Temperature Coefficients for DC Resistance of Match and Reference Attenuators
|
|
|
- Jeffery Kelley
- 5 years ago
- Views:
Transcription
1 Temperature Coefficients for DC Resistance of Match and Reference Attenuators Raul Monsalve SESE, Arizona State University October 2, 2013
2 Description This report presents the measurements of DC resistance of the match standard (from Agilent 85033E calibration kit) and the reference 6-dB and 10-dB Mini-Circuit attenuators chosen to establish the accuracy of the VNA calibration. The measurement proceeded as follows: The 6.5-digit multimeter was placed in the control room, subject to 5 C temperature variations. The load (match or attenuator) was connected to the multimeter using 50-cm leads. A female SMA connector was soldered to the end of the leads, in order to properly attach the load. The load, and part of the cables, were placed outside in order to monitor the resistance of the load subject to air temperature variations of 15 C. The resistance of the cables and its stability with time and temperature was established by shorting the ends and monitoring it for two days. It was found to be very stable (figures 1 and 2). The resistance of the match and attenuators was measured for at least two days each. The correlation of resistance with temperature was modeled with polynomials (figures 3 through 8). Relevant results are presented in table 1.
3 3 Description Figure 1 shows the stability of the leads + connector resistance. Figure 2 presents the correlation with temperature. The residuals obtained when fitting a constant, a slope, and a second-order polynomial, to the correlation are within ±1 mω. Therefore, the simplest model is assumed for the resistance: a constant of 50 mω. The residuals of ±1 mω are considered for the computation of the uncertainty. Figures 3 and 4 show the dependence of the Mini-Circuits 6-dB attenuator on temperature. The resistance of the leads and connector (50 mω) has been removed from the data. The residuals of a first- and second-order fit are ± 8 mω. No improvement is appreciated by going to second-order. Figures 5 and 6 show the dependence of the Mini-Circuits 10-dB attenuator on temperature. The resistance of the leads and connector (50 mω) has been removed from the data. The residuals of a first- and second-order fit are ± 2 mω. Even though the margin is the same, using a second-order fit improves the profile of the residuals with temperature (red is flatter than blue on the lower panel of figure 6). Because of this, a second-order model is preferred. Figures 7 and 8 show the dependence of the match standard on temperature. The resistance of the leads and connector (50 mω) has been removed from the data. The residuals of a first- and second-order fit are ± 4 mω. No improvement is appreciated by going to second-order.
4 4 Summary The model for the resistance measurement is: m = LR + (a + bt + ct 2 ) + Residuals. (1) The LR term represents the resistance of the leads and connectors. The terms in parenthesis represent the polynomial model. Only the 10-dB attenuator is actually modeled with a second-order polynomial. The other two cases are modeled as a slope, with c = 0. The uncertainty assigned to a resistance value derived from the models is the sum of the uncertainty in the cable resistance ( LR) and the residuals of the fit. The following table summarizes the results, using the notation of the previous equation. Table: (1) Fit coefficients for the attenuators and match. Load LR [Ω] a [Ω] b [mω/ C] c [mω/( C) 2 ] LR [Ω] Residuals [Ω] Total [Ω] 6-dB Attn ±0.001 ±0.008 ± dB Attn ±0.001 ±0.002 ±0.003 Match ±0.001 ±0.004 ±0.005
5 5 Resistance of Leads + Connector resistance of leads + connector [Ω] Figure: (1) Stability of resistance of cables and female SMA connector. It was obtained connecting a short standard at the connector.
6 Resistance of Leads + Connector resistance of leads + connector [Ω] fit residuals [mω] Figure: (2) Correlation of resistance with temperature. The lower panel shows the residuals after fitting a constant (green), slope (blue), and quadratic (red). If a margin of ±1 mω is assumed, a simple constant value for the leads + connector of 0.05 mω can be used.
7 Resistance of 6-dB Attenuator resistance of 6 db attenuator [Ω] Figure: (3) Dependence of resistance of Mini-circuits 6-dB attenuator on temperature. It was measured for 70 hours. The resistance of cables and connector has been subtracted.
8 Resistance of 6-dB Attenuator resistance of 6 db attenuator [Ω] fit residuals [mω] Figure: (4) Correlation of resistance with temperature. The lower panel shows the residuals after fitting a slope (blue) and quadratic (red). No improvement is observed when a quadratic model is used. Therefore, a first-order model is used and residuals of ± 8 mω are assumed.
