Introduction to Computational Fluid Dynamics
Introduction to Computational Fluid Dynamics is a self-contained introduction to a new subject, arising through the amalgamation of classical fluid dynamics and numerical analysis supported by powerful computers. Written in the style of a text book for advanced level B.Tech, M.Tech and M.Sc. student...
Otros Autores: | , , |
---|---|
Formato: | Libro electrónico |
Idioma: | Inglés |
Publicado: |
[Place of publication not identified]
Pearson Education Canada
2009
|
Edición: | 1st edition |
Materias: | |
Ver en Biblioteca Universitat Ramon Llull: | https://discovery.url.edu/permalink/34CSUC_URL/1im36ta/alma991009628040606719 |
Tabla de Contenidos:
- Cover
- About the Authors
- Preface
- Acknowledgements
- Contents
- Part I: Finite Difference Method for Partial Differential Equations
- Chapter 1: Introduction and Mathematical Preliminaries
- 1.1 Introduction
- 1.2 Typical Partial Differential Equations in Fluid Dynamics
- 1.3 Types of Second-order Equations
- 1.3.1 Characteristics of Second-Order Equations
- 1.4 Well-posed Problems
- 1.4.1 Examples of Well-Posed Problems
- 1.4.2 An Ill-Posed Problem
- 1.5 Properties of Linear and Quasilinear Equations
- 1.5.1 Qualitative Properties of Partial Differential Equations
- 1.6 Physical Character of Subsonic and Supersonic Flows
- 1.7 Second-order Wave Equations
- 1.7.1 Cauchy Problem for the Wave Equation
- 1.7.2 Domain of Dependence and Range of Influence
- 1.8 System of First-order Equations
- 1.8.1 Classification and Types of First-Order Systems
- 1.8.2 Conservation Form and Conservation-Law Form
- 1.9 Weak Solutions
- 1.10 Summary
- 1.11 Key Terms
- Chapter 2: Finite Difference and Finite Volume Discretisations
- 2.1 Introduction
- 2.2 Finite Difference Discretisation
- 2.3 Discretisation of Derivatives
- 2.4 Consistency, Convergence, and Stability
- 2.5 Finite Volume Discretisation
- 2.5.1 Cell-Centred Scheme
- 2.6 Face Area and Cell Volume
- 2.6.1 Equivalence Between Finite Difference and Finite Volume Methods
- 2.7 Summary
- 2.8 Key Terms
- 2.9 Exercise 2
- Chapter 3: Equations of Parabolic Type
- 3.1 Introduction
- 3.2 Finite Difference Scheme for Heat Conduction Equation
- 3.2.1 FTCS Scheme: Truncation Error and Consistency
- 3.2.2 Modified Equation
- 3.2.3 FTCS Scheme: Convergence
- 3.2.4 FTCS Scheme: Stability
- 3.2.5 Derivative Boundary Conditions
- 3.3 Crank-Nicholson Implicit Scheme
- 3.4 Analogy with Schemes for Ordinary Differential Equations.
- 3.4.1 Thomas Algorithm for Tridiagonal Systems
- 3.4.2 Crank-Nicholson Scheme: Truncation Error, Consistency, and Convergence
- 3.4.3 Dissipative and Dispersive Errors
- 3.4.4 Stability of the Crank-Nicholson Scheme
- 3.5 A Note on Implicit Methods
- 3.6 Leap-frog and DuFort-Frankel Schemes
- 3.6.1 Truncation Error of the DuFort-Frankel Scheme
- 3.6.2 Stability of DuFort-Frankel Scheme
- 3.7 Operator Notation
- 3.8 The Alternating Direction Implicit (ADI) Method
- 3.8.1 ADI Scheme
- 3.8.2 Splitting and Approximate Factorisation
- 3.8.3 Stability of the ADI Scheme
- 3.8.4 Program 3.1: adi.f
- 3.9 Summary
- 3.10 Key Terms
- 3.11 Exercise 3
- Chapter 4: Equations of Hyperbolic Type
- 4.1 Introduction
- 4.2 Explicit Schemes
- 4.2.1 FTCS Scheme
- 4.2.2 FTFS Scheme
- 4.2.3 Upwind Scheme: First Order
- 4.2.4 Upwind Scheme: Modified Equation
- 4.2.5 The Lax Scheme
- 4.2.6 Consistency of Lax Scheme
- 4.2.7 Lax Scheme: Modified Equation
- 4.2.8 The Leap-Frog Scheme
- 4.3 Lax-Wendroff Scheme and Variants
- 4.3.1 Lax-Wendroff Scheme: Modified Equation
- 4.3.2 Two-Step Lax-Wendroff Scheme
- 4.3.3 The MacCormack Scheme
- 4.3.4 Upwind Scheme: Warming-Beam
- 4.4 Implicit Schemes
- 4.5 More on Upwind Schemes
- 4.6 Scalar Conservation Law: Lax-Wendroff and Related Schemes
- 4.6.1 Program 4.1: Ixmc.f
- 4.6.2 Implicit Schemes for Scalar Conservation Law
- 4.7 Hyperbolic System of Conservation Laws
- 4.7.1 System of Conservation Laws
- 4.8 Second-order Wave Equation
- 4.8.1 Stability of the Leap-Frog Scheme for the Wave Equation
- 4.8.2 An Implicit Scheme for the Second-Order Wave Equation
- 4.8.3 Stability of the Implicit Scheme
- 4.9 Method of Characteristics for Second-order Hyperbolic Equations
- 4.10 Model Convection-Diffusion Equation
- 4.10.1 Steady Convection-Diffusion Equation.
