Abstract:Abstract. We briefly review two different methods of applying Lie group theory in the numerical solution of ordinary differential equations. On specific examples we show how the symmetry preserving discretization provides difference schemes for which the "first differential approximation" is invariant under the same Lie group as the original ordinary differential equation.
“…As was discussed in Section 3.6, the invariant Lagrangian schemes (32) and (33) using (34) are exact for the Galilean invariant solution (10). We verify this by numerically computing this solution and calculating the l ∞ -norm and the RMSE.…”
Section: Exact Algebraic Solutionmentioning
confidence: 71%
“…In order to complete the numerical scheme (32) and (33) it is necessary to formulate an equation for the grid velocity. In the purely Lagrangian scheme one uses the discretization of the relation (7), which is…”
“…The mesh is said to be equidistributing for ρ on a b The function ρ is called mesh density function or monitor function. For the practical implementation it is advantageous to convert the relation (36) into a differential equation. This is done by first using the equivalent expression where ξ j , = j N 1 ,..., , is the discrete computational coordinate.…”
“…For partial differential equations (PDEs) the first application of Lie group theory to numerical methods is, to our knowledge, due to Shokin and Yanenko [45,49]. Their approach "Differential approximation" is quite different from ours (for a comparison see [33]).…”
The Korteweg-de Vries equation is one of the most important nonlinear evolution equations in the mathematical sciences. In this article invariant discretization schemes are constructed for this equation both in the Lagrangian and in the Eulerian form. We also propose invariant schemes that preserve the momentum. Numerical tests are carried out for all invariant discretization schemes and related to standard numerical schemes. We find that the invariant discretization schemes give generally the same level of accuracy as the standard schemes with the added benefit of preserving Galilean transformations which is demonstrated numerically as well.arXiv:1409.4340v1 [math-ph]
“…As was discussed in Section 3.6, the invariant Lagrangian schemes (32) and (33) using (34) are exact for the Galilean invariant solution (10). We verify this by numerically computing this solution and calculating the l ∞ -norm and the RMSE.…”
Section: Exact Algebraic Solutionmentioning
confidence: 71%
“…In order to complete the numerical scheme (32) and (33) it is necessary to formulate an equation for the grid velocity. In the purely Lagrangian scheme one uses the discretization of the relation (7), which is…”
“…The mesh is said to be equidistributing for ρ on a b The function ρ is called mesh density function or monitor function. For the practical implementation it is advantageous to convert the relation (36) into a differential equation. This is done by first using the equivalent expression where ξ j , = j N 1 ,..., , is the discrete computational coordinate.…”
“…For partial differential equations (PDEs) the first application of Lie group theory to numerical methods is, to our knowledge, due to Shokin and Yanenko [45,49]. Their approach "Differential approximation" is quite different from ours (for a comparison see [33]).…”
The Korteweg-de Vries equation is one of the most important nonlinear evolution equations in the mathematical sciences. In this article invariant discretization schemes are constructed for this equation both in the Lagrangian and in the Eulerian form. We also propose invariant schemes that preserve the momentum. Numerical tests are carried out for all invariant discretization schemes and related to standard numerical schemes. We find that the invariant discretization schemes give generally the same level of accuracy as the standard schemes with the added benefit of preserving Galilean transformations which is demonstrated numerically as well.arXiv:1409.4340v1 [math-ph]
“…Another technique relies on the concept of differential approximations. It consists in finding a numerical scheme such that its differential approximation is invariant under the Lie group admitted by the equation [161][162][163]. It generally leads to only partially invariant schemes.…”
Section: Lie Groups and Numerical Integratorsmentioning
Article de synthèseThe French "Année de la Mécanique": some views on recent advances in solid and fluid mechanics / L'année de la mécanique : quelques points de vue sur des avancées récentes en mécanique des solides et des fluides Lie groups and continuum mechanics: where do we stand today?Groupes de Lie et mécanique des milieux continus : où en sommes-nous aujourd'hui ?
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