Mutual Inductance. L (1) l

Size: px
Start display at page:

Download "Mutual Inductance. L (1) l"

Transcription

1 Mutual Inductance Developers Objectives Preparation Background JD Mitchell, AB Overby and K Meehan The objectives of this experient are to design and construct a transforer and deterine its losses as well as odeling it in Pspice. Read section 9.0 of Engineering Electroagnetics, section 3. of Fundaentals of Electric Circuits, and the pages 6 30 of PSpice For Basic Circuit Analysis regarding self inductance and utual inductance. Inductance (L), or self-inductance, is the ratio of the linkage agnetic flux to the current (I) producing the flux (Edinister 69). Flux linkage is the product of the nuber of turns (N), linking each of those turns. Inductance has units of henries (H), and the agnetic flux Wb where one Henry is ual to one Weber-turn per Apere. Eqs. shows a forula for A the inductance of a solenoid, where µ is the pereability of the core, N is the nuber of turns, S is the cross sectional area, and l is the length of the solenoid. N S L () l Note that Eqs. is applicable only to linear edia, in which the flux is proportional to the current (Buck 93). Inductance can also be defined as the property whereby an inductor exhibits opposition to a change in the current flowing through it (Alexander 6). Mutual Inductance When two coils are in close proxiity to each other the flux which results fro current flow, in one coil will link with the other coil inducing current flow in that coil. Mutual inductance (M), easured in henries, is the ability of an inductor to induce current flow across another inductor in close proxiity (Alexander 557). Mutual inductance is illustrated in Figure. M L L I Figure : Flux is generated by current flowing through L. The flux which links to L is while the flux which links to L is. When the agnetic flux of an inductor links to another inductor the two inductors are said to be agnetically coupled. The total agnetic flux, shown in Eqs., is the su of each flux

2 coponent. In Eqs., represents the flux which links to L while represents the flux which links to L. The voltage () induced in L is given by: The voltage () induced in L is given by: The utual inductance is given by or Transforers () d N (N = nuber of turns of L) (3) dt d N (N = nuber of turns of L) (4) dt d M N (5) di NN S (6) l M A transforer is a device coprising of two or ore coils, usually sharing the sae core. Transforers take advantage of utual inductance for various purposes, including stepping up and stepping down voltage, circuit isolation, and filtering. The side of a transforer connected to a voltage source is called the priary winding while the side of a transforer connected to a load is called the secondary winding. The circuit in figure shows an ideal transforer which has no losses. However, all practical transforers have losses which are caused by the resistance of the copper windings, R, the core losses due to hysteresis, R, flux leakages to the air,, and the finite pereability of the core,. An uivalent circuit for the non-ideal transforer is shown in figure. Figure : Non-ideal transforer uivalent circuit. R RM M Ideal Transforer

3 To find the values of R,, R, and two tests are used: the open circuit test and the short circuit test. The open circuit test involves easuring the current passing through the priary winding of the transforer and the power dissipated by the priary winding while the secondary winding is open. The short circuit test involves the sae procedure as the open circuit test except that the secondary winding is shorted. Figures 3 and 4 show the wire diagras for the open circuit test and the short circuit test respectively. Figure 3: Open circuit test wire diagra. Diagra courtesy of Figure 4: Short circuit test wire diagra. Diagra courtesy of irginia Tech ECE departent The results fro the short and open circuit tests provide the expressions for the losses associated with non-ideal transforers. These expressions are given below, where, I,, and I are open circuit voltage, open circuit current, short circuit voltage, and short circuit current respectively. R (7) P (8) I RM P (9) I R I R (0)

