Lab Introduction

Total Page:16

File Type:pdf, Size:1020Kb

Lab Introduction Cir cuit s 212 Lab Lab #1 Lab Introduction Special Information for this Lab’s Report Because this is a one-week lab, please hand in your lab report for this lab at the beginning of next week’s lab. The purpose of this lab is to allow you to become familiar with the laboratory equipment and processes. Labs will be performed in groups of two or three students. Each person will turn in his or her own copy of the required work for the lab. For this lab, one person from your group will need to check out the following from the EECS Shop. · An analog probe kit with a breadboard (metal toolbox) Figure 1. A typical breadboard. The arrows indicate the direction of conduction. The 64 inner columns conduct vertically with an open break in the middle. The outer 2 rows on the top and bottom conduct horizontally (with an open break in the middle for some types of breadboards). Parts List • 1 - 2 k Resistor • 1 - 3 k Resistor • 1 - 10 k Resistor Date Last Modified: 2/5/2018 5:57 PM 1 Definitions Voltmeter – A device for measuring voltage between two points. A perfect voltmeter behaves like an open (infinite resistance) circuit. Voltage is measured by connecting the two voltmeter terminals to the two points of the circuit where the voltage (potential difference) is to be measured (see Fig. 4 below). Therefore, the voltmeter has no effect on the circuit because placing an (ideally) infinite resistance across any two points in the circuit will not affect its operation. Figure 2. Using a voltmeter for voltage measurement. Notice that no any change to the original circuit connections need to be done. We simply connect the terminals of the voltmeter across the component where the voltage is to be measured (resistor 4 in this case). Ammeter – A device for measuring the electric current through a circuit path. A perfect ammeter behaves like a short (zero resistance) circuit like a wire. Current is measured by inserting the ammeter in series within the electric current flow path and, therefore, the ammeter has no effect on the circuit because it looks like a perfectly conducting wire (see Fig. 3 below). Figure 3. Using an ammeter for current measurement. Notice that we need to make a break in the circuit and connect this break by the two terminals of the ammeter, i.e., to interpolate the ammeter in the current path so that the electric current flows through the ammeter. Ohmmeter – A device that measures the electric resistance between two terminals of a component or a circuit. If the resistance of a resistor is to be measured, the resistor should NOT be connected to an external circuit from both terminals. Date Last Modified: 2/5/2018 5:57 PM 2 Multi-meter – A device that can function as an ammeter, voltmeter, or an ohmmeter. Most of modern multi-meters are digital multimeters (DMM’s). There are generally two types of DMM’s: hand-held DMM’s and bench-top (or bench-attached) DMM’s (like the ones attached to your benches in the lab). Function Generator (FG) – A device that produces voltage signals as functions of time. Common signals that a FG can produce are sine waves, square waves, triangle waves, ramp waves, and noise. Common controls that a FG has include amplitude, frequency, and DC offset. Arbitrary Waveform Generator (AWG)– A device that is like a function generator in that it produces voltage signals. However, an arbitrary waveform generator can produce any waveform (audio, television, digital data, sinusoids, etc.). AWG’s have interfaces like FG’s. They can generate analog signals from saved digital files (like signals generated by MATLAB or any other computer tool, or files of signals acquired from real analog signals by an oscilloscope) Digital Storage Oscilloscope (DSO) – A DSO measures voltage signals as a function of time. The time-varying voltage can be recorded and saved as a data file (containing the voltage value at each sampling time) to be used for computer processing or re- generation when loaded to an AWG. Experiment 1. Using Multi-meters to Measure Voltage and Current Figure 4. Using your breadboard and provided circuit components, build the circuit shown in Fig. 4. The Hewlett-Packard power supply has three adjustable outputs. Use the +20V connection to supply 12V for V2 and the +6V connection to supply the 5V for V1. Select the appropriate meter and adjust the voltages before you connect power to the circuit. Use the COM terminal to provide the 0V potentials (this will be the ground point to your circuit). The green terminal is a connection Date Last