TOPIC 2 WAVEGUIDE AND COMPONENTS

Similar documents
ELEC4604. RF Electronics. Experiment 2

Waveguides GATE Problems

Photograph of the rectangular waveguide components

Microwave and optical systems Introduction p. 1 Characteristics of waves p. 1 The electromagnetic spectrum p. 3 History and uses of microwaves and

INTRODUCTION OF WAVEGUIDES

Waveguides. Metal Waveguides. Dielectric Waveguides

COAXIAL / CIRCULAR HORN ANTENNA FOR A STANDARD

EC Transmission Lines And Waveguides

ECSE 352: Electromagnetic Waves

ELECTROMAGNETIC WAVES AND ANTENNAS

EC6503 Transmission Lines and WaveguidesV Semester Question Bank

Lec7 Transmission Lines and waveguides (II)

Unit 5 Waveguides P a g e 1

USE OF MICROWAVES FOR THE DETECTION OF CORROSION UNDER INSULATION

Rectangular waveguides

Keywords Cross-polarization, phasing length, return loss, multimode horn

SRI VENKATESWARA COLLEGE OF ENGINEERING DEPARTMENT OF ELECTRONICS AND COMMUNICATION ENGINEERING Date : UNIVERSITY QUESTIONS AND ANSWERS

Practical Measurements of Dielectric Constant and Loss for PCB Materials at High Frequency

2/18/ Transmission Lines and Waveguides 1/3. and Waveguides. Transmission Line A two conductor structure that can support a TEM wave.

UNIT - V WAVEGUIDES. Part A (2 marks)

We are IntechOpen, the world s leading publisher of Open Access books Built by scientists, for scientists. International authors and editors

THE ELECTROMAGNETIC FIELD THEORY. Dr. A. Bhattacharya

EC TRANSMISSION LINES AND WAVEGUIDES TRANSMISSION LINES AND WAVEGUIDES

Fundamentals of Electromagnetics With Engineering Applications by Stuart M. Wentworth Copyright 2005 by John Wiley & Sons. All rights reserved.

Aperture Antennas. Reflectors, horns. High Gain Nearly real input impedance. Huygens Principle

7. Experiment K: Wave Propagation


TCET 2220/TC 410 Transmission Systems

Fiber Optic Communications Communication Systems

Microwave Engineering

3. (a) Derive an expression for the Hull cut off condition for cylindrical magnetron oscillator. (b) Write short notes on 8 cavity magnetron [8+8]

CHAPTER 2 MICROSTRIP REFLECTARRAY ANTENNA AND PERFORMANCE EVALUATION

Γ L = Γ S =

EMG4066:Antennas and Propagation Exp 1:ANTENNAS MMU:FOE. To study the radiation pattern characteristics of various types of antennas.

RAJIV GANDHI COLLEGE OF ENGINEERING AND TECHNOLOGY Kirumampakkam,Puducherry DEPARTMENT OF ELECTRONICS AND COMMUNICATION ENGINEERING

RF AND MICROWAVE ENGINEERING

R.K.YADAV. 2. Explain with suitable sketch the operation of two-cavity Klystron amplifier. explain the concept of velocity and current modulations.

DESIGN AND FABRICATION OF CAVITY RESONATORS

Monoconical RF Antenna

Useful general references for this experiment are Cheng [1], and Ramo et al [2].

1. Evolution Of Fiber Optic Systems

SUPPLEMENTARY INFORMATION

INSTITUTE OF AERONAUTICAL ENGINEERING Dundigal, Hyderabad ELECTRONICS AND COMMUNIACTION ENGINEERING QUESTION BANK

Hours / 100 Marks Seat No.

Introduction: Planar Transmission Lines

Wave & Electromagnetic Spectrum Notes

Lecture #3 Microstrip lines

PRINCIPLES OF RADAR. By Members of the Staff of the Radar School Massachusetts Institute of Technology. Third Edition by J.

Dielectric Circular Waveguide Loaded with Dielectric Material

A NOVEL DUAL-BAND PATCH ANTENNA FOR WLAN COMMUNICATION. E. Wang Information Engineering College of NCUT China

EC ANTENNA AND WAVE PROPAGATION

KULLIYYAH OF ENGINEERING

Fiber Optic Communication Systems. Unit-04: Theory of Light.

COMPARATIVE ANALYSIS BETWEEN CONICAL AND GAUSSIAN PROFILED HORN ANTENNAS

CHAPTER 5 THEORY AND TYPES OF ANTENNAS. 5.1 Introduction

1. What are the applications of loop antenna? (May2011) 2. Define Pattern Multiplication (May2011)

(i) Determine the admittance parameters of the network of Fig 1 (f) and draw its - equivalent circuit.