4 References Edinister, J., & Edinister, J. (0). Schau's outline of electroagnetics. New York: McGraw-Hill. Charles K. Alecander and Matthew N.O. Sadik, (004). Fundaentals of Electric Circuits, 4 th edittion, McGraw-Hill. Hayt, W. H., & Buck, J. A. (006). Engineering electroagnetics. Boston: McGraw-Hill Higher Education. Tront, J. G. (005). Pspice for basic circuit analysis. Dubuque, IA: McGraw-Hill. Johnson, David W. "Transforer Equivalent Circuit." CLAYMORE. 7 Apr Web. 4 Aug. 0. < Materials. ea. ¼ diaeter iron core. ea. 00 Ω resistor (shunt) 3. ea. k Ω resistor (load) 4. Magnet Wire 5. ea. dual trace oscilloscope 6. ea. ANDY board 7. ea. ellean oscilloscope 8. ¼ heat shrink tubing. Procedure Modeling:. Design a : transforer with between 00 and 00 turns per inductor, sharing the sae ferrite core. Place the heat sink tubing about the ferrite core so that when the core is reoved the inductor keeps its shape.. Design separate air core inductors with the sae diaeter as your ferrite core. 3. Using PSpice, odel and perfor an AC sweep on your transforer with a kω load across the secondary winding. Use a 5 sine wav as the voltage source. 4. Deterine the fruency response of your ideal transforer. 5. Perfor the short circuit and open circuit tests and deterine the values of the loss coponents for a non-ideal transforer. When easuring current use a 00Ω shunt resistor. To calculate power, use the easured current and voltage across the priary side of the transforer. 6. Deterine the transfer function of your non-ideal transforer circuit. 7. Using MATLAB create a bode plot of the transfer function. Measureents: 8. Use the elleon oscilloscope to perfor a fruency sweep of your transforer. How does it copare to the Bode plot? 9. Deterine the cutoff fruencies. PSpice: 0. Model your transforer with its loss coponents and perfor an AC sweep fro 0Hz MHz. How does this plot copare to the others.. Repeat steps to 0 for a transforer with an air core.

5 . Repeat steps to 0 for two inductors with separate air cores in close proxiity to one another. (Try to ake the touch) 3. How do the loss coponents copare for a transforer with a ferrite core, a transforer with an air core, and for two inductors with separate cores copare. What is the cause of these differences? Modeling an Ideal Transforer: The FRM_LINEAR eleent fro the analog library is used to odel an ideal transforer in Pspice. To ake the transforer ideal, open the Property Editor window for the FRM_LINEAR eleent and ake sure that the COUPLING colun is set to. The COUPLING colun sets the coupling coefficient (k) of the transforer. The coupling coefficient is a easure of the agnetic coupling between two coils (Alexander 566). A axiu k of would ean coplete agnetic coupling between coils, while a k of 0 eans no agnetic coupling between coils. The uation for k is shown below. M k () L L The circuit used to odel and ideal transistor is shown in figure 5. OFF = 0 AMPL = 5 FREQ = 60 0 R T R4 G R LOAD k Figure 5: The ideal transforer in PSpice. R and R represent the loss of the windings. R4 is used as a duy resistor to satisfy a PSpice ruireent that there be DC path between any node and ground. Figure 6 shows the Transforer Property Editor. The values of your inductances ust be entered into the Property Editor coluns L_ALUE and L_ALUE. L_ALUE and L_ALUE control the turns ratio of the transforer using the forula Z n, () Z where Z and Z are the ipedances of the priary and secondary respectively and n is the turns ratio of the transforer. So for the transforer in figure 6, n = 3. Figure 7 shows the results of tie doain analysis of the ideal transforer.

6 Figure 7: Transient Analysis of an ideal transforer. Modeling Mutual Inductance Another way to odel the circuit shown in figure 7 is to use the K_Linear eleent found in the analog library. Using the K_Linear eleent, users can specify the aount of agnetic coupling between up to 6 different inductor eleents. To use the K_Linear eleent, the coupling coefficient and inductors to be coupled ust be selected. Figure 8 shows the circuit diagra of a circuit odeled using K_Linear while Figure 9 shows the property editor window for the K_Linear eleent. Just as before R4 is being used as a duy resistor. In figure 8 the coupling coefficient is set to, aking the transforer ideal, and the inductors selected are L and L. R R OFF = 0 AMPL = 5 FREQ = 60 L 0uH L 0uH LOAD k 0 R4 00MEG K K K_Linear COUPLING = Figure 8: Transforer odeled using K_Linear. Figure 9: K_Linear Property Editor Window.

