- •Foreword
- •Preface
- •Contents
- •Symbols
- •1 Electromagnetic Field and Wave
- •1.1 The Physical Meaning of Maxwell’s Equations
- •1.1.1 Basic Source Variables
- •1.1.2 Basic Field Variables
- •1.1.3 Maxwell’s Equations in Free Space
- •1.1.4 Physical Meaning of Maxwell’s Equations
- •1.1.5 The Overall Physical Meaning of Maxwell’s Equations
- •1.2 Electromagnetic Power Flux
- •1.2.1 The Transmission of Electromagnetic Power Flux
- •1.2.2 Capacitors—Electrical Energy Storage
- •1.2.3 Inductor—Magnetic Energy Storage
- •1.2.4 Examples of Device Properties Analysis
- •1.3.1 Boundary Conditions of the Electromagnetic Field on the Ideal Conductor Surface
- •1.3.2 Air Electric Wall
- •2 Microwave Technology
- •2.1 The Theory of Microwave Transmission Line
- •2.1.1 Overview of Microwave Transmission Line
- •2.1.2 Transmission State and Cutoff State in the Microwave Transmission Line
- •2.1.3 The Concept of TEM Mode, TE Mode, and TM Mode in Microwave Transmission Line
- •2.1.4 Main Characteristics of the Coaxial Line [4]
- •2.1.5 Main Characteristics of the Waveguide Transmission Line
- •2.1.6 The Distributed Parameter Effect of Microwave Transmission Line
- •2.2 Application of Transmission Line Theories in EMC Research
- •3 Antenna Theory and Engineering
- •3.1 Field of Alternating Electric Dipole
- •3.1.1 Near Field
- •3.1.2 Far Field
- •3.2 Basic Antenna Concepts
- •3.2.1 Directivity Function and Pattern
- •3.2.2 Radiation Power
- •3.2.3 Radiation Resistance
- •3.2.4 Antenna Beamwidth and Gain
- •3.2.6 Antenna Feed System
- •4.1.1 Electromagnetic Interference
- •4.1.2 Electromagnetic Compatibility
- •4.1.3 Electromagnetic Vulnerability
- •4.1.4 Electromagnetic Environment
- •4.1.5 Electromagnetic Environment Effect
- •4.1.6 Electromagnetic Environment Adaptability
- •4.1.7 Spectrum Management
- •4.1.9 Spectrum Supportability
- •4.2 Essences of Quantitative EMC Design
- •4.2.2 Three Stages of EMC Technology Development
- •4.2.3 System-Level EMC
- •4.2.4 Characteristics of System-Level EMC
- •4.2.5 Interpretations of the EMI in Different Fields
- •4.3 Basic Concept of EMC Quantitative Design
- •4.3.1 Interference Correlation Relationship
- •4.3.2 Interference Correlation Matrix
- •4.3.3 System-Level EMC Requirements and Indicators
- •4.3.5 Equipment Isolation
- •4.3.6 Quantitative Allocation of Indicators
- •4.3.7 The Construction of EMC Behavioral Model
- •4.3.8 The Behavior Simulation of EMC
- •4.3.9 Quantitative Modeling Based on EMC Gray System Theory
- •5.2 Solution Method for EMC Condition
- •5.3 EMC Modeling Methodology
- •5.3.1 Methodology of System-Level Modeling
- •5.3.2 Methodology for Behavioral Modeling
- •5.3.3 EMC Modeling Method Based on Gray System Theory
- •5.4 EMC Simulation Method
- •6.1 EMC Geometric Modeling Method for Aircraft Platform
- •6.2.1 Interference Pair Determination and Interference Calculation
- •6.2.2 Field–Circuit Collaborative Evaluation Technique
- •6.2.3 The Method of EMC Coordination Evaluation
- •6.3 Method for System-Level EMC Quantitative Design
- •6.3.2 The Optimization Method of Single EMC Indicator
- •6.3.3 The Collaborative Optimization Method for Multiple EMC Indicators
- •7.1 The Basis for EMC Evaluation
- •7.2 The Scope of EMC Evaluation
- •7.2.1 EMC Design
- •7.2.2 EMC Management
- •7.2.3 EMC Test
- •7.3 Evaluation Method
- •7.3.1 The Hierarchical Evaluation Method
- •7.3.2 Evaluation Method by Phase
- •8 EMC Engineering Case Analysis
- •8.1 Hazard of Failure in CE102, RE102, and RS103 Test Items
- •8.2 The Main Reasons for CE102, RE102, and RS103 Test Failures
- •8.2.1 CE102 Test
- •8.2.2 RE102 Test
- •8.2.3 RS103 Test
- •8.3 The Solutions to Pass CE102, RE102, and RS103 Tests
- •8.3.1 The EMC Failure Location
- •8.3.2 Trouble Shooting Suggestions
- •A.1 Pre-processing Function
- •A.2 Post-processing Function
- •A.3 Program Management
- •A.4 EMC Evaluation
- •A.5 System-Level EMC Design
- •A.6 Database Management
- •References
1.1 The Physical Meaning of Maxwell’s Equations |
7 |
enclosed by the curved surface. In other words, the charge is the source of the electric flux density vector.
