Classical Fluid Mechanics - Michael Belevich - E-Book

Classical Fluid Mechanics E-Book

Michael Belevich

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Beschreibung

This textbook primarily explains the construction of the classical fluid model to readers in a holistic manner. Secondly, the book also explains some possible modifications of the classical fluid model which either make the model applicable in some special cases (viscous or turbulent fluids) or simplify it in accordance with the specific mechanical properties (hydrostatics, two-dimensional flows, boundary layers, etc.).
The book explains theoretical concepts in two parts. The first part is dedicated to the derivation of the classical model of the perfect fluid. The second part of the book covers important modifications to the fluid model which account for calculations of momentum, force and the laws of energy conservation. Concepts in this section include the redefinition of the stress tensor in cases of viscous or turbulent flows and laminar and turbulent boundary layers.
The text is supplemented by appropriate exercises and problems which may be used in practical classes. These additions serve to teach students how to work with complex systems governed by differential equations.
Classical Fluid Mechanics is an ideal textbook for students undertaking semester courses on fluid physics and mechanics in undergraduate degree programs.

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Veröffentlichungsjahr: 2017

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Table of Contents
Welcome
Table of Contents
Title Page
BENTHAM SCIENCE PUBLISHERS LTD.
End User License Agreement (for non-institutional, personal use)
Usage Rules:
Disclaimer:
Limitation of Liability:
General:
FOREWORD
PREFACE
Conflict of interest
Acknowledgements
Part I Model of continuum
Bodies and Their Characteristics
Abstract
1.1. INTRODUCTION
1.2. SPACE OF EVENTS AND FRAMES OF REFERENCE
1.3. MOTION
1.4. MASS OF A BODY
1.5. FORCE
NOTES
Basic Hypotheses and Laws
Abstract
2.1. The continuity hypothesis
2.2. Integral parameters and their densities
2.2.1. Parts of a Body
2.2.2. Integral Parameters of Continuum
2.2.3. Integral Characteristics of the Spatial Domain
2.2.4. About Differences
Integral Parameter vs Local Parameter
2.3. Deformation: The Euler and Lagrangian coordinates
2.4. Conservation laws
2.4.1. Integral Conservation Laws
2.4.2. Differential Conservation Laws
2.4.3. Transfer Theorem
2.4.4. Differential Conservation Laws (Continuation)
NOTES
Rates of Change of Characteristics of Continuum
Abstract
3.1. The rate of change of location: Trajectories of motion
3.2. The Rate of Change of a Scalar Function: Index Summation Convention
3.3. The rate of change of a vector function
NOTES
Minimum Information About Tensors
Abstract
4.1. TENSORS AND TENSOR OPERATIONS
4.1.1. Introduction
4.1.2. Tensor of Rank 2 and its Components
4.1.3. Algebraic Tensor Operations
4.1.4. Differential Tensor Operations
4.2. SOME SPECIAL TENSORS
4.3. EIGENVALUE PROBLEM
NOTES
Deformation
Abstract
5.1. Stretching and rotation
5.1.1. Polar Decomposition Theorem
5.1.2. Rotation Tensor
5.1.3. Stretch Tensor
5.2. Kinematics of deformation
NOTES
The Continuity Equation
Abstract
6.1. The rate of volume expansion
6.2. Differential conservation laws and balance equations
6.3. The continuity equation
NOTES
Fluid Dynamics
Abstract
7.1. Momentum of a body and the rate of its change. The basic principle of dynamics
7.2. Body forces and contact forces
7.3. The equation of motion
7.4. The equation of motion of the perfect fluid
7.5. The Euler equation in component form
7.6. Summary
NOTES
Energy
Abstract
8.1. Kinetic energy and its balance
8.2. The internal energy and its balance
Postulate
8.3. Summary
8.4. The equation of state
8.5. Model of the fluid: Discussion of the results
NOTES
Part II Applications of the fluid model
Perfect Fluid
Abstract
9.1. Introduction
9.1.1. Problem Posing in the Perfect Fluid Mechanics
9.1.2. The Equation of Motion in the Lamb Form
9.1.3. Remarks on Applications of the Model
9.2. Hydrostatics
9.3. Barotropic model
9.3.1. Stationary Flow; the Bernoulli Equation
9.3.2. Trajectories and Streamlines
9.3.3. Nonstationary Flow; the Vorticity Equation
NOTES
Incompressible Perfect Fluid
Abstract
10.1. Barotropic model
10.1.1. The Helmholtz Equation
10.1.2. The Lagrange and Helmholtz Theorems
10.2. Two-dimensional flow
10.2.1. Stream Function
10.2.2. Streamlines of Stationary Flow
10.2.3. Fluid Flow Through a Contour
10.3. The potential flow
10.4. Relationship between velocity potential and stream function
NOTES
Viscous Fluid
Abstract
11.1. Peculiarities of the perfect fluid model
11.2. The equation of motion of the viscous fluid
11.3. The equation of motion of the viscous fluid in component form
11.4. Problem formulation in fluid mechanics of the viscous fluid
11.5. Viscous dissipation and the energy balance
NOTES
Related Topics
Abstract
12.1. The heat equation
12.2. Free convection
12.3. What fluid is viscous?
12.3.1. Equations in the Non-dimensional Form
12.3.2. The Dynamic Similarity
12.4. Non-dimensional form of the heat equation
NOTES
Turbulent Fluid
Abstract
13.1. The hydrodynamic instability
13.2. The developed turbulence
13.3. The averaging problem
13.4. The Reynolds equation
13.5. The energy balance
NOTES
Boundary Layers
Abstract
14.1. Th laminar boundary layer
14.1.1. The Thickness of the Boundary Layer
14.1.2. Boundary Layer Equations
14.1.3. Separation of the Boundary Layer
14.2. Thermal boundary layer
14.3. The turbulent boundary layer
14.3.1. Introduction
14.3.2. General View of a Mean Velocity Profile
14.3.3. Flow Near a Smooth Wall
14.3.4. Influence of Roughness. The Roughness Parameter
NOTES
Part III Supplement
Fluid Mechanics from an Observer’s Viewpoint
Abstract
15.1. Introduction
15.2. Causal Fluid Model
15.2.1. General Considerations
15.2.2. Basic Notions
15.2.3. Conservation Laws
Integral Conservation Laws
Differential Conservation Laws
15.2.4. Thermodynamics and Total Energy Conservation Law
15.2.5. The Equations of Momentum and Internal Energy Balance
15.2.6. Definition of the Stress Tensor
15.3. Standard fluid model
15.3.1. Measures and Mass Conservation Law
15.3.2. Metric Tensor and the Kinetic Energy Conservation Law
15.3.3. Thermodynamics and the Total Energy Conservation Law
15.3.4. The Momentum and Internal Energy Balance Equations
15.3.5. Definition of the Stress Tensor
15.4. Comparison of the standard and causal fluid models
15.4.1. Standard Model as a Limit Case for the Causal Model
15.4.2. Basic Definitions, Axioms and Theorems
15.4.3. Some Parallels Between Basic Notions of the Fluid Models
15.5. Concluding remarks
NOTES
Exercises
16.1. Vector Fields, Trajectories and World Lines
16.2. Properties of the 2nd rank tensors
16.3. Working with components and the summation rule
16.4. Hydrostatics and the perfect fluid
16.5. Viscous fluid
16.6. The heat equation
16.7. Turbulent fluid
NOTES
List of Notations
Latin letters
Greek letters
Mathematical symbols
Text Books for Further Reading
References

