What s Your (real or imaginary) LCR IQ?

Similar documents
Advanced Test Equipment Rentals ATEC (2832) LCR MEASUREMENT PRIMER. ISO 9001 Certified

Single Phase Parallel AC Circuits

LCR Measurement Primer

ES51919/ES51920 LCR meter chipset

Sinusoidal Steady State Analysis (AC Analysis) Part I

Annexure-I. network acts as a buffer in matching the impedance of the plasma reactor to that of the RF

0-2 Operations with Complex Numbers

0-2 Operations with Complex Numbers

Electricity and Light Pre Lab Questions

REACTANCE. By: Enzo Paterno Date: 03/2013

AC Circuit Analysis and Measurement Lab Assignment 8

LCR Series Circuits. AC Theory. Introduction to LCR Series Circuits. Module. What you'll learn in Module 9. Module 9 Introduction

AC Circuits Homework Set

RLC Series Circuit. We can define effective resistances for capacitors and inductors: 1 = Capacitive reactance:

Electric Circuit Theory

LINEAR CIRCUIT ANALYSIS (EED) U.E.T. TAXILA 09

AC Circuit. a) Learn the usage of frequently used AC instrument equipment (AC voltmeter, AC ammeter, power meter).

EXP. NO. 3 Power on (resistive inductive & capacitive) load Series connection

2. The following diagram illustrates that voltage represents what physical dimension?

Chapter 2 Circuit Elements

Sinusoidal Steady-State Analysis

EE 3120 Electric Energy Systems Study Guide for Prerequisite Test Wednesday, Jan 18, pm, Room TBA

AE60 INSTRUMENTATION & MEASUREMENTS DEC 2013

Handout 11: AC circuit. AC generator

SINUSOIDAL STEADY STATE CIRCUIT ANALYSIS

Impedance. Reactance. Capacitors

Lecture #3. Review: Power

y(d) = j

mywbut.com Lesson 16 Solution of Current in AC Parallel and Seriesparallel

EE-0001 PEEE Refresher Course. Week 1: Engineering Fundamentals

CHAPTER 45 COMPLEX NUMBERS

Power Factor Improvement

A capacitor is a device that stores electric charge (memory devices). A capacitor is a device that stores energy E = Q2 2C = CV 2

Consider a simple RC circuit. We might like to know how much power is being supplied by the source. We probably need to find the current.

Learnabout Electronics - AC Theory

ECE 241L Fundamentals of Electrical Engineering. Experiment 6 AC Circuits

Announcements: Today: more AC circuits

Power and Energy Measurement

Bridge Measurement 2.1 INTRODUCTION Advantages of Bridge Circuit

ELECTROMAGNETIC OSCILLATIONS AND ALTERNATING CURRENT

Sinusoids and Phasors

Chapter 33. Alternating Current Circuits

Lecture 6: Time-Dependent Behaviour of Digital Circuits

Sinusoidal Steady-State Analysis

1 Phasors and Alternating Currents

Work, Energy and Power

1 CHAPTER 13 ALTERNATING CURRENTS + A B FIGURE XIII.1

Work, Energy and Power

Physics 142 AC Circuits Page 1. AC Circuits. I ve had a perfectly lovely evening but this wasn t it. Groucho Marx

Lecture 23 Date: Multi-port networks Impedance and Admittance Matrix Lossless and Reciprocal Networks

Transformer. Transformer comprises two or more windings coupled by a common magnetic circuit (M.C.).

Lecture 6: Impedance (frequency dependent. resistance in the s- world), Admittance (frequency. dependent conductance in the s- world), and

ECE145A/218A Course Notes

2. Basic Components and Electrical Circuits

Power System Analysis Prof. A. K. Sinha Department of Electrical Engineering Indian Institute of Technology, Kharagpur

RLC Circuit (3) We can then write the differential equation for charge on the capacitor. The solution of this differential equation is

Chapter 9 Objectives

Welcome! Device Characterization with the Keithley Model 4200-SCS Characterization System.