9 9 Resistance of 10-dB Attenuator resistance of 10 db attenuator [Ω] Figure: (5) Dependence of resistance of Mini-circuits 10-dB attenuator on temperature. It was measured for 83 hours. The resistance of cables and connector has been subtracted.
10 Resistance of 10-dB Attenuator resistance of 10 db attenuator [Ω] fit residuals [mω] Figure: (6) Correlation of resistance with temperature. The lower panel shows the residuals after fitting a slope (blue) and quadratic (red). Improvement is noticed when a quadratic model is used. Therefore, a second-order model is used and residuals of ± 2 mω are assumed.
11 Resistance of Match resistance of match [Ω] Figure: (7) Dependence of resistance of match on temperature. It was measured for 60 hours. The resistance of cables and connector has been subtracted.
12 Resistance of Match resistance of match [Ω] fit residuals [mω] Figure: (8) Correlation of resistance with temperature. The lower panel shows the residuals after fitting a slope (blue) and quadratic (red). No improvement is noticed when a quadratic model is used. Therefore, a first-order model is used and residuals of ± 4 mω are assumed.
Performance of Antenna Measurement Setup
Performance of Antenna Measurement Setup Raul Monsalve SESE, Arizona State University November 27, 213 2 Description This report is divided into two parts: PART 1: Check of recovered instrumental S-parameters
VNA Tools II S-parameter uncertainty calculation
VA Tools II S-parameter uncertainty calculation Michael Wollensack METAS 5. May 0 Michael Wollensack METAS Outline Introduction VA Measurement Model Database Uncertainty Visualization Results Michael Wollensack
Lab 4 RC Circuits. Name. Partner s Name. I. Introduction/Theory
Lab 4 RC Circuits Name Partner s Name I. Introduction/Theory Consider a circuit such as that in Figure 1, in which a potential difference is applied to the series combination of a resistor and a capacitor.
Experiment 2: Laboratory Experiments on Ferroelectricity
Experiment 2: Laboratory Experiments on Ferroelectricity 1. Task: Measure the dielectric constant εr of a TGS crystal as a function of temperature from room temperature up to 70 C at a frequency of about
First Look at Good-Quality EDGES Data
First Look at Good-Quality EDGES Data Raul Monsalve SESE, Arizona State University May 3, 214 Description These slides present the result of the first look at EDGES data taken between (and including) days
Preliminary Rejection of Global 21-cm Models with EDGES High-Band (ongoing work)
Preliminary Rejection of Global 21-cm Models with EDGES High-Band (ongoing work) Raul Monsalve CASA, University of Colorado Boulder SESE, Arizona State University November 23, 216 2 Description Here I
A simplified method of VNA uncertainty estimation
A simplified method of VNA uncertainty estimation Markus Zeier, Johannes Hoffmann, Jurg Ruefenacht, Michael Wollensack METAS ANAMET Workshop, PTB Braunschweig, 17.12.2014 ANAMET 1 METAS Outline Introduction
Prepare for this experiment!
Notes on Experiment #8 Theorems of Linear Networks Prepare for this experiment! If you prepare, you can finish in 90 minutes. If you do not prepare, you will not finish even half of this experiment. So,
Comparison of MLCC and X2Y Technology for Use in Decoupling Circuits
Comparison of MLCC and X2Y Technology for Use in Decoupling Circuits Dale L. Sanders James P. Muccioli Anthony A. Anthony X2Y Attenuators, LLC 37554 Hills Tech Dr. Farmington Hills, MI 48331 248-489-0007
Experiment 1: Laboratory Experiments on Ferroelectricity
Experiment 1: Laboratory Experiments on Ferroelectricity 1. Task: 1. Set up a Sawyer-Tower circuit to measure ferroelectric hysteresis curves. 2. Check the D(E) curves for a capacitor, a resistor and an
Experiment #6. Thevenin Equivalent Circuits and Power Transfer
Experiment #6 Thevenin Equivalent Circuits and Power Transfer Objective: In this lab you will confirm the equivalence between a complicated resistor circuit and its Thevenin equivalent. You will also learn
Contents. Transmission Lines The Smith Chart Vector Network Analyser (VNA) ü structure ü calibration ü operation. Measurements
Contents Transmission Lines The Smith Chart Vector Network Analyser (VNA) ü structure ü calibration ü operation Measurements Göran Jönsson, EIT 2015-04-27 Vector Network Analysis 2 Waves on Lines If the
THE search for higher accuracy in measurements of S-
IEEE TRANSACTIONS ON MICROWAVE THEORY AND TECHNIQUES, VOL. XX, NO. XX, JANUARY 2XX 1 One-Port Direct/Reverse Method for Characterizing VNA Calibration Standards Raul A. Monsalve, Member, IEEE, Alan E.
