Compressible Flow Propulsion and Digital Approaches in Fluid Mechanics
By Michel Ledoux and Abdelkhalak El Hami
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Compressible Flow Propulsion and Digital Approaches in Fluid Mechanics - Michel Ledoux
Table of Contents
Cover
Title
Copyright
Preface
1 The Flow of Viscous Fluids. Flow in the Vicinity of a Wall: Boundary Layers and Films
1.1. Introduction
1.2. Characteristics and classification of boundary layers
1.3. The outer boundary layers: an analytical approach
1.4. Examples of analytical approach: outer flows
1.5. Examples of analytical approach: inner flows
1.6. Outer boundary layers: integral methods
1.7. Channels and films
2 One-dimensional Compressible Flows: Fully Reversible Flows
2.1. Introduction
2.2. One-dimensional adiabatic and reversible flows
2.3. Applications. Reversible adiabatic flows
3 One-dimensional Compressible Flows: Irreversible Flows
3.1. Introduction
3.2. Irreversible flow: straight shock wave
3.3. Partially irreversible flows: shock wave in a nozzle
3.4. Conclusion
4 Modeling and Numerical Simulations
4.1. Introduction
4.2. Methodology description and simulation approach
4.3. Modeling and simulation of coupled systems
4.4. Variational formulation
4.5. Finite element approximation
4.6. The vibro-acoustic problem
4.7. The hydro-elastic problem
4.8. Applications
4.9. Conclusion
5 Numerical Simulation of a Vertical-axis Wind Turbine
5.1. Introduction
5.2. Construction of the rotor geometry and definition of the computational domain
5.3. Analysis of the results
5.4. Conclusion
Appendix: General Equations of Fluid Mechanics
A.1. Review
A.2. Writing the laws
A.3. The equations: expanded form and simplifications
A.4. Table of adiabatic flows
A.5. Straight shock table
Bibliography
Index
End User License Agreement
List of Tables
3 One-dimensional Compressible Flows: Irreversible Flows
Table 3.1. Velocities of some military or civilian projectiles
4 Modeling and Numerical Simulations
Table 4.1. CL and CD
Table 4.2. Data of the problem
5 Numerical Simulation of a Vertical-axis Wind Turbine
Table 5.1. Number of elements of sub-domains
Table 5.2. Relationship between angular velocity and time step
Table 5.3. Parameters used in numerical simulations
Table 5.4. Experimental device for the validation of the CFD model
Table 5.5. Values of σ and Ct parameters
List of Illustrations
1 The Flow of Viscous Fluids. Flow in the Vicinity of a Wall: Boundary Layers and Films
Figure 1.1. Stokes’ first problem. Representation of the velocity profile at two moments of time
Figure 1.2. Stokes’ second problem
Figure 1.3. Couette flow. On the left: Couette flow between two plates. On the right: application of this model as an approximation to Couette viscometer
Figure 1.4. Flow in annular space
Figure 1.5. Flat plate in the path of wind
Figure 1.6. Various approximations of the Blasius profile for boundary layer. For a color version of this figure, see www.iste.co.uk/ledoux/fluid.zip
Figure 1.7. Pont du Gard. Left: diagram of the aqueduct. Right: Pont du Gard, such as it is depicted on the €5 note
Figure 1.8. Pont du Gard: the system of coordinates
Figure 1.9. Relation between dz and dx
Figure 1.10. Hacking the aqueduct
Figure 1.11. A household incident
2 One-dimensional Compressible Flows: Fully Reversible Flows
Figure 2.1. Graphical representation of the function
Figure 2.2. Displacement of the representative point of the flow on the curve.