Modified: 2/5/2018 5:57 PM 3 to common ground and is not necessary for this experiment. It will not be connected in most of our experiments. You will be using the bench-attached DMM to measure the voltage across R1 and the current through R1. When you use a meter to measure a parameter of a circuit, the meter becomes part of the circuit! When using the multi-meter as a voltmeter, it has a huge internal resistance on the order of 50M Ohms. When using the multi-meter as an ammeter (current meter) it offers almost zero internal resistance. Therefore, when measuring different parameters, you will connect the meter differently! To measure the voltage across R1, get a red cord and a blue cord from your probe kit. Insert the red cord in the jack designated for Volt readings. Insert the blue cord in the common (black) jack in the middle. Attach a red clip and black clip to the other ends of the respective cords. Clip the red clip to the side of R1 that you expect to have the highest potential. Clip the black clip to the opposite side. Make sure that the V button is depressed on your meter when measuring voltage. Your meter should now display the voltage across R1. If the reading is negative, the side with the red clip is at a lower potential than the side with the black clip. Record this reading in your lab notebooks. Because the voltmeter has such a huge internal resistance, almost no current was diverted through the meter when taking the above reading. However, when we are taking current readings this will not be the case! Because the ammeter has almost no resistance, if you connect it in the same fashion as above, almost all of the current will be diverted through the ammeter and it will not pass through R1. You will have then made a huge change to your circuit! The ammeter must be connected in series with R1 to determine the current flowing through it. To do this, first shut the power off to your circuit. Then remove the high side lead of R1 from the breadboard. Connect it to the black lead of the ammeter. Now connect the red lead to the portion of the circuit where the high side of R1 was. Now on the meter, move the red cord from the voltmeter jack to the ammeter jack. Also, depress the mA button on the meter when measuring current. When you are sure you have made the correct connections go ahead and turn on the power to your circuit. Your meter should now display the current flowing through R1 in milliamps. If there is a negative sign in front of the reading, the current is flowing the opposite direction of what you expected. Record this measurement in your lab notebooks. Note. The current through R1 can be measured anywhere in its current path. For example, the ammeter can be inserted with the upper or lower terminal of the resistor. Either way the same current flowing through the resistor will be flowing through the ammeter. Date Last Modified: 2/5/2018 5:57 PM 4 Experiment 2. Using the Function Generator and Oscilloscope In this experiment you will generate three different waveforms using the function generator (FG) and display these waveforms using the oscilloscope. These waveforms are: Signals to be generated and screen captured 1. A 1 V amplitude square wave with a 1ms period 2. 2sin(ωt), where ω=2f, with f = 1.5 kHz. 3. A 0.5 V amplitude triangle wave with a 20ms period and a DC offset of +2V Experiment 2 Deliverables The deliverables for Experiment 2 are labeled images of the three different waveforms screen-captured from the oscilloscope to the computer. The parts of the image that should be labeled are: 1. The major waveform characteristics: amplitude (Peak-Peak), period (Period), frequency (Frequency) and DC offset (Average – N Cycles). 2. The Trigger Position indicator. 3. The Trigger Level. 4. The Ground Position Indicator. 5. The “Volts/Div” reading corresponding to the amplitude and “Time/Div” corresponding to the period The instructions that follow will show you how to set the FG and oscilloscope to display these waveforms, and then screen-capture the images of the waveforms to the computer. Using the BNC-to-BNC cable from your probe kit, connect the function generator (FG) output directly to the oscilloscope (use Channel 1) input as shown in Fig. 5 below. BNC-to-BNC Cable Figure 5. Date Last Modified: 2/5/2018 5:57 PM 5 Set the Frequency on the FG Press the “Freq” key on the FG to display the current frequency setting. To adjust this, you may do one of three things; you can use the arrows soft keys to adjust the frequency to the required number. Alternatively, you can turn the knob to increase or decrease the frequency.
