In this paper a recently developed approach for the design of adaptive discontinuous Galerkin finite element methods is applied to physically relevant problems arising in inviscid compressible fluid flows governed by the Euler equations of gas dynamics. In particular, we employ (weighted) type I a p
Computational Methods for Self-similar Solutions of the Compressible Euler Equations
โ Scribed by Ravi Samtaney
- Publisher
- Elsevier Science
- Year
- 1997
- Tongue
- English
- Weight
- 894 KB
- Volume
- 132
- Category
- Article
- ISSN
- 0021-9991
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โฆ Synopsis
as an initial value problem with appropriate boundary conditions. In this paper, we seek the self-similar solutions Computations of self-similar solutions of the compressible Euler equations as a boundary value problem in similarity coordinates of the compressible Euler equations as a boundary value ( ฯญ x/t, ฯญy/t) are presented. Two new implicit methods namely problem after a suitable self-similar transformation is the implicit Godunov method and the implicit Equilibrium Flux made. The self-similar transformation reduces the number Method are presented. The Jacobians for the implicit methods are
of independent variables by one. The solution we seek is analytically evaluated. In general the self-similar solutions exhibit a steady solution in the ( ฯต x/t, ฯต y/t ) space. We believe sharper discontinuities than corresponding solutions of the initial value problem. แฎ 1997 Academic Press that, intuitively, it is easier to deal with a steady state solution than one which is time-dependent. In addition, many of the test problems in the literature on numerical
๐ SIMILAR VOLUMES
## Communicated by W. Wendland The existence of global measure-valued solutions to the Euler equations describing the motion of an ideal compressible and heat conducting fluid is proved. The motion is considered in a bounded domain i2 c R 3 with impermeable boundary. The solution is a limit of an
An adaptive least-squares finite element method is used to solve the compressible Euler equations in two dimensions. Since the method is naturally diffusive, no explicit artificial viscosity is added to the formulation. The inherent artificial viscosity, however, is usually large and hence does not