2006
DOI: 10.1117/12.675858
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<title>Degradation of fast electrons energy and atomic hydrogen generation in an emission plume from atomic power stations</title>

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“…In order to find power Q n which the electron radiates in the interval of wavelengths dn it is necessary to sum dn over all collisions. Assuming the diffusion to be isotropic, the electron deceleration time w10 À6 s and taking into account results presented in Kolotkov et al (2006), after summation we obtain the amount of energy from 0.1 to 2$10 À12 erg cm À3 emitted in the wavelength interval 844.7e4200 A.…”
Section: Estimation Of H and Oh Concentration In The Emission Plume Rmentioning
confidence: 99%
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“…In order to find power Q n which the electron radiates in the interval of wavelengths dn it is necessary to sum dn over all collisions. Assuming the diffusion to be isotropic, the electron deceleration time w10 À6 s and taking into account results presented in Kolotkov et al (2006), after summation we obtain the amount of energy from 0.1 to 2$10 À12 erg cm À3 emitted in the wavelength interval 844.7e4200 A.…”
Section: Estimation Of H and Oh Concentration In The Emission Plume Rmentioning
confidence: 99%
“…As collisions of electrons with atoms occurs rarely (in comparison with the frequency of the radiated electromagnetic wave), it is possible to consider the consecutive collisions as independent, and the energy radiated at many collisions is simply the sum of the energies radiated by the separate collisions. As the act of scattering occurs very quickly in comparison with the period of the field oscillation, it is possible to write down the formula for the quantity of the bremsstrahlung electron energy in the frequency interval dn per second (Zel'dovich and Raizer, 1966;Kolotkov et al, 2006):…”
Section: Estimation Of H and Oh Concentration In The Emission Plume Rmentioning
confidence: 99%
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