Voltage Standing Wave Ratio Measurement and Prediction
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A Review of Electric Impedance Matching Techniques for Piezoelectric Sensors, Actuators and Transducers
Review A Review of Electric Impedance Matching Techniques for Piezoelectric Sensors, Actuators and Transducers Vivek T. Rathod Department of Electrical and Computer Engineering, Michigan State University, East Lansing, MI 48824, USA; [email protected]; Tel.: +1-517-249-5207 Received: 29 December 2018; Accepted: 29 January 2019; Published: 1 February 2019 Abstract: Any electric transmission lines involving the transfer of power or electric signal requires the matching of electric parameters with the driver, source, cable, or the receiver electronics. Proceeding with the design of electric impedance matching circuit for piezoelectric sensors, actuators, and transducers require careful consideration of the frequencies of operation, transmitter or receiver impedance, power supply or driver impedance and the impedance of the receiver electronics. This paper reviews the techniques available for matching the electric impedance of piezoelectric sensors, actuators, and transducers with their accessories like amplifiers, cables, power supply, receiver electronics and power storage. The techniques related to the design of power supply, preamplifier, cable, matching circuits for electric impedance matching with sensors, actuators, and transducers have been presented. The paper begins with the common tools, models, and material properties used for the design of electric impedance matching. Common analytical and numerical methods used to develop electric impedance matching networks have been reviewed. The role and importance of electrical impedance matching on the overall performance of the transducer system have been emphasized throughout. The paper reviews the common methods and new methods reported for electrical impedance matching for specific applications. The paper concludes with special applications and future perspectives considering the recent advancements in materials and electronics. -
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 = . -
Impedance Matching
Impedance Matching Advanced Energy Industries, Inc. Introduction The plasma industry uses process power over a wide range of frequencies: from DC to several gigahertz. A variety of methods are used to couple the process power into the plasma load, that is, to transform the impedance of the plasma chamber to meet the requirements of the power supply. A plasma can be electrically represented as a diode, a resistor, Table of Contents and a capacitor in parallel, as shown in Figure 1. Transformers 3 Step Up or Step Down? 3 Forward Power, Reflected Power, Load Power 4 Impedance Matching Networks (Tuners) 4 Series Elements 5 Shunt Elements 5 Conversion Between Elements 5 Smith Charts 6 Using Smith Charts 11 Figure 1. Simplified electrical model of plasma ©2020 Advanced Energy Industries, Inc. IMPEDANCE MATCHING Although this is a very simple model, it represents the basic characteristics of a plasma. The diode effects arise from the fact that the electrons can move much faster than the ions (because the electrons are much lighter). The diode effects can cause a lot of harmonics (multiples of the input frequency) to be generated. These effects are dependent on the process and the chamber, and are of secondary concern when designing a matching network. Most AC generators are designed to operate into a 50 Ω load because that is the standard the industry has settled on for measuring and transferring high-frequency electrical power. The function of an impedance matching network, then, is to transform the resistive and capacitive characteristics of the plasma to 50 Ω, thus matching the load impedance to the AC generator’s impedance. -
RF Matching Network Design Guide for STM32WL Series
AN5457 Application note RF matching network design guide for STM32WL Series Introduction The STM32WL Series microcontrollers are sub-GHz transceivers designed for high-efficiency long-range wireless applications including the LoRa®, (G)FSK, (G)MSK and BPSK modulations. This application note details the typical RF matching and filtering application circuit for STM32WL Series devices, especially the methodology applied in order to extract the maximum RF performance with a matching circuit, and how to become compliant with certification standards by applying filtering circuits. This document contains the output impedance value for certain power/frequency combinations, that can result in a different output impedance value to match. The impedances are given for defined frequency and power specifications. AN5457 - Rev 2 - December 2020 www.st.com For further information contact your local STMicroelectronics sales office. AN5457 General information 1 General information This document applies to the STM32WL Series Arm®-based microcontrollers. Note: Arm is a registered trademark of Arm Limited (or its