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ECE 5011: Antennas
ECE 5011: Antennas Course Description Electromagnetic radiation; fundamental antenna parameters; dipole, loops, patches, broadband and other antennas; array theory; ground plane effects; horn and reflector antennas; pattern synthesis; antenna measurements. Prior Course Number: ECE 711 Transcript Abbreviation: Antennas Grading Plan: Letter Grade Course Deliveries: Classroom Course Levels: Undergrad, Graduate Student Ranks: Junior, Senior, Masters, Doctoral Course Offerings: Spring Flex Scheduled Course: Never Course Frequency: Every Year Course Length: 14 Week Credits: 3.0 Repeatable: No Time Distribution: 3.0 hr Lec Expected out-of-class hours per week: 6.0 Graded Component: Lecture Credit by Examination: No Admission Condition: No Off Campus: Never Campus Locations: Columbus Prerequisites and Co-requisites: Prereq: 3010 (312), or Grad standing in Engineering, Biological Sciences, or Math and Physical Sciences. Exclusions: Not open to students with credit for 711. Cross-Listings: Course Rationale: Existing course. The course is required for this unit's degrees, majors, and/or minors: No The course is a GEC: No The course is an elective (for this or other units) or is a service course for other units: Yes Subject/CIP Code: 14.1001 Subsidy Level: Doctoral Course Programs Abbreviation Description CpE Computer Engineering EE Electrical Engineering Course Goals Teach students basic antenna parameters, including radiation resistance, input impedance, gain and directivity Expose students to antenna radiation properties, propagation (Friis transmission -
The Bruene Directional Coupler and Transmission Lines Abstract
Bruene Coupler and Transmission lines. Version 1.3 October 18, 2009 1 The Bruene Directional Coupler and Transmission Lines Gary Bold, ZL1AN. [email protected] Abstract The Bruene directional coupler indicates \forward" and “reflected” power. Its operation is invariably explained using transmission line concepts, which leads some to wrongly believe that it must always be connected directly to a line. There are also many misconceptions about what happens on a transmission line, and in particular, what happens at the source end. This document addresses these misconceptions. Unfortunately, many derivations require complex exponential notation, phasor representations of voltage and current, and network theorems. There isn't any alternative if rigor is to be maintained. Section 1 gives some background on the Bruene coupler. Section 2 explains its operation when terminated in a resistance. Section 3 works a simple numerical example on a matched transmission line and load. Section 3 repeats this calculation for a mismatched line and load. Section 4 explains the correct interpretation of the powers read by the Bruene meter. Section 5 explains that a mismatched source always generates additional reflections, and shows how the steady-state waves on the line build up by summing these reflections. Section 6 develops the theory of section 6 further, and shows how the ¯nal waves build up in the mismatched line example given in section 4. Five appendices follow: Appendix A develops the general theory of line reflection where both source and load are mismatched, and the line may be lossy. Appendix B works a simple example to illustrate appendix A. -
25. Antennas II
25. Antennas II Radiation patterns Beyond the Hertzian dipole - superposition Directivity and antenna gain More complicated antennas Impedance matching Reminder: Hertzian dipole The Hertzian dipole is a linear d << antenna which is much shorter than the free-space wavelength: V(t) Far field: jk0 r j t 00Id e ˆ Er,, t j sin 4 r Radiation resistance: 2 d 2 RZ rad 3 0 2 where Z 000 377 is the impedance of free space. R Radiation efficiency: rad (typically is small because d << ) RRrad Ohmic Radiation patterns Antennas do not radiate power equally in all directions. For a linear dipole, no power is radiated along the antenna’s axis ( = 0). 222 2 I 00Idsin 0 ˆ 330 30 Sr, 22 32 cr 0 300 60 We’ve seen this picture before… 270 90 Such polar plots of far-field power vs. angle 240 120 210 150 are known as ‘radiation patterns’. 180 Note that this picture is only a 2D slice of a 3D pattern. E-plane pattern: the 2D slice displaying the plane which contains the electric field vectors. H-plane pattern: the 2D slice displaying the plane which contains the magnetic field vectors. Radiation patterns – Hertzian dipole z y E-plane radiation pattern y x 3D cutaway view H-plane radiation pattern Beyond the Hertzian dipole: longer antennas All of the results we’ve derived so far apply only in the situation where the antenna is short, i.e., d << . That assumption allowed us to say that the current in the antenna was independent of position along the antenna, depending only on time: I(t) = I0 cos(t) no z dependence! For longer antennas, this is no longer true. -
Nested Loop Antennas This Low-Cost Five Band Loop Array Blends Into the Background