Microwave Impedance Measurement for Nanoelectronics
276 M. RNDUS, K. HOFFMNN, MICROWVE IMPEDNCE MESUREMEN FOR NNOELECRONICS Microwave Impedance Measurement for Nanoelectronics Martin RNDUS, Karel HOFFMNN Dept. of Electromagnetic Field, Czech echnical University
Experiment 06 - Extraction of Transmission Line Parameters
ECE 451 Automated Microwave Measurements Laboratory Experiment 06 - Extraction of Transmission Line Parameters 1 Introduction With the increase in both speed and complexity of mordern circuits, modeling
POLYTECHNIC UNIVERSITY Electrical Engineering Department. EE SOPHOMORE LABORATORY Experiment 2 DC circuits and network theorems
POLYTECHNIC UNIVERSITY Electrical Engineering Department EE SOPHOMORE LABORATORY Experiment 2 DC circuits and network theorems Modified for Physics 18, Brooklyn College I. Overview of Experiment In this
Fig. 1-1 Current Flow in a Resistive load
1 Electric Circuits: Current flow in a resistive load flows either from (-) to () which is labeled below as Electron flow or the Conventional flow from () to (-). We will use conventional flow in this
DesignCon Evaluation of Relative Humidity and Temperature Effects on Scattering Parameters in Transmission Systems 1
DesignCon 21 Evaluation of Relative Humidity and Temperature Effects on Scattering Parameters in Transmission Systems 1 Ji Li, Penn State Harrisburg jxl994@psu.edu, (717)-948-6278 Mark Minns, Penn State
ENSC387: Introduction to Electromechanical Sensors and Actuators LAB 3: USING STRAIN GAUGES TO FIND POISSON S RATIO AND YOUNG S MODULUS
ENSC387: Introduction to Electromechanical Sensors and Actuators LAB 3: USING STRAIN GAUGES TO FIND POISSON S RATIO AND YOUNG S MODULUS 1 Introduction... 3 2 Objective... 3 3 Supplies... 3 4 Theory...
Capacitance Measurement
Overview The goal of this two-week laboratory is to develop a procedure to accurately measure a capacitance. In the first lab session, you will explore methods to measure capacitance, and their uncertainties.
Contents. Transmission Lines The Smith Chart Vector Network Analyser (VNA) ü structure ü calibration ü operation. Measurements
Contents Transmission Lines The Smith Chart Vector Network Analyser (VNA) ü structure ü calibration ü operation Measurements Göran Jönsson, EIT 2017-05-12 Vector Network Analysis 2 Waves on Lines If the
Product Data. Brüel & Kjær B. Sound Intensity Calibrator Type 3541
Product Data Sound Intensity Calibrator Type 3541 USES: Sound intensity and particle velocity calibrations Sound pressure calibration Measurement of pressure-residual intensity index FEATURES: Intensity
Projectile Motion. x = v ox t (1)
Projectile Motion Theory Projectile motion is the combination of different motions in the x and y directions. In the x direction, which is taken as parallel to the surface of the earth, the projectile
resistance in the circuit. When voltage and current values are known, apply Ohm s law to determine circuit resistance. R = E/I ( )
DC Fundamentals Ohm s Law Exercise 1: Ohm s Law Circuit Resistance EXERCISE OBJECTIVE When you have completed this exercise, you will be able to determine resistance by using Ohm s law. You will verify
MET 301 EXPERIMENT # 2 APPLICATION OF BONDED STRAIN GAGES
MET 301 EPERIMENT # 2 APPLICATION OF BONDED STRAIN GAGES 1. Objective To understand the working principle of bonded strain gauge and to study the stress and strain in a hollow cylindrical shaft under bending,
Three Axis Magnetic Field Transducer x-h3x-xx_e3d-2.5khz-1-0.2t
DESCRIPTION: TYPICAL APPLICATIONS: The is a high accuracy magnetic flux density-toanalogue-voltage transducer with a highlevel and temperature compensated output signal for each of the three components
Waves on Lines. Contents. ! Transmission Lines! The Smith Chart! Vector Network Analyser (VNA) ! Measurements
Waves on Lines If the wavelength to be considered is significantly greater compared to the size of the circuit the voltage will be independent of the location. amplitude d! distance but this is not true
EXPERIMENT 5A RC Circuits
EXPERIMENT 5A Circuits Objectives 1) Observe and qualitatively describe the charging and discharging (decay) of the voltage on a capacitor. 2) Graphically determine the time constant for the decay, τ =.
