Implicit boundary equations for conservative Navier–Stokes equations

Co-existence of the physical and numerical boundary conditions makes implicit boundary treatment a particularly difficult problem in modern CFD simulations. Previous studies adopted space–time extrapolation or specially designed partial differential equations on the boundaries that are different fro...

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Veröffentlicht in:Journal of computational physics 2018-12, Vol.375, p.641-658
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description Co-existence of the physical and numerical boundary conditions makes implicit boundary treatment a particularly difficult problem in modern CFD simulations. Previous studies adopted space–time extrapolation or specially designed partial differential equations on the boundaries that are different from those of interior points. They are often formulated in terms of primitive variables, and are very challenging for complicated boundary types to be converted to, and implemented in, the conservative variables that are preferred in numerical simulations. More importantly, different boundary equations or different extrapolation techniques may compromise the stability, accuracy, or convergence rate of the A-stable schemes that are developed for interior points. A new methodology for implicit boundary treatment is proposed in this study. By introducing a simple correction matrix T, a set of generalized equations ∂Q/∂t=(I+T)R are developed in terms of conservative variables. It is applicable for both the interior domain (T=0) and the boundaries (T≠0). It is in a partial differential equation form, satisfies the boundary conditions accurately, independent of the time and spatial discretizations. Any one-sided schemes can be used on the boundaries but still maintain the upwind property. Implicit solution techniques are made significantly easy to implement using, for example, the data-parallel lower–upper relation method and the Newton method (combined with the GMRES method for subsidiary iterations). Numerical experiments show that the proposed methodology produces stable simulations for very large CFL numbers and preserve the imposed boundary values accurately. •An implicit boundary treatment consisting of a generalized boundary equation in PDE form and its implicit solution techniques is proposed.•A correction matrix T is introduced in the original NS equations to realize the desired boundary conditions.•One-sided spatial schemes can be directly applied to discretize the conservative equations on boundary points, and are still shown stable.•The boundary residuals are computed more accurately, and accelerate the convergence rates of implicit solutions significantly.•Computer code implementation is made significantly easy, especially for multidimensional problems.
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Previous studies adopted space–time extrapolation or specially designed partial differential equations on the boundaries that are different from those of interior points. They are often formulated in terms of primitive variables, and are very challenging for complicated boundary types to be converted to, and implemented in, the conservative variables that are preferred in numerical simulations. More importantly, different boundary equations or different extrapolation techniques may compromise the stability, accuracy, or convergence rate of the A-stable schemes that are developed for interior points. A new methodology for implicit boundary treatment is proposed in this study. By introducing a simple correction matrix T, a set of generalized equations ∂Q/∂t=(I+T)R are developed in terms of conservative variables. It is applicable for both the interior domain (T=0) and the boundaries (T≠0). It is in a partial differential equation form, satisfies the boundary conditions accurately, independent of the time and spatial discretizations. Any one-sided schemes can be used on the boundaries but still maintain the upwind property. Implicit solution techniques are made significantly easy to implement using, for example, the data-parallel lower–upper relation method and the Newton method (combined with the GMRES method for subsidiary iterations). Numerical experiments show that the proposed methodology produces stable simulations for very large CFL numbers and preserve the imposed boundary values accurately. •An implicit boundary treatment consisting of a generalized boundary equation in PDE form and its implicit solution techniques is proposed.•A correction matrix T is introduced in the original NS equations to realize the desired boundary conditions.•One-sided spatial schemes can be directly applied to discretize the conservative equations on boundary points, and are still shown stable.•The boundary residuals are computed more accurately, and accelerate the convergence rates of implicit solutions significantly.•Computer code implementation is made significantly easy, especially for multidimensional problems.</description><identifier>ISSN: 0021-9991</identifier><identifier>EISSN: 1090-2716</identifier><identifier>DOI: 10.1016/j.jcp.2018.09.010</identifier><language>eng</language><publisher>Cambridge: Elsevier Inc</publisher><subject>Boundary conditions ; Boundary value problems ; Computational fluid dynamics ; Computational physics ; Computer simulation ; Extrapolation ; Fluid dynamics ; Generalized boundary equations ; Implicit boundary conditions ; Implicit time integration ; Mathematical models ; Navier-Stokes equations ; Newton methods ; NS equations ; Numerical analysis ; Partial differential equations ; Simulation</subject><ispartof>Journal of computational physics, 2018-12, Vol.375, p.641-658</ispartof><rights>2018 Elsevier Inc.</rights><rights>Copyright Elsevier Science Ltd. 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It is in a partial differential equation form, satisfies the boundary conditions accurately, independent of the time and spatial discretizations. Any one-sided schemes can be used on the boundaries but still maintain the upwind property. Implicit solution techniques are made significantly easy to implement using, for example, the data-parallel lower–upper relation method and the Newton method (combined with the GMRES method for subsidiary iterations). 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subjects Boundary conditions
Boundary value problems
Computational fluid dynamics
Computational physics
Computer simulation
Extrapolation
Fluid dynamics
Generalized boundary equations
Implicit boundary conditions
Implicit time integration
Mathematical models
Navier-Stokes equations
Newton methods
NS equations
Numerical analysis
Partial differential equations
Simulation
title Implicit boundary equations for conservative Navier–Stokes equations
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