a) Subsonic flow in the converging and diverging parts. b) Sonic flow at the throat, subsonic flow in the converging and diverging parts. c) Sonic flow at the throat, subsonic flow in the converging part and supersonic flow in the diverging part
Figure 2.3. The compressed-air generator and its valve
Figure 2.4. The tire and its air leak
Figure 2.5. Pressure cooker and its valve
Figure 2.6. A supersonic generator within everyone’s reach
Figure 2.7. Schematic representation of a supersonic wind tunnel
Figure 2.8. Small missile engine
Figure 2.9. Leakages from a nitrogen tank
3 One-dimensional Compressible Flows: Irreversible Flows
Figure 3.1. Shock wave in a tube
Figure 3.2. Small shock tube
Figure 3.3. Shock wave attached to a supersonic projectile
Figure 3.4. Industrial accident
Figure 3.5. Thermocouple testing device
Figure 3.6. Measurement of the response time of a thermocouple
Figure 3.7. High-temperature chemistry
Figure 3.8. Outlet pressure adjustment by the shock wave. a) Upstream of the shock wave; b) Downstream of the shock wave
Figure 3.9. Emptying a reservoir
Figure 3.10. Adjustment of the position of the shock wave in de Laval nozzle
Figure 3.11. Diagram of the propeller
4 Modeling and Numerical Simulations
Figure 4.1. Flow in a pipe
Figure 4.2. Computational domain
Figure 4.3. Mesh
Figure 4.4. Velocity distribution throughout the pipe. For a color version of this figure, see www.iste.co.uk/ledoux/fluid.zip
Figure 4.5. Static pressure contour. For a color version of this figure, see www.iste.co.uk/ledoux/fluid.zip
Figure 4.6. Velocity profile at the pipe outlet in laminar regime
Figure 4.7. Axial variation of pressure
Figure 4.8. Distribution of the turbulence kinetic energy. For a color version of this figure, see www.iste.co.uk/ledoux/fluid.zip
Figure 4.9. Profile of velocity at the pipe outlet in turbulent regime
Figure 4.10. Laminar flow around a cylinder
Figure 4.11. Presentation of the computational domain
Figure 4.12. Mesh detail: O-type mesh
Figure 4.13. Static pressure contour. For a color version of this figure, see www.iste.co.uk/ledoux/fluid.zip
Figure 4.14. Velocity contour around the cylinder. For a color version of this figure, see www.iste.co.uk/ledoux/fluid.zip
Figure 4.15. Pressure contour around the cylinder. For a color version of this figure, see www.iste.co.uk/ledoux/fluid.zip
Figure 4.16. Velocity distribution around the cylinder. For a color version of this figure, see www.iste.co.uk/ledoux/fluid.zip
Figure 4.17. Convergence of the solution for Δt = 1 s
Figure 4.18. Convergence of the solution for Δt = 0,2 s
Figure 4.19. Convergence of the solution for Δt = 0,02 s
Figure 4.20. Aerodynamic study of the NACA profile
Figure 4.21. Computational domain
Figure 4.22. C-type mesh
Figure 4.23. Velocity for α = 0°. For a color version of this figure, see www.iste.co.uk/ledoux/fluid.zip
Figure 4.24. Velocity for α = 4°. For a color version of this figure, see www.iste.co.uk/ledoux/fluid.zip
Figure 4.25. Velocity for α = 8°. For a color version of this figure, see www.iste.co.uk/ledoux/fluid.zip
Figure 4.26. Velocity for α = 10°. For a color version of this figure, see www.iste.co.uk/ledoux/fluid.zip
Figure 4.27. Velocity for α = 15°. For a color version of this figure, see www.iste.co.uk/ledoux/fluid.zip
Figure 4.28. Velocity for α = 20°. For a color version of this figure, see www.iste.co.uk/ledoux/fluid.zip
Figure 4.29. Pressure for α = 0°. For a color version of this figure, see www.iste.co.uk/ledoux/fluid.zip
Figure 4.30. Pressure for α = 4°. For a color version of this figure, see www.iste.co.uk/ledoux/fluid.zip
Figure 4.31. Pressure for α = 10°. For a color version of this figure, see www.iste.co.uk/ledoux/fluid.zip
Figure 4.32. Pressure for α = 15°. For a color version of this figure, see www.iste.co.uk/ledoux/fluid.zip
Figure 4.33. Pressure for α = 20°. For a color version of this figure, see www.iste.co.uk/ledoux/fluid.zip
Figure 4.34. Thin plate immersed in a tank (75% filled with water)
Figure 4.35. Experimental setup
Figure 4.36. Image of a mode rendered by the display monitor
Figure 4.37. Experimentally found deflections of the first modes
Figure 4.38. Modification of the sixth mode as a function of the immersion rate: (a) in the air, (b) partial immersion, (c) full immersion