Nested Loop Antennas This low-cost five band loop array blends into the background. G. Scott Davis, N3FJP This multi-band nested loop antenna array replaces my tribander Yagi, which is only up 20 feet. Inspired by suggestions from Bill Wisel, K3KEI, I first tried a full wave 20 meter band square loop antenna. On the air comparisons with my low Yagi confirmed instantly that this design was a hands-down winner for working both local and distant stations. I replaced that mono-band loop with a nested loop array for the 20, 17, 15, 12, and 10 meter bands. The antenna blends into the surroundings, so I needed the morning sun shining directly on it to snap the lead photo. This became a nice father-son project with my son Brad, KB3MNE. Here’s how we built the antenna. Construction We constructed the square loops shown in Figure 1 according to the dimensions in Table 1. The loops hang from a tree limb in the vertical plane. Because I feed them This stealthy nested loop is almost invisible among the trees. from the bottom corners, the loops radiate horizontal polarization. Calculate the perimeter size, P, of each holes through the pipe for the loop wire. screws into the PVC to hang the dipole loop by dividing the frequency in MHz After you run the wire through the holes, connectors seen in Figure 2. wrap a bit of electrical tape on each side of into 1005 feet. Table 1 shows the loop Matching and Feeding dimensions. Start with the 20 meter loop, the wire next to the pipe to keep the wire from sliding and to give the pipe additional Each loop antenna feed point impedance is the largest loop. -
Evaluation of Short-Term Exposure to 2.4 Ghz Radiofrequency Radiation
GMJ.2020;9:e1580 www.gmj.ir Received 2019-04-24 Revised 2019-07-14 Accepted 2019-08-06 Evaluation of Short-Term Exposure to 2.4 GHz Radiofrequency Radiation Emitted from Wi-Fi Routers on the Antimicrobial Susceptibility of Pseudomonas aeruginosa and Staphylococcus aureus Samad Amani 1, Mohammad Taheri 2, Mohammad Mehdi Movahedi 3, 4, Mohammad Mohebi 5, Fatemeh Nouri 6 , Alireza Mehdizadeh3 1 Shiraz University of Medical Sciences, Shiraz, Iran 2 Department of Medical Microbiology, Faculty of Medicine, Hamadan University of Medical Sciences, Hamadan, Iran 3 Department of Medical Physics and Medical Engineering, School of Medicine, Shiraz University of Medical Sciences, Shiraz, Iran 4 Ionizing and Non-ionizing Radiation Protection Research Center (INIRPRC), Shiraz University of Medical Sciences, Shiraz, Iran 5 School of Medicine, Shiraz University of Medical Sciences, Shiraz, Iran 6 Department of Pharmaceutical Biotechnology, School of Pharmacy, Hamadan University of Medical Sciences, Hamadan, Iran Abstract Background: Overuse of antibiotics is a cause of bacterial resistance. It is known that electro- magnetic waves emitted from electrical devices can cause changes in biological systems. This study aimed at evaluating the effects of short-term exposure to electromagnetic fields emitted from common Wi-Fi routers on changes in antibiotic sensitivity to opportunistic pathogenic bacteria. Materials and Methods: Standard strains of bacteria were prepared in this study. An- tibiotic susceptibility test, based on the Kirby-Bauer disk diffusion method, was carried out in Mueller-Hinton agar plates. Two different antibiotic susceptibility tests for Staphylococcus au- reus and Pseudomonas aeruginosa were conducted after exposure to 2.4-GHz radiofrequency radiation. The control group was not exposed to radiation. -
A Guide for Radio Operators BROCHURE RADIO TRANSM ANG 3/27/97 8:47 PM Page 2
BROCHURE RADIO TRANSM ANG 3/27/97 8:47 PM Page 17 A Guide for Radio Operators BROCHURE RADIO TRANSM ANG 3/27/97 8:47 PM Page 2 Aussi disponible en français. 32-EN-95539W-01 © Minister of Public Works and Government Services Canada 1996 BROCHURE RADIO TRANSM ANG 3/27/97 8:47 PM Page 3 CUTTING THROUGH... INTERFERENCE FROM RADIO TRANSMITTERS A Guide for Radio Operators This brochure is primarily for amateur and General Radio Service (GRS, commonly known as CB) radio operators. It provides basic information to help you install and maintain your station so you get the best performance and the most enjoyment from it. You will learn how to identify the causes of radio interference in nearby electronic equipment, and how to fix the problem. What type of equipment can be affected by radio interference? Both radio and non-radio devices can be adversely affected by radio signals. Radio devices include AM and FM radios, televisions, cordless telephones and wireless intercoms. Non-radio electronic equipment includes stereo audio systems, wired telephones and regular wired intercoms. All of this equipment can be disturbed by radio signals. What can cause radio interference? Interference usually occurs when radio transmitters and electronic equipment are operated within close range of each other. Interference is caused by: ■ incorrectly installed radio transmitting equipment; ■ an intense radio signal from a nearby transmitter; ■ unwanted signals (called spurious radiation) generated by the transmitting equipment; and ■ not enough shielding or filtering in the electronic equipment to prevent it from picking up unwanted signals. What can you do? 1. -
