energy absorbed by the H2O molecules passes through a stationary medium containing water vapor.

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Translated from Izvestiya Akademii Nauk SSSR, Mekhanika Zhidkosti i Gaza, No. 3, pp. 141–151, May–June, 1986.

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Levin, V.A., Sorokin, A.A. & Starik, A.M. Water vapor cooling when radiation of wavelength λ=2.8 μm is absorbed. Fluid Dyn 21, 456–465 (1986). https://doi.org/10.1007/BF01409734

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  • DOI: https://doi.org/10.1007/BF01409734

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