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INTRODUCTION TO MICROWAVE ENGINEERING
33

Microwave engineering ch1

Jan 23, 2018

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Muhammad Azwir
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Page 1: Microwave engineering ch1

INTRODUCTION TO MICROWAVE ENGINEERING

Page 2: Microwave engineering ch1

WEEK 1

• CLASS 1: Introduction to Microwave Engineering, Applications of Microwave Engineering, Maxwelll’s Equations

• CLASS 2: The wave equation and basic plane wave solutions, Poynting’s Theorem and Wave Power

Page 3: Microwave engineering ch1

WEEK 2

• CLASS 3: Plane wave reflection from a media interface, Refraction, Diffraction

• CLASS 4: S-Parameters, Propagation in good conductors: skin effect

Page 4: Microwave engineering ch1

INTRODUCTIONWhat is “Micro”wave?

3 x 10^8 Hz(lambda = 1m)

3 x 10^11 Hz(lambda = 1mm)

Page 5: Microwave engineering ch1

SO WHAT?The complication of small wavelengths are many….

Because the size of the device is ~ lambda, the phases of voltage and current over the device changes

Page 6: Microwave engineering ch1

APPLICATIONS OF

MICROWAVE ENGINEERING

Why Study Microwave?

Page 7: Microwave engineering ch1

Our love for small (and thin!) wireless devices

If we operate at smaller lambda (err…higher frequencies), our

devices become BIG (electronically!)

Page 8: Microwave engineering ch1

The 5G standard (operating at 28 GHz) will be 100

times faster than 4G, with data rate of ~ 10GB/sec!

Our love for juice!

Page 9: Microwave engineering ch1

Microwave signal travel by LOS, enabling high capacity satellite

links! Thus live footballs!

Our love for direct broadcast!

Page 10: Microwave engineering ch1

REVISITING OUR ELDERS“IF I HAVE SEEN FURTHER, IT IS BY STANDING ON THE SHOULDERS OF GIANTS”

- ISAAC NEWTON

! THE MAXWELL’S EQUATIONS !(Macroscopic electric and magnetic phenomena are described by these equations)

Page 11: Microwave engineering ch1

Differential Form of Maxwell’s Equation

Gauss’s Law

Gauss’s Magnetism Law

Faraday’s Law

Ampere’s Law

Page 12: Microwave engineering ch1

DIVERGENT VS.

CURL

Page 13: Microwave engineering ch1

Electric Flux Density

#1 Gauss’s Law

{

Electric charge acts as sources or sinks for Electric Fields

Electric Charge Density{

Page 14: Microwave engineering ch1

Magnetic Flux Density

#2 Gauss’s Magnetism Law

{Magnetic monopoles do not exist!

Page 15: Microwave engineering ch1

#3 Faraday’ LawA magnetic field changing in time gives rise to an E-field circulating around it

https://phet.colorado.edu/sims/html/faradays-law/latest/faradays-law_en.html

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#4 Ampere’s Law

A time-changing Electric Flux Density (D) gives rise to a Magnetic Field that

circles the D field

A flowing electric current (J) gives rise to a Magnetic Field that circles the

current

In Wires In Wireless

Page 17: Microwave engineering ch1

DC

Conclusion of Maxwell’s Equation

{{

AC

A changing magnetic field gives rise to a changing electric field…and a changing electric field gives rise to a changing magnetic field - which itself will produce a

changing electric field which will give rise to ..... ?!??!!

Page 18: Microwave engineering ch1

Electromagnetic Propagation

Page 19: Microwave engineering ch1

THE WAVE (MOVING, OR, PROPAGATING!)• The wave equation and basic plane wave solutions, Poynting’s

Theorem and Wave Power

Page 20: Microwave engineering ch1

THE WAVE EQUATIONIn general, the wave equation is a mathematical relationship between the

speed (v) of a wave and its wavelength (λ) and frequency (f).

v = λf

From the two equation, we see that the EM wave (E and H) is varying in space (x, y, z) and also time (t)

HW1: Derive this!

Page 21: Microwave engineering ch1

THE PLANE WAVEA special case when E and H is not varying in x and y direction, forming

only a “plane” moving upwards/downwards along z-axis

z (-kz)

E0x

E0

Equation (1) - Board

Page 22: Microwave engineering ch1

What happens to H?By solving the wave equation for an x directed E-field (as was derived

on the board) travelling in the z-direction, we find that it is alwaysACCOMPANIED BY A y-DIRECTED H-FIELD

z (-kz)

E0x

E0

y

Equation (2) - Board

Page 23: Microwave engineering ch1

If both E and H is travelling in the z-direction perpendicular to each other (TEM Wave),

WHAT DOES IT’S PROPAGATION REPRESENT?

ENERGYTEM WAVE

Poynting Vector, P

ENERGY

P = E X H

Page 24: Microwave engineering ch1

z (-kz)

E0x

E0

y

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• Example Question (on board)

Page 26: Microwave engineering ch1

PROPAGATION IN LOSSY MEDIUM• CLASS 3: Plane wave reflection from a media interface,

Refraction, Diffraction

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The wave equation remains same but the “wave number/propagation constant” is COMPLEX

We’re introduced to a new term that symbolises loss. In a lossless media (i.e, free-space),

sigma =0

MAIN ISSUE

Page 28: Microwave engineering ch1

The general effect of a complex “k” is a travelling wave that changes its amplitude with distance

Equation (3) - Board

WAVE EQUATION WITH COMPLEX ‘K’

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REGARDLESS OF PROPAGATION(IN FREE SPACE/ A MEDIUM)…

What is the speed of the electromagnetic wave?

Equation (4) - Board

Page 30: Microwave engineering ch1

PLANE WAVE REFLECTION FROM A MEDIA INTERFACE

Free-Space

Derivation on the Board

Page 31: Microwave engineering ch1

S-PARAMETERS…OR, “scattering” parameters are measures of reflection and transmission of voltage

waves through a two-port electrical network.

Page 32: Microwave engineering ch1

S-parameters come in a matrix, with the number of rows and columns equal to the number of ports

}{

REFLECTED

TRANSMITTED

Page 33: Microwave engineering ch1

THE END CH 1