Titlebook: Riemann Solvers and Numerical Methods for Fluid Dynamics; A Practical Introduc Eleuterio F. Toro Book 19971st edition Springer-Verlag Berli

MUTE

The Riemann Problem for the Euler Equations,o non-linear systems of hyperbolic conservation laws. The key ingredient of the scheme is the solution of the Riemann problem. The purpose of this chapter is to provide a detailed presentation of the complete, exact solution to the Riemann problem for the one-dimensional, time-dependent Euler equati

EXCEL

平淡而無(wú)味

巧辦法

Random Choice and Related Methods,ems of hyperbolic conservation laws. In 1976, Chorin [65] successfully implemented a modified version of the method to solve the Euler equations of Gas Dynamics. In essence, to implement the RCM one requires (i) exact solutions of local Riemann problems and (ii) a random sampling procedure to pick u

Liberate

Flux Vector Splitting Methods,e incorporated into the discretisation schemes. There are essentially two approaches for identifying upwind directions, namely the . [130]studied in Chap. 6, and the . (FVS) approach [269], [299] to be studied in this chapter. These two approaches are respectively referred to as the . and the . [357

Calibrate

microscopic

The HLL and HLLC Riemann Solvers,The resulting Riemann solvers have become known as HLL Riemann solvers. In this approach an ., unlike the Riemann solvers presented previously in Chaps. 4 and 9. The central idea is to assume a wave configuration for the solution that consists of two waves separating three constant states. Assuming

偽證

保守

disrupt

High-Order and TVD Methods for Scalar Problems,ysical) oscillations in the vicinity of large gradients. It is well-known that high-order linear (constant coefficients) schemes produce unphysical oscillations in the vicinity of large gradients. This was illustrated by some numerical results shown in Chap. 5. On the other hand, the class of ., def