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Discover an innovative and fresh approach to teaching classical electromagnetics at a foundational level
Introduction to Electromagnetic Waves with Maxwell's Equations delivers an accessible and practical approach to teaching the well-known topics all electromagnetics instructors must include in their syllabus. Based on the author's decades of experience teaching the subject, the book is carefully tuned to be relevant to an audience of engineering students who have already been exposed to the basic curricula of linear algebra and multivariate calculus.
Forming the backbone of the book, Maxwell's equations are developed step-by-step in consecutive chapters, while related electromagnetic phenomena are discussed simultaneously. The author presents accompanying mathematical tools alongside the material provided in the book to assist students with retention and comprehension. The book contains over 100 solved problems and examples with stepwise solutions offered alongside them. An accompanying website provides readers with additional problems and solutions.
Readers will also benefit from the inclusion of:
Perfect for third-and fourth-year undergraduate students in electrical engineering, mechanical engineering, applied maths, physics, and computer science, Introduction to Electromagnetic Waves with Maxwell's Equations will also earn a place in the libraries of graduate and postgraduate students in any STEM program with applications in electromagnetics.
Ozgur Ergul, PhD, is Professor at the Middle East Technical University in Ankara, Turkey. His research focus is on the development of fast and accurate algorithms for the solution of electromagnetics problems involving large and complicated structures, integral equations, iterative methods, parallel programming, and high-performance computing.
Preface 15
Mathematical Notation 23
List of Symbols 27
Special Functions 31
Frequently Used Identities 33
Tools to Understand Maxwell's Equations 37
0 Preliminary 39
0.1 Scalar and Vector Fields 40
0.2 Cartesian Coordinate Systems 42
0.3 Basic Vector Operations 42
0.4 Orthogonal Coordinate Systems 43
0.4.1 Properties of a Cartesian Coordinate System 43
0.4.2 Cylindrical Coordinate System 44
0.4.3 Spherical Coordinate System 45
0.5 Electrostatics, Magnetostatics, and Electromagnetics 47
0.6 Time in Electromagnetics 49
0.7 Final Remarks 51
1 Gauss' Law 53
1.1 Integral Form of Gauss' Law 54
1.1.1 Differential Surface With Direction 55
1.1.2 Dot Product 56
1.1.3 Flux of Vector Fields 62
1.1.4 Meaning of Gauss' Law and Its Application 66
1.1.5 Examples 67
1.2 Using the Integral Form of Gauss' Law 69
1.2.1 Examples 71
1.3 Differential Form of Gauss' Law 73
1.3.1 Electric Charge Density 73
1.3.2 Divergence of Vector Fields 75
1.3.3 Divergence Theorem and the Differential Form of Gauss' Law 81
1.3.4 Examples 83
1.4 Using the Differential Form of Gauss' Law 85
1.4.1 Examples 88
1.5 Boundary Conditions for Normal Electric Fields 89
1.6 Static Cases and Coulomb's Law 92
1.6.1 Superposition Principle 93
1.6.2 Coulomb's Law and Electric Force 99
1.6.3 Examples 101
1.7 Gauss' Law and Dielectrics 106
1.7.1 Electric Dipole 112
1.7.2 Polarization 113
1.7.3 Equivalent Polarization Charges 115
1.7.4 Examples 120
1.8 Final Remarks 123
1.9 Exercises 124
1.10 Questions 127
2 Ampere's Law 133
2.1 Integral Form of Ampere's Law 134
2.1.1 Differential Length With Direction 135
2.1.2 Circulation of Vector Fields 137
2.1.3 Meaning of Ampere's Law and Its Application 140
2.1.4 Examples 143
2.2 Using the Integral Form of Ampere's Law 145
2.2.1 Examples 147
2.3 Differential Form of Ampere's Law 151
2.3.1 Electric Current Density 152
2.3.2 Cross Product 154
2.3.3 Curl of Vector Fields 157
2.3.4 Stoke's Theorem and the Differential Form of Ampere's Law 164
