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Electromagnetic Field Theory and Transmission Lines G. S. N. Raju

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Electromagnetic Field Theory and Transmission Lines

Electromagnetic Field Theory and Transmission Lines

G.S.N. Raju

M.E., Ph.D (IIT-KGP), FIE, FIETE

Department of Electronics and Communications Engineering College of Engineering, Andhra University Visakhapatnam, India

To my brother, Prof. Krishnam Raju [MSc (Math.Physics), PhD], a man of academic excellence with impeccable character, and a great administrator who has made me what I am today.

Copyright © 2006 Dorling Kindersley (India) Pvt. Ltd

Licensees of Pearson Education in South Asia

No part of this eBook may be used or reproduced in any manner whatsoever without the publisher’s prior written consent.

This eBook may or may not include all assets that were part of the print version. The publisher reserves the right to remove any material present in this eBook at any time.

ISBN 9788131701713

eISBN 9788131799932

Head Office: A-8(A), Sector 62, Knowledge Boulevard, 7th Floor, NOIDA 201 309, India

Registered Office: 11 Local Shopping Centre, Panchsheel Park, New Delhi 110 017, India

PREFACE

Electromagnetic Field Theory and Transmission Lines is a core subject for all the students of BE/BTech in Electronics and Communication Engineering, Electronics Engineering, Electrical Engineering, Electronic Instrumentation Engineering, MSc (Electronics), MSc (Applied Physics), AMIETE, AMIE, and other courses throughout the world. EMF theory is essential for the design and analysis of all communication and radar systems. Moreover, it has numerous applications in all fields of life. It is a universal theory and has many advantages over the circuit theory which has limited applications. It is also useful in biomedical engineering in connection with radiation therapy. It is extremely useful to interpret electromagnetic interference in the systems for compatibility studies. The behaviour of electromagnetic waves between the transmitter and receiver can be understood only with the concepts of the electromagnetic field (EMF) theory.

I have been teaching this important subject for several years, referring to books written by several experts like Kraus, Jordan, Hayt, Kreyszig and Narayana Rao. However, the general belief is that no single book available caters to the needs of a complete course required for undergraduate and post graduate programmes. In view of this, an attempt is being made to bring out a simplified book on the subject of Electromagnetic Field Theory and Transmission Lines.

I hope that this book will be extremely useful for students, teachers, professionals, engineers, technicians, designers and also for short-term course organisers.

Any suggestions to improve the book will be welcome.

ACKNOWLEDGEMENT

I am grateful to my gurus, Prof. B.N. Das and Prof. Ajoy Chakraborty of IIT Kharagpur, who taught me fundamentals of Applied Electromagnetics.

I thank all my colleagues, Prof. Madhusudhan Rao, Prof. Venkata Rao, Prof. Veena Kumari, Dr. Hari Babu, Prof. Raja Rajeswari, Prof. Satyanarayana Reddy, Dr. Mallikarjuna Rao, Mrs. Santa Kumari, Dr. Gopala Rao, Mr. Sampath Kumar and Dr. Panduranga Reddy for their cooperation throughout.

It is a privilege to convey my gratitude with warm regards and respects to SriK.Raghu, Chairman, Raghu Engineering College, and Sri S.V.S.S. Rama Chandra Raju, former PF Commissioner and Director, Raghu Engineering College, for their kind appreciation of my efforts in teaching and research and for giving me unmatched support in all my academic endeavors. I also thank Sri N.V. Rama Raju for extending support in my academic and professional efforts.

I am most grateful to Prof. K.C. Reddy, a renowned economist and Chairman, Council for Higher Education, Government of Andhra Pradesh for releasing the International edition of the book on Antennas and Wave Propagation and for his kind appreciation of the book.

I convey my gratitude to Prof. Y.C. Simhadri, Hon’ble Vice-Chancellor of Andhra University for his full support with encouragement and also for sending an excellent message of appreciation for Antennas and Wave Propagation

I am thankful to Prof. D. Ganapathi Rao, who is kind enough to release the Indian edition of the book.

It is a privilege to thank Radm. S. Mohapatra, former Director, Dr. K. Satyanarayana, Director, Dr. V. Bhujanga Rao, Associate Director, Sri B. Vara Prasada Rao, Deputy Director and Senior Scientist, Cdr. T.K. Guha Roy, NSTL for their keen interest and moral support to my work in electromagnetics.

I am grateful to Prof. P.S. Rao, Principal, and Prof. P. Soma Raju, Secretary and Correspondent, GVP College of Engineering for their kind appreciation of Antennas and Wave Propagation

I cherish the association of all my research scholars Mallikarjuna Rao, Sridevi, Gopala Rao, Misra, Sudhakar, Baba, Padma Raju, Chandra Bhushana Rao, Prasad,

Habibullah Khan, Subrahmanyam, Narayana, Sadasiva Rao, Gutti, Mallikarjuna Prasad, K.V.S.N. Raju, Murali Krishna, Rajesh and Swamy in putting their efforts for their Ph.D. degrees. I thank my friends, Prof. Appa Rao, Prof. K.V.L.P. Raju, Prof. Paramahamsa and Gopala Krishnam Raju for the moral support given to me throughout.

