Back to the Basics Setting up a VHF/UHF Station Back to the Basics Your First VHF/UHF Station Topics That Will Be Covered: Lradios Lbase/Mobile Vs
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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. -
Simulation and Measurements of VSWR for Microwave Communication Systems
Int. J. Communications, Network and System Sciences, 2012, 5, 767-773 http://dx.doi.org/10.4236/ijcns.2012.511080 Published Online November 2012 (http://www.SciRP.org/journal/ijcns) Simulation and Measurements of VSWR for Microwave Communication Systems Bexhet Kamo, Shkelzen Cakaj, Vladi Koliçi, Erida Mulla Faculty of Information Technology, Polytechnic University of Tirana, Tirana, Albania Email: [email protected], [email protected], [email protected], [email protected] Received September 5, 2012; revised October 11, 2012; accepted October 18, 2012 ABSTRACT Nowadays, microwave frequency systems, in many applications are used. Regardless of the application, all microwave communication systems are faced with transmission line matching problem, related to the load or impedance connected to them. The mismatching of microwave lines with the load connected to them generates reflected waves. Mismatching is identified by a parameter known as VSWR (Voltage Standing Wave Ratio). VSWR is a crucial parameter on deter- mining the efficiency of microwave systems. In medical application VSWR gets a specific importance. The presence of reflected waves can lead to the wrong measurement information, consequently a wrong diagnostic result interpretation applied to a specific patient. For this reason, specifically in medical applications, it is important to minimize the re- flected waves, or control the VSWR value with the high accuracy level. In this paper, the transmission line under dif- ferent matching conditions is simulated and experimented. Through simulation and experimental measurements, the VSWR for each case of connected line with the respective load is calculated and measured. Further elements either with impact or not on the VSWR value are identified. -
Ant-433-Heth
ANT-433-HETH Data Sheet by Product Description HE Series antennas are designed for direct PCB Outside 8.89 mm mounting. Thanks to the HE’s compact size, they Diameter (0.35") are ideal for internal concealment inside a product’s housing. The HE is also very low in cost, making it well suited to high-volume applications. HE Series Inside 6.4 mm Diameter (0.25") antennas have a very narrow bandwidth; thus, care in placement and layout is required. In addition, they are not as efficient as whip-style antennas, so they are generally better suited for use on the transmitter end where attenuation is often required Wire 15.24 mm Diameter (0.60") anyway for regulatory compliance. Use on both 1.3 mm 6.35 mm transmitter and receiver ends is recommended only (0.05") (0.25") in instances where a short range (less than 30% of whip style) is acceptable. 38.1 mm (1.50") Features • Very low cost • Compact for physical concealment Recommended Mounting • Precision-wound coil No ground plane or traces No electircal • Rugged phosphor-bronze construction under the antenna connection on this • Mounts directly to the PCB pad. For physical 38.10 mm support only. (1.50") Electrical Specifications 1.52 mm Center Frequency: 433MHz 7.62 mm (Ø0.060") Recom. Freq. Range: 418–458MHz (0.30") 3.81 mm Wavelength: ¼-wave 12.70 mm (0.50") (0.15") VSWR: ≤ 2.0 typical at center Peak Gain: 1.9dBi Impedance: 50-ohms Connection: Through-hole Oper. Temp. Range: –40°C to +80°C Electrical specifications and plots measured on a 7.62 x 19.05 Ground plane on cm (3.00" x 7.50") reference ground plane 50-ohm microstrip line bottom layer for counterpoise Ordering Information ANT-433-HETH (helical, through-hole) – 1 – Revised 5/16/16 Counterpoise Quarter-wave or monopole antennas require an associated ground plane counterpoise for proper operation. -
Slotted Line-SWR
Lab 2: Slotted Line and SWR Meter NAME NAME NAME Introduction: In this lab you will learn how to characterize and use a 50-ohm slotted line, crystal detector, and standing wave ratio (SWR) meter to measure an unknown impedance. The apparatus used is shown below. The slotted line is a (rigid) continuation of the coaxial transmission lines. Its characteristic impedance is 50 ohms. It has a thin slot in its outer conductor, cut along z. A probe rides within (but not touching) the slot to sample the transmission line voltage. The probe can be moved along z to sample the standing wave ratio at different locations. It can also be moved into and out of the slot by means of a micrometer in order to adjust the signal strength. The probe is connected to a crystal (diode) detector that converts the time-varying microwave voltage to a DC value with the help of a low speed modulation envelope (1 kHz) on the microwave signal. The DC voltage is measured using the SWR meter (HP 415D). 1 Using Slotted Line to Measure an Unknown Impedance: The magnitude of the line voltage as a function of position is: + −2 jβ l + j(θ −2β l ) jθ V ()z = V0 1− Γe = V0 1+ Γ e with Γ = Γ e and l the distance from the load towards the generator. Notice that the voltage magnitude has maxima and minima at different locations. + Vmax = V0 (1+ Γ ) when θ − 2β l = π + Vmin = V0 (1− Γ ) when θ − 2β l = 0 V 1+ Γ The SWR is defined as: SWR = max = . -
