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Numerical investigation of non-isothermal phase change phenomena in vertical Bridgman crystal growth
Authors:Jie Liu  Wen-Qiang Lu
Affiliation:1. Department of Mechanical and Manufacturing Engineering, Parsons Building, Trinity College Dublin, Ireland;2. Centre for Engineering and Renewable Energy, Faculty of Computing and Engineering, Magee Campus, Ulster University, BT48 7JL Northern Ireland, United Kingdom;1. Illinois Institute of Technology and TermoMechanica Inc., Kenilworth, IL 60043, USA;2. Leibniz Institute for Crystal Growth (IKZ), Max-Born-Str. 2, 12489 Berlin, Germany;1. SIMAP-EPM, 1340 Rue de la Piscine, BP 75, F-38402 Saint Martin d’Hères, France;2. Le Rubis SA, BP 16, 38560 Jarrie, Grenoble, France;1. University of Carthage, Institut National des Sciences Appliquées et de Technologie (INSAT), Laboratoire de Recherche Matériaux, Mesures et Applications, B.P. 676, 1080 Tunis Cedex, Tunisia;2. CEA, LITEN, Department of Solar Technologies, National Institute of Solar Energy, F-73375 Le Bourget du Lac, France;3. Laboratoire de Mécanique des Fluides et d’Acoustique, CNRS/Université de Lyon, École Centrale de Lyon/Université Lyon 1/INSA de Lyon, ECL, 36 Avenue Guy de Collongue, 69134 Ecully Cedex, France;4. Institut de Mécanique des Fluides de Toulouse, UMR CNRS/INP/UPS 5502, UFR MIG, Université Paul Sabatier, 118 Route de Narbonne, 31062 Toulouse Cedex, France;1. Department of Mechanical Engineering, Mississippi State University, Mississippi State, MS 39762, USA;2. Center for Advanced Vehicular Systems, Mississippi State University, 200 Research Boulevard, MS 39759, USA;3. Army Research Laboratory, Weapons and Materials Research Directorate, Aberdeen Proving Ground, MD 21005, USA
Abstract:The non-isothermal phase change phenomena during the vertical Bridgman growth process for HgCdTe are numerically investigated using an interface capturing finite element scheme. The influence of the growth parameters such as Bi, Ste, U and the flow parameters including GrT and GrS on the non-isothermal phase change phenomena are obtained. Some new features about the melt/crystal interface shape, the temperature field near the interface and the flow field are revealed by comparing the non-isothermal phase change with the isothermal phase change. Furthermore, the comparison of the non-isothermal interfacial characteristics between the pure diffusion, the natural convection and the double-diffusive convection is made and the obvious differences are presented.
Keywords:
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