Recommended publications
  • 1806-A Electronic Voltmeter, Manual
    OPERATING INSTRUCTIONS TYPE 1806-A ELECTRONIC VOLTMETER Form 1806-0100-C March, 1967 Copyright 1963 General Radio Company West Concord, Massachusetts, USA GENERAL RADIO COMPANY WEST CONCORD, MASSACHUSETTS, USA SPECIFICATIONS DC VO~TMETER Voltage Ro.nge: Four ranges, 1.5, 15, 150, and 1500 V, full scale, positive or negative. Minimum reading is 0.005 V. Input Resistance: 100 M!'l, ±5%; also "open grid" on all but the 1500-V range. Grid current is less than I0-10 A. Accuracy: ±2% of indicated value from one-tenth of full scale to full scale; ±0.2% of full scale from one-tenth of full scale to zero. Scale is logarithmic from one-tenth of full scale to full scale, permitting constant-percentage readability over that range. AC VOLTMETER Voltage Range: Four ranges, 1.5, 15, 150, and 1500 V, full scale. Minimum reading on most sensitive range is 0.1 V. Input Impedance: Probe, approximately 25 Mn in parallel with 2 pF; with TYPE 1806-P2 Range Multiplier, 2500 M!'l in parallel with 2 pF; at binding post on panel, 25 Mn in parallel with 30 pF. Accuracy: At 400 c/ s, ±2% of indicated value from 1.5 V to 1500 V; ±3% of indicated value from 0.1 V to 1.5 V. Waveform Error: On the higher ac-voltage ranges, the instrument operates as a peak voltmeter, calibrated to read rms values of a sine wave or 0.707 of the peak value of a complex wave. On distorted waveforms the percentage deviation of the reading from the rms value may be as large as the percentage of harmonics present.
    [Show full text]
  • The Accuracy Comparison of Oscilloscope and Voltmeter Utilizated in Getting Dielectric Constant Values
    Proceeding The 1st IBSC: Towards The Extended Use Of Basic Science For Enhancing Health, Environment, Energy And Biotechnology 211 ISBN: 978-602-60569-5-5 The Accuracy Comparison of Oscilloscope and Voltmeter Utilizated in Getting Dielectric Constant Values Bowo Eko Cahyono1, Misto1, Rofiatun1 1 Physics Departement of MIPA Faculty, Jember University, Jember – Indonesia, e-mail: [email protected] Abstract— Parallel plate capacitor is widely used as a sensor for many purposes. Researches which have used parallel plate capacitor were investigation of dielectric properties of soil in various temperature [1], characterization if cement’s dielectric [2], and measuring the dielectric constant of material in various thickness [3]. In the investigation the changing of dielectric constant, indirect method can be applied to get the dielectric constant number by measuring the voltage of input and output of the utilized circuit [4]. Oscilloscope is able to measure the voltage value although the common tool for that measurement is voltmeter. This research aims to investigate the accuracy of voltage measurement by using oscilloscope and voltmeter which leads to the accuracy of values of dielectric constant. The experiment is carried out by an electric circuit consisting of ceramic capacitor and sensor of parallel plate capacitor, function generator as a current source, oscilloscope, and voltmeters. Sensor of parallel plate capacitor is filled up with cooking oil in various concentrations, and the output voltage of the circuit is measured by using oscilloscope and also voltmeter as well. The resulted voltage values are then applied to the equation to get dielectric constant values. Finally the plot is made for dielectric constant values along the changing of cooking oil concentration.
    [Show full text]
  • Equivalent Resistance
    Equivalent Resistance Consider a circuit connected to a current source and a voltmeter as shown in Figure 1. The input to this circuit is the current of the current source and the output is the voltage measured by the voltmeter. Figure 1 Measuring the equivalent resistance of Circuit R. When “Circuit R” consists entirely of resistors, the output of this circuit is proportional to the input. Let’s denote the constant of proportionality as Req. Then VRIoeq= i (1) This is the same equation that we would get by applying Ohm’s law in Figure 2. Figure 2 Interpreting the equivalent circuit. Apparently Circuit R in Figure 1 acts like the single resistor Req in Figure 2. (This observation explains our choice of Req as the name of the constant of proportionality in Equation 1.) The constant Req is called “the equivalent resistance of circuit R as seen looking into the terminals a- b”. This is frequently shortened to “the equivalent resistance of Circuit R” or “the resistance seen looking into a-b”. In some contexts, Req is called the input resistance, the output resistance or the Thevenin resistance (more on this later). Figure 3a illustrates a notation that is sometimes used to indicate Req. This notion indicates that Circuit R is equivalent to a single resistor as shown in Figure 3b. Figure 3 (a) A notion indicating the equivalent resistance and (b) the interpretation of that notation. Figure 1 shows how to calculate or measure the equivalent resistance. We apply a current input, Ii, measure the resulting voltage Vo, and calculate Vo Req = (1) Ii The equivalent resistance can also be measured using and ohmmeter as shown in Figure 4.
