Steady-State Analysis of PWM Z-Bridge Source DC-DC Converter

Total Page:16

File Type:pdf, Size:1020Kb

Steady-State Analysis of PWM Z-Bridge Source DC-DC Converter Steady-State Analysis of PWM Z-Bridge Source DC-DC Converter A thesis submitted in the partial fulfillment of the requirements for the degree of Master of Science in Electrical Engineering By Lokesh Kathi B.Tech., Koneru Lakshmaiah University, Guntur, India, 2013 2015 Wright State University WRIGHT STATE UNIVERSITY GRADUATE SCHOOL January 5, 2016 I HEREBY RECOMMEND THAT THE THESIS PREPARED UNDER MY SUPERVISION BY Lokesh Kathi ENTITLED Steady-State Analysis of PWM Z- Bridge Source DC-DC Converter BE ACCEPTED IN PARTIAL FULFILLMENT OF THE REQUIREMENTS FOR THE DEGREE OF Master of Science in Electrical Engineering. ‘ Marian K. Kazimierczuk, Ph.D. Thesis Director Brian Rigling, Ph.D. Chair Department of Electrical Engineering College of Engineering and Computer Science Committee on Final Examination Marian K. Kazimierczuk, Ph.D. Yan Zhuang, Ph.D. Lavern Alan Starman, Ph.D. Robert E. W. Fyffe, Ph.D. Vice President for Research and Dean of the Graduate School Abstract Lokesh, Kathi. M.S.E.E., Department of Electrical Engineering, Wright State Uni- versity, 2015. Steady-state analysis of pulse-width modulated (pwm) z-bridge source dc-dc converter. A pwm z-bridge source dc-dc converter has a potential to play a prominent role in renewable energy applications, as it provides boosted and regulated output voltage and also behaves as an intermediate buffer between the source and the load. A complete circuit analysis of the z-bridge source converter is needed to understand the operation of this converter. Steady-state analysis of pulse-width modulated (pwm) z-bridge source dc-dc converter operating in continuous conduction mode (ccm) is given. Expressions describing waveforms of voltages across and currents through the all components of the pwm z-bridge source dc-dc converter to operate in steady- state condition are derived. The output-to-input voltage conversion ratio for ideal (lossless) and non-ideal (lossy) conditions are derived. Expressions for the minimum z-network inductance, the minimum filter inductance, and the minimum z-network capacitor are derived to operate converter in ccm. To determine the total power loss in pwm z-bridge source dc-dc converter, power loss expressions for each and every component and the overall efficiency of the pwm z-bridge source dc-dc converter are determined. Using power loss expressions, the efficiency analysis graphs are plotted using matlab to obtain the suitable operating region for the pwm z-bridge source dc-dc converter in terms of duty cycle, output current, and input voltage. An example of pwm z-bridge source dc-dc converter is considered and steady-state analysis is performed in saber. The simulation reults of designed pwm z-bridge source dc-dc converter are used to validate the theoretical results.Plant characteristics of pwm z-bridge source dc-dc converter are performed and the results are reported. iii Contents 1 Introduction 2 1.1 Switching-Mode Voltage Regulators . ... 2 1.2ThesisObjectives .............................. 3 1.3ThesisOutline................................ 3 2 Overview of Z-Source Inverters 5 2.1OriginofZ-SourceNetwork . 5 2.2Z-SourceInverters.............................. 6 2.3 PWM Z-Source DC-DC Converter with a Simplified Circuit Representation ............................... 11 2.4 Transfiguration of PWM Z-Source DC-DC Converter circuit to a Circuit of Simplified Bridge Network Representation . 12 3 Steady-State Analysis of PWM Z-Bridge Source DC-DC Converter in CCM 14 3.1 Circuit description of a PWM Z-Bridge Source Converter . ..... 14 3.2Assumptions................................. 