On the construction and properties of WENO schemes order five, seven, nine, eleven and thirteen. Part 1. Construction and stability

Currently, different nonlinear numerical schemes of the spatial approximation are used in numerical simulation of boundary value problems for hyperbolic systems of partial differential equations (e. g. gas dynamics equations, MHD, deformable rigid body, etc.). This is due to the need to improve the...

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Main Author: Nikolay Mikhaylovitch Evstigneev
Format: Article
Language:Russian
Published: Institute of Computer Science 2016-10-01
Series:Компьютерные исследования и моделирование
Subjects:
Online Access:http://crm.ics.org.ru/uploads/crmissues/crm_2016_5/2016.08.02.pdf
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spelling doaj-ced7d6d03b004fb5926cdaf687cebdff2020-11-24T21:37:59ZrusInstitute of Computer ScienceКомпьютерные исследования и моделирование2076-76332077-68532016-10-018572175310.20537/2076-7633-2016-8-5-721-7532498On the construction and properties of WENO schemes order five, seven, nine, eleven and thirteen. Part 1. Construction and stabilityNikolay Mikhaylovitch EvstigneevCurrently, different nonlinear numerical schemes of the spatial approximation are used in numerical simulation of boundary value problems for hyperbolic systems of partial differential equations (e. g. gas dynamics equations, MHD, deformable rigid body, etc.). This is due to the need to improve the order of accuracy and perform simulation of discontinuous solutions that are often occurring in such systems. The need for non-linear schemes is followed from the barrier theorem of S. K. Godunov that states the impossibility of constructing a linear scheme for monotone approximation of such equations with approximation order two or greater. One of the most accurate non-linear type schemes are ENO (essentially non oscillating) and their modifications, including WENO (weighted, essentially non oscillating) scemes. The last received the most widespread, since the same stencil width has a higher order of approximation than the ENO scheme. The benefit of ENO and WENO schemes is the ability to maintain a high-order approximation to the areas of non-monotonic solutions. The main difficulty of the analysis of such schemes comes from the fact that they themselves are nonlinear and are used to approximate the nonlinear equations. In particular, the linear stability condition was obtained earlier only for WENO5 scheme (fifth-order approximation on smooth solutions) and it is a numerical one. In this paper we consider the problem of construction and stability for WENO5, WENO7, WENO9, WENO11, and WENO13 finite volume schemes for the Hopf equation. In the first part of this article we discuss WENO methods in general, and give the explicit expressions for the coefficients of the polynomial weights and linear combinations required to build these schemes. We prove a series of assertions that can make conclusions about the order of approximation depending on the type of local solutions. Stability analysis is carried out on the basis of the principle of frozen coefficients. The cases of a smooth and discontinuous behavior of solutions in the field of linearization with frozen coefficients on the faces of the final volume and spectra of the schemes are analyzed for these cases. We prove the linear stability conditions for a variety of Runge-Kutta methods applied to WENO schemes. As a result, our research provides guidance on choosing the best possible stability parameter, which has the smallest effect on the nonlinear properties of the schemes. The convergence of the schemes is followed from the analysis.http://crm.ics.org.ru/uploads/crmissues/crm_2016_5/2016.08.02.pdfWENO schemesnonlinear schemesstability of numerical schemeshyperbolic systems of differential equationsHopf equation
collection DOAJ
language Russian
format Article
sources DOAJ
author Nikolay Mikhaylovitch Evstigneev
spellingShingle Nikolay Mikhaylovitch Evstigneev
On the construction and properties of WENO schemes order five, seven, nine, eleven and thirteen. Part 1. Construction and stability
Компьютерные исследования и моделирование
WENO schemes
nonlinear schemes
stability of numerical schemes
hyperbolic systems of differential equations
Hopf equation
author_facet Nikolay Mikhaylovitch Evstigneev
author_sort Nikolay Mikhaylovitch Evstigneev
title On the construction and properties of WENO schemes order five, seven, nine, eleven and thirteen. Part 1. Construction and stability
title_short On the construction and properties of WENO schemes order five, seven, nine, eleven and thirteen. Part 1. Construction and stability
title_full On the construction and properties of WENO schemes order five, seven, nine, eleven and thirteen. Part 1. Construction and stability
title_fullStr On the construction and properties of WENO schemes order five, seven, nine, eleven and thirteen. Part 1. Construction and stability
title_full_unstemmed On the construction and properties of WENO schemes order five, seven, nine, eleven and thirteen. Part 1. Construction and stability
title_sort on the construction and properties of weno schemes order five, seven, nine, eleven and thirteen. part 1. construction and stability
publisher Institute of Computer Science
series Компьютерные исследования и моделирование
issn 2076-7633
2077-6853
publishDate 2016-10-01
description Currently, different nonlinear numerical schemes of the spatial approximation are used in numerical simulation of boundary value problems for hyperbolic systems of partial differential equations (e. g. gas dynamics equations, MHD, deformable rigid body, etc.). This is due to the need to improve the order of accuracy and perform simulation of discontinuous solutions that are often occurring in such systems. The need for non-linear schemes is followed from the barrier theorem of S. K. Godunov that states the impossibility of constructing a linear scheme for monotone approximation of such equations with approximation order two or greater. One of the most accurate non-linear type schemes are ENO (essentially non oscillating) and their modifications, including WENO (weighted, essentially non oscillating) scemes. The last received the most widespread, since the same stencil width has a higher order of approximation than the ENO scheme. The benefit of ENO and WENO schemes is the ability to maintain a high-order approximation to the areas of non-monotonic solutions. The main difficulty of the analysis of such schemes comes from the fact that they themselves are nonlinear and are used to approximate the nonlinear equations. In particular, the linear stability condition was obtained earlier only for WENO5 scheme (fifth-order approximation on smooth solutions) and it is a numerical one. In this paper we consider the problem of construction and stability for WENO5, WENO7, WENO9, WENO11, and WENO13 finite volume schemes for the Hopf equation. In the first part of this article we discuss WENO methods in general, and give the explicit expressions for the coefficients of the polynomial weights and linear combinations required to build these schemes. We prove a series of assertions that can make conclusions about the order of approximation depending on the type of local solutions. Stability analysis is carried out on the basis of the principle of frozen coefficients. The cases of a smooth and discontinuous behavior of solutions in the field of linearization with frozen coefficients on the faces of the final volume and spectra of the schemes are analyzed for these cases. We prove the linear stability conditions for a variety of Runge-Kutta methods applied to WENO schemes. As a result, our research provides guidance on choosing the best possible stability parameter, which has the smallest effect on the nonlinear properties of the schemes. The convergence of the schemes is followed from the analysis.
topic WENO schemes
nonlinear schemes
stability of numerical schemes
hyperbolic systems of differential equations
Hopf equation
url http://crm.ics.org.ru/uploads/crmissues/crm_2016_5/2016.08.02.pdf
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