- 4.10.2 Linear Convection-Diffusion Equation: FTCS Scheme
- 4.10.3 First-Order Upwind Scheme for Convection-Diffusion Equation
- 4.10.4 Burgers Equation
- 4.11 Summary
- 4.12 Key Terms
- 4.13 Exercise 4
- Chapter 5: Equations of Elliptic Type
- 5.1 Introduction
- 5.2 The Laplace Equation in Two Dimension
- 5.3 Iterative Methods for Solution of Linear Algebraic Systems
- 5.3.1 The Jacobi and the Gauss-Seidel Schemes
- 5.4 Solution of the Pentadiagonal System
- 5.4.1 Program 5.1: sor.f
- 5.5 Approximate Factorisation Schemes
- 5.5.1 Analysis of Line Gauss-Seidel Scheme for the Laplace Equation
- 5.5.2 Time-Dependent Analogy
- 5.5.3 Program 5.2: afl.f
- 5.6 Grid Generation Example
- 5.7 Body-fitted Grid Generation Using Elliptic-type Equations
- 5.7.1 Solution of the Algebraic Equations by AFI Scheme
- 5.8 Some Observations of AF Schemes
- 5.9 Multi-grid Method
- 5.9.1 Program 5.3: mgc.f
- 5.10 Summary
- 5.11 Key Terms
- 5.12 Exercise 5
- Chapter 6: Equations of Mixed Elliptic-Hyperbolic Type
- 6.1 Introduction
- 6.2 Tricomi Equation
- 6.3 Transonic Computations Based on TSP Model
- 6.3.1 Finite Difference Discretisation
- 6.3.2 Implementation of Boundary Conditions
- 6.3.3 Iterative Solution of the Discretised Equations
- 6.3.4 Artificial Viscosity and Conservative Schemes
- 6.3.5 Computational Results
- 6.3.6 Program 6.1 tsc.f
- 6.4 Summary
- 6.5 Key Terms
- 6.6 Exercise 6
- Part II: Computational Fluid Dynamics
- Chapter 7: The Basic Equations of Fluid Dynamics
- 7.1 Introduction
- 7.2 Basic Conservation Principles
- 7.3 Unsteady Navier-Stokes Equations in Integral Form
- 7.4 Navier-Stokes Equations in Differential Form
- 7.4.1 Compressible Two-Dimensional Equations in Vector Form
- 7.4.2 Incompressible Navier-Stokes Equations in Cartesian Coordinates
- 7.4.3 Dimensionless Form of the Basic Equations.