4.Physical meaning of Gauss’s law for magnetism
In free space, the net magnetic flux that passes through any closed curved surface is zero; that is, there is no source magnetic charge of the magnetic flux density vector.
5.Physical meaning of the law of charge conservation
For a system of volume V and external surface S, the net charge in the system changes only when there is charge in or out. If the system has no charge exchange with the outside world, that is, the system is a charge-closed system, then the net charge within the system is constant. In other words, the charge can only be transferred in the form of current, but cannot be generated or disappeared by itself.
1.1.5 The Overall Physical Meaning of Maxwell’s Equations
The significance of Maxwell’s equations in the electromagnetic field theory is the same as the significance of Newton’s laws of mechanics in theoretical mechanics. Any real electromagnetic field behavior obeys Maxwell’s equations. In the scope of nonrelativity, the behavior of electromagnetic fields must obey Maxwell’s equations in integral form. From the form of the equations, Maxwell’s equations describe the relationship between the electromagnetic field quantities E and H and their source quantities ρ, J, which is illustrated in Fig. 1.1, where the arrow “ →” indicates direct relationship, and “~~ → ” indicates a time-varying relationship.
Of all the relationships reflected in Maxwell’s equations, there are two situations that need further discussion.
Fig. 1.1 Overall physical meaning of the electromagnetic field law
8 |
|
|
|
|
|
1 Electromagnetic Field and Wave |
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
Fig. 1.2 Overall physical meaning of EMF laws when all physical variables are nontime varying
(1)All physical variables are time invariant. At this time, the relationship between the field quantities E and H and their source quantities ρ and J is shown as Fig. 1.2. The electromagnetic field law at this time is:
S E · d s 0 |
(1.2a) |
||
C H · d s |
S J · d a |
(1.2b) |
|
S ε0 E · d a |
V ρ d V |
(1.2c) |
|
S μ0 H · d a 0 |
(1.2d) |
||
S |
J · d a 0 |
(1.2e) |
…
In this case, there is no mutual coupling between E and H. Only two sides of “→” can be retained in Fig. 1.1. This situation is a static (or nontime-varying) electromagnetic field issue.
2.Source quantities are zero, i.e., ρ 0, J 0. In this situation, the expression of the relationship between the electromagnetic field quantities E and H and their source quantities ρ and J is shown in Fig. 1.3. The electromagnetic field law in this situation can be written as
d |
|
C E · d s − dt S μ0 H · d a |
(1.3a) |
1.1 The Physical Meaning of Maxwell’s Equations |
9 |
|||||
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
Fig. 1.3 Overall physical meaning of EMF law when the source quantities are zero
|
d |
|
|
C H · d s |
|
S ε0 E · d a |
(1.3b) |
dt |
|||
S ε0 E · d a 0 |
(1.3c) |
||
S μ0 H • d a 0 |
(1.3d) |
From Fig. 1.3, we see that in the region without charge and current, the timevarying electromagnetic field can still exist through mutual coupling, and this form of existence is called the electromagnetic wave. Free space is a typical medium for electromagnetic wave propagation.
Now, we further explain |
C H · d s |
|
d |
S ε0 E · d a. After transformation, the |
||||||
|
dt |
|||||||||
formula can be rewritten as |
C H · d s |
d |
S ε0 E · d a |
S |
∂ |
(ε0 E) · d a. |
∂ |
ε0 E |
||
dt |
|
∂ t |
∂ t |
and the current J satisfies the same equation in generating magnetic field in form. ∂∂t (ε0 E) is added to electromagnetic field law by Maxwell for the mathematical integrity. This term is called the displacement current term. After adding this item to Ampere’s law and combined with Faraday’s law of electromagnetic induction, the existence of electromagnetic waves is theoretically proved. At first, people only thought that this was a mathematical treatment because there was no experimental evidence of the existence of electromagnetic waves. It was not until 1888, nine years after Maxwell’s death, that Hertz’s electromagnetic experiments proved the genius prophecy of Maxwell.
The purpose of revisiting the overall physical meaning of Maxwell’s equations is to provide our reader systematical explanation that the characteristics of the electronic circuits in DC (frequency 0 Hz) or low frequency (frequency < 100 kHz) and the characteristics of the electronic circuits in RF (frequency > 1 MHz) or microwave (frequency > 1 GHz) are essentially different.
Now, we explain the above with examples.