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Table of Contents
1 Cover
4 Preface
5 1 Turbulent Channel Flow to Reτ = 590 in Discrete Mechanics 1.1. Introduction 1.2. Discrete mechanics formulation 1.3. Turbulent flow in channel 1.4. Conclusion 1.5. References
6 2 Atomization in an Acceleration Field1 2.1. Introduction 2.2. Generation of droplets through vibrations normal to the liquid layer 2.3. Rayleigh–Taylor instability at the crest of an axial wave 2.4. Recent work 2.5. Conclusion 2.6. References
7 3 Numerical Simulation of Pipes with an Abrupt Contraction Using OpenFOAM 3.1. Introduction 3.2. Modeling an abrupt contraction in a pipe 3.3. Numerical results 3.4. Conclusion and future prospects 3.5. References
8 4 Vaporization of an Equivalent Pastille 4.1. Introduction 4.2. Equations for the problem 4.3. Linear analysis of the liquid phase 4.4. Some results 4.5. Conclusion 4.6. References
9 5 Thermal Field of a Continuously-Fed Drop Subjected to HF Perturbations 5.1. Drops in a liquid-propellant rocket engine 5.2. A continuously fed droplet 5.3. Equations of the problem 5.4. Linearized equations 5.5. Linearized equations for small harmonic perturbations 5.6. Thermal field in the drop when neglecting internal convection 5.7. Conclusion 5.8. Appendix 1: Coefficients that come into play in linearized equations 5.9. Appendix 2: Solving the thermal equation 5.10. Appendix 3: The case of the equivalent pastille 5.11. Appendix 4: 2D representation for the spherical drop 5.12. References
10 6 Study of the Three-Dimensional and Non-Stationary Flow in a Rotor of the Savonius Wind Turbine 6.1. Introduction 6.2. Mathematical modeling of the problem 6.3. Numerical resolution 6.4. Validation of the results 6.5. Results and discussion 6.6. Conclusion 6.7. Acknowledgments 6.8. References
12 Index
List of Tables
1 Chapter 1Table 1.1. Curvature in the zone y+ > δn calculated by model-free simulati...
2 Chapter 4Table 4.1. Six types of configuration when there is an exchange coefficient at t...
List of Illustrations
1 Chapter 1Figure 1.1. Discrete geometric structure: a set of primitive planar facets S are...Figure 1.2. Turbulent channel with Reτ = 590; average velocity profiles in reduc...Figure 1.3. (a) Turbulent channel with Reτ = 590 (Denaro et al. 2011), r = f(y+)...Figure 1.4. Turbulent channel with Reτ = 590, results of unit-2 (Denaro et al. 2...Figure 1.5. Turbulent channel with Reτ = 590, comparison between the results of ...Figure 1.6. Turbulent channel with Reτ = 590. Results of the TDM model (dots) co...Figure 1.7. Turbulent channel with Reτ = 590. The reduced turbulent viscosity μd...Figure 1.8. Turbulent channel with Reτ = 590, results from MKM99