- 7.4.4 Incompressible Two-Dimensional Equations: Dimensionless Form
- 7.4.5 Observations on the Basic Equations
- 7.5 Boundary Conditions for Navier-Stokes Equations
- 7.6 Reynolds Averaged Navier-Stokes Equations
- 7.7 Boundary-layer, Thin-layer and Associated Approximations
- 7.8 Euler Equations for Inviscid Flows
- 7.8.1 Certain Observations on Euler and Navier-Stokes Equations
- 7.9 Boundary Conditions for Euler Equations
- 7.9.1 Far-field Boundary Conditions for Euler Equations
- 7.10 The Full Potential Equation
- 7.10.1 Potential Equation in Conservative Form
- 7.10.2 Boundary Conditions for the Full Potential Equation
- 7.10.3 Transonic Small Perturbation Model
- 7.10.4 Oswatitsch Reduction
- 7.10.5 Cole's and Other Forms of the TSP Equation
- 7.11 Inviscid Incompressible Irrotational Flow
- 7.12 Summary
- 7.13 Key Terms
- Chapter 8: Grid Generation
- 8.1 Introduction
- 8.2 Co-ordinate Transformation
- 8.3 Differential Equation Methods
- 8.4 Algebraic Methods
- 8.4.1 Calculation of the Arc Length
- 8.4.2 Desired Arc Length Distribution
- 8.4.3 Calculation of the Angle θ on the Aerofoil and Cut
- 8.4.4 Calculation of ymin and nmax
- 8.4.5 Δn - Distribution on the Aerofoil and the Cut
- 8.4.6 Mesh Spacing in n-Direction
- 8.4.7 Calculation of x and y at Nodal Points
- 8.4.8 Cubic Spline
- 8.5 Transfinite Interpolation Methods
- 8.6 Unstructured Grid Generation
- 8.7 Mesh Adaptation
- 8.7.1 Moving Mesh
- 8.7.2 Mesh Enrichment
- 8.8 Summary
- 8.9 Key Terms
- 8.10 Exercise 8
- Chapter 9: Inviscid Incompressible Flow
- 9.1 Introduction
- 9.2 Potential Flow Problem
- 9.3 Panel Methods
- 9.3.1 AMO Smith Method for a Lifting Airfoil
- 9.3.2 Influence Coefficients
- 9.4 Panel Methods (Continued)
- 9.4.1 Mathematical Preliminaries for Morino-Kuo Method
- 9.4.2 Flow Past an Aerofoil.
- 9.4.3 A Constant-Potential Panel Method
- 9.4.4 Morino-Kuo Method
- 9.4.4.1 Pressure coefficient, forces, and moments
- 9.4.5 Program 9.1: Morinoprogram.c
- 9.4.6 Discretisation Error in Panel Methods
- 9.5 More on Panel Methods
- 9.6 Panel Methods for Subsonic and Supersonic Flows
- 9.7 Summary
- 9.8 Key Terms
- 9.9 Exercise 9
- Chapter 10: Inviscid Compressible Flow
- 10.1 Introduction
- 10.1.1 Transonic Controversy
- 10.2 Small-perturbation Flow
- 10.2.1 Subsonic Flow Past a Thin Profile
- 10.2.2 Supersonic Small-Perturbation Flow
- 10.3 Numerical Solution of the Full Potential Equation
- 10.3.1 Rotated Difference Scheme
- 10.3.2 Conservative Schemes for the Potential Equation
- 10.4 Full Potential Solution in Generalised Coordinates
- 10.4.1 Spatial Differencing and Artificial Viscosity
- 10.4.2 AF2 Iteration Scheme
- 10.4.3 Boundary Conditions
- 10.4.4 Computational Results of Full-Potential Solution
- 10.5 Observations on the Full Potential Model
- 10.6 Euler Model
- 10.6.1 Governing Equations in Two Dimension
- 10.6.2 Numerical Methods for the Euler Model
- 10.6.3 Explicit and Implicit Schemes
- 10.6.4 Review of Acceleration Techniques
- 10.6.5 Finite Volume Discretisation
- 10.6.6 Artificial Dissipation
- 10.7 Boundary Conditions
- 10.7.1 Time Stepping Scheme
- 10.7.2 Acceleration Techniques
- 10.8 Computed Examples Based on the Euler Model
- 10.9 Supersonic Flow Field Computation
- 10.9.1 Examples of Supersonic Flow Computation
- 10.10 Summary
- 10.11 Key Terms
- 10.12 Exercise 10
- Chapter 11: Boundary Layer Flow
- 11.1 Introduction
- 11.2 The Boundary Layer: Physical Considerations
- 11.2.1 Separation of the Boundary Layer from the Surface
- 11.2.2 Turbulence
- 1 1.2.3 Measures of Boundary Layer Thickness
- 11.3 The Boundary Layer Equations
- 1 1.3.1 Assumptions of the Boundary Layer Theory.
- 11.3.2 The Boundary Layer Equations for Laminar Flow.