14 3.3 Shoot-Through State (Time Interval 0 <t ≤ DT ) ............ 16 3.4 Non Shoot-Through State (Time Interval DT <t ≤ T ) ......... 19 3.5 DC Voltage Transfer Function (MV DC ).................. 25 4 Derivations of Expressions for Passive Components 27 4.1 Minimum Inductance of Z-Network Inductor to Operate in CCM.... 27 4.2 Minimum Inductance of Filter Inductor to Operate in CCM . ..... 29 iv 4.3 Minimum Capacitance Values for Z-Network and Filter Capacitors in CCM..................................... 31 4.3.1 Minimum Capacitance of Z-Network Capacitor in CCM at Shoot-Through State (0 <t ≤ DT )................. 31 4.3.2 Minimum Capacitance of Z-Network Capacitor in CCM at Non Shoot-Through State (DT <t ≤ T )................. 33 4.4 Design Example and Simulation Results . 34 4.5 Efficiency, Power Losses, and DC Voltage Conversion Factor of Z-BridgeSourceDC-DCConverter . 39 5 Plant Characteristics of PWM Z-Bridge Source DC-DC Converter in CCM 44 5.1 PWM Z-Bridge Source DC-DC Converter with Varying Duty Cycle . 44 5.2 PWM Z-Bridge Source DC-DC Converter With Varying Load Resistance 46 5.3 PWM Z-Bridge Source DC-DC Converter With Varying Input Voltage . 49 6 Conclusion 52 6.1Summary .................................. 52 6.2FutureWork................................. 53 6.3ThesisContributions ............................ 53 7 Bibliography 55 v List of Figures 2.1 Circuit of a x-shaped z-source network. 5 2.2 Circuit of a z-source bridge network. 6 2.3 Circuit of Wheatstone bridge network. 7 2.4 Circuit of the basic framework of a z-source converter/inverter for all types of power conversions. (a) Circuit with the z-source x-shaped network. (b) Circuit with the z-source bridge network. 8 2.5 Circuit of multi-level inverter with z-source bridge network at shoot-through state. (a) Circuit, when the switch is on. (b) Equivalent circuit, when the switch is on. 9 2.6 Circuit of multi-level inverter with the z-source bridge network at non-shoot-through state.. (a) Circuit, when the switch is off. (b) Equivalent circuit, when the switch is off. 11 2.7 Circuit of the pwm dc-dc converter with z-source x-shaped network. 12 2.8 Simplified circuit representation of pwm z-bridge source dc-dc converter. 12 3.1 Circuit of a pwm z-bridge source dc-dc converter. 14 3.2 Circuit of the pwm z-bridge source dc-dc converter with identical z-network inductors and capacitors. 16 vi 3.3 Circuit of the pwm z-bridge source dc-dc converter, when switch is on and diode is off. 16 3.4 pwm z-bridge source dc-dc converter at shoot-through state. (a) Equivalent circuit with Kirchoff current loops, when the switch is on and diode is off. (b) Equivalent circuit with the filter circuit replaced with dc current source iLf . (c) Equivalent circuit with the two z-network inductor L and capacitor C network are replaced with two ac current sources iL 18 3.5 Circuit of the pwm z-bridge source dc-dc converter, when the switch is off & the diode is on. 20 3.6 Simplified circuit of the pwm z-bridge source dc-dc converter with Kirchoff voltage loops, when the switch is off and the diode is on. 20 3.7 Equivalent circuit of the pwm z-bridge source dc-dc converter with the filter circuit is replaced with a dc current source, when the switch is off and the diode is on. 21 3.8 Circuit of the pwm z-bridge source dc-dc converter with Kirchoff current loops, when the switch is off and the diode is on. 21 3.9 Voltage waveforms of the z-bridge source dc-dc converter in ccm. 23 3.10 Current waveforms of the z-bridge source dc-dc converter in ccm. 24 4.1 ccm/dcm boundary of pwm z-bridge source dc-dc converter for normalized load current with respect to z-network inductance as a function of duty cycle. 28 vii 4.2 ccm/dcm boundary of pwm z-bridge source dc-dc converter for normalized load resistance with respect to z-network inductance as a function of duty cycle. 