Class C Pool of Questions
Class C Pool of Questions T2 1. What is the most common repeater frequency offset in the 2 meter band? T2 2. What is the national calling frequency for FM simplex operations in the 70 cm band? T2 3. What is a common repeater frequency offset in the 70 cm band? T2 4. What is an appropriate way to call another station on a repeater if you know the other station's call sign? T2 5. How should you respond to a station calling CQ? T2 6. What must an amateur operator do when making on-air transmissions to test equipment or antennas? T2 7. Which of the following is true when making a test transmission? T2 8. What is the meaning of the procedural signal “CQ”? T2 9. What brief statement is often transmitted in place of “CQ” to indicate that you are listening on a repeater? T2 10. What is a band plan, beyond the privileges established by the SMA? T2 11. Which of the following is an SMA rule regarding power levels used in the amateur bands, under normal, non-distress circumstances? T2 12. Which of the following is a guideline to use when choosing an operating frequency for calling CQ? T2B – VHF/UHF operating practices: SSB phone; FM repeater; simplex; splits and shifts; CTCSS; DTMF; tone squelch; carrier squelch; phonetics; operational problem resolution; Q signals T2 1. What is the term used to describe an amateur station that is transmitting and receiving on the same frequency? T2 2. What is the term used to describe the use of a sub-audible tone transmitted with normal voice audio to open the squelch of a receiver? T2 3. -
Compact Integrated Antennas Designs and Applications for the Mc1321x, Mc1322x, and Mc1323x
Freescale Semiconductor Document Number: AN2731 Application Note Rev. 2, 12/2012 Compact Integrated Antennas Designs and Applications for the MC1321x, MC1322x, and MC1323x 1 Introduction Contents 1 Introduction . 1 With the introduction of many applications into the 2 Antenna Terms . 2 2.4 GHz band for commercial and consumer use, 3 Basic Antenna Theory . 3 Antenna design has become a stumbling point for many 4 Impedance Matching . 5 customers. Moving energy across a substrate by use of an 5 Antennas . 8 RF signal is very different than moving a low frequency 6 Miniaturization Trade-offs . 11 voltage across the same substrate. Therefore, designers 7 Potential Issues . 12 who lack RF expertise can avoid pitfalls by simply 8 Recommended Antenna Designs . 13 following “good” RF practices when doing a board 9 Design Examples . 14 layout for 802.15.4 applications. The design and layout of antennas is an extension of that practice. This application note will provide some of that basic insight on board layout and antenna design to improve our customers’ first pass success. Antenna design is a function of frequency, application, board area, range, and costs. Whether your application requires the absolute minimum costs or minimization of board area or maximum range, it is important to understand the critical parameters so that the proper trade-offs can be chosen. Some of the parameters necessary in selecting the correct antenna are: antenna © Freescale Semiconductor, Inc., 2005, 2006, 2012. All rights reserved. tuning, matching, gain/loss, and required radiation pattern. This note is not an exhaustive inquiry into antenna design. It is instead, focused toward helping our customers understand enough board layout and antenna basics to aid in selecting the correct antenna type for their application as well as avoiding the typical layout mistakes that cause performance issues that lead to delays. -
Broadband Antenna 1
Broadband Antenna Broadband Antenna Chapter 4 1 Broadband Antenna Learning Outcome • At the end of this chapter student should able to: – To design and evaluate various antenna to meet application requirements for • Loops antenna • Helix antenna • Yagi Uda antenna 2 Broadband Antenna What is broadband antenna? • The advent of broadband system in wireless communication area has demanded the design of antennas that must operate effectively over a wide range of frequencies. • An antenna with wide bandwidth is referred to as a broadband antenna. • But the question is, wide bandwidth mean how much bandwidth? The term "broadband" is a relative measure of bandwidth and varies with the circumstances. 3 Broadband Antenna Bandwidth Bandwidth is computed in two ways: • (1) (4.1) where fu and fl are the upper and lower frequencies of operation for which satisfactory performance is obtained. fc is the center frequency. • (2) (4.2) Note: The bandwidth of narrow band antenna is usually expressed as a percentage using equation (4.1), whereas wideband antenna are quoted as a ratio using equation (4.2). 4 Broadband Antenna Broadband Antenna • The definition of a broadband antenna is somewhat arbitrary and depends on the particular antenna. • If the impendence and pattern of an antenna do not change significantly over about an octave ( fu / fl =2) or more, it will classified as a broadband antenna". • In this chapter we will focus on – Loops antenna – Helix antenna – Yagi uda antenna – Log periodic antenna* 5 Broadband Antenna LOOP ANTENNA 6 Broadband Antenna Loops Antenna • Another simple, inexpensive, and very versatile antenna type is the loop antenna. -
