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Home , Electromagnetism

Basic AND ITS APPLICATIONS Series Editors E.R. Dobbs S.B. Palmer Warwick University

This series of short texts on advanced topics for students, scientists and will appeal to readers seeking to broaden their knowledge of the physics underlying modern . Each text provides a concise review of the fundamental physics and current developments in the area, with references to and the primary literature to facilitate further study, Additionally texts providing a core course in physics are included to form a ready reference collection. The rapid pace of technological change today is based on the most recent scientific advances. This series is, therefore, particularly suitable for those engaged in research and development, who frequently require a rapid summary of another topic in physics or a new application of physical principles in their work. Many of the texts will also be suitable for final year undergraduate and postgraduate courses.

1. in Metals and Semiconductors R.G. Chambers 2. Basic Digital l.A. Strong 3. AC and DC Network Theory Anthony l. Painton and Harry M. Howarth 4. Nuclear and R.J. Blin-Stoyle 5. Thermal Physics Second edition C.B.P. Finn 6. Physics and Techniques T.A. Delchar 7. Basic Electromagnetism E.R. Dobbs Basic Electromagnetism

E. R. Dobbs Emeritus Professor of Physics Universityof London

Springer-+Business Media, B.V. First edition 1993

© 1993 E.R. Dobbs Originally published by Chapman and HalI in 1993

Typeset in 10/12 Times by Thomson Press (India) Ltd, New Delhi

ISBN 978-0-412-55570-1 ISBN 978-94-011-2112-5 (eBook) DOI 10.1007/978-94-011-2112-5

Apart from any fair dealing for the purposes or research or private study, or criticism or review, as permitted under the UK Copyright Designs and Patents Act, 1988, this publication may not be reproduced, stored, Of transmitted, in any form or by any means, without the prior permission in writing of tl1$: publishers, or in the case of reprographic reproduction only in accordance with the terms of the licences issued by the Copyright Licensing Agency in the UK, or in accordance with the terms of licences issued by the appropriate Reproduction Rights Organization outside the UK. Enquiries concerning reproduction outside the terms stated here should be sent to the publishers at the London address printed on this page. The publisher makes no representation, express or implied, with regard to the accuracy of the information contained in this book and cannot accept any legal responsibility or liability for any errors or omissions that may be made.

A Catalogue record for this book is available from the British Library

Library of Congress Cataloging-in-Publication data

Dobbs, Roland, 1924- Basic electromagnetism / E. R. Dobbs.-lst ed. p. cm. -(Physics and its applications ; 7) Inc1udes index.

1. Electromagnetism. 1. Title. II. Series. QC760.D62 1993 93-7067 537-dc20 CIP

I§ Printed on permanent acid-free text paper, manufactured in accordance with the proposed ANSIjNISO Z 39.48-199X and ANSI Z 39.48-1984 Contents

Preface ix

List of symbols xiii 1 Introduction 1 2 4 2.1 's law 4 2.2 Gauss's law 8 2.3 14 2.4 Electrostatic 19 2.5 22 3 Electric potential and fields 30 3.1 Poisson's and Laplace's 30 3.2 Solutions of Laplace's 33 3.3 Electrical images 36 3.4 41 4 47 4.1 47 4.2 Lorentz 51 4.3 Biot-Savart law 57 4.4 between currents 60 4.5 's law and 61

5 Electromagnetism 66 5.1 Faraday's law 66 5.2 Applications of Faraday's law 72 vi Contents

6 79 6.1 of 79 6.2 Characteristics of Band H 84 6.3 Magnetism in matter 87 6.4 Production of magnetic fields 96 7 's equations 102 7.1 Gauss's and Faraday's laws 102 7.2 Ampere's and Maxwell's laws 103 7.3 and 105 7.4 Free space and matter 106 8 Electromagnetism and relativity 113 8.1 Lorentz transformations 113 8.2 Fields of moving charges 116 8.3 Vector potentials 123 8.4 Energy of electromagnetic 129 8.5 Retarded potentials 132 9 Electromagnetic waves in space 135 9.1 Wave equations 135 9.2 Plane waves 137 9.3 Spherical waves 141 9.4 Energy density and energy flow 143 10 Electromagnetic waves in dielectrics 147 10.1 Polarization of dielectrics 147 10.2 Wave parameters in dielectrics 151 10.3 Absorption and dispersion 154 11 Reflection and refraction 160 11.1 Boundary relations 160 11.2 Fresnel's equations 164 11.3 Energy flow at a boundary 168 11.4 Total internal reflection 171 12 Electromagnetic waves in conductors 173 12.1 Wave parameters in conductors 174 12.2 Wave impedance and reflectance 177 12.3 Energy flow and pressure 178 12.4 Plasmas 180 13 Generation of electromagnetic waves 183 13.1 Hertzian 183 13.2 Radiant energy and power 187 Contents vii