28 4.3 ccm/dcm boundary of pwm z-bridge source dc-dc converter for normalized load current with respect to filter inductance as a function of duty cycle. 30 4.4 ccm/dcm boundary of pwm z-bridge source dc-dc converter for normalized load resistance with respect to filter inductance as a function of duty cycle. 30 4.5 ccm/dcm boundary of pwm z-bridge source dc-dc converter for normalized filter inductance with respect to z-network inductance as a function of duty cycle. 31 4.6 Variation in efficiency η as a function of output current IO of z-bridge source dc-dc converter 35 4.7 Power and output voltage waveforms of pwm z-bridge source dc-dc converter in ccm. 38 4.8 Current waveforms of z-network inductor and filter inductor of pwm z-bridge source dc-dc converter in ccm. 38 4.9 Variation in efficiency η as a function of input voltage VI of pwm z-bridge source dc-dc converter. 41 4.10 Variation in efficiency η as a function of load resistance RL of z-bridge source dc-dc converter. 41 viii 4.11 Variation in efficiency η as a function of to duty cycle D of z-bridge source dc-dc converter. 42 4.12 Variation in dc voltage conversion factor MV DC as a function of duty cycle D of z-bridge source dc-dc converter. 42 4.13 Variation in duty cycle D as a function of output current IO of z-bridge source dc-dc converter. 43 4.14 Variation in efficiency η as a function of output current IO of z-bridge source dc-dc converter. 43 5.1 Circuit of the pwm z-bridge source dc-dc converter circuit with the varying duty cycle. 44 5.2 Gate-source voltage, output voltage, and power waveforms of the pwm z-bridge source dc-dc converter with the varying duty cycle. 45 5.3 Z-network capacitor voltage and output voltage waveforms of the pwm z-bridge source dc-dc converter with the varying duty cycle.
Recommended publications
  • MGM's Jawaharlal Nehru Engineering College
    MGM’s Jawaharlal Nehru Engineering College Laboratory Manual Electrical Power Transmission & Distribution For Second Year (EEP) Students Manual made by Prof. P.A. Gulbhile AuthorJNEC,Aurangabad. FORWARD It is my great pleasure to present this laboratory manual for second year EEP engineering students for the subject of Electrical Power Transmission & Distribution. Keeping in view the vast coverage required for visualization of concepts of Electrical Power Transmission with simple language. As a student, many of you may be wondering with some of the questions in your mind regarding the subject and exactly what has been tried is to answer through this manual. Faculty members are also advised that covering these aspects in initial stage itself, will greatly relieved the minfuture as much of the load will be taken care by the enthusiasm energies of the students once they are conceptually clear. H.O.D. LABORATORY MANNUAL CONTENTS This manual is intended for the second year students of Electrical Electronics & Power engineering branch in the subject of Electrical Power Transmission & Distribution. This manual typically contains practical/Lab Sessions related layouts, sheets of different parts in electrical power transmission & distribution system as well as study of different models of transmission line, measurement of parameters of transmission line and various aspects related the subject to enhance understanding. Although, as per the syllabus, only descriptive treatment is prescribed ,we have made the efforts to cover various aspects of electrical Power Transmission & Distribution subject covering types of different transmission lines , their circuit diagrams and phasor diagrams, electrical design of overhead transmission line , electrical design of overhead transmission line, elaborative understandable concepts and conceptual visualization.