    [Show full text]
  • Part 2 - Condenser Testers and Testing Correctly Part1 Condenser Testers and Testing Correctly.Doc Rev
    Part 2 - Condenser Testers and Testing Correctly Part1_Condenser_Testers_And_Testing_Correctly.doc Rev. 2.0 W. Mohat 16/04/2020 By: Bill Mohat / AOMCI Western Reserve Chapter If you have read Part 1 of this Technical Series on Condensers, you will know that the overwhelming majority of your condenser failures are due to breakdown of the insulating plastic film insulating layers inside the condenser. This allows the high voltages created by the “arcing” across your breaker points to jump through holes in the insulating film, causing your ignition system to short out. These failures, unfortunately, only happen at high voltages (often 200 to 500Volts AC)….which means that the majority of “capacitor testers" and "capacitor test techniques" will NOT find this failure mode, which is the MAJORITY of the condenser failure you are likely to encounter. Bottom line is, to test a condenser COMPLETELY, you must test it in three stages: 1) Check with a ohmmeter, or a capacitance meter, to see if the condenser is shorted or not. 2) Assuming your condenser is not shorted, use a capacitance meter to make sure it has the expected VALUE of capacitance that your motor needs. 3) Assuming you pass these first two step2, you then need to test your condenser on piece of test equipment that SPECIFICALLY tests for insulation breakdown under high voltages. (As mentioned earlier, you ohmmeter and capacitance meter only put about one volt across a capacitor when testing it. You need to put perhaps 300 or 400 times that amount of voltage across the condenser, to see if it’s insulation has failed, allowing electricity to “arc across" between the metal plates when under high voltage stress.
    [Show full text]
  • Voltage and Power Measurements Fundamentals, Definitions, Products 60 Years of Competence in Voltage and Power Measurements
    Voltage and Power Measurements Fundamentals, Definitions, Products 60 Years of Competence in Voltage and Power Measurements RF measurements go hand in hand with the name of Rohde & Schwarz. This company was one of the founders of this discipline in the thirties and has ever since been strongly influencing it. Voltmeters and power meters have been an integral part of the company‘s product line right from the very early days and are setting stand- ards worldwide to this day. Rohde & Schwarz produces voltmeters and power meters for all relevant fre- quency bands and power classes cov- ering a wide range of applications. This brochure presents the current line of products and explains associated fundamentals and definitions. WF 40802-2 Contents RF Voltage and Power Measurements using Rohde & Schwarz Instruments 3 RF Millivoltmeters 6 Terminating Power Meters 7 Power Sensors for URV/NRV Family 8 Voltage Sensors for URV/NRV Family 9 Directional Power Meters 10 RMS/Peak Voltmeters 11 Application: PEP Measurement 12 Peak Power Sensors for Digital Mobile Radio 13 Fundamentals of RF Power Measurement 14 Definitions of Voltage and Power Measurements 34 References 38 2 Voltage and Power Measurements RF Voltage and Power Measurements The main quality characteristics of a parison with another instrument is The frequency range extends from DC voltmeter or power meter are high hampered by the effect of mismatch. to 40 GHz. Several sensors with differ- measurement accuracy and short Rohde & Schwarz resorts to a series of ent frequency and power ratings are measurement time. Both can be measures to ensure that the user can required to cover the entire measure- achieved through utmost care in the fully rely on the voltmeters and power ment range.