Dual-band Antenna Feed Solution for 5G. A dual-band coaxial- and waveguide fed antenna feed for reflector LUKAS MARED

MICROWAVE WAVEGUIDES and COAXIAL CABLE

Keysight Technologies Techniques for Advanced Cable Testing

FINAL EXAM 12/12/03 EECS FALL 2003

Waveguide Calibration with Copper Mountain Technologies VNA

MICROWAVE AND RADAR LAB (EE-322-F) LAB MANUAL VI SEMESTER

Simulation and manufacturing of a miniaturized Exponential UWB TEM horn antenna for UWB Radar applications

Waves, Wavelength, Frequency and. Bands. Al Penney VO1NO

Antennas 1. Antennas

Projects in microwave theory 2009

ECE 3065: Electromagnetic Applications Final Exam (Spring 2004)

A Mode Based Model for Radio Wave Propagation in Storm Drain Pipes

ANTENNA INTRODUCTION / BASICS

A New TEM Horn Antenna Designing Based on Plexiglass Antenna Cap

DEPARTMENT OF ELECTRONICS AND COMMUNICATION ENGINEERING SUBJECT CODE: EC 1305 SUBJECT: TRANSMISSION LINES AND WAVEGUIDES (FOR FIFTH SEMESTER ECE)

Chapter 15: Radio-Wave Propagation

Design of a prime-focus feed with backward radiation

Chapter 4 The RF Link

ELEC4604. RF Electronics. Experiment 1

Department of Electrical Engineering University of North Texas

PRIME FOCUS FEEDS FOR THE COMPACT RANGE

Electromagnetic Wave Analysis of Waveguide and Shielded Microstripline 1 Srishti Singh 2 Anupma Marwaha

Cut-off of Resonant Modes in Truncated Conical Cavities

APPLIED ELECTROMAGNETICS: EARLY TRANSMISSION LINES APPROACH

Antenna & Propagation. Basic Radio Wave Propagation

Design and Implementation of Quasi Planar K-Band Array Antenna Based on Travelling Wave Structures

UWB leaky lens antenna design and simulation for waveguide measurements

EFFECT ON PERFORMANCE CHARACTERISTICS OF RECTANGULAR PATCH ANTENNA WITH VARYING HEIGHT OF DIELECTRIC COVER

Chapter 41 Deep Space Station 13: Venus

An Introduction to Antennas

I.E.S-(Conv.)-1996 Some useful data:

Notes 21 Introduction to Antennas

MEASUREMENT OF COMPLEX PERMITTIVITY AND COMPLEX PERMEABILITY OF MATERIALS. H. Alenkowicz*, B. Levitas**

Fiber Optic Communication Systems. Unit-05: Types of Fibers.

KINGS COLLEGE OF ENGINEERING. DEPARTMENT OF ELECTRONICS AND COMMUNICATION ENGINEERING Academic Year (Even Sem) QUESTION BANK (AUTT-R2008)

Impedance Matching For L-Band & S- Band Navigational Antennas

L-BAND COPLANAR SLOT LOOP ANTENNA FOR INET APPLICATIONS

Antennas and Propagation. Chapter 4: Antenna Types

CHAPTER 3 METHODOLOGY AND SOFTWARE TOOLS

ANTENNAS AND WAVE PROPAGATION EC602

Antenna Fundamentals

Localization and Identifying EMC interference Sources of a Microwave Transmission Module

University of KwaZulu-Natal

Transcription:

TOPIC 2 WAVEGUIDE AND COMPONENTS

COURSE LEARNING OUTCOME (CLO) CLO1 Explain clearly the generation of microwave, the effects of microwave radiation and the propagation of electromagnetic in a waveguide and its accessories CLO2 Apply given mathematical equations or Smith Chart to solve problem related to microwave propagation.

CLO3 Handle systematically the related microwave communication equipment in performing the assigned practical work.

Understand the characteristic of waveguide Upon completion of this topic, students should be able to: 1. Define a) Critical (cut-off) frequency b) Critical (cut-off) wavelength 2. Explain the following terminologies: Group velocity, Phase velocity, propagation wavelength, waveguide characteristic impedance 3. Calculate the item no.1 and no. 2 for rectangular and circular waveguide

Rectangular Waveguide With; a = broad dimension b = narrow dimension x = length waveguide Dimensions of the waveguide which determines the operating frequency range

Dimensions of the waveguide which determines the operating frequency range: 1. The size of the waveguide determines its operating frequency range. 2. The frequency of operation is determined by the dimension a. 3. This dimension is usually made equal to one half the wavelength at the lowest frequency of operation, this frequency is known as the waveguide cutoff frequency. 4. At the cutoff frequency and below, the waveguide will not transmit energy. At frequencies above the cutoff frequency, the waveguide will propagate energy.

