A Direct Solver in Phase Space for Semiclassical Boltzmann Model Equation in General Coordinates
碩士 === 國立臺灣大學 === 應用力學研究所 === 102 === I solved the Semiclassical Boltzmann BGK model equations and Semiclassical Boltzmann Ellipsoidal BGK model equations by flux vector splitting method, and we can adjust Prandtl number is correct by Ellipsoidal BGK model. And then, we can adjust the level of raref...
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ndltd-TW-102NTU054990482016-03-09T04:24:22Z http://ndltd.ncl.edu.tw/handle/64618591246437662836 A Direct Solver in Phase Space for Semiclassical Boltzmann Model Equation in General Coordinates 半古典波茲曼模型方程式在廣義座標下之相空間直接解法 Nan-Huei Jiang 江南輝 碩士 國立臺灣大學 應用力學研究所 102 I solved the Semiclassical Boltzmann BGK model equations and Semiclassical Boltzmann Ellipsoidal BGK model equations by flux vector splitting method, and we can adjust Prandtl number is correct by Ellipsoidal BGK model. And then, we can adjust the level of rarefied flow by relaxation time in BGK model. The result of simulation could be validated in different Mach numbers and literature. In addition, we transformed Cartesian coordinate system to generalized coordinate system in order to solve the curved boundary on structure mesh, and compared the difference in Bose–Einstein statistics, Fermi–Dirac statistics, and Maxwell-Boltzmann statistics. The present numerical methods combined total variation diminishing in discrete space and implicit methods in discrete time, and solved the Semiclassical Boltzmann BGK model equations in generalized coordinate system. Weighted Essentially Non-Oscillatory (WENO) are applied to initial value problem. Jaw-Yen Yang 楊照彥 2014 學位論文 ; thesis 131 zh-TW |
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碩士 === 國立臺灣大學 === 應用力學研究所 === 102 === I solved the Semiclassical Boltzmann BGK model equations and Semiclassical Boltzmann Ellipsoidal BGK model equations by flux vector splitting method, and we can adjust Prandtl number is correct by Ellipsoidal BGK model. And then, we can adjust the level of rarefied flow by relaxation time in BGK model. The result of simulation could be validated in different Mach numbers and literature. In addition, we transformed Cartesian coordinate system to generalized coordinate system in order to solve the curved boundary on structure mesh, and compared the difference in Bose–Einstein statistics, Fermi–Dirac statistics, and Maxwell-Boltzmann statistics.
The present numerical methods combined total variation diminishing in discrete space and implicit methods in discrete time, and solved the Semiclassical Boltzmann BGK model equations in generalized coordinate system. Weighted Essentially Non-Oscillatory (WENO) are applied to initial value problem.
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author2 |
Jaw-Yen Yang |
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Jaw-Yen Yang Nan-Huei Jiang 江南輝 |
author |
Nan-Huei Jiang 江南輝 |
spellingShingle |
Nan-Huei Jiang 江南輝 A Direct Solver in Phase Space for Semiclassical Boltzmann Model Equation in General Coordinates |
author_sort |
Nan-Huei Jiang |
title |
A Direct Solver in Phase Space for Semiclassical Boltzmann Model Equation in General Coordinates |
title_short |
A Direct Solver in Phase Space for Semiclassical Boltzmann Model Equation in General Coordinates |
title_full |
A Direct Solver in Phase Space for Semiclassical Boltzmann Model Equation in General Coordinates |
title_fullStr |
A Direct Solver in Phase Space for Semiclassical Boltzmann Model Equation in General Coordinates |
title_full_unstemmed |
A Direct Solver in Phase Space for Semiclassical Boltzmann Model Equation in General Coordinates |
title_sort |
direct solver in phase space for semiclassical boltzmann model equation in general coordinates |
publishDate |
2014 |
url |
http://ndltd.ncl.edu.tw/handle/64618591246437662836 |
work_keys_str_mv |
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