7 Note that in PSpice Figure 0 is uivalent to Figure. Figure 0 Figure The pin nuber assigned in PSpice can be deterined by double clicking on the pin in question.

ELECTRICAL ENGINEERING [UKSSSC (JE) ELECTRICAL/ELECTRONICS]

ELECTRICAL ENGINEERING [UKSSSC (JE) ELECTRICAL/ELECTRONICS] Class Centre-Pithuwala Karanpur; HO: Shila bypass road near Governent polytechnic Pithuwala Dehradun Mob:084495973,0943406 Web: www.engineeringacadey.co.in E-ail:engineeringacadeyddn@gail.co. How uch energy

More information

Impact of the Reactive Power Compensation on Harmonic Distortion Level

Impact of the Reactive Power Compensation on Harmonic Distortion Level pact of the Reactive Power Copensation on Haronic Distortion Level J. A. M. eto,. C. Jesus, L. L. Piesanti Departaento de Tecnologia Universidade Regional do oroeste do Estado do Rio Grande do Sul juí

More information

ALTERNATING CURRENT (A.C. CIRCUITS)

ALTERNATING CURRENT (A.C. CIRCUITS) AENANG UEN (SHO) 3-4 PAGE: AENANG UEN (A.. US) Alternating current An electrical current, agnitude of which changes with tie and polarity reverses periodically is called alternating current (A.) he sinusoidal

More information

a 2 R ja 2 x l2 R c jx m1

a 2 R ja 2 x l2 R c jx m1 Electric Machinery Labs NQN_version.0 Lab Exercise 6: Siulation of Inrush Currents in Three-Phase Transforers Students ID Group Date I. Introduction: Transforer plays an iportant role in the power transission

More information

Part 9: Basic AC Theory

Part 9: Basic AC Theory Part 9: Basic AC Theory 9.1 Advantages Of AC Systes Dealing with alternating current (AC) supplies is on the whole ore coplicated than dealing with DC current, However there are certain advantages of AC

More information

UNIT - II CONTROLLED RECTIFIERS (Line Commutated AC to DC converters) Line Commutated Converter

UNIT - II CONTROLLED RECTIFIERS (Line Commutated AC to DC converters) Line Commutated Converter UNIT - II CONTROLLED RECTIFIERS (Line Coutated AC to DC converters) INTRODUCTION TO CONTROLLED RECTIFIERS Controlled rectifiers are line coutated ac to power converters which are used to convert a fixed

More information

Einstein Classes, Unit No. 102, 103, Vardhman Ring Road Plaza, Vikas Puri Extn., Outer Ring Road New Delhi , Ph. : ,

Einstein Classes, Unit No. 102, 103, Vardhman Ring Road Plaza, Vikas Puri Extn., Outer Ring Road New Delhi , Ph. : , AENAING CUEN PAC 7. Introduction : Q. What is direct current? Solution : Direct current does not change direction with tie. Q. What is alternating current? Solution : Alternating currents and voltages

More information

EE2003 Circuit Theory Chapter 13 Magnetically Coupled Circuits

EE2003 Circuit Theory Chapter 13 Magnetically Coupled Circuits EE003 Circuit Theory Chapter 3 Magnetically Coupled Circuits Copyright The McGraw-Hill Companies, Inc. Permission required for reproduction or display. Magnetically Coupled Circuit Chapter 3 3. What is

More information

Electromagnetic Induction

Electromagnetic Induction Chapter 16 Electromagnetic Induction In This Chapter: Electromagnetic Induction Faraday s Law Lenz s Law The Transformer Self-Inductance Inductors in Combination Energy of a Current-Carrying Inductor Electromagnetic

More information

ELEC2202 Communications Engineering Laboratory Frequency Modulation (FM)

ELEC2202 Communications Engineering Laboratory Frequency Modulation (FM) ELEC Counications Engineering Laboratory ---- Frequency Modulation (FM) 1. Objectives On copletion of this laboratory you will be failiar with: Frequency odulators (FM), Modulation index, Bandwidth, FM

