Solution to systems of hyperbolic conservation laws may be discontinuous. Example of such systems are the Euler equations and Shallow Water equations. To solve systems of hyperbolic conservation laws, numerical methods which can resolve discontinuities have been developed. One family of such methods is the RK(Runge-Kutta)-ENO(Essentially Non-Oscillatory) shock-capturing scheme. Here we study the modified equation of RK-ENO methods by solving the 1D isen-tropic Euler equations. For fast shocks the numerical orbit in phase plane is a single continuous curve. But for slow shocks it may be discontinuous. The results are compared with numerical orbits by LxF(Lax-Friedrichs) scheme for the modified equation. Undersökning av den interna strukturen...
Essentially nonoscillatory (ENO) and weighted ENO (WENO) methods on equidistant Cartesian grids are ...
A wide class of difference equations is described for approximating discontinuous time dependent sol...
In this work the essentially non-oscillatory schemes (ENO) and the weighted essentially non-oscillat...
ii In this paper we describe the construction, analysis, and application of ENO ( Essentially Non-Os...
An essentially nonoscillatory (ENO) formulation is described for hyperbolic systems of conservation ...
In recent years, a class of numerical schemes for solving hyperbolic partial differential equations ...
In recent years, a class of numerical schemes for solving hyperbolic partial differential equations ...
The present work is concerned with an application of the theory of characteristics to conservation l...
The present work is concerned with an application of the theory of characteristics to conservation l...
The present work is concerned with an application of the theory of characteristics to conservation l...
AbstractWe consider hyperbolic 1-conservation laws. Such laws appear in problems of traffic flow, fl...
In the computation of discontinuous solutions of hyperbolic conservation laws, TVD (total-variation-...
ENO (essentially non-oscillatory) schemes can provide uniformly high order accuracy right up to disc...
AbstractThe theoretical understanding of discrete shock transitions obtained by shock capturing sche...
The high speed flow of complex materials can often be modeled by the compressible Euler Equations co...
Essentially nonoscillatory (ENO) and weighted ENO (WENO) methods on equidistant Cartesian grids are ...
A wide class of difference equations is described for approximating discontinuous time dependent sol...
In this work the essentially non-oscillatory schemes (ENO) and the weighted essentially non-oscillat...
ii In this paper we describe the construction, analysis, and application of ENO ( Essentially Non-Os...
An essentially nonoscillatory (ENO) formulation is described for hyperbolic systems of conservation ...
In recent years, a class of numerical schemes for solving hyperbolic partial differential equations ...
In recent years, a class of numerical schemes for solving hyperbolic partial differential equations ...
The present work is concerned with an application of the theory of characteristics to conservation l...
The present work is concerned with an application of the theory of characteristics to conservation l...
The present work is concerned with an application of the theory of characteristics to conservation l...
AbstractWe consider hyperbolic 1-conservation laws. Such laws appear in problems of traffic flow, fl...
In the computation of discontinuous solutions of hyperbolic conservation laws, TVD (total-variation-...
ENO (essentially non-oscillatory) schemes can provide uniformly high order accuracy right up to disc...
AbstractThe theoretical understanding of discrete shock transitions obtained by shock capturing sche...
The high speed flow of complex materials can often be modeled by the compressible Euler Equations co...
Essentially nonoscillatory (ENO) and weighted ENO (WENO) methods on equidistant Cartesian grids are ...
A wide class of difference equations is described for approximating discontinuous time dependent sol...
In this work the essentially non-oscillatory schemes (ENO) and the weighted essentially non-oscillat...