    [Show full text]
  • (Ohmmeter). Aims: • Calibrating of a Sensitive Galvanometer for Measuring a Resistance
    Exp ( ) Calibrating of a sensitive galvanometer for measuring a resistance (Ohmmeter). Aims: • Calibrating of a sensitive galvanometer for measuring a resistance. The theory When a galvanometer is used as an ohmmeter for measuring an ohmic resistance R, the deviation angle θ of the galvanometer’s coil is directly proportional to the flowing current through the coil and inversely proportional to the value of the resistance. The deviation will reach to the maximum end when the resistance equals to zero or the current has the maximum value. For this reason, the scale will be divide by inversely way in comparison with the ammeter and the voltmeter. The original circuit as shown in Fig(1) consists of a dry cell(E) , rheostat and ammeter (A) are connected in series with small resistor s has the range of 1 omega. The two terminals of “s” are connected in parallel to another combination includes a sensitive galvanometer “G” which has internal resistance “r” and a resistors box “R”, this combination is called the measuring circuit. When the value of R equals zero, and by moving the rheostat in the original circuit, it is possible to set the flowing electric current in measuring the circuit as a maximum value od deviation in the galvanometer. By assigning different values of R, the deviation θ is decreasing with increasing the value of R or by another meaning when the flowing current through the galvanometer decreases. Therefore, the current through the galvanometer is inversely proportional to the value of R according the following Figure 1: Ohmmeter Circuit diagram equation; V=I(R+r) R=V/I-r or R=V/θ-r 1 | P a g e This is a straight-line equation between R and (1/θ) as shown in Fig(2).
    [Show full text]
  • Massachusetts Institute of Technology Department of Electrical Engineering and Computer Science
    Massachusetts Institute of Technology Department of Electrical Engineering and Computer Science 6.002 - Circuits and Electronics Fall 2004 Lab Equipment Handout (Handout F04-009) Prepared by Iahn Cajigas González (EECS '02) Updated by Ben Walker (EECS ’03) in September, 2003 This handout is intended to provide a brief technical overview of the lab instruments which we will be using in 6.002: the oscilloscope, multimeter, function generator, and the protoboard. It incorporates much of the material found in the individual instrument manuals, while including some background information as to how each of the instruments work. The goal of this handout is to serve as a reference of common lab procedures and terminology, while trying to build technical intuition about each instrument's functionality and familiarizing students with their use. Students with previous lab experience might find it helpful to simply skim over the handout and focus only on unfamiliar sections and terminology. THE OSCILLOSCOPE The oscilloscope is an electronic instrument based on the cathode ray tube (CRT) – not unlike the picture tube of a television set – which is capable of generating a graph of an input signal versus a second variable. In most applications the vertical (Y) axis represents voltage and the horizontal (X) axis represents time (although other configurations are possible). Essentially, the oscilloscope consists of four main parts: an electron gun, a time-base generator (that serves as a clock), two sets of deflection plates used to steer the electron beam, and a phosphorescent screen which lights up when struck by electrons. The electron gun, deflection plates, and the phosphorescent screen are all enclosed by a glass envelope which has been sealed and evacuated.
    [Show full text]
  • Using Multimeters
    ORESU-G1-77-005 C. 3 Usingmultimeters lVlarine electrorocs boats gPIII I,,",.", I,'59< ~4'pg,g!gg By EdwardKolbe DC voltmeter CommercialFisheries Engineer, OSU Marine ScienceCenter, Newport Most multirnetersare designedfor measuringboth DC and AC voltages. AssistantProfessor of Agricultural Engineering This bulletin concentrates on how to Oregon State University measureDC voltages;procedures for making AC measurementsare similar. First, plug one of the leadsinto the Multimeters measure electrical voltage, negativeterminal, properly called a resistance,and current, For wiring and jack, marked ! or "COM" for troubleshootingon boats,they can be common! . Standard electrical practice extremelyuseful. Applications include: usesthe black wire for the ground, checkingthe continuity of wiring