Book contents
- Frontmatter
- Contents
- List of Figures
- Preface
- 1 Introduction
- I BASIC THEORY
- II NUMERICAL IMPLEMENTATION
- 7 From the GRP Algorithm to Scientific Computing
- 8 Geometric Extensions
- 9 A Physical Extension: Reacting Flow
- 10 Wave Interaction in a Duct — A Comparative Study
- A Entropy Conditions for Scalar Conservation Laws
- B Convergence of the Godunov Scheme
- C Riemann Solver for a γ-Law Gas
- D The MUSCL Scheme
- Bibliography
- Glossary
- Index
9 - A Physical Extension: Reacting Flow
Published online by Cambridge University Press: 20 August 2009
- Frontmatter
- Contents
- List of Figures
- Preface
- 1 Introduction
- I BASIC THEORY
- II NUMERICAL IMPLEMENTATION
- 7 From the GRP Algorithm to Scientific Computing
- 8 Geometric Extensions
- 9 A Physical Extension: Reacting Flow
- 10 Wave Interaction in a Duct — A Comparative Study
- A Entropy Conditions for Scalar Conservation Laws
- B Convergence of the Godunov Scheme
- C Riemann Solver for a γ-Law Gas
- D The MUSCL Scheme
- Bibliography
- Glossary
- Index
Summary
In this chapter we consider the system of equations governing compressible reacting flow. The fluid is a homogeneous mixture of two species. The evolution of the flow under the mechanical conservation laws of mass, momentum and energy is coupled to the (continuous or abrupt) conversion of the “unburnt” species to the “burnt” one. We take the simplest model of such a reaction, namely, an irreversible exothermic process. The equation of state of the fluid depends on its chemical composition. The resulting (augmented) system is still nonlinear hyperbolic (in the sense of Chapter 4) and is amenable to the GRP methodology. The basic hypotheses are presented in Section 9.1, leading to the derivation of the characteristic relations and jump conditions. In Section 9.2 we describe the classical Chapman—Jouguet model of deflagrations and detonations, and the Zeldovich—von Neumann—Döring (Z—N—D) solution is presented in Section 9.3. In Section 9.4 we study the generalized Riemann problem for the system of reacting flow. The treatment here is close to that of the basic GRP case (Section 5.1), but there are significant differences because of the reaction equation. In Section 9.5 we outline briefly the resulting GRP numerical scheme and study a physical problem of ozone decomposition.
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- Generalized Riemann Problems in Computational Fluid Dynamics , pp. 269 - 304Publisher: Cambridge University PressPrint publication year: 2003