13.3 Antennas 189 13.4 193 14 Guided waves 196 14.1 Waveguide equation 196 14.2 Rectangular waveguides 198 14.3 Waveguide modes 202 14.4 Cavities 205 Further reading 210 Appendix A Electromagnetic quantities 211 Appendix B 214 Appendix C Physical constants 216 Appendix D Electromagnetic spectrum 217 Appendix E Vector 218 Appendix F Lorentz transformations 221 Appendix G Exercises 223 Appendix H Answers to exercises 236 Index 239 Preface

Electricity and magnetism are basic to our understanding of the properties of matter and yet are often regarded as the difficult parts of an undergraduate course in physics, or engin• eering. In the first six chapters of this book answers are developed from first principles to such questions as: What is ? What is electromagnetism? Why are some materials magnetic and others non-magnetic? What is magnetism? These questions can be answered in two related ways. On the one hand the classical explanation is in terms of classical concepts: electric (q), electric and magnetic fields (E and B) and electric currents. On the other hand the microscopic (or 'atomic') explanation is in terms of concepts: electrons, nuclei, electron orbits in , electron and . Microscopic explanations underlie classical ones, but they do not deny them. The great triumphs of classical theory are , gravitation, , electro• magnetism and relativity. Historically the classical theories began at the time of Newton (seventeenth century) and were completed by Maxwell (nineteenth century) and by Einstein (early twentieth century). Microscopic explanations began with 1.1. Thomson's discovery of the electron in 1897. For most physical phenomena it is best to seek a classical explanation first, especially for phenomena at room temperature, or low energy, when quantum effects are small. This book presents classical theory in a logical, self-consistent sequence, but reference is made to microscopic (quantum) theory at each appropriate stage. Electromagnetism began in 1819 with the discovery by that an electric current is associated with a and was followed in 1820 by Ampere's discovery that two wires carrying Preface

electric currents exerted magnetic forces on one another. But it was Faraday's discovery of electromagnetic induction in 1831, or as he put it, the conversion of magnetism into electricity, that finally showed that electricity and magnetism were not distinct, separate phenomena, but interacted when there were time-varying electric or magnetic fields. The beauty of electromagnetism is that Faraday's experiments led to a symmary of the whole of electromagnetism in just the four equations of Maxwell's theory, which relate E and B in space with fixed and moving charges, together with the electromagnetic force law. These equations are greatly simplified when we deal with statics, that is, variables that do not depend on time t, or stationary variables. Maxwell's equations then simplify and separate into two independent pairs of equations: 1. The first pair describe the electrostatic field E for fixed charges and are known as Gauss's law and the law. They summarize electrostatics. 2. The second pair describe the magnetostatic field B for steady currents (charges moving at constant speed) and are known as Gauss's law and Ampere's law. They summarize magnetostatics. In electrostatics only the E field appears and iJE/iJt = 0; in statics only the Bfield appears and fJB/fJt = O. So under these conditions, electricity and magnetism are classically distinct, separate phenomena. But if you charge a capacitor (q varying with time) or move a (B at a point varying in time) then E and B are no longer independent and new terms in the equations due to electromagnetism appear, as first discovered by Faraday (Faraday's law) and Maxwell (Maxwell's law). The development of the subject in this text is therefore first electro• statics, then magnetostatics, followed by electromagnetism and magnetism. The seventh chapter summarizes electromagnetism in terms of Maxwell's equations, which are then used to study the propagation and generation of electromagnetic waves. The first seven chapters often comprise a first course in electromagnetism for undergraduates. In studying the solutions of Maxwell's equations you will find answers to such questions as: What is an electromagnetic wave? Why does a travel through space at the speed of ? How is a radio wave generated? Why does light pass through a straight tunnel when a radio wave does not? How does· light travel down a curved glass fibre? Preface xi

Before studying these solutions, Chapter 8 discusses the remarkable fact that the classical laws of electromagnetism are fully consistent with Einstein's special . The following four chapters provide solutions of Maxwell's equations for the propagation of electromagnetic waves in free space, in dielectrics, across interfaces and in conductors, respectively. In Chapter 13 the generation of radio waves from and of from other antennas is explained, while the final chapter shows how these waves can be transmitted down waveguides and coaxial lines. In conclusion, the use of resonant and re-entrant cavities leads to a discussion of the classical theory of radiation and its usefulness as a limiting case of the quantum theory of radiation. The spectrum of electromagnetic waves covers an enormous range of , from the very low frequencies (VLF), used to communicate with submerged submarines, to the enormous frequencies (10 24 ) associated with some cosmic rays from . The complete spectrum is illustrated in Appendix 0, where it is characterized by both the classical, wave properties of (v) and wavelength (A.) and the quantized, properties of energy