which is usuallythe negativeterminal. locating breaksin opencircuits; testing The other lead usually red, to signify fusesand diodes;measuring battery the "hot" sideof the circuit! goesinto voltageand voltagedrop over wires and the positivejack, marked + !. After eIectricalloads; identifying "hot" and selectingthe proper DC voltagerange groundedwires; locatingshort circuitsor with the selector switch, measure DC smallcurrent leaks;and checking voltageby touchingthe -! lead to the alternator and generator output, negativeterminal or wire and the + ! A multimeter, also called a volt-ohm- lead to the positiveterminaI or wire. milliammeter VOM!, is actually three Selectingthe proper voltagerange is toob in one.It is a voltmetercapable of important. It is achieved
    [Show full text]
  • Electronic Voltmeters and Ammeters - Alessandro Ferrero, Halit Eren
    ELECTRICAL ENGINEERING – Vol. II - Electronic Voltmeters and Ammeters - Alessandro Ferrero, Halit Eren ELECTRONIC VOLTMETERS AND AMMETERS Alessandro Ferrero Dipartimento di Elettrotecnica, Politecnico di Milano, Italy Halit Eren Curtin University of Technology, Perth, Western Australia Keywords: currents, voltages, measurements, standards, analog voltmeters, digital voltmeters, microvoltmeters, oscilloscopes Contents 1. Introduction. 2. Analog Meters 2.1. DC Analog Voltmeters and Ammeters 2.2. AC Analog Voltmeters and Ammeters 2.3. True rms Analog Voltmeters 3. Digital Meters 3.1. Dual-Slope DVMs 3.2. Successive-Approximation ADCs 3.3. AC Digital Voltmeters and Ammeters 3.4. Frequency Response of AC Meters 4. Radio-Frequency Microvoltmeters 5. Vacuum-Tube Voltmeters and Oscilloscopes 5.1. Analog Oscilloscopes 5.2. Digital Storage Oscilloscopes (DSOs) 5.3. Portable Oscilloscopes 5.4. High-Voltage Oscilloscopes Appendix Glossary Bibliography Biographical Sketches Summary Voltage UNESCOand current measurements are – esse EOLSSntial parts of engineering and science. Instruments that measure voltages and currents are called voltmeters and ammeters, respectively. ThereSAMPLE are two distinct types of voltmeterCHAPTERS and ammeter, which differ from each other by the operating principle that they are based on: electromechanical instruments and electronic instruments, which also include oscilloscopes. Electromechanical voltmeters and ammeters, including thermal-type instruments, represent early technology, but still are used in many applications. Basic elements of voltages and currents from the basic physical principles have been introduced in the electromechanical voltage and current measurements section. Also, voltage and currents standards have been dealt with in detail in other articles. ©Encyclopedia of Life Support Systems (EOLSS) ELECTRICAL ENGINEERING – Vol. II - Electronic Voltmeters and Ammeters - Alessandro Ferrero, Halit Eren In this article, modern electronic voltmeters and ammeters are discussed.
    [Show full text]
  • TI S4 Audio Frequency Test Apparatus.Pdf
    TECHNICAL INSTRUCTION S.4 Audio-frequency Test Apparatus BRITISH BROADCASTING , CORPORATION ENGINEERING DlVlSlON - ', : . iv- TECHNICAL INSTRUCTION S.4 Third Issue 1966 instruction S.4 Page reissued May. 1966 CONTENTS Page Section I . Amplifier Detector AD14 . 1.1 Section 2 . Variable Attenuator AT119 . Section 3 . Wheatstone Bridge BG/I . Section 4 . Calibration IJnit CALI1 . Section 5. Harmonic Routine Tester FHP/3 . Section 6 . 0.B. Testing Unit 0BT/2 . Section . 7 . Fixed-frequency Oscillators OS/9. OS/ 10. OS/ IOA . Section 8 . Variable-frequency Oscillators TS/5 .. TS/7 . 1' . TS/8 . TS/9 . TS/ 10. TS/ 1OP . Section 9 . Portable Oscillators PTS/9 . PTS/IO . ... PTS/12 . PTS/13 . PTS/l5 .... PTS/l6 .... Appendix . The Zero Phase-shift Oscillator with Wien-bridge Control Section 10. Transmission Measuring Set TM/I . Section 1 I . Peak Programme Meter Amplifiers PPM/2 ..... PPM/6 . TPM/3 . Section 12 Valve Test Panels VT/4. VT/5 "d . Section 13. Microphone Cable Tester MCT/I . Section 14 . Aural Sensitivity Networks ASN/3. ASN/4 Section 15 . Portable Amplifier Detector PAD19 . Section 16. Portable Intermodulation Tester PIT11 Section 17. A.C. Test Meters ATM/I. ATM/IP . Section 18 . Routine Line Testers RLT/I. RLT/IP . Section 19. Standard Level Panel SLP/3 . Section 20 . A.C. Test Bay AC/55 . Section 21 . Fixed-frequency Oscillators: OS2 Series Standard Level Meter ME1611 . INSTRUCTION S.4 Page reissued May 1966 ... CIRCUIT DIAGRAMS AT END Fig. 1. Amplifier Detector AD14 Fig. 2. Wheatstone Bridge BG/1 Fig. 3. Harmonic Routine Tester FHP/3 Fig. 4. Oscillator OS/9 Fig.