2.3.5 Examples 165
2.4 Using the Differential Form of Ampere's Law 169
2.4.1 Examples 172
2.5 Boundary Conditions for Tangential Magnetic Fields 173
2.6 Gauss' Law and Ampere's Law 176
2.7 Static Cases, Biot-Savart Law, and Ampere's Force Law 179
2.7.1 Superposition Principle 180
2.7.2 Ampere's Force Law and Magnetic Force 190
2.7.3 Examples 194
2.8 Ampere's Law and Magnetic Materials 200
2.8.1 Magnetic Dipole 206
2.8.2 Magnetization 208
2.8.3 Equivalent Magnetization Currents 210
2.8.4 Examples 217
2.9 Final Remarks 218
2.10 Exercises 219
2.11 Questions 221
3 Faraday's Law 225
3.1 Integral Form of Faraday's Law 226
3.1.1 Meaning of Faraday's Law and Its Application 227
3.1.2 Lorentz Force Law 229
3.2 Using the Integral Form of Faraday's Law 231
3.2.1 Examples 236
3.3 Differential Form of Faraday's Law 240
3.4 Boundary Conditions for Tangential Electric Fields 242
3.5 Combining Faraday's Law with Gauss' and Ampere's Laws 244
3.6 Static Cases and Electric Scalar Potential 246
3.6.1 Gradient of Scalar Fields 248
3.6.2 Examples 252
3.6.3 Gradient Theorem 253
3.6.4 Gradient in Gauss' Law, Ampere's Law, and Faraday's Law 254
3.6.5 Electric Potential Energy 257
3.6.5.1 Electric Potential Energy of Discrete Charge Distributions 261
3.6.5.2 Stored Electric Potential Energy by an Electric Dipole 263
3.6.5.3 Stored Electric Potential Energy in Charge Distributions 265
3.6.5.4 Electric Potential Energy and Electric Force 269
3.6.6 Examples 272
3.6.7 Poisson's Equation and Laplace's Equation 276
3.6.8 Examples 283
3.6.9 Finding Electric Scalar Potential From Electric Field Intensity 283
3.6.10 Examples 286
3.6.11 Electrostatic Boundary Value Problems 288
3.6.12 Examples 291
3.7 Final Remarks 294
3.8 Exercises 294
3.9 Questions 296
4 Gauss' Law for Magnetic Fields 299
4.1 Integral and Differential Forms of Gauss' law for Magnetic Fields 300
4.1.1 Meaning of Gauss' law for Magnetic Fields 302
4.1.2 Examples 304
4.2 Boundary Conditions for Normal Magnetic Fields 306
4.2.1 Examples 307
4.3 Static Cases and Magnetic Vector Potential 308
4.3.1 Magnetic Vector Potential and Coulomb's Gauge 309
4.3.2 Examples 318
4.3.3 Magnetic Potential Energy 321
4.3.3.1 Magnetic Potential Energy of Discrete Current Distributions 323
4.3.3.2 Stored Magnetic Potential Energy by a Magnetic Dipole 324
4.3.3.3 Stored Magnetic Potential Energy in Current Distributions 326
4.3.3.4 Magnetic Potential Energy and Magnetic Force 329
4.3.4 Examples 332
4.4 Combining All Maxwell's Equations 334
4.4.1 Wave Equations 336
4.4.2 Wave Equations for Potentials 343
4.4.3 Time-Harmonic Sources and Helmholtz Equations 349
4.4.4 Examples 354
4.5 Final Remarks 359
4.6 Exercises 360
4.7 Questions 363
5 Basic Solutions of Maxwell's Equations 365
5.1 Summary of Maxwell's Equations, Wave Equations, and Helmholtz Equations 366
5.1.1 Examples 375
5.2 Electromagnetic Propagation and Radiation 377
5.2.1 Hertzian Dipole 382
5.2.2 Examples 385
5.3 Plane Waves 389
5.3.1 Examples 400
5.3.2 Polarization of Plane Waves 401
5.3.3 Examples 407
5.3.4 Power of Plane Waves 409
5.3.5 Reflection and Refraction of Plane Waves 412
5.3.6 General Case for Reflection and Refraction 416
5.3.6.1 Perpendicular Polarization 418
5.3.6.2 Parallel Polarization 421
5.3.7 Examples 423
5.3.8 Total Internal Reflection 427
5.3.9 Total Transmission 430
5.3.10 Examples 434
5.3.11 Reflection and Transmission for Two Parallel Interfaces 437
5.4 Final Remarks 440
5.5 Exercises 440
5.6 Questions 443
6 Analyses of Conducting Objects 447
6.1 Ohm's Law 449
6.2 Joule's Law 452
6.3 Relaxation Time 453
6.4 Boundary Conditions for Conducting Media 456
6.5 Analyses of Perfectly Conducting Objects 457
6.5.1 Electric Scalar Potential for PECs 458
6.5.2 Boundary Conditions for PECs 458
6.5.3 Basic Responses of PECs 460