subsidiaries) in the US and/or elsewhere. Table 1. Acronyms Acronym Definition BALUN Balanced to unbalanced circuit BOM Bill of materials BPSK Binary phase-shift keying (G)FSK Gaussian frequency-shift keying modulation (G)MSK Gaussian minimum-shift keying modulation GND Ground (circuit voltage reference) LNA Low-noise power amplifier LoRa Long-range proprietary modulation PA Power amplifier PCB Printed-circuit board PWM Pulse-width modulation RFO Radio-frequency output RFO_HP High-power radio-frequency output RFO_LP Low-power radio-frequency output RFI_N Negative radio-frequency input (referenced to GND) RFI_P Positive radio-frequency input (referenced to GND) Rx Receiver SMD Surface-mounted device SRF Self-resonant frequency SPDT Single-pole double-throw switch SP3T Single-pole triple-throw switch Tx Transmitter RSSI Received signal strength indication NF Noise figure ZOPT Optimal impedance AN5457 - Rev 2 page 2/76 AN5457 General information References [1] T. -
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. -
Reflection Coefficient Analysis of Chebyshev Impedance Matching Network Using Different Algorithms
ISSN: 2319 – 8753 International Journal of Innovative Research in Science, Engineering and Technology Vol. 1, Issue 2, December 2012 Reflection Coefficient Analysis Of Chebyshev Impedance Matching Network Using Different Algorithms Rashmi Khare1, Prof. Rajesh Nema2 Department of Electronics & Communication, NIIST/ R.G.P.V, Bhopal, M.P., India 1 Department of Electronics & Communication, NIIST/ R.G.P.V, Bhopal, M.P., India 2 Abstract: This paper discuss the design and implementation of broadband impedance matching network using chebyshev polynomial. The realization of 4-section impedance matching network using micro-strip lines each section made up of different materials is carried out. This paper discuss the analysis of reflection in 4-section chebyshev impedance matching network for different cases using MATLAB. Keywords: chebyshev polynomial , reflection, micro-strip line, matlab. I. INTRODUCTION In many cases, loads and termination for transmission lines in practical will not have impedance equal to the characteristic impedance of the transmission line. This result in high reflections of wave transverse in the transmission line and correspondingly a high vswr due to standing wave formations, one method to overcome this is to introduce an arrangement of transmission line section or lumped elements between the mismatched transmission line and its termination/loads to eliminate standing wave reflection. This is called as impedance matching. Matching the source and load to the transmission line or waveguide in a general microwave network is necessary to deliver maximum power from the source to the load. In many cases, it is not possible to choose all impedances such that overall matched conditions result. These situations require that matching networks be used to eliminate reflections. -
Coupled Transmission Lines As Impedance Transformer
Downloaded from orbit.dtu.dk on: Sep 25, 2021 Coupled Transmission Lines as Impedance Transformer Jensen, Thomas; Zhurbenko, Vitaliy; Krozer, Viktor; Meincke, Peter Published in: IEEE Transactions on Microwave Theory and Techniques Link to article, DOI: 10.1109/TMTT.2007.909617 Publication date: 2007 Document Version Peer reviewed version Link back to DTU Orbit Citation (APA): Jensen, T., Zhurbenko, V., Krozer, V., & Meincke, P. (2007). Coupled Transmission Lines as Impedance Transformer. IEEE Transactions on Microwave Theory and Techniques, 55(12), 2957-2965. https://doi.org/10.1109/TMTT.2007.909617 General rights Copyright and moral rights for the publications made accessible in the public portal are retained by the authors and/or other copyright owners and it is a condition of accessing publications that users recognise and abide by the legal requirements associated with these rights. Users may download and print one copy of any publication from the public portal for the purpose of private study or research. You may not further distribute the material or use it for any profit-making activity or commercial gain You may freely distribute the URL identifying the publication in the public portal If you believe that this document breaches copyright please contact us providing details, and we will remove access to the work immediately and investigate your claim. 1 Coupled Transmission Lines as Impedance Transformer Thomas Jensen, Vitaliy Zhurbenko, Viktor Krozer, Peter Meincke Technical University of Denmark, Ørsted•DTU, ElectroScience, Ørsteds Plads, Building 348, 2800 Kgs. Lyngby, Denmark, Phone:+45-45253861, Fax: +45-45931634, E-mail: [email protected] Abstract— A theoretical investigation of the use of a coupled line transformer. -
Chapter 25: Impedance Matching