    [Show full text]
  • A History of Impedance Measurements
    A History of Impedance Measurements by Henry P. Hall Preface 2 Scope 2 Acknowledgements 2 Part I. The Early Experimenters 1775-1915 3 1.1 Earliest Measurements, Dc Resistance 3 1.2 Dc to Ac, Capacitance and Inductance Measurements 6 1.3 An Abundance of Bridges 10 References, Part I 14 Part II. The First Commercial Instruments 1900-1945 16 2.1 Comment: Putting it All Together 16 2.2 Early Dc Bridges 16 2.3 Other Early Dc Instruments 20 2.4 Early Ac Bridges 21 2.5 Other Early Ac Instruments 25 References Part II 26 Part III. Electronics Comes of Age 1946-1965 28 3.1 Comment: The Post-War Boom 28 3.2 General Purpose, “RLC” or “Universal” Bridges 28 3.3 Dc Bridges 30 3.4 Precision Ac Bridges: The Transformer Ratio-Arm Bridge 32 3.5 RF Bridges 37 3.6 Special Purpose Bridges 38 3,7 Impedance Meters 39 3.8 Impedance Comparators 40 3.9 Electronics in Instruments 42 References Part III 44 Part IV. The Digital Era 1966-Present 47 4.1 Comment: Measurements in the Digital Age 47 4.2 Digital Dc Meters 47 4.3 Ac Digital Meters 48 4.4 Automatic Ac Bridges 50 4.5 Computer-Bridge Systems 52 4.6 Computers in Meters and Bridges 52 4.7 Computing Impedance Meters 53 4.8 Instruments in Use Today 55 4.9 A Long Way from Ohm 57 References Part IV 59 Appendices: A. A Transformer Equivalent Circuit 60 B. LRC or Universal Bridges 61 C. Microprocessor-Base Impedance Meters 62 A HISTORY OF IMPEDANCE MEASUREMENTS PART I.
    [Show full text]
  • Model 372 Series 3 Ohmmeter INSTRUCTION MANUAL
    Model 372 Series 3 Ohmmeter INSTRUCTION MANUAL About this Manual To the best of our knowledge and at the time written, the information contained in this document is technically correct and the procedures accurate and adequate to operate this instrument in compliance with its original advertised specifications. Notes and Safety Information This Operator’s Manual contains warning headings which alert the user to check for hazardous conditions. These appear throughout this manual where applicable and are defined below. To ensure the safety of operating performance of this instrument, these instructions must be adhered to. Warning, refer to accompanying documents. Caution, risk of electric shock. Technical Assistance SIMPSON ELECTRIC COMPANY offers assistance Monday through Friday, 8:00 am to 4:30 pm Central Time. Contact Technical Support or Customer Service at (715) 588-3311 or visit our website at http://www.simpsonelectric.com Warranty and Returns SIMPSON ELECTRIC COMPANY warrants each instrument and other articles manu- factured by it to be free from defects in material and workmanship under normal use and service, its obligation under this warranty being limited to making good at its factory or other article of equipment which shall within one (1) year after delivery of such instrument or other article of equipment to the original purchaser be returned intact to it, or to one of its authorized service centers, with transportation charges prepaid, and which its examination shall disclose to its satisfaction to have been thus defective; this warranty being expressly in lieu of all other warranties expressed or implied and of all other obligations or liabilities on its part, and SIMPSON ELECTRIC COMPANY neither assumes nor authorizes any other persons to assume for it any other liability in connection with the sales of its products.
    [Show full text]