IMPROVING SOIL MEASUREMENTS FOR BOUNDARY LAYER RESEARCH
IMPROVING SOIL MEASUREMENTS FOR BOUNDARY LAYER RESEARCH Hannelore Bloemink, Jan Bijma Royal Netherlands Meteorological Institute (KNMI) Instrumentation Division P.O. Box 201, 3730 AE De Bilt, The Netherlands
Topic 1.2 Measurement and Uncertainties Uncertainty and error in measurement. Random Errors
Uncertainty and error in measurement Random Errors Definition of Random Error Random errors are sources of uncertainties in the measurement, whose effect can be reduced by a repeated experiment, and taking
Lab E3: The Wheatstone Bridge
E3.1 Lab E3: The Wheatstone Bridge Introduction The Wheatstone bridge is a circuit used to compare an unknown resistance with a known resistance. The bridge is commonly used in control circuits. For instance,
Exercise 1: Thermistor Characteristics
Exercise 1: Thermistor Characteristics EXERCISE OBJECTIVE When you have completed this exercise, you will be able to describe and demonstrate the characteristics of thermistors. DISCUSSION A thermistor
Electrical Circuits Lab Series RC Circuit Phasor Diagram
Electrical Circuits Lab. 0903219 Series RC Circuit Phasor Diagram - Simple steps to draw phasor diagram of a series RC circuit without memorizing: * Start with the quantity (voltage or current) that is
Steady State Frequency Response Using Bode Plots
School of Engineering Department of Electrical and Computer Engineering 332:224 Principles of Electrical Engineering II Laboratory Experiment 3 Steady State Frequency Response Using Bode Plots 1 Introduction
Qualification Test Report
Qualification Test Report 501-97 28Jun10 Rev E Connector, Shielded, Miniature Circular DIN, PCB Mounted 1. INTRODUCTION 1.1. Purpose Testing was performed on Tyco Electronics Mini DIN Printed Circuit Board
Experiment 5 Voltage Divider Rule for Series Circuits
Experiment 5 Voltage Divider Rule for Series Circuits EL - DC Fundamentals By: Walter Banzhaf, E.K. Smith, and Winfield Young University of Hartford Ward College of Technology Objectives:. For the student
Keysight Technologies Measurement Uncertainty of VNA Based TDR/TDT Measurement. Application Note
Keysight Technologies Measurement Uncertainty of VNA Based TDR/TDT Measurement Application Note Table of Contents Introduction... 3 S-parameter measurement uncertainty of VNA... 4 Simplification of systematic
University of Illinois at Chicago Spring ECE 412 Introduction to Filter Synthesis Homework #4 Solutions
Problem 1 A Butterworth lowpass filter is to be designed having the loss specifications given below. The limits of the the design specifications are shown in the brick-wall characteristic shown in Figure
New Methods for Measuring the Effective Source Reflection Coefficient of Microwave Generators. Jens Leinhos, Thomas Reichel and Jochen Simon
New Methods for Measuring the Effective Source Reflection Coefficient of Microwave Generators Jens Leinhos, Thomas Reichel and Jochen Simon Contents l l l l l l l l l Introduction Measurement Procedures
3. Basic building blocks. Analog Design for CMOS VLSI Systems Franco Maloberti
Inverter with active load It is the simplest gain stage. The dc gain is given by the slope of the transfer characteristics. Small signal analysis C = C gs + C gs,ov C 2 = C gd + C gd,ov + C 3 = C db +
SKIN EFFECT : ELECTROMAGNETIC WAVE OR DIFFUSION?