    [Show full text]
  • Physics 517/617 Experiment 1 Instrumentation and Resistor Circuits
    Physics 517/617 Experiment 1 Instrumentation and Resistor Circuits 1) Study the operation of the oscilloscope, multimeter, power supplies, and wave generator. For the oscilloscope you should try to understand the function of all the knobs or buttons on the front panel. Some buttons may have several functions and some of the functions will not be relevant for this class. Try to follow the examples in p. 38-42 of the instruction manual. 2) Verify Ohm’s law by measuring and then plotting voltage vs. current for a resistor. Fit your graph(s) to extract the measured resistance. Use a resistor of your choice. Repeat the measurement with a resistor of a much higher value (e.g. 10-100X) than your previous choice. Use a DC power supply for the circuit. 3) Measure the DC resistance of your multimeter (on voltage scale) using a resistor divider, which consists of two resistors in series with one of them being the multimeter resistor. How does your measurement of the multimeter’s resistance compare to the specs of the meter? Note: You do not need to measure the current in this experiment. 4) The RMS (Root Mean Square) value of a voltage (or current) is defined as t 1 2 VRMS = Ú V dt t 0 Show that VRMS = V0 / 2 for a sine wave voltage, V = V0 sinwt. Note: The multimeter only measures the RMS value of a voltage or current. † 5)† This exercise is intended to make you† familiar with some of the very useful functions of the oscilloscope. Send a 1 kHz sine wave with an amplitude of 1 V and DC offset of 1 V into the scope.
    [Show full text]
  • Realization of AC Bridges Using Labview. Details: Explanation
    Realization of AC Bridges Using LabView. Introduction: AC Bridges are used to measure the values of unknown resistance, inductance, and capacitance. Although, AC bridges are believed to be very convenient and provides accurate result of the measurement. The construction of the bridges is very simple. The bridge has four arms, one AC supply source and the balance detector. It works on the principle that the balance ratio of the impedances will give the balance condition to the circuit which is determined by the null detector. The bridges have four arms, two have non-inductive resistance and the other two have inductances with negligible resistance. Software Used: LabView LabVIEW is essentially a graphical programming language (technically it’s a development environment, and the language is “G”, but in common usage it’s a language). Instead of typing words like with C++,Python, or other text-based languages, you place and connect visual objects around your screen. Using LABVIEW the AC bridges can be Solved at an ease with proper visualization and insights. The graphical programming approach enables us to build or Solve AC bridges for different number of applications such as measuring the frequency of the audio signals, filtration of undesirable signals etc. Details: AC Bridges that have been analyzed using LabView are: (1) Maxwell’s Inductance Bridge. (2) DeSauty’s Capacitance Bridge. (3) Wheatstone’s Resistance Bridge. Explanation: Maxwell’s Inductance Bridge: A Maxwell bridge is a modification to a Wheatstone bridge used to measure an unknown inductance in terms of calibrated resistance and inductance or resistance and capacitance. Let us consider w=314, Let us consider E to be a constant (let it be 100V).
    [Show full text]
  • Department of Physics Second Allied Physics Iii
    KUNTHAVAI NAACHIYAR GOVERNMENT ARTS COLLEGE FOR WOMEN, THANJAVUR. DEPARTMENT OF PHYSICS SECOND ALLIED PHYSICS III 18K4CHAP3 UNIT - I 1. Dr. S. SNEGA, DEPARTMENT OF PHYSICS, THANJAVUR. UNIT - II 2. Dr. N. GEETHA, DEPARTMENT OF PHYSICS, THANJAVUR. UNIT-III 3. Ms. D.S. VASANTHI DEPARTMENT OF PHYSICS, THANJAVUR. UNIT-I: CURRENT ELECTRICITY AND NUCLEAR PHYSICS Kirchhoff’s law –Wheatstone’s bridge – Metre Bridge – Carey foster’s bridge – Measurement of specific resistance – Potentiometer – Calibration of low range voltmeter Nucleus – Nuclear Size – Charge – Mass and Spin – Shell Model – Nuclear fission and fusion – Liquid drop model – Binding energy – Mass defect KIRCHHOFF’S RULES Ohm’s law is useful only for simple circuits. For more complex circuits, Kirchhoff ’s rules can be used to find current and voltage. There are two generalized rules: i) Kirchhoff ’s current rule ii) Kirchhoff ’s voltage rule. Kirchhoff’s first rule (Current rule or Junction rule) It states that the algebraic sum of the currents at any junction of a circuit is zero. It is a statement of conservation of electric charge. All charges that enter a given junction in a circuit must leave that junction since charge cannot build up or disappear at a junction. Current entering the junction is taken as positive and current leaving the junction is taken as negative. I1 + I2 – I3 – I4 – I5 = 0 (or) I1 + I2 = I3 + I4 + I5 Kirchhoff’s Second rule (Voltage rule or Loop rule) It states that in a closed circuit the algebraic sum of the products of the current and resistance of each part of the circuit is equal to the total emf included in the circuit.