Voltage Standing Wave Ratio Measurement and Prediction
International Journal of Physical Sciences Vol. 4 (11), pp. 651-656, November, 2009 Available online at http://www.academicjournals.org/ijps ISSN 1992 - 1950 © 2009 Academic Journals Full Length Research Paper Voltage standing wave ratio measurement and prediction P. O. Otasowie* and E. A. Ogujor Department of Electrical/Electronic Engineering University of Benin, Benin City, Nigeria. Accepted 8 September, 2009 In this work, Voltage Standing Wave Ratio (VSWR) was measured in a Global System for Mobile communication base station (GSM) located in Evbotubu district of Benin City, Edo State, Nigeria. The measurement was carried out with the aid of the Anritsu site master instrument model S332C. This Anritsu site master instrument is capable of determining the voltage standing wave ratio in a transmission line. It was produced by Anritsu company, microwave measurements division 490 Jarvis drive Morgan hill United States of America. This instrument works in the frequency range of 25MHz to 4GHz. The result obtained from this Anritsu site master instrument model S332C shows that the base station have low voltage standing wave ratio meaning that signals were not reflected from the load to the generator. A model equation was developed to predict the VSWR values in the base station. The result of the comparism of the developed and measured values showed a mean deviation of 0.932 which indicates that the model can be used to accurately predict the voltage standing wave ratio in the base station. Key words: Voltage standing wave ratio, GSM base station, impedance matching, losses, reflection coefficient. INTRODUCTION Justification for the work amplitude in a transmission line is called the Voltage Standing Wave Ratio (VSWR). -
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. -
Ec6503 - Transmission Lines and Waveguides Transmission Lines and Waveguides Unit I - Transmission Line Theory 1
EC6503 - TRANSMISSION LINES AND WAVEGUIDES TRANSMISSION LINES AND WAVEGUIDES UNIT I - TRANSMISSION LINE THEORY 1. Define – Characteristic Impedance [M/J–2006, N/D–2006] Characteristic impedance is defined as the impedance of a transmission line measured at the sending end. It is given by 푍 푍0 = √ ⁄푌 where Z = R + jωL is the series impedance Y = G + jωC is the shunt admittance 2. State the line parameters of a transmission line. The line parameters of a transmission line are resistance, inductance, capacitance and conductance. Resistance (R) is defined as the loop resistance per unit length of the transmission line. Its unit is ohms/km. Inductance (L) is defined as the loop inductance per unit length of the transmission line. Its unit is Henries/km. Capacitance (C) is defined as the shunt capacitance per unit length between the two transmission lines. Its unit is Farad/km. Conductance (G) is defined as the shunt conductance per unit length between the two transmission lines. Its unit is mhos/km. 3. What are the secondary constants of a line? The secondary constants of a line are 푍 i. Characteristic impedance, 푍0 = √ ⁄푌 ii. Propagation constant, γ = α + jβ 4. Why the line parameters are called distributed elements? The line parameters R, L, C and G are distributed over the entire length of the transmission line. Hence they are called distributed parameters. They are also called primary constants. The infinite line, wavelength, velocity, propagation & Distortion line, the telephone cable 5. What is an infinite line? [M/J–2012, A/M–2004] An infinite line is a line where length is infinite. -
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. -
Unit V Microwave Antennas and Measurements
UNIT V MICROWAVE ANTENNAS AND MEASUREMENTS Horn antenna and its types, micro strip and patch antennas. Network Analyzer, Measurement of VSWR, Frequency and Power, Noise, cavity Q, Impedance, Attenuation, Dielectric Constant and antenna gain. ------------------------------------------------------------------------------------------------------------------------------- DEFINITION: A conductor or group of conductors used either for radiating electromagnetic energy into space or for collecting it from space.or Is a structure which may be described as a metallic object, often a wire or a collection of wires through specific design capable of converting high frequency current into em wave and transmit it into free space at light velocity with high power (kW) besides receiving em wave from free space and convert it into high frequency current at much lower power (mW). Also known as transducer because it acts as coupling devices between microwave circuits and free space and vice versa. Electrical energy from the transmitter is converted into electromagnetic energy by the antenna and radiated into space. On the receiving end, electromagnetic energy is converted into electrical energy by the antenna and fed into the receiver. Basic operation of transmit and receive antennas. Transmission - radiates electromagnetic energy into space Reception - collects electromagnetic energy from space In two-way communication, the same antenna can be used for transmission and reception. Short wavelength produced by high frequency microwave, allows the usage -