SKIN EFFECT : ELECTROMAGNETIC WAVE OR DIFFUSION? At high frequencies current in a conductor flows mainly on its surface, and this is known as the skin effect. Two possible mechanisms are given in the published
Operational Amplifiers
Operational Amplifiers A Linear IC circuit Operational Amplifier (op-amp) An op-amp is a high-gain amplifier that has high input impedance and low output impedance. An ideal op-amp has infinite gain and
LM34 - Precision Fahrenheit Temperature Sensor
- Precision Fahrenheit Temperature Sensor Features Typical Application Calibrated directly in degrees Fahrenheit Linear +10.0 mv/ F scale factor 1.0 F accuracy guaranteed (at +77 F) Parametric Table Supply
ECE 523/421 - Analog Electronics University of New Mexico Solutions Homework 3
ECE 523/42 - Analog Electronics University of New Mexico Solutions Homework 3 Problem 7.90 Show that when ro is taken into account, the voltage gain of the source follower becomes G v v o v sig R L r o
Lecture 13. Vector Network Analyzers and Signal Flow Graphs
HP8510 Lecture 13 Vector Network Analyzers and Signal Flow Graphs 1 Vector Network Analyzers HP8510 Agilent 8719ES R&S ZVA67 VNA 2 ports, 67 GHz port 1 port 2 DUT Agilent N5247A PNA-X VNA, 4 ports, 67
Thermocouple Calibrations and Heat Transfer Coefficients
Laboratory Experiment 5: Thermocouple Calibrations and Heat Transfer Coefficients Presented to the University of California, San Diego Department of Mechanical and Aerospace Engineering MAE 170 Prepared
Experiment 3. Electrical Energy. Calculate the electrical power dissipated in a resistor.
Experiment 3 Electrical Energy 3.1 Objectives Calculate the electrical power dissipated in a resistor. Determine the heat added to the water by an immersed heater. Determine if the energy dissipated by
Practical 1 RC Circuits
Objectives Practical 1 Circuits 1) Observe and qualitatively describe the charging and discharging (decay) of the voltage on a capacitor. 2) Graphically determine the time constant for the decay, τ =.
Final Exam. 55:041 Electronic Circuits. The University of Iowa. Fall 2013.
Final Exam Name: Max: 130 Points Question 1 In the circuit shown, the op-amp is ideal, except for an input bias current I b = 1 na. Further, R F = 10K, R 1 = 100 Ω and C = 1 μf. The switch is opened at
Generalized four-point characterization method for resistive and capacitive contacts
Generalized four-point characterization method for resistive and capacitive contacts Brian S. Kim 1,a),b), Wang Zhou 1,a), Yash D. Shah 1,c), Chuanle Zhou 1, N. Işık 2,d), and M. Grayson 1,e) 1 Department
FILM DIELECTRICS USED IN FILM CAPACITOR PRODUCTS
FILM DIELECTRICS USED IN FILM CAPACITOR PRODUCTS Overview PARAMETER Dielectric constant: DIELECTRIC (1) KT KN KI KP UNIT at 1 khz 3.3 3.0 3.0. Dissipation factor at 1 khz 50 40 3 1 10-4 at 10 khz 110 6
Solar cells E Introduction. Equipment used for this experiment is displayed in Fig. 2.1.
2.0 Introduction Equipment used for this experiment is displayed in Fig. 2.1. Figure 2.1 Equipment used for experiment E2. List of equipment (see Fig. 2.1): A: Solar cell B: Solar cell C: Box with slots
Prepare for this experiment!