Classical Fluid Mechanics

Authored by

Michael Belevich

St.Petersburg
Russia

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FOREWORD

Writing a new fluid dynamics textbook is a challenging task. In 1895, Sir Horace Lamb established a very high standard with the first edition of Hydrodynamics. This classical presentation was followed by other excellent introductions into the field of fluid mechanics, among them Landau and Lifshitz, 1959, and Batchelor, 1967. The strength of M.Belevich’s book is in its rigorous and systematic approach to developing the mathematical model of fluid dynamics from the first principles. It carefully explains the underlying hypothesis and simplifications used to establish equations that govern motions of a fluid. Extensive use of vector and tensor analysis results in a compact and generalized narrative, without the restrictions of a particular coordinate system.

This textbook is by no means a comprehensive description of the field of fluid dynamics. Some of important problems (e.g. waves) were deliberately left out of the book’s framework. Since the text is based on a course that is taught to students who specialize in geophysical fluid dynamics, more engineering aspects of fluid mechanics (such as turbomachines and airfoils) are also not covered.

The book’s content not only provides a general description of fluid dynamics, but also teaches how to apply universal principles to build a mathematical model of a particular problem. The distinctive feature of M. Belevich’s book is a somewhat non-standard approach of describing the dynamics of fluid from the point of view of the observer (chapter 15). It allows to underline some physical aspects of fluid mechanics which are usually not explicitly established in most textbooks.