    [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]
  • I INVESTIGATION of METHODS for DETECTING NEEDLE INSERTION INTO BLOOD VESSELS by Ehsan Qaium BS in Mechanical Engineering, Virgi
    INVESTIGATION OF METHODS FOR DETECTING NEEDLE INSERTION INTO BLOOD VESSELS by Ehsan Qaium BS in Mechanical Engineering, Virginia Tech, 2012 Submitted to the Graduate Faculty of the Swanson School of Engineering in partial fulfillment of the requirements for the degree of Master of Science in Mechanical Engineering University of Pittsburgh 2018 i UNIVERSITY OF PITTSBURGH SWANSON SCHOOL OF ENGINEERING This thesis was presented by Ehsan Bin Qaium It was defended on April 19,2018 and approved by William Clark, PhD, Professor Jeffrey Vipperman, PhD, Professor Cameron Dezfulian, MD, Associate Professor Thesis Advisor: William Clark, PhD, Professor ii Copyright © by Ehsan Qaium 2018 iii INVESTIGATION OF METHODS FOR DETECTING NEEDLE INSERTION INTO BLOOD VESSELS Ehsan Qaium, M.S. University of Pittsburgh, 2018 Peripheral intravenous IV (pIV) placement is the mainstay for providing therapies in modern medicine. Although common, approximately 107 million difficult pIV placements each year require multiple attempts to establish IV access. Delays in establishing IV access lead to increased patient pain, delayed administration of life saving medicine, and increased cost to the institution. Current solutions involve using visual vein finders, ultrasounds and a central line if peripheral IV insertion attempts fail. The objective of this study was to investigate methods by which entry into a blood vessel could be detected, and to design and test a novel medical device that increases the likelihood of successful pIV placement on the first attempt. Two types of measurement methods (static and transient) were investigated in this study. Static measurement involved measurements performed with a multimeter and a Wheatstone bridge. The multimeter measurement was unsuccessful due to the effect of polarization.
    [Show full text]
  • Basic Bridge Circuits
    AN117 Dataforth Corporation Page 1 of 6 DID YOU KNOW ? Samuel Hunter Christie (1784-1865) was born in London the son of James Christie, who founded Christie's Fine Art Auctioneers. Samuel studied mathematics at Trinity College and, upon graduation, taught mathematics at the Royal Military Academy for almost 50 years. Christie made many contributions to magnetic science, such as the dependence of magnetic forces on temperature and solar ray effects on terrestrial magnetism. In 1833, he published a paper on the magneto-electric conductivity of various metals, illustrating how wire conductance varies inversely with length and directly as the square of wire diameter. Embedded in this paper was the description of a circuit used to measure and compare wire conductance. Charles Wheatstone (an English physicist and inventor) recognized the value of Christie's circuit; he was the first to put this circuit, which bears his name, to extensive use and to develop many significant applications for it. To this day (162 years later), the Wheatstone bridge remains the most sensitive and accurate method for precisely measuring resistance values. Samuel Christie never got recognition for his bridge circuit. At a royalty of five cents for every bridge circuit used, imagine what Christie’s original circuit invention would be worth today. Basic Bridge Circuits Preamble Analytical investigations throughout this document focus Bridge circuits have been in use for well over 150 years. on the R-ohm type bridge, which means all bridge To date, the bridge is still the most economical circuit resistors are “R” ohms when not exposed to the field technique for accurately measuring resistance.