6.5.4 Concerns in Geometric Representations of PECs 462
6.5.5 Electrostatics for PECs 464
6.5.6 Method of Images 466
6.5.7 Examples 470
6.6 Maxwell's Equations in Conducting Media 474
6.6.1 Complex Permittivity 476
6.6.2 Power and Energy in Conducting Media 478
6.6.3 Plane Waves in Conducting Media 479
6.6.4 Power of Plane Waves in Conducting Media 483
6.6.5 Reflection from PECs 484
6.6.6 Examples 494
6.7 Capacitance 503
6.7.1 Capacitance and Electric Potential Energy 504
6.7.2 Parallel-Plate Capacitors 505
6.7.3 Spherical Capacitors 513
6.7.4 Cylindrical Capacitors 518
6.7.5 Examples 520
6.8 Resistance 528
6.8.1 Examples 535
6.9 Inductance 544
6.9.1 Examples 553
6.10 Final Remarks 559
6.11 Exercises 560
6.12 Questions 565
7 Transmission of Electromagnetic Waves 569
7.1 Antennas and Wireless Transmission 570
7.1.1 Basic Properties of Antennas 571
7.1.2 Antenna Design Parameters 582
7.1.3 Antenna Types 585
7.1.3.1 Antenna Arrays 588
7.1.4 Friis Transmission Equation 600
7.1.5 Examples 603
7.2 Waveguides 613
7.2.1 Transverse and Axial Fields 614
7.2.2 Rectangular Waveguides 617
7.2.2.1 Transverse Magnetic Modes 618
7.2.2.2 Transverse Electric Modes 620
7.2.2.3 Non-Existing Modes 623
7.2.2.4 Important Properties of Modes 624
7.2.3 Parallel-Plate Waveguides 628
7.2.4 Examples 630
7.3 Transmission Line Theory 635
7.3.1 Telegrapher's Equations 637
7.3.1.1 Transmission Line With a Load 641
7.3.1.2 Special Cases 643
7.3.1.3 Common Cases 646
7.3.2 Voltage and Current Patterns 647
7.3.3 Examples 651
7.4 Concluding Remarks 658
7.5 Exercises 658
7.6 Questions 663
8 Concluding Chapter 669
8.1 Electromagnetic Spectrum 670
8.1.1 Radio Waves (3 Hz to 300 GHz) 671
8.1.2 Microwaves (300 MHz to 300 GHz) 672
8.1.3 Infrared Radiation (300 GHz to 400 THz) 673
8.1.4 Visible Range (400 THz to 800 THz) 674
8.1.5 Ultraviolet Radiation (800 THz to 30 PHz) 675
8.1.6 X-Rays (30 PHz to 30 EHz) 676
8.1.7 Gamma Rays (Above 30 EHz) 678
8.2 Brief History of Electromagnetism (Electricity, Magnetism, and a Little Optics) 679
8.3 Electromagnetism in Action 685
8.3.1 Snapshots From Nature 686
8.3.1.1 Blue Sky, Bright Sun, Red Sunset 686
8.3.1.2 Rainbow in Pocket 687
8.3.1.3 Green Leaf, Red Apple, Blue Sea 688
8.3.1.4 Electromagnetic Waves From Space 689
8.3.1.5 Magnetic Earth 690
8.3.2 Snapshots From Technology 691
8.3.2.1 Telegraph to Cellular Phones 691
8.3.2.2 Home: Where Electromagnetism Happens 693
8.3.2.3 Looking Inside Body 694
8.3.2.4 Seeing World with Sensors and Radars 696
8.3.2.5 Atoms Under Microscope 699
8.4 How to Solve Maxwell's Equations 700
8.4.1 Full-Wave Methods 705
8.4.1.1 Differential-Equation Solvers 706
8.4.1.1.1 Finite-Difference Time-Domain Method (FDTD): 706
8.4.1.1.2 Finite Element Method (FEM): 707
8.4.1.2 Integral-Equation Solvers 708
8.4.1.2.1 Method of Moments (MoM): 709
8.4.1.2.2 Acceleration Algorithms: 709
8.4.1.2.3 FMM and MLFMA: 711
8.4.2 Asymptotic Techniques 711
8.4.2.0.1 Quasistatic Approximations: 712
8.4.2.0.2 Geometrical Optics: 713
8.4.2.0.3 Uniform Geometrical Theory of Diffraction: 713
8.4.2.0.4 Physical Optics: 714
Bibliography 717
Index 725
I took my first serious course on electromagnetics 23 years ago. My favorite professor introduced us to our main textbook - a very famous primer, as I learned several years later. Even though I am not good at remembering conversations, particularly scientific ones, I still recall the following, with some dramatic visual details probably contributed by my imagination:
I completed my BSc and PhD at the same university, spending a total of eight years on top of five undergraduate years, and I had a chance to be a teaching assistant for numerous electromagnetics courses. We used the same book in all the undergraduate courses. In fact, I am still addicted to it, without any regret!