Performance Expectations for Reduced-Size Antennas
High Frequency Design From February 2010 High Frequency Electronics Copyright © 2010 Summit Technical Media, LLC SMALL ANTENNAS Performance Expectations for Reduced-Size Antennas By Gary Breed Editorial Director λ very device that L/ = 0.167 and RRad = 5.5 ohms. The feed- This month’s tutorial article transmits and/or point impedance will be 5.5 –jX, where X is a presents a summary of Ereceives radio sig- large capacitance, as high as 1500 ohms in the the advantages and limita- nals needs an antenna. case of thin dipole. This 5.5 –j1500 ohm tions of electrically-small When that device has a impedance must be matched to the system antennas like those used in small size or limited impedance, typically 50 ohms. many wireless devices space for a classic reso- Small loops and monopoles have similarly nant antenna, various low radiation resistance with high reactance. techniques are used to implement reduced- Matching to highly reactive loads is inherent- size antennas. Those techniques may include ly narrow bandwidth, since the magnitude of inductive or capacitive loading, meandered or the reactance changes rapidly with frequency. spiral construction, high dielectric constant Achieving a broader bandwidth match materials to slow down wave propagation, and requires either complex networks or the intro- embedded structures incorporated into the duction of lossy components. packaging. Each of these methods imposes The use of meandered lines, spirals, fractal some type of limitation when compared to patterns effectively distribute the required monopole, dipole, or resonant loop antennas. inductance over the length of the antenna, This tutorial looks at the key limitations of and can result in higher radiation resistance small antennas, with the intention of illus- and lower loss matching networks. -
Radio and Electronics Cookbook
Radio and Electronics Cookbook Radio and Electronics Cookbook Edited by Dr George Brown, CEng, FIEE, M5ACN OXFORD AUCKLAND BOSTON JOHANNESBURG MELBOURNE NEW DELHI Newnes An imprint of Butterworth-Heinemann Linacre House, Jordan Hill, Oxford OX2 8DP 225 Wildwood Avenue, Woburn, MA 01801-2041 A division of Reed Educational and Professional Publishing Ltd A member of the Reed Elsevier plc group First published 2001 © Radio Society of Great Britain 2001 All rights reserved. No part of this publication may be reproduced in any material form (including photocopying or storing in any medium by electronic means and whether or not transiently or incidentally to some other use of this publication) without the written permission of the copyright holder except in accordance with the provisions of the Copyright, Designs and Patents Act 1988 or under the terms of a licence issued by the Copyright Licensing Agency Ltd, 90 Tottenham Court Road, London, England W1P 0LP. Applications for the copyright holder’s written permission to reproduce any part of this publication should be addressed to the publishers British Library Cataloguing in Publication Data A catalogue record for this book is available from the British Library ISBN 0 7506 5214 4 RSGB Lambda House Cranborne Road Potters Bar Herts EN6 3JE Composition by Genesis Typesetting, Laser Quay, Rochester, Kent Printed and bound in Great Britain Contents Preface ix 1. A medium-wave receiver 1 2. An audio-frequency amplifier 4 3. A medium-wave receiver using a ferrite-rod aerial 9 4. A simple electronic organ 12 5. Experiments with the NE555 timer 17 6. -
An Easy Dual-Band VHF/UHF Antenna
An Easv Dual-Band VHFIUHF Antenna Why settle for the performance your rubber duck offers? Build this portable J-pole and boost your signal for next to nothing! You've just opened the box that contains Don't let the veloci9 facfor throw you. 2952 V your new H-T and you're eager to get on L~t4 f The concept is easy to understand. Put the air. But the rubber duck antenna simply, the time required for a signal to that came with your radio is not working where: traveI down a length of wire is longer than well. Sometimes you can't reach the local b4= the length of the 3/4-wavelength the time required for the same signal to repeater. And even when you can, your radiator in inches travel the same distance in free space. This buddies tell you that your signal is noisy. L,, = the length of the l/d-waveleng& delay-the velocity factor-is expressed If you have 20 mhutes to spare, why not stub in inches in terms of the speed of light, either as a buiId a Iow-cost J-pok antemathat's guar- V = the velocity factor of the TV percentage or a decimal fraction. Knowing anteed to oGtperform yourrubber duck?My twin lead the velocity factor is important when design is a dual-band J-pole. If you own a f = the design frequency in MHz you're building antennas and working with 2-meterno-cm B-Ti this antenna will im- Tbese equations are more straight- prove your signal on both bands.