Unit V Microwave Antennas and Measurements
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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 = . -
Department of Electronics and Communication Engineering EC8651 – Transmission Line and Waveguide Unit III - MCQ Bank 1
ChettinadTech Dept of ECE Department of Electronics and Communication Engineering EC8651 – Transmission Line and Waveguide Unit III - MCQ Bank 1. Slotted line is a transmission line configuration that allows the sampling of a) electric field amplitude of a standing wave on a terminated line b) magnetic field amplitude of a standing wave on a terminated line c) voltage used for excitation d) current that is generated by the source Answer: a Explanation: Slotted line allows the sampling of the electric field amplitude of a standing wave on a terminated line. With this device, SWR and the distance of the first voltage minimum from the load can be measured, from this data, load impedance can be found. 2. A slotted line can be used to measure _____ and the distance of _____________ from the load. a) SWR, first voltage minimum b) SWR, first voltage maximum c) characteristic impedance, first voltage minimum d) characteristic impedance, first voltage maximum Answer: a Explanation: With a slotted line, SWR and the distance of the first voltage minimum from the load can be measured, from this data, load impedance can be found. Page 1 EC8651– Transmission Line and Waveguide ChettinadTech Dept of ECE 3. A modern device that replaces a slotted line is: a) Digital CRO b) generators c) network analyzers d) computers Answer: c Explanation: Although slotted lines used to be the principal way of measuring unknown impedance at microwave frequencies, they have largely been superseded by the modern network analyzer in terms of accuracy, versatility and convenience. 4. If the standing wave ratio for a transmission line is 1.4, then the reflection coefficient for the line is: a) 0.16667 b) 1.6667 c) 0.01667 d) 0.96 Answer: a Explanation: ┌= (SWR-1)/ (SWR+1). -
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). -
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. -
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. -
EECS 117A Demonstration 2 Microwave Measurement Instruments
University of California, Berkeley Spring 2007 EECS 117 Prof. A. Niknejad EECS 117A Demonstration 2 Microwave Measurement Instruments NAME Introduction. Please review the general sinusoidal wave concepts in Secs. 3.1–3.9 of Inan & Inan. Note carefully Section 3.3. In this demonstration you will learn how to use a “50 ohm” slotted line, crystal detector, and standing wave ratio meter to obtain the wavelength λ and voltage standing wave ratio S on a coaxial transmission line. In a later demonstration you will use these techniques to measure and control impedances and reflection coefficients on a microwave transmission system. The apparatus used is shown below. The slotted line is a (rigid) continuation of the coaxial transmission lines “a” connected at each end. 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, and can also be moved into and out of the slot by means of a micrometer. The probe is connected to a crystal (diode) detector that converts the time-varying microwave voltage to dc. The dc voltage is measured using the standing wave ratio (SWR) meter. MICROMETER HP 415D b SWR METER DETECTOR TUNER HP 612 A UHF SIGNAL a TERMINATION GENERATOR a GR SLOTTED LINE POINT (LOAD) Z = 0 Z Suppose a sinusoidal voltage wave j(ωt−βz) v+(t) = Re hV+ e i (1) travels from the RF generator through the slotted line and is incident on a load (resistor, capacitor etc.) at z = 0. -
SCALAR NETWORK ANALYSIS: an ATTRACTIVE and Cosl-EFFECTIVE TECHNIQUE for TESTING MICROWAVE COMPONENTS
SCALAR NETWORK ANALYSIS: AN ATTRACTIVE AND COSl-EFFECTIVE TECHNIQUE FOR TESTING MICROWAVE COMPONENTS Hugo Vitian Network Measurements Division 1400 Fountain Grove Parkway Santa Rosa, CA 95401 RF ~ Microwave Measurement Symposium and Exhibition Flio- HEWLETT ~~ PACKARD www.HPARCHIVE.com Scalar Network Analysis: an Attractive and Cost-Effective Technique for Testing Microwave Components ABSTRACT Scalar network characterization is an economic alternative to vector network analysis; in particular, in a productive environment where ease-of-use, throughput and low cost are key considerations. However, scalar measurements are not restricted to frequency response measurements on linear networks. Scalar network analyzers are very powerful analysis tools to characterize amplifiers, mixers, modulators, and other components as a function of signal level or control parameter, as well as for cable testing in frequency- and distance-domains. This presentation describes the fundamental measurement concepts and discusses some specific examples. Author: Hugo Vifian, Engineering Section Manager for economy vector network analyzers, HP Network Measurements Division, Santa Rosa, CA. Diplom-Ingenieur and PhD from Swiss Federal Institute of Technology, (ETH). With HP since 1969, projects include HP 8755 frequency response test set, HP 8505 RF vector network analyzer, HP 8756 and 8757 scalar network analyzers. 2 www.HPARCHIVE.com INTRODUCTION TO SCALAR NETWORK MEASUREMENTS Introduction: Even though scalar microwave measurements have been made ever since high frequencies were discovered, they were not really addressed, as such, but INTRODUCTION TO SCALAR rather called power measurements or NETWORK MEASUREMENTS VSWR measurements, etc. It was not until modern network analysis with vector error correction was intro duced that the rather obvious term magnitude or scalar measurements became more popular. -
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 Calibration Free Vector Network Analyzer
Scholars' Mine Masters Theses Student Theses and Dissertations Summer 2013 A calibration free vector network analyzer Arpit Kothari Follow this and additional works at: https://scholarsmine.mst.edu/masters_theses Part of the Electrical and Computer Engineering Commons Department: Recommended Citation Kothari, Arpit, "A calibration free vector network analyzer" (2013). Masters Theses. 7125. https://scholarsmine.mst.edu/masters_theses/7125 This thesis is brought to you by Scholars' Mine, a service of the Missouri S&T Library and Learning Resources. This work is protected by U. S. Copyright Law. Unauthorized use including reproduction for redistribution requires the permission of the copyright holder. For more information, please contact [email protected]. i A CALIBRATION FREE VECTOR NETWORK ANALYZER by ARPIT KOTHARI A THESIS Presented to the Faculty of the Graduate School of the MISSOURI UNIVERSITY OF SCIENCE AND TECHNOLOGY In Partial Fulfillment of the Requirements for the Degree MASTER OF SCIENCE IN ELECTRICAL ENGINEERING 2013 Approved by Dr. Reza Zoughi, Advisor Dr. Daryl Beetner Dr. David Pommerenke ii 2013 Arpit Kothari All Rights Reserved iii ABSTRACT Recently, two novel single-port, phase-shifter based vector network analyzer (VNA) systems were developed and tested at X-band (8.2 - 12.4 GHz) and Ka-band (26.4 – 40 GHz), respectively. These systems operate based on electronically moving the standing wave pattern, set up in a waveguide, over a Schottky detector and sample the standing wave voltage for several phase shift values. Once this system is fully characterized, all parameters in the system become known and hence theoretically, no other correction (or calibration) should be required to obtain the reflection coefficient, (Γ), of an unknown load. -
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.