Figure 4.39. The first five eigen modes of the plate, respectively in the air and in full immersion in water
Figure 4.40. Modification of the sixth mode depending on the immersion rate
Figure 4.41. FRF of the dry plate and fully immersed plate. For a color version of this figure, see www.iste.co.uk/ledoux/fluid.zip
Figure 4.42. Dimensions of the tube. For a color version of this figure, see www.iste.co.uk/ledoux/fluid.zip
Figure 4.43. Tetrahedral mesh (2879 nodes, 12360 elements). For a color version of this figure, see www.iste.co.uk/ledoux/fluid.zip
Figure 4.44. Contours of static temperature(k). For a color version of this figure, see www.iste.co.uk/ledoux/fluid.zip
Figure 4.45. Contour of Velocity Magnitude (m/s). For a color version of this figure, see www.iste.co.uk/ledoux/fluid.zip
Figure 4.46. Velocity vectors. For a color version of this figure, see www.iste.co.uk/ledoux/fluid.zip
5 Numerical Simulation of a Vertical-axis Wind Turbine
Figure 5.1. NACA 0021 profile
Figure 5.2. Computational domain and boundary conditions
Figure 5.3. Mesh images: general (a), around the rotor (b) and in the vicinity of the blades (c)
Figure 5.4. Control volume used for the discretization of transport equations, adapted from ANSYS Inc. [CON 11]
Figure 5.5. Straight-bladed Darrieus wind turbine
Figure 5.6. Validation of the proposed CFD model compared with the experimental and numerical results of a Darrieus wind turbine [CAS 11]
Figure 5.7. Transient evolution of the torque coefficient during 10 rotation cycles
Figure 5.8. Azimuthal evolution of the aerodynamic torque
Figure 5.9. Instantaneous torque for various tip speed ratios. For a color version of this figure, see www.iste.co.uk/ledoux/fluid.zip
Figure 5.10. Velocity contours for various tip speed ratios. For a color version of this figure, see www.iste.co.uk/ledoux/fluid.zip
Figure 5.11. Image of the 2D mesh model for various numbers of blades
Figure 5.12. Azimuthal evolution of the aerodynamic torque for various numbers of blades. For a color version of this figure, see www.iste.co.uk/ledoux/fluid.zip
Figure 5.13. Velocity contours for various numbers of blades. For a color version of this figure, see www.iste.co.uk/ledoux/fluid.zip
Mathematical and Mechanical Engineering Set
coordinated by
Abdelkhalak El Hami
Volume 4
Compressible Flow Propulsion and Digital Approaches in Fluid Mechanics
Michel Ledoux
Abdelkhalak El Hami
Wiley LogoFirst published 2017 in Great Britain and the United States by ISTE Ltd and John Wiley & Sons, Inc.
Apart from any fair dealing for the purposes of research or private study, or criticism or review, as permitted under the Copyright, Designs and Patents Act 1988, this publication may only be reproduced, stored or transmitted, in any form or by any means, with the prior permission in writing of the publishers, or in the case of reprographic reproduction in accordance with the terms and licenses issued by the CLA. Enquiries concerning reproduction outside these terms should be sent to the publishers at the undermentioned address:
ISTE Ltd
27-37 St George’s Road
London SW19 4EU
UK
www.iste.co.uk
John Wiley & Sons, Inc.
111 River Street
Hoboken, NJ 07030
USA
www.wiley.com
© ISTE Ltd 2017
The rights of Michel Ledoux and Abdelkhalak El Hami to be identified as the authors of this work have been asserted by them in accordance with the Copyright, Designs and Patents Act 1988.
Library of Congress Control Number: 2016959823
British Library Cataloguing-in-Publication Data
A CIP record for this book is available from the British Library
ISBN 978-1-78630-112-3
Preface
Mathematical physics was brought into existence by the development of mechanics. It originated in the study of the planetary motions and of the falling of heavy bodies, which had led Newton to formulate the fundamental laws of mechanics, as early as 1687. Even though the mechanics of continuous media, first as solid mechanics, and later as fluid mechanics, is a more recent development, its roots can be found in Isaac Newton’s Philosophiaenaturalis principia mathematica (Mathematical Principles of Natural Philosophy), several pages of which are dedicated to the falling streams of liquid.
