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EMLAB 1 Introduction to EM theory 1

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Page 1: EMLAB 1 Introduction to EM theory 1. EMLAB 2 Electromagnetic phenomena The globe lights up due to the work done by electric current (moving charges)

EMLAB

1

Introduction to EM theory 1

Page 4: EMLAB 1 Introduction to EM theory 1. EMLAB 2 Electromagnetic phenomena The globe lights up due to the work done by electric current (moving charges)

EMLAB

4Electromagnetic wave – Crosstalk

Page 6: EMLAB 1 Introduction to EM theory 1. EMLAB 2 Electromagnetic phenomena The globe lights up due to the work done by electric current (moving charges)

EMLAB

6

Electromagnetic wave : automotive radar

Moving charges on the antenna generate electromagnetic waves.

Page 9: EMLAB 1 Introduction to EM theory 1. EMLAB 2 Electromagnetic phenomena The globe lights up due to the work done by electric current (moving charges)

EMLAB

9

• EM theory helps understand how electrical signals propagate along con-ductors as well as free space.

• Predicts voltages and currents using the concept of electric and magnetic field.

Importance of electromagnetic theory

Page 10: EMLAB 1 Introduction to EM theory 1. EMLAB 2 Electromagnetic phenomena The globe lights up due to the work done by electric current (moving charges)

EMLAB

10

Basic laws – Maxwell equations

0

B

D

DJH

BE

t

t

1. Electromagnetic phenomena are explained by the four Maxwell equations.

2. Through the equations, electric field and magnetic field are coupled to each other.

3. Quantities on the right hand side are the source terms.

4. Quantities on the left side are the resulting phenomena.

5. The independent variables are current den-sity vector J and charge density .

Maxwell equations

'

'

')]ˆ(ˆ[4

1

'4

)]ˆ(ˆ[

V

V

jkR

dtR

dR

ej

JRRJ

JRRJE

Solution (free space)

Page 11: EMLAB 1 Introduction to EM theory 1. EMLAB 2 Electromagnetic phenomena The globe lights up due to the work done by electric current (moving charges)

EMLAB

11

Electromagnetic theory

Electric field (E)

Magnetic field (H)

Electro-magnetic field (E,H )

Sources (q, J)

Material (ε, μ)

Mathematics

Coordinate systems

Vector calculus (diver-gence, curl, gradient)

EM-theory

Material

Page 12: EMLAB 1 Introduction to EM theory 1. EMLAB 2 Electromagnetic phenomena The globe lights up due to the work done by electric current (moving charges)

EMLAB

12Contents

1. Electric field

① Coulomb’s law

② Gauss’s law (divergence)

③ Electric potential (gradient)

④ Capacitance

⑤ Ohm’s law

2. Magnetic field

① Biot-Savart law

② Ampere’s law (curl)

③ Inductance

1. Sources

① Charge

② Current

2. Material

① Conductor (semi-conductor, lossy material)

② Dielectric (insulator)

③ Magnetic material

Page 13: EMLAB 1 Introduction to EM theory 1. EMLAB 2 Electromagnetic phenomena The globe lights up due to the work done by electric current (moving charges)

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13

3. Electro-magnetic field

① Faraday’s law

② Displacement current

③ Maxwell’s equations

④ Plane wave

⑤ Reflection/transmission

4. Transmission lines

① Impedance matching

② Smith chart

③ Waveguides

5. Radiation

Page 14: EMLAB 1 Introduction to EM theory 1. EMLAB 2 Electromagnetic phenomena The globe lights up due to the work done by electric current (moving charges)

EMLAB

14

Electric field

A charged particle undergoes acceleration which is proportional to the electric field nearby.

EF q

Page 15: EMLAB 1 Introduction to EM theory 1. EMLAB 2 Electromagnetic phenomena The globe lights up due to the work done by electric current (moving charges)

EMLAB

15

Coulomb’s law

1. The electric field is generated by the charge Q and spread into the space.

2. The speed of electric field transmission is the same as the speed of light.

rE ˆ4 2

0r

Q

Page 16: EMLAB 1 Introduction to EM theory 1. EMLAB 2 Electromagnetic phenomena The globe lights up due to the work done by electric current (moving charges)

EMLAB

16

Electrons(-) are absorbed.(+) charges are generated

Electrons(-) are generated. (+) charges are absorbed.

Generation of charges : battery

e2ZnZn 2

234 HNH222NH e

Electrons are generated via electro-chemical reaction.

An amount of positive charges are generated such that the terminal voltages are sus-tained.

Page 17: EMLAB 1 Introduction to EM theory 1. EMLAB 2 Electromagnetic phenomena The globe lights up due to the work done by electric current (moving charges)

EMLAB

17

B

A

dVr

rrE)(

Potential distribution near charged plates

VE

Charges emanate from a battery.

Page 18: EMLAB 1 Introduction to EM theory 1. EMLAB 2 Electromagnetic phenomena The globe lights up due to the work done by electric current (moving charges)

EMLAB

18Induction charging

Droplets of an inkjet printer emission.

A conducting sphere can be charged by induction.

Page 19: EMLAB 1 Introduction to EM theory 1. EMLAB 2 Electromagnetic phenomena The globe lights up due to the work done by electric current (moving charges)

EMLAB

19Micro-machine

MEMS devices can be con-trolled by electrostatic forces.

Page 20: EMLAB 1 Introduction to EM theory 1. EMLAB 2 Electromagnetic phenomena The globe lights up due to the work done by electric current (moving charges)

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20

Magnetic field

A charged particle in mo-tion generates magnetic field nearby.

In the same way, current s generate magnetic field nearby.

Page 21: EMLAB 1 Introduction to EM theory 1. EMLAB 2 Electromagnetic phenomena The globe lights up due to the work done by electric current (moving charges)

EMLAB

21

Motion of a charge in a magnetic field

BvF q

Charged particles in motion are influenced by magnetic fields

Page 22: EMLAB 1 Introduction to EM theory 1. EMLAB 2 Electromagnetic phenomena The globe lights up due to the work done by electric current (moving charges)

EMLAB

22

Biot-Savart law

24

ˆ

R

Idd

Rs

H

'rrR 'r

r

sId

Direction of H-field

Current segment

The generated magnetic field can be predicted by Biot-Savart’s law

Page 23: EMLAB 1 Introduction to EM theory 1. EMLAB 2 Electromagnetic phenomena The globe lights up due to the work done by electric current (moving charges)

EMLAB

23

loop closed

IdsH

Ampere’s law