Unit 21 Capacitance in AC Circuits

MTI TN113: The Series to Parallel Impedance Transformation

Module 4. Single-phase AC circuits. Version 2 EE IIT, Kharagpur

Electrical Circuits Lab Series RC Circuit Phasor Diagram

CHAPTER 5. BRIDGES AND THEIR APPLICATION Resistance Measurements. Dr. Wael Salah

Electronics. Basics & Applications. group talk Daniel Biesinger

PARALLEL A.C. CIRCUITS

Series and Parallel ac Circuits

Sinusoidal Steady-State Analysis

NABTEB Past Questions and Answers - Uploaded online

AC Circuits III. Physics 2415 Lecture 24. Michael Fowler, UVa

Power Systems - Basic Concepts and Applications - Part I

EE221 Circuits II. Chapter 14 Frequency Response

Circuit Analysis-II. Circuit Analysis-II Lecture # 5 Monday 23 rd April, 18

Alternating Current Circuits. Home Work Solutions

Chapter 2 Circuit Elements

EE221 Circuits II. Chapter 14 Frequency Response

Experiment Aim: Students will describe the magnitude of resistance and define the EMF (electromotive force) of a cell.

CHAPTER 5 DC AND AC BRIDGE

Alternating Current Circuits

NETWORK ANALYSIS ( ) 2012 pattern

CIRCUIT ANALYSIS II. (AC Circuits)

ELECTROMAGNETIC INDUCTION

How to measure complex impedance at high frequencies where phase measurement is unreliable.

Review of DC Electric Circuit. DC Electric Circuits Examples (source:

Learning Material Ver 1.2

The process of analysing a circuit using the Laplace technique can be broken down into a series of straightforward steps:

TH2821B Portable LCR Meter

To investigate further the series LCR circuit, especially around the point of minimum impedance. 1 Electricity & Electronics Constructor EEC470

Get Discount Coupons for your Coaching institute and FREE Study Material at ELECTROMAGNETIC INDUCTION

Chapter 10: Sinusoids and Phasors

Capacitor. Capacitor (Cont d)

1. (50 points, BJT curves & equivalent) For the 2N3904 =(npn) and the 2N3906 =(pnp)

Power and Energy Measurement

Chapter 2. Engr228 Circuit Analysis. Dr Curtis Nelson

LM34 - Precision Fahrenheit Temperature Sensor

Resonant Matching Networks

This is Qucs. It shows a plot from a 100pF capacitor. Left is S11 and S21 and right is smith S11.

Electrical Engineering Fundamentals for Non-Electrical Engineers

Chapter 2 Voltage-, Current-, and Z-source Converters

An Introduction to the Smith Chart for Amateur Radio. Jesse Sheinwald, N2CA

A R E S O N A N T D U M M Y L O A D

Transcription:

Chroma Systems Solutions, Inc. What s Your (real or imaginary) LCR IQ? 11021, 11025 LCR Meter Keywords:. Impedance, Inductance, Capacitance, Resistance, Admittance, Conductance, Dissipation Factor, 4-Terminal Measurements, Auto- Ranging, Averaging, Load Correction, Open-Short compensation.

Title: Product Family: What s Your (real or imaginary) LCR IQ? 11021, 11025 LCR Meters Take this quiz and test your knowledge of impedance measurements. True Or False: 1. Impedance is comprised of Inductance, Capacitance and Resistance. 2. Impedance is the total opposition a circuit provides to the flow of AC current at a specified frequency (i.e. AC resistance). 3. Impedance is made up of real resistance and imaginary reactance. Reactance is calculated as 2πfL for an inductor and 1/2πfC for a capacitor All devices can be represented by a series or parallel combination of resistance and reactance. 6. Admittance, the reciprocal of Impedance, is often used instead of impedance in order to simplify mathematical calculations. 7. Conductance is the reciprocal of pure resistance, yet pure values don t actually exist 8. The dissipation factor (D f ) is the ratio of the real part of impedance to the imaginary part. Q is its reciprocal. 9. A low value of D f for a capacitor, or high value of Q for an inductor means that the component is nearly pure. 10. All of these impedance parameters can be measured directly using an LCR Meter Your Score*: 8-10: Congrats, you re a real LCR Wizard! Complex Quantities Rule! 4-7: LCR is a necessary evil. Imaginary components exist to muddle the measurements. 0-3: You slept through Dr. Scott s class and could really give a flying lima bean about LCR! Chroma Systems Solutions, Inc. Page 2 of 8