I thank Prof. Sarvarayudu, Prof. Raghuram, Prof. Prabhakara Rao, Prof. P.V.D.S. Rao of JNTU and Prof. Subbaiah of Nagarjuna University for their keen interest and appreciation for the book.

I thank Mr. Narayana, a sincere and hardworking scholar for assisting in proof reading with interest and devotion.

I love all my students who are always fond of my teaching, guidance and discipline.

I extend my regards to all senior authors and experts in Electromagnetic Field Theory for their invaluable contributions.

I am extremely grateful to the Department of Electronics and Communication Engineering, College of Engineering, Andhra University, for the encouragement given through out my teaching and research career.

I am grateful to the reviewers of this book for their excellent positive feedback.

I thank the most intelligent and Pro-poor Doctor Dr. G. Prasad, M.D., D.M., for his support and happiness given to me during preparation of the book. I also thank Dr. B. Dharani Priya for her appreciation of the book.

I express my thanks for the support extended by our technical and office staff, Koteswara Rao, Somayajulu, Sahu, Prasada Reddy, Appala Raju, Srinivas, Babji, Ramesh, Adilakshmi, Nara Hari, Ramana, Tavudu and Kondamma. The assistance given by Sankar is acknowledged with thanks for preparing the manuscript.

I take this opportunity to convey my respects to my parents Venkatrama Raju and Sitama and thanks to my wife Kanaka Durga, daughter Narmada Devi (B.Tech-CSE) and son Venkata Krishna Varma (B.Tech) IIT-Delhi for their love, affection, help and patience throughout the preparation of the book.

Finally, I thank all those who helped me directly and indirectly in bringing out this book.

2.14Potential

2.40Properties

2.47Properties

2.48Dipole

2.50Capacitance

3.3Fundamentals

3.9Ampere’s

3.10Differential

3.17Scalar

3.23Standard

3.24Energy

3.25Energy

3.26Expression

4.10Proof

4.19Boundary

4.20Time

4.21Retarded

4.22Maxwell’s

4.23Helmholtz

5.4Wave

5.13Summary

5.16Summary

5.17Wave

5.22Direction

5.23Wave

5.24Waves

6.12Waves

6.13Derivation

6.14Propagation

6.15TEM

6.16Excitation

6.17Evanescent

6.18Wave

7.19Smith

INTRODUCTION

This introduction provides

c a list of some applications of EMF theory

c a comparison between EMF and Circuit theories: the reasons why EMF theory is superior and why it is essential for engineers and scientists

c small and large value representation, frequency ranges of TV channels and so on for general information

c information about the notations used in this book

c comprehensive background of the parameters, symbols, units and meanings

2 ELECTROMAGNETIC FIELD THEORY AND TRANSMISSION LINES

Electromagnetic Field (EMF) Theory is often called Electromagnetics. It is a subject which deals with electric field, magnetic field and also electromagnetic fields and phenomena.

EMF Theory is essential to design and analyse all communication and radar systems. In fact, it is also used in Bio-systems and in this context it is called Bioelectromagnetics.

Electromagnetic Field Theory is used in

1.Wireless communications

2.Satellite communications

3.TV communications

4.Cellular communications

5.Radio broadcast

6.Mobile communications

7.Microwave communications

8.All types of antenna analysis and design

9.All types of transmission lines and waveguides

10.Bio-medical systems

11.Electrical machines

12.Speed-trap radars

13.Weather forecast radars

14.Remote sensing radars

15.Radio astronomy radars

16.Ground mapping radars

17.Meteorological radars

18.Plasmas

19.Electromagnetic interference and compatibility

20.Electromechanical energy conversion systems

21.Electric motors

22.Cyclotrons

23.Nuclear research

24.Radiation therapy

25.Heating deep tissues

26.Stimulating Bio-physiological responses

27.Relieving some pathological conditions

28.Induction heating

29.Melting

30.Forging

31.Surface hardening

32.Annealing

33.Soldering

34.Dielectric heating

35.Joining plastic sheets

36.Sealing plastic sheets

37.Agriculture

38.Reducing acidity in vegetables to improve taste

39.Telephones

40.Fibre optic communications

41.Lasers

42.Masers

43.Electric relays

44.Transformers

45.Microwave ovens

The design and analysis of a system, device or circuit requires the use of some theory or the other. The analysis of a system is universally defined as one by which the output is obtained from the given input and system details. On the other hand, the design of a system is one by which the system details are obtained, from the given input and output. These two important tasks are executed by two most popular theories, namely, circuit and electromagnetic theories. The differences between them are listed on next page.