The book is complemented by a carefully selected set of exercises. It provides consistent and self-sustained introduction to fluid dynamics, giving enough details to be used either in class or for self-study. It can be used to acquire knowledge in particular aspects of hydromechanics, and also as a source of inspiration for students, researchers and teachers in the field of classical fluid mechanics.

Ilya Rivin Environmental Modeling Center National Weather Service National Oceanic and Atmospheric Administration USA

PREFACE

This book presents the basis of the classical fluid mechanics and its content corresponds to a one-semester course which I am teaching from past several years to the 2nd year students of the Russian State Hydrometeorological University in St. Petersburg.

The goal of this book is twofold. Firstly, I wanted to provide a reader with a holistic idea of the fluid model and the way it is constructed. To show him, how the model of the fluid is developed, what main hypotheses lie in its basis and what general conclusions based on observations (the so-called laws of nature) make up the model. Secondly, I wished to demonstrate some possible modifications of the initial model which either make the model applicable in some special cases (viscous or turbulent fluid) or simplify it in accordance with peculiarity of a particular problem (hydrostatics, two-dimensional flows, boundary layers, etc.).

The whole theoretical material of the book naturally falls into two parts. The first part is fully dedicated to development of the model of the fluid in the Cauchy form. Here, the basic notions are introduced, main hypotheses are discussed and necessary postulates, which actually make up the model of continuum, are formulated. Non-coordinate tensor form of equations is actively used. This shortens formulas and makes results more readable. With that end in view, a brief introduction in tensor analysis is given in Ch.4. This part results in derivation of the perfect fluid model which turns out to be the simplest although quite efficient model.

In the second part of the book the most important modifications of the developed model are considered. First of all this concerns the redefinition of the stress tensor which is needed when viscosity is taken into account. Another important modification is connected with averaging of equations of the model which is necessary in case of turbulent flows. The concept of the boundary layer is also rather fruitful. Both laminar and turbulent boundary layers are discussed in Ch.14.

It is clear, that all this does not exhaust theoretical fluid mechanics, and that in the study of many important problems, it is necessary to refer to other books, at times rather special. However the basis of all such particular cases of the fluid mechanics is the same, and this book is aimed to discuss this topic.

Exercises and problems which are solved by students in practical classes are integral part of this book. They are chosen so as to teach students to work with complex systems of differential equations, since different fluid models are just such. We are training skills in writing equations in vector-matrix form, transition to component form of notation, applying of the index summation convention. Special attention is paid to formalizing of a verbal description of a problem (choice of coordinate systems, their orientation, accounting directions and symmetries inherent in the problem, etc.) as well as the mathematical problem posing. The system of fluid mechanics equations is quite complex and does not have analytic solutions in most interesting cases. Therefore, the main goal of these exercises is to elaborate the ability to see a particular problem from different viewpoints and to estimate its possible simplifications.

Theoretical fluid mechanics is very mathematized discipline, so the reader must meet certain requirements. Knowledge of the following topics of algebra and calculus is assumed: determinants, matrices, eigenvalue problem, vector spaces, calculus, vector analysis, differential equations.

All required information about tensors is given in Ch.4.

Conflict of interest

The author confirms that author has no conflict of interest to declare for this publication.

Acknowledgements

Besides my explicit and implicit teachers, I would like to especially thank those of my friends and colleagues, who patiently and sometimes willingly discussed with me various aspects of this course. These are primarily Dr. S.A.Fokin and A.A.Tron’. Their remarks, comments and suggestions were very helpful.

M.Belevich St.Petersburg Russia

Part I

Model of continuum

A scientific law is a statement … possessing such attributes: 1) it is true only under certain conditions; 2) under these conditions, it is true always and everywhere without any exceptions…; 3) conditions under which this statement is true, are never realized in fact fully, but only partially and approximately. Therefore, it’s impossible to say literally that scientific laws are found in the study of reality (are discovered). They are devised (are invented) based on the study of experimental data in such a way that they then may be used to obtain new judgments of given judgments on the reality (including, for prediction purely logical way). Scientific laws themselves can not be verified and can not be refuted by experience. They can be justified or not, depending on how well or poorly they perform the above-mentioned role.

A. Zinoviev Yawning Heights

Bodies and Their Characteristics

Michael Belevich
St.Petersburg, Russia

Abstract

This introductory chapter tries to explain what we are going to do, what do notions such as fluid and a model of a physical phenomenon mean, what for, such models are developed, and what features of a phenomenon a model should be necessarily able to describe and so on.

Keywords: Body, Body configuration, Coordinate basis, Event, Fluid, Force, Frame of reference, Mass, Model, Motion, Place, Space-time continuum, System of coordinates, Trajectory, World-line.