Notes on Experiment #8 Theorems of Linear Networks Prepare for this experiment! If you prepare, you can finish in 90 minutes. If you do not prepare, you will not finish even half of this experiment. So,
Product Series Specification Document
Product Series 3.96mm pitch board-to-board connectors - Socket SCOPE This document covers 3.96mm socket connectors. The connector will perform to the specifications outlined. All tests have been performed
Series CCT-58S Multi-Throw DC 18 GHz, SP7T & SP8T Normally Open Coaxial Switch
PART NUMBER CCT-58S DESCRIPTION Commercial Normally Open Multi-throw, DC-18 GHz The CCT-58S/CT-58S is an internally terminated, broadband, multi-throw, electromechanical coaxial switch designed to switch
Surface Mount Chip Capacitors
Features High '' Factor at high frequencies High RF power capabilities Low High self resonant frequencies Excellent stability across temperature range Small size High Frequency Measurement and Performance
Imformation of C091D series
Imformation of C09D series The QTY of contacts is -pin to -pin, the connection method for the thread type, pinhole connections for welding type, press-fit and PCB type. This series of connectors to prevent
Chapter 5 Objectives
Chapter 5 Engr228 Circuit Analysis Dr Curtis Nelson Chapter 5 Objectives State and apply the property of linearity State and apply the property of superposition Investigate source transformations Define
ESE319 Introduction to Microelectronics. Feedback Basics
Feedback Basics Stability Feedback concept Feedback in emitter follower One-pole feedback and root locus Frequency dependent feedback and root locus Gain and phase margins Conditions for closed loop stability
Contents. ! Transmission Lines! The Smith Chart! Vector Network Analyser (VNA) ! Measurements. ! structure! calibration! operation
Contents! Transmission Lines! The Smith Chart! Vector Network Analyser (VNA)! structure! calibration! operation! Measurements Göran Jönsson, EIT 2009-11-16 Network Analysis 2! Waves on Lines! If the wavelength
Microwave Loss Reduction in Cryogenically Cooled Conductors R. Finger and A. R. Kerr
NATIONAL RADIO ASTRONOMY OBSERVATORY ELECTRONICS DIVISION INTERNAL REPORT NO. 321 Microwave Loss Reduction in Cryogenically Cooled Conductors R. Finger and A. R. Kerr July 3, 2008 NATIONAL RADIO ASTRONOMY
Experiment 4. RC Circuits. Observe and qualitatively describe the charging and discharging (decay) of the voltage on a capacitor.
Experiment 4 RC Circuits 4.1 Objectives Observe and qualitatively describe the charging and discharging (decay) of the voltage on a capacitor. Graphically determine the time constant τ for the decay. 4.2
Last Revision: August,
A3-1 HALL EFFECT Last Revision: August, 21 2007 QUESTION TO BE INVESTIGATED How to individual charge carriers behave in an external magnetic field that is perpendicular to their motion? INTRODUCTION The
Mechatronics II Laboratory EXPERIMENT #1: FORCE AND TORQUE SENSORS DC Motor Characteristics Dynamometer, Part I
Mechatronics II Laboratory EXPEIMENT #1: FOCE AND TOQUE SENSOS DC Motor Characteristics Dynamometer, Part I Force Sensors Force and torque are not measured directly. Typically, the deformation or strain
Low-profile Master Type (Slim Type) The thinnest possible body contributes to reduced size, height and weight of the set product
RS NS Low-profile Master Type (Slim Type) The thinnest possible body contributes to reduced size, height and weight of the set product Typical Specifications Items Specifications tolerance ±0% Maximum
CALYS 80P. Field pressure calibrator with high accuracy 0.01%
Field pressure calibrator with high accuracy 0.01% CALYS 80P is a field pressure calibrator within CALYS range with high accuracy of 0.01%. Description CALYS 80P is a field pressure calibrator within CALYS
EMRP ENG05 Metrology for Solid State Lighting D2.4.1 Report on junction temperature vs. voltage characteristics for the selected SSL
EMRP ENG05 Metrology for Solid State Lighting D2.4.1 Report on junction temperature vs. voltage characteristics for the selected SSL György Andor, MKEH Petri Kärhä, Aalto University Introduction Five different
by A.Tonina*, R.Iuzzolino*, M.Bierzychudek* and M.Real* S. Solve + R. Chayramy + and M. Stock +
Bilateral Comparison of 1.018 V and 10 V Standards between the INTI (Argentina) and the BIPM, August to October 2009 (part of the ongoing BIPM key comparison BIPM.EM-K11.a and b) by A.Tonina*, R.Iuzzolino*,
THERE MUST BE 50 WAYS TO FIND YOUR VALUES: AN EXPLORATION OF CIRCUIT ANALYSIS TECHNIQUES FROM OHM S LAW TO EQUIVALENT CIRCUITS