(hv) and temperature (hv/k B ). Classical electromagnetism provides a theory of the wave properties of radiation over a wide frequency range, including, for example, the diffraction of X-rays by crystals, but for the interactions of radiation with matter classical theory only applies in the long wavelength, low frequency, low energy (hv« kB T) limit. The generation of electromagnetic radiation is similarly the classical process of acceleration of electrons in producing a radio wave, where the wavelength is macroscopic, but quantum processes are involved in the production of X-rays by electronic transitions in atoms, or rays by nucleonic transitions in nuclei, where the wavelength are microscopic. The production of light by laser is an interesting example of the combination of the classical process of reflection with the quantum process of stimulated emission. In this book the limits of classical electromagnetism are explained and the usefulness of the wave and particle properties of radiation are discussed, so that the reader is provided with an understanding of the applicability and limitations of classical theory. The international system of units (SI units) are used throughout and are listed for each electromagnetic quantity in Appendix A. Since Gaussian units are still used in some research papers on electro• magnetism, Appendix B lists Maxwell's equations in these units and states the conversion from the Gaussian to the SI system. The Xll Preface physical constants used in the text are listed in Appendix C with their approximate values and units. In Appendices E and F there are summaries of the most useful relations in vector calculus and . Finally, each chapter, except Chapters 1 and 7, has a set of associated exercises in Appendix G with answers in Appendix H.

ACKNOWLEDGEMENTS This book owes much to the many undergraduates who have participated in my tutorials and lectures on electromagnetism at the Universities of Cambridge, Lancaster and London for more than twenty years. Of the numerous texts I have consulted, none has been so illuminating as Volume 2 of the Feynman Lectures on Physics by R.P. Feynman, R.B. Leighton and M. Sands (Addison-Wesley, London, 1964). This new, revised edition is a combination of my Electricity and Magnetism (Routledge & Kegan Paul, London, 1984) and my Electromagnetic Waves (Routledge & Kegan Paul, London, 1985). It is a pleasure to thank colleagues in the Universities of London and Sussex for their helpful comments, especially Professor E.l. Burge for a number of improvements to Electricity and Magnetism, after he had used it for a first course to undergraduates in Physics at Royal Hollaway, University of London. Thanks are due to the University of London for' permission to reproduce some problems (marked L) from BSc course unit examinations taken at the end of their first year by students reading Physics at Bedford College. It is a plesure to thank Mrs Sheila Pearson for her accurate and rapid typingofthe original manuscripts and my wife for her constant support and encouragement over many years. List of symbols

A Magnetic vector potential A Area B Magnetic field B C Closed loop; c D Electric displacement d Distance Iff E e Electronic charge

fFm F Force FE Electrical force Fa Gravitational force f Focal length G ; conductance H Magnetizing field Hm h 1 Electric current 1m Surface magnetizing current i Cartesian unit vector i Surface if Solenoidal surface current density im Magnetization surface current density j Cartesian unit vector j Electric current density xiv List of symbols jr Conduction current density jm Magnetization current density jp Polarization current density k Cartesian unit vector k Wave vector k Coupling coefficient; wave number kg Waveguide wave number kB Boltzmann constant kR' kr Real and imaginary parts of k = kR - ikr L Self I Length dl Electric current element M Magnetization M mutual inductance m Magnetic dipole moment m Mass N Number density; total number of turns n Unit normal vector n Number of turns per unit length; refractive index nR , nr Real and imaginary parts of n = nR - inr P Electric polarization P Total radiated power P n Legendre function P ; electron Po Permanent electric dipole moment Pr Radiation pressure Q Total ; quadrupole moment; quality factor q Electric charge ~ Reluctance R Electrical resistance; reflectance Ro Reflectance at normal incidence Rr Radiation resistance r Distance vector r Distance; cylindrical or spherical radius ro Classical electron radius f/ , electromagnetic energy flux S Surface area vector s Distance vector s Distance; contour T Torque vector T Temperature; transmittance List of symbols xv

Tc Curie temperature TF Fermi temperature t Time U Energy u Energy density; relative velocity V Volume; potential difference v Velocity vector VF Fermi velocity W Mechanical work x Cartesian coordinate y y Cartesian coordinate Z Wave impedance; atomic number Zo Wave impedance of free space z Cartesian coordinate IX Polarizability f3 Absorption coefficient y Electrical conductivity; damping constant () Loss angle; skin depth e Absolute eo Electric constant; permittivity of free space er Relative permittivity; constant

eR, eI Real and imaginary parts of e = eR - ieI es Static value of relative permittivity e"" High frequency limit of relative permittivity () Spherical polar coordinate {)c Critical angle (of incidence) A Electric charge per unit length; wavelength Ac Cut-off wavelength of waveguide Ag Waveguide wavelength of waveguide Ao Free space wavelength of radiation p of a particle JiB Bohr magneton Ji Absolute permeability Jio Magnetic constant; permeability of free space Jir Relative permeability v Frequency P Electric Pr Free charge density Pp Polarization charge density (]' Surface charge density XVI List of symbols

G'f Surface density of free charges G'p Surface density of polarization charges G' 0 Resonant scattering cross-section G'R Rayleigh scattering cross-section G'T Thomson scattering cross-section T Volume of integration; mean time between (/J Magnetic flux 4J Electric (scalar) potential; cylindrical polar coordinate; phase angle of a wave Xe Xm t/J Spherical polar coordinate; azimuthal angle; D General scalar function dD Element of solid angle OJ Angular velocity of frequency OJ e Cut-off (angular) frequency of waveguide

OJ L Larmor (angular) frequency OJo Resonant (angular) frequency

OJp (angular) frequency