    [Show full text]
  • Shunt Calibration of Strain Gage Instrumentation
    MICRO-MEASUREMENTS Strain Gages and Instruments Tech Note TN-514 Shunt Calibration of Strain Gage Instrumentation I. Introduction the gage. Furthermore, the electrical contacts for inserting the resistor can introduce a significant uncertainty in The need for calibration arises frequently in the use the resistance change. On the other hand, decreasing of strain gage instrumentation. Periodic calibration is the resistance of a bridge arm by shunting with a larger required, of course, to assure the accuracy and/or linearity resistor offers a simple, potentially accurate means of of the instrument itself. More often, calibration is necessary simulating the action of a strain gage. This method, known to scale the instrument sensitivity (by adjusting gage factor as shunt calibration, places no particularly severe tolerance or gain) in order that the registered output correspond requirements on the shunting resistor, and is relatively conveniently and accurately to some predetermined input. insensitive to modest variations in contact resistance. It is An example of the latter situation occurs when a strain also more versatile in application and generally simpler to gage installation is remote from the instrument, with implement. measurable signal attenuation due to leadwire resistance. In this case, calibration is used to adjust the sensitivity Because of its numerous advantages, shunt calibration is of the instrument so that it properly registers the strain the normal procedure for verifying or setting the output signal produced by the gage. Calibration is also used to set of a strain gage instrument relative to a predetermined the output of any auxiliary indicating or recording device mechanical input at the sensor.
    [Show full text]
  • CHAPTER-7 Underground Cables
    CHAPTER-7 Underground Cables Construction of Underground Cables: Fig.shows the general Construction of Underground Cables. The various parts are : Cores or Conductors: A cable may have one or more than one core (conductor) depending upon the type of service for which it is intended. For instance, the 3-conductor cable shown in Fig. 11.1 is used for 3- phase service. The conductors are made of tinned copper or aluminium and are usually stranded in order to provide flexibility to the cable. Insulation: Each core or conductor is provided with a suitable thickness of insulation, the thickness of layer depending upon the voltage to be withstood by the cable. The commonly used materials for insulation are impregnated paper, varnished cambric or rubber mineral compound. Metallic sheath: In order to protect the cable from moisture, Conductor gases or other damaging liquids (acids or alkalies) in the soil and atmosphere, a metallic sheath of lead or aluminium is provided over the insulation as shown in Fig. 11.1 Bedding: Over the metallic sheath is applied a layer of bedding which consists of a fibrous material like jute or hessian tape. The purpose of bedding is to protect the metallic sheath against corrosion and from mechanical injury due to armouring. Armouring: Over the bedding, armouring is provided which consists of one or two layers of galvanised steel wire or steel tape. Its purpose is to protect the cable from mechanical injury while laying it and during the course of handling. Armouring may not be done in the case of some cables. Serving: In order to protect armouring from atmospheric conditions, a layer of fibrous material (like jute) similar to bedding is provided over the armouring.
    [Show full text]
  • Applying the Wheatstone Bridge Circuit by Karl Hoffmann
    Applying the Wheatstone Bridge Circuit by Karl Hoffmann W1569-1.0 en Applying the Wheatstone Bridge Circuit by Karl Hoffmann Contents: 1 Introduction ...................................................................................................................................1 2 Elementary circuits with strain gages..........................................................................................5 2.1 Measurements on a tension bar..............................................................................................6 2.2 Measurements on a bending beam.........................................................................................7 2.3 Measurements on a twisted shaft ...........................................................................................8 3 Analysis