Steady State Solver for the Navier Stokes Equations

碩士 === 國立臺灣大學 === 機械工程學研究所 === 87 === To obtain a steady state solution for the Navier Stokes equations, the time approach method is usually applied. If the convection is integrated explicitly, the time step is limited by the stability condition. On the other hand, if the convection is i...

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Main Authors: Lo Shih-Peng, 羅時朋
Other Authors: 顏瑞和
Format: Others
Language:zh-TW
Published: 1998
Online Access:http://ndltd.ncl.edu.tw/handle/70963295924095746163
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spelling ndltd-TW-087NTU004890072016-02-01T04:12:42Z http://ndltd.ncl.edu.tw/handle/70963295924095746163 Steady State Solver for the Navier Stokes Equations 流場穩態計算法則之發展研究 Lo Shih-Peng 羅時朋 碩士 國立臺灣大學 機械工程學研究所 87 To obtain a steady state solution for the Navier Stokes equations, the time approach method is usually applied. If the convection is integrated explicitly, the time step is limited by the stability condition. On the other hand, if the convection is integrated implicitly, the nonlinear convection terms are solved iteratively. In this research a novel steady state solver was proposed. This method is based on the fully implicit time integration scheme and it is applied to the fractional time splitting scheme. In order to come to the convergence solution quickly, In the step to solve the pressure . The Laplace form of the pressure in the steady state is imposed . In the second step the equations consists of convection and diffusion terms for the velocity variables. This nonlinear convection term is linearized by lagging the convective velocity. The resulting equation is solved by the biorthogonal conjugate gradient method. The numerical experiments show that this method is promising, but further study is needed to understand whether this method can be applied to different kinds of the problems. 顏瑞和 1998 學位論文 ; thesis 0 zh-TW
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description 碩士 === 國立臺灣大學 === 機械工程學研究所 === 87 === To obtain a steady state solution for the Navier Stokes equations, the time approach method is usually applied. If the convection is integrated explicitly, the time step is limited by the stability condition. On the other hand, if the convection is integrated implicitly, the nonlinear convection terms are solved iteratively. In this research a novel steady state solver was proposed. This method is based on the fully implicit time integration scheme and it is applied to the fractional time splitting scheme. In order to come to the convergence solution quickly, In the step to solve the pressure . The Laplace form of the pressure in the steady state is imposed . In the second step the equations consists of convection and diffusion terms for the velocity variables. This nonlinear convection term is linearized by lagging the convective velocity. The resulting equation is solved by the biorthogonal conjugate gradient method. The numerical experiments show that this method is promising, but further study is needed to understand whether this method can be applied to different kinds of the problems.
author2 顏瑞和
author_facet 顏瑞和
Lo Shih-Peng
羅時朋
author Lo Shih-Peng
羅時朋
spellingShingle Lo Shih-Peng
羅時朋
Steady State Solver for the Navier Stokes Equations
author_sort Lo Shih-Peng
title Steady State Solver for the Navier Stokes Equations
title_short Steady State Solver for the Navier Stokes Equations
title_full Steady State Solver for the Navier Stokes Equations
title_fullStr Steady State Solver for the Navier Stokes Equations
title_full_unstemmed Steady State Solver for the Navier Stokes Equations
title_sort steady state solver for the navier stokes equations
publishDate 1998
url http://ndltd.ncl.edu.tw/handle/70963295924095746163
work_keys_str_mv AT loshihpeng steadystatesolverforthenavierstokesequations
AT luóshípéng steadystatesolverforthenavierstokesequations
AT loshihpeng liúchǎngwěntàijìsuànfǎzézhīfāzhǎnyánjiū
AT luóshípéng liúchǎngwěntàijìsuànfǎzézhīfāzhǎnyánjiū
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