Circuit theory

Field theory

1.Deals with voltage (V) and Deals with Electric ( E ) and Magnetic current (I) (H) fields

2.V and I are scalars E and H are vectors

3.V and I are produced from E and E and H are produced from V and I H respectively respectively

4.V and I are functions of time (t) E and H are functions time ( t) and space variables (x, y, z) or (ρ, φ, z) or (r, θ, φ)

5.Radiation effects are neglectedRadiation effects can be considered

6.Using circuit theory, transmitterUsing field theory, the medium also can and receiver circuits can bebe designed and analysed analysed and designed. But it cannot be used to design or analyse a medium like free space

7.This is simplified approximationThis is a more accurate theory of field theory

8.The variables of circuit theory, V The variables of field theory, E and H and I are integrated effects ofare integrated effects of variables of variables of field theory E and H circuit theory V and I

9.Circuit theory cannot be Field theory can be used where circuit used to analyse or design atheory fails to hold good for the analysis complete communication systemand design of a communication system

10.Is useful at low frequenciesIs useful at all frequencies, particularly at high frequencies

11.At low frequencies the length ofAt high frequencies the length of connecting wires is very muchconnecting components are of the order smaller than λ of λ

12.Cannot be applied in free spaceIs applicable in free space

13.Is simple Is complex but it is simplified by using appropriate mathematics

14.Basic laws are Ohms law,Basic laws are Coulomb’s law, Gauss’s Kirchoff’s laws law, Ampere’s circuit law

15.Basic theorems are Thevenin’s, Basic theorems are Reciprocity, Nortan’s, Reciprocity, Helmholtz, Stoke’s, Divergence and Superposition, Maximum powerPoynting theorems transfer theorems

16.Basic equations are Mesh/LoopBasic equations are Maxwell, Poission, equations Laplace and Wave

ParameterNotationDefinition

Unit name /symbol

Frequency fIt is the reciprocal of oneHertz (Hz) time period of a periodic1 Hz = 1 cycle/sec waveform

Energy

Power

Charge

WIt is the work done whenJoule (J) force is exerted through a1 Joule = 107 ergs distance of one metre

PIt is the time rate of Watt (W) energy

1 W = 1 Joule/sec or 1 W = 1 volt × 1 amp

QIt is the product of Coulomb (C) current and time 1 C = 1 A-sec

Resistance RIt is the ratio of voltageOhm ( Ω) and current 1 Ω = 1 volt/1 amp

ConductanceGIt is the reciprocal of R Mho 1 Mho = oltV1 Amp1

Resistivity

ρ It is the resistance meas-Ohm-metre ured between two parallel faces of a unit cube

Conductivity σ It is the reciprocal of Mho/metre resistivity

ElectromotiveEmf, VIt is the ratio of power to Volt force current 1 Volt = 1 J/C or watt/amp

Electric flux

ψ It is displaced charge Coulomb (C)

weber (wb) 1 wb = 1 volt-sec

Magnetomotive

CapacitanceC

Farads (F) 1 F = 1 C/1 Volt

ParameterNotationDefinition

InductanceL

Permittivity

Permeability

Permittivity

Permeability

Relative

Farad/metre (F/m)

DifferentialdLSmall

Area SProduct of two lengths m

DifferentialdSProduct of two m 2 area differential lengths

ParameterNotationDefinition

/symbol

Differentiald υ Product of differential m 3 volume length, width and breadth

Volume υ Product of length, width m 3 and breadth

Angular ω 2 πf rad/sec frequency

Wavelength λ v/f m Electric V

potential

Magnetic V m

dLH . Ampere scalar potential

Surface charge ρs Q/S c/m2 density

Line charge ρ L Q/L c/m density

Volume ρυ Q/ υ c/m3 charge density

Propagation γα + jβ dB/m constant

Attenuation α It is a measure of dB/m constant reduction of EM wave as it progresses

Depth of δ It is the depth at which δ = 1/ α (m) penetration an EM wave is attenuated or skin depth to 37 percent of original value

Phase constant β It is a measure of phase rad/m shift of EM wave

Group velocityv g It is the velocity with m/sec which energy propagates in a guided structure

Phase velocityvp It defines a point of m/sec constant phase

VSWR SV max /V min No unit

ParameterNotationDefinition

/symbol

Reflection

coefficient

= wave Incident wave Reflected

Transmission T wave Incident Transmittewaved No unit coefficient

ParameterNotationDefinition Unit name /symbol

Force F It is the product of massNewton (N) and acceleration 1 Newton 2 sec Kgm- =

Electric field E It is the force per oneVolt/m or Newton/C strength Coulomb

Conduction Jc It is defined as the ratio A/m2 current density of current to area

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