THERE MUST BE 50 WAYS TO FIND YOUR VALUES: AN EXPLORATION OF CIRCUIT ANALYSIS TECHNIQUES FROM OHM S LAW TO EQUIVALENT CIRCUITS Kristine McCarthy Josh Pratti Alexis Rodriguez-Carlson November 20, 2006 Table
STATEWIDE CAREER/TECHNICAL EDUCATION COURSE ARTICULATION REVIEW MINUTES
STATEWIDE CAREER/TECHNICAL EDUCATION COURSE ARTICULATION REVIEW MINUTES Articulation Agreement Identifier: _ELT 107/ELT 108 (2011-1) Plan-of-Instruction version number (e.g.; INT 100 (2007-1)). Identifier
Practical Considerations and Solutions for Temperature-Dependent S-Parameter Measurement for Accurate Parameter Extraction of
Practical Considerations and Solutions for Temperature-Dependent S-Parameter Measurement for Accurate Parameter Extraction of Advanced RF Devices Gavin Fisher, Application Engineer Andrej Rumiantsev, Product
Experiment 2-5. Wheatstone Bridge experiment
Experiment 2-5. Wheatstone Bridge experiment Use the Wheatstone Bridge to measure the unknown electrical resistance and learn the structure and principles of the Wheatstone Bridge. In the laboratory, the
Magnetic field outside a straight conductor (Item No.: P )
Magnetic field outside a straight conductor (Item No.: P2430500) Curricular Relevance Area of Expertise: Physics Education Level: University Topic: Electricity and Magnetism Subtopic: Magnetic Field and
ECE 241L Fundamentals of Electrical Engineering. Experiment 5 Transient Response
ECE 241L Fundamentals of Electrical Engineering Experiment 5 Transient Response NAME PARTNER A. Objectives: I. Learn how to use the function generator and oscilloscope II. Measure step response of RC and
User Manual VX4750 Function Generator Module
User Manual VX4750 Function Generator Module 070-9151-05 This document applies for firmware version 2.60 and above. Copyright Tektronix, Inc. All rights reserved. Tektronix products are covered by U.S.
Quantifying and Verifying trace stability of vector network analyzers at frequencies below 1GHz
1 Quantifying and Verifying trace stability of vector network analyzers at frequencies below 1GHz Hamdi Mani, Chris Groppi, Judd Bowman Abstract we describe measurements done to check the low frequency
Determining Characteristic Impedance and Velocity of Propagation by Measuring the Distributed Capacitance and Inductance of a Line
Exercise 2-1 Determining Characteristic Impedance and Velocity EXERCISE OBJECTIVES Upon completion of this exercise, you will know how to measure the distributed capacitance and distributed inductance
Physical Structure of Matter. Hall effect in p-germanium Solid-state Physics, Plasma Physics. What you need:
Solid-state Physics, Plasma Physics Physical Structure of Matter What you can learn about Semiconductor Band theory Forbidden zone Intrinsic conductivity Extrinsic conductivity Valence band Conduction
Math 1320, Section 10 Quiz IV Solutions 20 Points
Math 1320, Section 10 Quiz IV Solutions 20 Points Please answer each question. To receive full credit you must show all work and give answers in simplest form. Cell phones and graphing calculators are
Advancements in mm-wave On-Wafer Measurements: A Commercial Multi-Line TRL Calibration Author: Leonard Hayden Presenter: Gavin Fisher
Advancements in mm-wave On-Wafer Measurements: A Commercial Multi-Line TRL Calibration Author: Leonard Hayden Presenter: Gavin Fisher The title of this section is A Commercial Multi-Line TRL Calibration
Ohm s Law is a formula used to calculate the relationship between voltage, current and resistance in an electrical circuit.
Quantity What is Ohm s Law? Ohm s Law is a formula used to calculate the relationship between voltage, current and resistance in an electrical circuit. To students of electronics, Ohm s Law (E = IR) is
Chip Inductors. LCCM Series Chip Common Mode Filter FEATURES CONSTRUCTION
FEATURES Small wire wound chip inductor with ferrite core and 2 common mode lines. Highly effective in noise suppression High common-mode impedance at noise band an low differential mode impedance at signal
Harnessing the Power of Arduino for the Advanced Lab
P P Herbert Jaeger + Harnessing the Power of Arduino for the Advanced Lab (Final Version) ALPhA Immersion Workshop July 27 29, 2017 Department of Physics Indiana University Purdue University Ft. Wayne,
Sophomore Physics Laboratory (PH005/105)
CALIFORNIA INSTITUTE OF TECHNOLOGY PHYSICS MATHEMATICS AND ASTRONOMY DIVISION Sophomore Physics Laboratory (PH5/15) Analog Electronics Active Filters Copyright c Virgínio de Oliveira Sannibale, 23 (Revision