After some adventures in mathematics abroad, I returned to my current location in 2013 as a member of the faculty. The Middle East Technical University has a deep-rooted history, and the Department of Electrical and Electronics Engineering is one of the best in the country. In addition, the electromagnetics group has always been strong in this university, with full professors when I arrived. I, a 33-year-old man, was like a kid in a candy store, where "candy" refers to things I could do. For the undergraduate courses, I was happy to accept materials from my seniors, Prof. Özlem Aydın Çivi and Prof. Nilgün Günalp, as they were well prepared and optimized (some notes were older than me). In fact, they saved my life. But, thinking about teaching electromagnetics, I always shared the feeling with others that something was not right. Certainly it was difficult to describe; it seemed to be felt only by humans who taught electromagnetics. I had a chance to speak to many professors, instructors, and
teaching assistants, not only from my university but also from diverse universities all over the world during scientific conferences. Conversations related to teaching materials often reached the same point, already familiar to me:
The force that made me write this book appeared in one of these conversations, with remarkable words from a respected professor.
To be honest, I still do not know if Feynman ever tried to teach electromagnetics in this way, which I now call the correct order. Whenever I start to investigate, I find myself studying electromagnetics in the amazing world of this extraordinary scientist. In fact, whether Feynman taught this way is not important. The message I got was that this is a task so important that even Feynman - a man who can teach everything - might not complete it. This is a task that I must do.
If an instructor is reading these sentences, I am sure that s/he has an idea for a new book on electromagnetics, if it is not already written. And this is amazing, considering that the material has been more or less the same for decades. Any instructor of an electromagnetics course at some point thinks that the material given to her/him (usually by her/his senior instructors) could be taught in a better way. But any attempt to change the classical order of basic/fundamental electromagnetics surprisingly evolves into a complicated task, discouraging the instructor from embarking on an adventure. We have to accept that writing a book on basic electromagnetics is an ambitious task, for several reasons:
This book is the end product of an attempt to complete this ambitious task. It presents the well-known topics that all instructors would naturally include in their syllabus, while using the correct order (a novel approach). What I found was stranger than the problem itself. This correct order becomes possible only with a necessary pedagogic approach, ironically considering the typical learning behaviors of the students of the new millennium instead of the traditional mechanisms.
Before explaining the exact structure of this book with the so-called correct order of topics, I should indicate for whom it is written. This book is for undergraduate students who wish to or have to learn electromagnetism for the first time. It is also for senior undergraduate and graduate students who wish to go deeper in primary topics. In addition to Maxwell's equations and their basic applications for canonical problems, the material presented in this book also contains information on the transmission of electromagnetic waves with fundamental details on antennas, waveguides, and transmission lines. These topics must be covered for completeness of the basic knowledge, but readers should understand that each is the topic of individual books that cannot be merged into a single one. Vector calculus and similar fundamental information are also provided and discussed where necessary, but readers are expected have a background in basic calculus.
As already revealed, this book presents basic electromagnetics from the perspective of Maxwell's equations, which is possible via a new pedagogic approach. To further clarify, we may consider a particular example, such as the topic of gradient. In this book, gradient is introduced in Section 3.6.1 (Chapter 3), after Gauss' law, Ampere's law, and much more material.
In typical textbooks, the concept of gradient is explained much earlier - usually at the very beginning - since it is a fundamental mathematical tool. Readers may find very specific books where gradient is explained in later chapters, but this is merely an example. In this book, the same strategy is used for all tools: e.g. for dot product, cross product, divergence, curl, etc. To describe the approach in one sentence, in this book, a tool is presented whenever it is required, not earlier or later. Continuing with the same example, if gradient was explained earlier (e.g. in the preliminary (zero) chapter of this book), then we would encounter the two major issues of the traditional approach:
It should be noted that gradient is not used in Gauss' law and Ampere's law (at least, not directly), so it can be placed in Faraday's law. This is the idea.
Based on the described approach, the sequence of material in this book is optimized. Specifically, readers will frequently find text such as the following (from Chapter 3):
To understand the integral form of Faraday's law, we need the concepts of differential length with direction (Section 2.2.1) and circulation of vector fields (Section 2.1.2). These are in addition to the concepts of dot product (Section 1.1.2), differential surface with direction (Section 1.1.1), and flux of vector fields (Section 1.1.3). Therefore, no new tool is required before we focus on the meaning and application of the integral form of Faraday's law.
All tools and concepts are carefully defined so that readers will know exactly which tools are needed to understand the topic ahead.
As also mentioned above, the structure of this book is suitable for young students of the new millennium. As some instructors might have realized, and I will describe directly, students of the new generation have (good or bad) a pragmatic learning behavior. According to this strategy, learning is a recursive approach of opening boxes inside larger boxes until the required information is reached. Continuing with examples, a student who desires to learn the differential form of Faraday's law needs Stokes' theorem. If s/he does not know Stokes' theorem, s/he must learn it (that is, immediately under the section of the differential form of Faraday's law in this book). But at the second level, Stokes' theorem needs the dot product, curl, circulation, and flux concepts. As all these concepts are also used in Gauss' and Ampere's laws, so the student is forwarded to these tools (in case information is missing). Of course, by adapting this strategy, my aim is not to generate lazy students. The arrangement of...
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