Microwave Impedance Measurements and Standards
NBS MONOGRAPH 82 MICROWAVE IMPEDANCE MEASUREMENTS AND STANDARDS . .5, Y 1 p p R r ' \ Jm*"-^ CCD 'i . y. s. U,BO»WOM t «• U.S. DEPARTMENT OF STANDARDS NATIONAL BUREAU OF STANDARDS THE NATIONAL BUREAU OF STANDARDS The National Bureau of Standards is a principal focal point in the Federal Government for assuring maximum application of the physical and engineering sciences to the advancement of technology in industry and commerce. Its responsibilities include development and main- tenance of the national standards of measurement, and the provisions of means for making measurements consistent with those standards; determination of physical constants and properties of materials; development of methods for testing materials, mechanisms, and struc- tures, and making such tests as may be necessary, particularly for government agencies; cooperation in the establishment of standard practices for incorporation in codes and specifications; advisory service to government agencies on scientific and technical problems; invention and development of devices to serve special needs of the Government; assistance to industry, business, and consumers in the development and acceptance of commercial standards and simplified trade practice recommendations; administration of programs in cooperation with United States business groups and standards organizations for the development of international standards of practice; and maintenance of a clearinghouse for the collection and dissemination of scientific, technical, and engineering information. The scope of the Bureau's activities is suggested in the following listing of its four Institutes and their organizational units. Institute for Basic Standards. Applied Mathematics. Electricity. Metrology. Mechanics. Heat. Atomic Physics. Physical Chem- istry. Laboratory Astrophysics.* Radiation Physics. Radio Stand- ards Laboratory:* Radio Standards Physics; Radio Standards Engineering. -
A Modern Directional Power/SWR Meter Every Ham Needs an RF Power Meter
A Modern Directional Power/SWR Meter Every ham needs an RF power meter. Here’s a high performance unit to build at home. Bill Kaune, W7IEQ first got the idea of designing and build- ing a power meter from a construction I article in The 1997 ARRL Handbook entitled “The Tandem Match — An Transceiver Directional Coupler Tuner Accurate Directional Wattmeter” by John 7:,13%7 32:(5 TRANSMITTER ANTENNA $17 86% INDUCTANCE 0 7 3 ANTENNA Grebenkemper, KI6WX. John described the SELECTION *(1( 9)2$ 3+21(6 &+ 92; %.,1 3$03 $*& 63/,7 15 7; 5; 021, ) 1% $1) /2&. 6&3 67(3 POWER difficulties of building an accurate power N 0,& ) ) ) ) ) METER meter using diodes to convert RF to dc because of the diode’s inherent nonlinearity. He describes a fairly complicated (at least it looked complicated to me) analog circuit that corrects for this nonlinear behavior and Reflected Power Forward Power that also calculates and displays SWR. Shortly after reading this article, I noticed 3(3: 6:5 several articles in QST that described a new $9*: Power Meter integrated circuit, the Analog Devices AD8307, that converts a low level RF signal QS1101Kaune01 into a voltage proportional to the logarithm of the signal’s power. I became intrigued Figure 1 — W7IEQ station setup, including the power meter being described here. with this device because it eliminated the difficulties associated with the use of diodes and would work over a wide range of pow- RF power flowing from the transmitter to over the two sections of RG-8 until they were 1 ers, from milliwatts to the legal limit. -
Module 2 : Transmission Lines Lecture 6 : Loss Less Transmission Line
Module 2 : Transmission Lines Lecture 6 : Loss Less Transmission Line Objectives In this course you will learn the following What is a loss-less transmission line? Variation of voltage and current on a loss less line. Standing waves on a loss-less line. Voltage standing wave ratio (VSWR) and its relation to the voltage reflection co-efficient. Importance of VSWR and its values for various impedances. Concept of return-loss (RL). Return loss a measure of reflection on the line. Module 2 : Transmission Lines Lecture 6 : Loss Less Transmission Line Analysis of Loss Less Transmission Line In any electrical circuit the power loss is due to ohmic elements. A loss less transmission line therefore implies and . For a loss less transmission line hence we get Propagation constant : That is, and . The charateristic impedance The reflection coefficient at any point on the line is The voltage and current expressions become Let the reflection coefficient at the load end be written in the amplitude and phase form as then we have As we move towards the generator the phase becomes more negative and point P rotates clockwise on the dotted circle. The radius of the circle is . Length of the vector OP gives the magnitude of the quantity Module 2 : Transmission Lines Lecture 6 : Loss Less Transmission Line Spatial Variation of Current & Voltage The previous equations indicate that the amplitudes of the voltage and current vary as a function of distance on the line. Wherever or even multiple of , the quantity in the brackets is maximum in the voltage expression, and minimum in the current expression.