Chapter 25: Impedance Matching Chapter Learning Objectives: After completing this chapter the student will be able to: Determine the input impedance of a transmission line given its length, characteristic impedance, and load impedance. Design a quarter-wave transformer. Use a parallel load to match a load to a line impedance. Design a single-stub tuner. You can watch the video associated with this chapter at the following link: Historical Perspective: Alexander Graham Bell (1847-1922) was a scientist, inventor, engineer, and entrepreneur who is credited with inventing the telephone. Although there is some controversy about who invented it first, Bell was granted the patent, and he founded the Bell Telephone Company, which later became AT&T. Photo credit: https://commons.wikimedia.org/wiki/File:Alexander_Graham_Bell.jpg [Public domain], via Wikimedia Commons. 1 25.1 Transmission Line Impedance In the previous chapter, we analyzed transmission lines terminated in a load impedance. We saw that if the load impedance does not match the characteristic impedance of the transmission line, then there will be reflections on the line. We also saw that the incident wave and the reflected wave combine together to create both a total voltage and total current, and that the ratio between those is the impedance at a particular point along the line. This can be summarized by the following equation: (Equation 25.1) Notice that ZC, the characteristic impedance of the line, provides the ratio between the voltage and current for the incident wave, but the total impedance at each point is the ratio of the total voltage divided by the total current. -
Output Impedance Matching with Fully Differential Operational Amplifiers
Texas Instruments Incorporated Amplifiers: Op Amps Output impedance matching with fully differential operational amplifiers By Jim Karki Member, Technical Staff, High-Performance Analog Introduction synthetic imped ance matching is more complex. So we Impedance matching is widely used in the transmission of will first look at the output impedance using only series signals in many end applications across the industrial, matching resistors, and then use that as a starting point to communications, video, medical, test, measurement, and consider the more complex synthetic impedance matching. military markets. Impedance matching is important to The fundamentals of FDA operation are presented in reduce reflections and preserve signal integrity. Proper Reference 1. Since the principles and terminology present- termination results in greater signal integrity with higher ed there will be used throughout this article, please see throughput of data and fewer errors. Different methods Reference 1 for definitions and derivations. have been employed; the most commonly used are source Standard output impedance termination, load termination, and double termination. An FDA works using negative feedback around the main Double termination is generally recognized as the best method to reduce reflections, while source and load termi- loop of the amplifier, which tends to drive the impedance nation have advantages in increased signal swing. With at the output terminals, VO– and VO+, to zero, depending source and load termination, either the source or the load on the loop gain. An FDA with equal-value resistors in (not both) is terminated with the characteristic imped- each output to provide differential output termination is ance of the transmission line. -
Determining the Proper Jumper Setting
DETERMINING THE PROPER JUMPER SETTING FOR IMPEDANCE MATCHING The jumper must be set in a position that correctly multiplies the impedance of the system to a level that is equal to or greater than the impedance of the amplifier. The jumper setting can be determined using the following simple steps: 1. Determine the amplifier's minimum impedance. The amplifier's minimum impedance is usually found following Wattage and Frequency Response in the amplifier's specification page of the manual. It may also be listed on the back panel of the amplifier near the speaker terminals. AC impedance is measured in ohms. 2. Identify the correct impedance-matching chart according to the amplifier's minimum impedance. There are two impedance matching charts, one for 8 ohm amplifiers and one for 4 ohm amplifiers. Choose the chart that describes your amplifier. If your amplifier is 6 ohm stable, use the 8 ohm chart. 3. Determine the impedance for each pair of speakers by referring to its manual. 4. Determine the total number of 4 ohm pairs of speakers. (rows on charts) 5. Determine the total number of 8 ohm pairs of speakers. (columns on charts) 6. Follow the appropriate row and column to determine jumper settings. IMPEDANCE MATCHING VOLUME CONTROLS Impedance matching volume controls eliminate the need for a speaker selector. By determining the drive capability of the amplifier with a few simple calculations, we can determine the number of speakers the system can safely operate. CONSIDERATIONS 1. Make sure that your amplifier has adequate wattage for the number of speakers. Watts per channel divided by the number of pairs should equal or exceed the individual speaker’s minimum wattage requirements.