How the Magic Numbers Appear Impedance is the basic electrical parameter used to characterize electronic circuits, components and materials. Impedance is the sum of alternating current oppositions (capacitive reactance, inductive reactance and resistance) by a circuit. It is represented by the symbol Z and is measured in ohms (Ω). So how do you get ohms out of complex quantities? A little imaginary math! Refer to the vector diagrams for a physical illustration of Impedance and its reciprocal parameter, Admittance. In a pure DC world, Ohm s Law tells us that Resistance = R = V/I But in the real AC world any LCR Wizard knows that the mixing of the following passive component POOF! Resistance + j Reactance = Impedance potions will produce the complex quantity of Impedance Abracadabra! POOF, there it is The magical value of Impedance (Z) R + jx = Z Where R is the real resistance and X is the imaginary reactance in an AC circuit. Measurement Parameters Seriously, every circuit has inductive and capacitive components. Measuring L, C and R will only give you a more precise analysis of the electrical characteristics of the device under test (DUT). Capacitance and inductance cause the voltage and current to be out of phase. The phase shift can be drawn in vector form illustrating the impedance (Z), its real part (RS), its imaginary part (jxs) and the phase angle (θ). All devices can be modeled as a real component (resistor) in series or parallel with a reactive component (capacitor or inductor). The subscript s or p denotes how the device will be modeled for a particular measurement. Impedances in series add, therefore the equivalent circuit for impedance would place RS and XS in series. To further analyze the electrical characteristics of your DUT, look at Admittance (Y) that is the reciprocal of Impedance (Z). Admittance is measured in siemens (S) and is comprised of real conductance (GP) and imaginary susceptance (BP) with a phase angle (φ). Admittances in parallel add, therefore the equivalent circuit for admittance would place GP and BP in parallel. In and Out of Phase Two other secondary parameters important to impedance measurements are the dissipation factor (D f ) and quality factor (Q). The quantities D f and Q are useful as a measurement of the purity of a Chroma Systems Solutions, Inc. Page 3 of 8

component or how close it is to being ideal ( real ) containing only resistance or reactance. D f is the ratio of the real part of impedance to the imaginary part. A low D f indicates that a capacitor is nearly pure. Q is the reciprocal of D f and is the ratio of the real part of admittance to the imaginary part. A high Q value indicates that an inductor is nearly pure. Conversely, a high D f or low Q value indicates that a resistance is nearly pure. Some sign conventions are necessary when discussing D f and Q. For capacitors and inductors D f and Q are considered positive as long as the real part of Z or Y is positive (as it will be for passive components). Note that transfer impedance of passive networks can exhibit negative real parts. For resistors, a common convention is to consider Q to be positive if the component is inductive (having a positive reactance) and to be negative if it is capacitive (having a negative reactance). The D f and Q factors are independent of the configuration of the equivalent circuit used to represent an impedance measurement. These series and parallel equivalent circuits both have the same value of complex impedance at a single frequency, but at any other frequency their impedances will be different. -j 1 ωc S +jx δ θ +R jωls +jx Z jωcp +jb Y -j 1 ωl P +jb δ θ G P +G -jx Z -jx δ θ +R -jb δ θ G P +G -jb Y C S L S C P R P or G P L P R P or G P IMPEDANCE ADMITTANCE Capacitive Inductive Capacitive Inductive Chroma Systems Solutions, Inc. Page 4 of 8

Measuring Impedance So how do you accurately measure impedance parameters to fully characterize your electrical device? Take a look at your LCR instrumentation. What is the measurement technique? What s the connection method? Can you test multiple parameters over a wide range of test frequencies and voltages? Does it provide Constant Source Impedance? How about auto-ranging or averaging capabilities? What kind of compensation does it provide? Can the instrument be remotely operated? Can the test results be saved internally or externally through a computer interface? Read on to find out if your current LCR instrumentation fully measures all parameters of passive components, precisely and expediently. Let s talk about LCR measurement techniques Digital signal generation and detection provides greater speed and accuracy of LCR measurements. As shown in Figure 2, carrying essentially the same current, the voltage across the DUT (Zx) and the voltage across the reference resistor (Rs) is measured. The voltage across Zx (= Vx) and the voltage across Rs (= Vs) are sampled multiple times per cycle of the applied sine wave excitation. The real and imaginary components of Vx and Vs are combined with the known characteristics of Rs to determine the apparent impedance of Zx. This circuitry and fast sampling rates, along with elaborate software driven control, can provide direct readout of all the impedance parameters previously discussed. IH Z X IL Z X I X PH PL = V X ( ) V S K K V X V S Figure 2: Measurement Sampling Circuit Four-Terminal Measurements are pretty much a given in obtaining accurate impedance IH measurements with today s LCR meters. One pair of leads applies the current (source) to the device while the other pair of leads measures PH (senses) the voltage across the device. This removes the series V DUT inductance and resistance error factor including contact resistance. It PL also removes the stray capacitance factor. Shielded coaxial cabling A will reduce most mutual inductance that occurs between the current IL leads and the voltmeter leads. This four-terminal connection technique is widely known as a Kelvin connection. Figure 3: Four-Terminal Measurement Chroma Systems Solutions, Inc. Page 5 of 8