and compensation of superimposed stresses, e.g. tension bar with bending moment .........................................................................................................................................10 4 Compensation of interference effects, especially temperature effects....................................14 5 Compensation of the influence of lead resistances. ..................................................................17 6 Table on different circuit configurations ..................................................................................20 7 Some remarks on the limits of the compensation of interference effects ...............................22 8 The linearity error of the Wheatstone bridge circuit...............................................................23
    [Show full text]
  • Practical Applications of Maxwell Bridge
    Practical Applications Of Maxwell Bridge Autogenous Chevy resort no idolaters sanitised irreconcilably after Sanson dung afar, quite hypostatic. If predicatory or tawdry Lyndon usually lie-in his andbeating tartly. shore overfondly or respray consequently and powerful, how oaken is Rog? Carbonated Nathanial resolving: he jut his Samaritanism impoliticly Fundamentals Of Electromagnetics With Engineering Applications. This pointed the way stay the application of electromagnetic radiation for such. The result is magnificent full-color modern narrative that bridges the various EE and. Presents the introductory theory and applications of Maxwell's equations to. Ii The weakening of springs due to frequent usage and temperature effects. Wheatstone Bridge Circuit Theory Example and Applications. Diploma Examination Dip IETE. Collaboratives might include proprioception, applications it expecting a practical applications back to practical. Related with Inverse Problems For Maxwell's Equations 349349-file. ACBridges are those circuits which are used to measured the unknown resistances. The first practical application outside of laboratory experiments was confuse the 1950s as a. Computational Electromagnetics Domain Decomposition. If the ultracapacitors within a large scale in assisting persons separated from the use of applications much more than for. Determining the correct Ultracapacitor for the application 4. UNIT II AC Bridge Measurement RGPV. What wood the applications of union bridge circuit Quora. And helps to really the decade between multi-scale and multi-physics and the hands-on. Handbook of Electronics Formulas and Calculations Volume 2. A Practical Instrumentation Amplifier-Based Bridge Circuit 350. ' z 2 rr. 1311 Maxwell's Equations for Static Electric Field 374. EMIR in DC Maxwell School. A practical form of Wheatstone bridge that consequence be used for measuring.
    [Show full text]
  • 2102311 Electrical Measurement and Instruments (Part II)
    2102311 Electrical Measurement and Instruments (Part II) ¾ Bridge Circuits (DC and AC) ¾ Electronic Instruments (Analog & Digital) ¾ Signal Generators ¾ Frequency and Time Interval Measurements ¾ Introduction to Transducers อาภรณ ธีรมงคลรศมั ี ตึกไฟฟา 6 ชนั้ หอง 306 Textbook: -A.D. Helfrick, and W.D. Cooper, “Modern Electronic Instrumentation and Measurement Techniques” Prentice Hall, 1994. - D.A. Bell, “Electronic Instrumentation and Measurements”, 2nd ed., Prentice Hell, 1994. ResistorResistor TypesTypes Importance parameters Value Tolerance Power rating Temperature coefficient Type Values (Ω) Power rating Tolerance (%) Temperature picture (W) coefficient (ppm/°C) Wire wound 10m~3k (power) 3~1k ±1~±10 ±30~±300 Wire wound (precision) 10m~1M 0.1~1 ±0.005~±1 ±3~±30 Carbon film 1~1M 0.1~3 ±2~±10 ±100~±200 Metal film 100m~1M 0.1~3 ±0.5~±5 ±10~±200 Metal film (precision) 10m~100k 0.1~1 ±0.05~±5 ±0.4~±10 Metal oxide film 100m~100k 1~10 ±2~±10 ±200~±500 Data: Transistor technology (10/2000) Resistor Values Color codes Resistor Values Alphanumeric 4 band color codes Color Digit Multiplier Tolerance Temperature (%) coefficient (ppm/°C) Most sig. fig. of value Silver 10-2 ±10 K Tolerance - - - Least sig. fig. Multiplier Gold 10-1 J of value ±5 Ex. Black 0 100 - - ±250 K Brown 1 101 ±1 F ±100 H Red 2 102 ±2 G ±50 G Green 3 Red Orange 3 10 - ±15 D Blue Brown - Yellow 4 104 - ±25 F R = 560 Ω ±2% Green 5 5 D E 10 ±0.5 ±20 Alphanumeric Blue 6 106 ±0.25 C ±10 C Violet 7 107 ±0.1 B ±5 B R, K, M, G, and T = 0 3 6 9 12 Gray 8 108 - ±1 A x10 , x10 , x10 , x10 , and x10 - White 9 109 - Ex.
    [Show full text]