Circular waveguide r = radius x = length waveguide

Characteristic of waveguide Waveguides are basically a device ("a guide") for transporting electromagnetic energy from one region to another. They are capable of directing power precisely to where it is needed, can handle large amounts of power and function as a high-pass filter.

The waveguide acts as a high pass filter in that most of the energy above a certain frequency (the cutoff frequency) will pass through the waveguide, whereas most of the energy that is below the cutoff frequency will be attenuated by the waveguide.

Critical (cut-off) Frequency, Fc The cutoff frequency is the frequency at which all lower frequencies are attenuated by the waveguide, and above the cutoff frequency all higher frequencies propagate within the waveguide. The cutoff frequency defines the high-pass filter characteristic of the waveguide: above this frequency, the waveguide passes power, below this frequency the waveguide attenuates or blocks power.

The cutoff frequency depends on the shape and size of the cross section of the waveguide. The larger the waveguide is, the lower the cutoff frequency for that waveguide is. The formula for the cutoff frequency of a rectangular cross sectioned waveguide is given by: - permeability - permittivity

Rectangular Waveguide Let us consider a rectangular waveguide with interior dimensions are a x b, Waveguide can support TE and TM modes. In TE modes, the electric field is transverse to the direction of propagation. In TM modes, the magnetic field that is transverse and an electric field component is in the propagation direction. The order of the mode refers to the field configuration in the guide, and is given by m and n integer subscripts, TE mn and TM mn. The m subscript corresponds to the number of halfwave variations of the field in the x direction, and The n subscript is the number of half-wave variations in the y direction.

Location of Modes

Rectangular Waveguide A particular mode is only supported above its cutoff frequency. The cutoff frequency is given by f c mn 2 2 2 2 1 m n c m n 2 a b 2 a b r r where c 8 3 10 m/s

Rectangular Waveguide

Formula

Dominant Mode The dominant mode is the mode with lowest cutoff frequency. It s always TE 10 The order of the next modes change depending on the dimensions of the guide.

Group and Phase velocity How fast is the wave traveling? Velocity is a reference distance divided by a reference time. Group velocity is the velocity at which the energy of the wave propagates. This means that the wave moves at the speed of vg. Phase velocity is the speed of movement of a point of constant phase in a continous wave. Group and phase velocities have the same value in free space and in parallel wire transmission lines.

Group and Phase velocity

The Phase velocity This is the velocity at which the overall shape of the wave s amplitudes, or the wave envelope, propagates. (= signal velocity) Here, phase velocity = group velocity (the medium is nondispersive)

Group velocity

Dispersion: phase/group velocity depends on frequency Black dot moves at phase velocity. Red dot moves at group velocity. This is normal dispersion (refractive index decreases with increasing λ)

Rectangular Waveguide Need to find the fields components of the em wave inside the waveguide E z H z E x H x E y H y We ll find that waveguides don t support TEM waves

The m and n represent the mode of propagation and indicates the number of variations of the field in the x and y directions Note that for the TM mode, if n or m is zero, all fields are zero.

Variation of wave impedance Wave impedance varies with frequency and mode

Rectangular Waveguide - Wave Propagation

Wave Guide Impedance Wave feature impedance for TE mode is ZTE = with; 377 1 0 ZTE = characteristic impedance for TE mode 377 = free space feature impedance = free space wavelength 0 = wavelength cut. 2

Wave Guide Impedance Wave feature impedance for TM mode is ZTM = 377 1 ( 0 ) 2 where; ZTM = characteristic impedance for TM mode 377 = free space feature impedance = free space wavelength 0 = wavelength cut.

Question Waveguide

The circular waveguide is used in many special applications in microwave techniques. It has the advantage of greater power handling capacity and lower attenuation for a given cutoff wavelength. However, the disadvantage of somewhat greater size and weight. The polarization of the transmitted wave can be altered due to the minor irregularities of the wall surface of the circular guide, whereas the rectangular wave guide the polarization is fixed

Description The wave of lowest frequency or the dominant mode in the circular waveguide is the TE 11 mode. The first subscript m indicates the number of full wave variations of the radial component of the electric field around the circumference of the waveguide. The second subscript n indicates the number of half wave variations across the diameter. The field configurations of TE 11 mode in the circular waveguide is shown in the diagram below

Applications of circular waveguide Rotating joints in radars to connect the horn antenna feeding a parabolic reflector (which must rotate for tracking) TE 01 mode suitable for long distance waveguide transmission above 10 GHz. Short and medium distance broad band communication (could replace / share coaxial and microwave links)

From the cutoff frequencies or the cutoff wavelengths, the phase velocity, the group velocity, the guide wavelength and the wave impedance of each mode can be found using the same equations as those for the rectangular waveguide.

Cut Off Wavelength

Example 1

Example 2

Solution