A Constant Source Test Voltage is one thing that is often overlooked when making impedance measurements with an LCR meter. The programmed test voltage is usually an open circuit voltage and not necessarily what the test device would see. The actual test voltage depends on the value of the measuring instrument s source impedance (Rs) and the impedance of the device being measured. For example in Figure 4, if the test voltage is programmed for 1 volt, the instrument source impedance 100Ω and the impedance of the test device 100Ω, the voltage to the device is really only 0.5 volts. You can see that this is generally not a factor when measuring high impedance, where the value is much larger than the source impedance and 7600 Source Resistance = 25Ω the majority of the test voltage is applied directly to the device. For devices that are test signal level dependent, the most common way of dealing with this issue is to use a measuring instrument that employs a constant voltage or voltage-leveling mode. V PROGRAM V P = 1V Z X = 25Ω V M = 0.5V DUT V MEASURE I MEASURE Figure 4: Test Voltage Across DUT Auto Ranging on an impedance-measuring instrument is intended to maintain maximum signal level and the highest signal to noise ratio for maximum measurement accuracy. In order to measure over wide impedance ranges an instrument must have several measurement ranges. The whole idea is to keep the measured impedance as close as possible to full scale on any given range. Perhaps most importantly, ranging is usually done automatically depending on the impedance of the test device, thus eliminating an improper selection by an operator resulting in erroneous measurement data. Averaging is another way of improving instrument measurement accuracy, by reducing unwanted signals and effects of unwanted noise, but of course does require that some measurement speed be sacrificed. In an averaging mode, the operator programs the number of measurements to be made; the LCR meter makes the measurements and calculates the average of these measurements for the final result. The more measurements averaged, the more the accuracy is enhanced. The cost of increased measurement time is well worth the investment when pinpointing a component s exact value especially in materials analysis and R&D applications. Chroma Systems Solutions, Inc. Page 6 of 8

Load Correction Open/Short Compensation reduces the effects from error sources between the DUT and the calibrated connection to the measuring instrument. Compensation will ensure the best measurement accuracy possible on a device at the selected test conditions. The traditional open/short routine measures the stray admittance (Y OPEN ) and residual impedance (Z SHORT ) of the test cable(s) to remove these quantities from the actual measured DUT value. The OPEN routine determines the correction that the instrument applies to high impedance measurements and the SHORT routine determines the correction necessary for low impedance measurements. Figure 5 illustrates the connection to the LCR Meter for open & short compensation using the four-terminal connection. OPEN DUT SHORT Figure 5: Open/Short Compensation Load Correction is a compensation technique that uses a load whose impedance is accurately known, and applies a correction to measurements of similar components to substantially improve measurement accuracy. The purpose of this being to correct for non linearity of the measuring instrument, test fixture or lead effects, all of which may be repeatable and thus can be added or subtracted each time a similar measurement is made. Load correction is only as good as the known accuracy and/or traceability of the load used in determining the correction. Z actual = Z measure +/- delta Z Where delta Z is the difference between the known and measured value of the standard Recent trends in electronic component manufacturing have placed increased demands on LCR instrumentation. Devices are moving to smaller packages, used at higher frequencies, and greater emphasis towards the more perfect component. All this creates new challenges in making contact with devices and measuring them with more speed and accuracy. Automation and features leading toward more reliable testing is the way of future LCR meters and test techniques. An understanding of test parameters and measurement techniques goes a long way in producing useful results. Chroma Systems Solutions, Inc. Page 7 of 8

Figure 6: 11021 LCR Meter *By the way, all statements in the quiz are true. Chroma Systems Solutions, Inc. Page 8 of 8