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RF & Microwave Engineering BETE-Spring 2009 Department of Electrical Engineering Air University Waveguides TEM,TE & TM Modes Lecture No. 13

Lec.13 Waveguides

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Page 1: Lec.13 Waveguides

RF & Microwave EngineeringBETE-Spring 2009

Department of Electrical EngineeringAir University

Waveguides

TEM,TE & TM Modes

Lecture No. 13

Page 2: Lec.13 Waveguides

RF & Microwave EngineeringBETE-Fall 2009

Basit Ali ZebDepartment of Electrical Engineering, AU

Introduction

• There are several ways by which electromagnetic waves can propagate.

– Coaxial cable.

– Microstrip Lines

– Free Space (Unguided)

– Wave Guide Structures

Page 3: Lec.13 Waveguides

RF & Microwave EngineeringBETE-Fall 2009

Basit Ali ZebDepartment of Electrical Engineering, AU

Why Waveguides?

• Transmission Lines can only support TEM Waves.

• At high frequency attenuation, skin effect, and power handling capability limits the use of Transmission Lines.

• Wave Guides are the solution at microwave frequencies giving us:– Medium to Large bandwidth – Lower signal Attenuation– Greater power handling capacity

A waveguide is a metallic hollow structure of meaningful

shape which is used for guided wave propagation at high frequencies in an efficient manner.

Page 4: Lec.13 Waveguides

RF & Microwave EngineeringBETE-Fall 2009

Basit Ali ZebDepartment of Electrical Engineering, AU

Types of Waveguides

• Rectangular

• Circular

• Elliptical

In this course, we will only focus on rectangular waveguides.

Theory of waveguides requires an understanding of

Maxwell Equations and basic calculus!!

Page 5: Lec.13 Waveguides

RF & Microwave EngineeringBETE-Fall 2009

Basit Ali ZebDepartment of Electrical Engineering, AU

Rectangular Waveguide

It is assumed that the waveguide is filled with a material of permittivity ε and permeability µ.

Page 6: Lec.13 Waveguides

RF & Microwave EngineeringBETE-Fall 2009

Basit Ali ZebDepartment of Electrical Engineering, AU

Concept of Modes

• We will first develop an extremely important property of EM waves that propagate in homogenous waveguides.

• This will lead to the concept of different “modes” that travel inside a waveguide

Page 7: Lec.13 Waveguides

RF & Microwave EngineeringBETE-Fall 2009

Basit Ali ZebDepartment of Electrical Engineering, AU

Solution of Maxwell’s Equations

Electric and Magnetic field components along x,y,zcoordinates

Ex,Ey and Hx,Hy are transverse components

Ez, Hz are longitudinal/axial components

Page 8: Lec.13 Waveguides

RF & Microwave EngineeringBETE-Fall 2009

Basit Ali ZebDepartment of Electrical Engineering, AU

Solution of Maxwell’s Equations

Page 9: Lec.13 Waveguides

RF & Microwave EngineeringBETE-Fall 2009

Basit Ali ZebDepartment of Electrical Engineering, AU

Solution of Maxwell’s Equations

Page 10: Lec.13 Waveguides

RF & Microwave EngineeringBETE-Fall 2009

Basit Ali ZebDepartment of Electrical Engineering, AU

Solution of Maxwell’s Equations

Page 11: Lec.13 Waveguides

RF & Microwave EngineeringBETE-Fall 2009

Basit Ali ZebDepartment of Electrical Engineering, AU

Solution of Maxwell’s Equations

Page 12: Lec.13 Waveguides

RF & Microwave EngineeringBETE-Fall 2009

Basit Ali ZebDepartment of Electrical Engineering, AU

Wave Modes

• Transverse Electric and Magnetic (TEM)

• Transverse Electric (TE)

• Transverse Magnetic (TM)

• In a given waveguide at a given frequency, several field configurations may satisfy Maxwell’s equations. These field configurations are called wave modes.

• Every mode has its own propagation characteristics: velocity, attenuation, and cutoff frequency.

Page 13: Lec.13 Waveguides

RF & Microwave EngineeringBETE-Fall 2009

Basit Ali ZebDepartment of Electrical Engineering, AU

Waveguide Modes

• TE mode• TM mode• TEM mode

Page 14: Lec.13 Waveguides

RF & Microwave EngineeringBETE-Fall 2009

Basit Ali ZebDepartment of Electrical Engineering, AU

TE Mode

Page 15: Lec.13 Waveguides

RF & Microwave EngineeringBETE-Fall 2009

Basit Ali ZebDepartment of Electrical Engineering, AU

Wavenumber

Page 16: Lec.13 Waveguides

RF & Microwave EngineeringBETE-Fall 2009

Basit Ali ZebDepartment of Electrical Engineering, AU

Wavenumber

Page 17: Lec.13 Waveguides

RF & Microwave EngineeringBETE-Fall 2009

Basit Ali ZebDepartment of Electrical Engineering, AU

Cuttoff Frequency

Waveguides always operate above a certain frequency called the “cut off frequency”. At a frequency below cutoff frequency, field attenuates very rapidly and no wave can propagate.

Page 18: Lec.13 Waveguides

RF & Microwave EngineeringBETE-Fall 2009

Basit Ali ZebDepartment of Electrical Engineering, AU

X-Band Waveguide

WR 90

Waveguide

in the lab!

Page 19: Lec.13 Waveguides

RF & Microwave EngineeringBETE-Fall 2009

Basit Ali ZebDepartment of Electrical Engineering, AU

TM Modes

Page 20: Lec.13 Waveguides

RF & Microwave EngineeringBETE-Fall 2009

Basit Ali ZebDepartment of Electrical Engineering, AU

TM Modes Cutoff frequency

Page 21: Lec.13 Waveguides

RF & Microwave EngineeringBETE-Fall 2009

Basit Ali ZebDepartment of Electrical Engineering, AU

TEM Mode

Page 22: Lec.13 Waveguides

RF & Microwave EngineeringBETE-Fall 2009

Basit Ali ZebDepartment of Electrical Engineering, AU

Mode Distributions