Thermophysical and transport properties of multicomponent gas plasmas at multiple temperatures |
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| Institution: | 1. Department of Medical Genetics, University of Antwerp and Antwerp University Hospital, Antwerp, Belgium;2. Department of Endocrinology, Diabetology and Metabolic Diseases, Antwerp University Hospital, Antwerp, Belgium;3. Laboratory of Experimental Medicine and Paediatrics, Faculty of Medicine and Health Sciences, University of Antwerp, Antwerp, Belgium;4. Department of Paediatrics, Antwerp University Hospital, Antwerp, Belgium;1. Graduate School of Frontier Sciences, The University of Tokyo, 5-1-5 Kashiwanoha, Kashiwa, Chiba, 277-8561, Japan;2. Graduate School of Engineering, The University of Tokyo, 7-3-1 Hongo, Bunkyo, Tokyo, 113-8656, Japan;1. National Key Laboratory of Science and Technology on Tunable Laser, Harbin Institute of Technology, Harbin 150080, China;2. Institute of Opto-electronics, Harbin Institute of Technology, Harbin 150080, China;3. Institute of Combustion Engineering, Harbin Institute of Technology, Harbin 150001, China;1. Department of Mechanical Engineering, KUCET, Kakatiya University, Warangal,Telangana, 506009, India;2. Department of Mechanical Engineering, UCE, Kakatiya University, Kothagudem, Telangana, India;1. Blood Transfusion Research Center, High Institute for Research and Education in Transfusion Medicine, Tehran, Iran;2. Fondazione IRCCS Ca’ Granda Ospedale Maggiore Policlinico, Angelo Bianchi Bonomi Hemophilia and Thrombosis Center and Fondazione Luigi Villa, Milan, Italy;3. Iranian Comprehensive Hemophilia Care Center, Tehran, Iran |
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| Abstract: | For a gas plasma, with the electrons at an elevated temperature with respect to the heavy particles temperature, a general method is presented using the rigorous kinetic theory to calculate the equilibrium composition and transport properties such as the viscosity, the thermal conductivity, the electrical conductivity, the electron diffusion coefficient and the mobility coefficient. The values for the noble gas plasmas and air plasma are determined for various pressures, electron temperature up to 50,000 K and electron to heavy particles temperature ratio up to two. However, the two-temperature calculations are made only for the cases where there are no molecular species present in the gas mixture. |
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