Applications of fluid mechanics to irrigation problems date back to antiquity, but the subject gained a key status during the industrial revolution. Energetics was vital to the development of knowledge-demanding, specialized industrial areas such as fluid supply, heat engineering, secondary energy production or propulsion. Either as carrier of sensible heat or as core of energy production processes, fluid is ubiquitous in all the high-technology industries of the century: aeronautics, aerospace, automotive, industrial combustion, thermal or hydroelectric power plants, processing industries, national defense, thermal and acoustic environment, etc.
Depending on the target audience, there are various approaches to fluid mechanics. Covering this diversity is what we are striving for in this work.
Regardless of the degree of difficulty of the approached subject, it is important for the reader to reflect on it while being fully aware of the laws to be written in one form or another. Various approaches to fluid mechanics are illustrated by examples in this work.
First of all, the student will have the opportunity to handle simplified tools, allowing him/her a convenient first approach of the subject. On the other hand, the practitioner will be provided with elementary dimensioning means.
Other problems may justify or require a more complex approach, involving more significant theoretical knowledge, in particular of calculus. This is once again a point on which students and practitioners who already master these subjects can converge.
A third approach, which is essential for today’s physics, especially when dealing with problems that are too complex to be accurately solved by simple calculations, resorts to numerical methods. This work illustrates these remarks.
Problem resolution relies in each chapter on reviews of fundamental notions. These reviews are not exhaustive, and the reader may find it useful to go back to textbooks for knowledge consolidation. Nevertheless, certain proofs referring to important points are resumed. As already mentioned, what matters is that the reader has a good grasp of what he/she writes.
Given that we target wide audiences, the deduction or review of general equations can be found in the appendices, to avoid the book becoming too cumbersome.
The attempt to effectively address audiences with widely varied levels of knowledge, expertise or experience in the field may seem an impossible task.
Drawing on their experience of teaching all these categories of audiences, the authors felt motivated and encouraged to engage in this daring enterprise.
Exploring subjects such as propulsion, compressible flows, and the numerical approach to Fluid Mechanics, this book primarily focuses on more complex problems, particularly on examples of industrial applications.
In Chapter 1 of this second volume, the subject of viscous fluids is resumed from an analytical perspective: the structure of flows at boundaries is taken into account; the boundary layer theory is extensively used; significant attention is given to integral methods; an introduction to this field in relation to non-Newtonian fluids is provided; viscous flows through piping systems are examined; some particular types of unsteady boundary layers are also addressed.
In high velocity fluid flows, the combination of thermodynamics and mechanics leads to behaviors that are highly characteristic of compressible fluids. Two chapters of this book focus on this part of fluid mechanics, a very important one especially in aeronautics and aerospace. The physics of nozzles, generators of jets producing the thrust of jet and rocket engines, is approached within the framework of one-dimensional flows.
Chapter 2 is dedicated to fully reversible, compressible one-dimensional flows.
Chapter 3 focuses on the emergence of local irreversibilities in such flows. The development of the theory of straight shock waves uses the example and the positioning of such shock waves in a nozzle.
The schematic and simplified form of flow is applicable to many practical cases and it validates the models described in the above mentioned chapters. In many cases, the high complexity of the flow renders oversimplification inappropriate. This is especially valid for turbulent or vortex flows in industrial applications. At present, the engineer or researcher has privileged access to computation tools covering a wide range of capacities.
Two chapters are dedicated to the numerical approach, which is required for problems involving structures that are too complex to be dealt with by elementary modeling.
Chapter 4 addresses modeling and simulation in fluid mechanics. Numerical computations are conducted in 2D, while flow variations in the vertical plane are neglected and blade tip losses are not taken into account.
The distribution of inlet wind velocity is considered uniform and the blades are considered straight.
Chapter 5 is dedicated to an industrial application. It