Document Number: SPIRE-UCF-DOC Issue 1.0. November Matt Griffin
Sensitivity of the SPIRE Detectors to Operating Parameters Document Number: SPIRE-UCF-DOC-9 Issue. November 4 7 Matt Griffin Contents. Introduction.... List of symbols... 3. Principles of semiconductor
Chapter 1: System of Linear Equations 1.3 Application of Li. (Read Only) Satya Mandal, KU. Summer 2017: Fall 18 Update
Chapter 1: System of Linear Equations 1.3 Application of Linear systems (Read Only) Summer 2017: Fall 18 Update Goals In this section, we do a few applications of linear systems, as follows. Fitting polynomials,
Core practical 12: Calibrate a thermistor in a potential divider circuit as a thermostat
Core practical 12 Teacher sheet circuit To determine the temperature variation of a thermistor To design a potential divider circuit that can be used to control temperature Specification links Although
To investigate further the series LCR circuit, especially around the point of minimum impedance. 1 Electricity & Electronics Constructor EEC470
Series esonance OBJECTIE To investigate further the series LC circuit, especially around the point of minimum impedance. EQUIPMENT EQUIED Qty Apparatus Electricity & Electronics Constructor EEC470 Basic
COMOSAR E-FIELD PROBE CALIBRATION REPORT
Page: 1/26 Issue: A Date: 2008/10/06 COMOSAR E-FIELD PROBE CALIBRATION REPORT Prepared By: Project Description: Prepared For (End User): LUC Jérôme, SATIMO SAR TEST BENCH Shenzhen Morlab Communication
Direct Current (DC): In a DC circuit the current and voltage are constant as a function of time. Power (P): Rate of doing work P = dw/dt units = Watts
Lecture 1: Introduction Some Definitions: Current (I): Amount of electric charge (Q) moving past a point per unit time I dq/dt Coulombs/sec units Amps (1 Coulomb 6x10 18 electrons) oltage (): Work needed
Advances in Radio Science
Advances in Radio Science 2003 1: 1 8 c Copernicus GmbH 2003 Advances in Radio Science Uncertainty of VNA S-parameter measurement due to non-ideal TMSO or LMSO calibration standards U. Stumper Physikalisch-Technische
Improvements to the UK Primary Standard Therapy Level Electron Beam Calorimeter
Radiotherapy Standards Users Group meeting NPL, 5 th June 2007 Improvements to the UK Primary Standard Therapy Level Electron Beam Calorimeter Mark Bailey, G A Bass, N D Lee, G A Mapp Contents 1. History
Homework Assignment 11
Homework Assignment Question State and then explain in 2 3 sentences, the advantage of switched capacitor filters compared to continuous-time active filters. (3 points) Continuous time filters use resistors
EE 242 EXPERIMENT 8: CHARACTERISTIC OF PARALLEL RLC CIRCUIT BY USING PULSE EXCITATION 1
EE 242 EXPERIMENT 8: CHARACTERISTIC OF PARALLEL RLC CIRCUIT BY USING PULSE EXCITATION 1 PURPOSE: To experimentally study the behavior of a parallel RLC circuit by using pulse excitation and to verify that
System Parameter Identification for Uncertain Two Degree of Freedom Vibration System
System Parameter Identification for Uncertain Two Degree of Freedom Vibration System Hojong Lee and Yong Suk Kang Department of Mechanical Engineering, Virginia Tech 318 Randolph Hall, Blacksburg, VA,
CALYS 120 IS. ATEX documenting multifunction calibrator with high accuracy 0.006%
ATEX documenting multifunction calibrator with high accuracy 0.006% is the top instrument of our range of ATEX documenting multifunction calibrators. Description is the top instrument of our range of ATEX
CDS. high density spring connection
CDS high density spring connection DENSTY STANDARD 1A CDS DENSTY A A spring connection CDS Series The originality of multipole connectors represents one of the core values of LE, a leading company in this
This section reviews the basic theory of accuracy enhancement for one-port networks.
Vector measurements require both magnitude and phase data. Some typical examples are the complex reflection coefficient, the magnitude and phase of the transfer function, and the group delay. The seminar
Hours / 100 Marks Seat No.
17322 21314 3 Hours / 100 Seat No. Instructions (1) All Questions are Compulsory. (2) Answer each next main Question on a new page. (3) Illustrate your answers with neat sketches wherever necessary. (4)
Lab 2. Characterization of Solar Cells
Lab 2. Characterization of Solar Cells Physics Enhancement Programme Department of Physics, Hong Kong Baptist University 1. OBJECTIVES To familiarize with the principles of commercial solar cells To characterize