More information

Secondary-side-only Simultaneous Power and Efficiency Control in Dynamic Wireless Power Transfer System

Secondary-side-only Simultaneous Power and Efficiency Control in Dynamic Wireless Power Transfer System 069060 Secondary-side-only Siultaneous Power and Efficiency Control in Dynaic Wireless Power Transfer Syste 6 Giorgio ovison ) Daita Kobayashi ) Takehiro Iura ) Yoichi Hori ) ) The University of Tokyo,

More information

AccuBridge TOWARDS THE DEVELOPMENT OF A DC CURRENT COMPARATOR RATIO STANDARD

AccuBridge TOWARDS THE DEVELOPMENT OF A DC CURRENT COMPARATOR RATIO STANDARD AccuBridge TOWARD THE DEVELOPMENT OF A DC CURRENT COMPARATOR RATO TANDARD Duane Brown,Andrew Wachowicz, Dr. hiping Huang 3 Measureents nternational, Prescott Canada duanebrown@intl.co, Measureents nternational,

More information

A HIGH POWER FACTOR THREE-PHASE RECTIFIER BASED ON ADAPTIVE CURRENT INJECTION APPLYING BUCK CONVERTER

A HIGH POWER FACTOR THREE-PHASE RECTIFIER BASED ON ADAPTIVE CURRENT INJECTION APPLYING BUCK CONVERTER 9th International onference on Power Electronics Motion ontrol - EPE-PEM Košice A HIGH POWER FATOR THREE-PHASE RETIFIER BASE ON AAPTIVE URRENT INJETION APPYING BUK ONVERTER Žarko Ja, Predrag Pejović EE

More information

Keywords: Equivalent Instantaneous Inductance, Finite Element, Inrush Current.

Keywords: Equivalent Instantaneous Inductance, Finite Element, Inrush Current. Discriination of Inrush fro Fault Currents in Power Transforers Based on Equivalent Instantaneous Inductance Technique Coupled with Finite Eleent Method Downloaded fro ijeee.iust.ac.ir at 5:47 IRST on

More information

Department of Electrical and Computer Engineering Lab 6: Transformers

Department of Electrical and Computer Engineering Lab 6: Transformers ESE Electronics Laboratory A Department of Electrical and Computer Engineering 0 Lab 6: Transformers. Objectives ) Measure the frequency response of the transformer. ) Determine the input impedance of

More information

EE 221 Circuits II. Chapter 13 Magnetically Coupled Circuits

EE 221 Circuits II. Chapter 13 Magnetically Coupled Circuits EE Circuits II Chapter 3 Magnetically Coupled Circuits Magnetically Coupled Circuits 3. What is a transformer? 3. Mutual Inductance 3.3 Energy in a Coupled Circuit 3.4 inear Transformers 3.5 Ideal Transformers

More information

AC Fundamental. Simple Loop Generator: Whenever a conductor moves in a magnetic field, an emf is induced in it.

AC Fundamental. Simple Loop Generator: Whenever a conductor moves in a magnetic field, an emf is induced in it. A Fundaental Siple oop Generator: Whenever a conductor oves in a agnetic field, an ef is induced in it. Fig.: Siple oop Generator The aount of EMF induced into a coil cutting the agnetic lines of force

More information

ANALYSIS AND SIMULATION OF PULSE TRANSFORMER CONSIDERING LEAKAGE INDUCTANCE AND CAPACITANCE

ANALYSIS AND SIMULATION OF PULSE TRANSFORMER CONSIDERING LEAKAGE INDUCTANCE AND CAPACITANCE ANALYSIS AND SIMULATION OF PULSE TRANSFORMER CONSIDERING LEAKAGE INDUCTANCE AND CAPACITANCE ABOLFAZL VAHEDI, HOSSEIN HEYDARI, and FARAMARZ FAGHIHI Electrical Engineering Departent, High Voltage & Magnetic

More information

PHYS 1444 Section 501 Lecture #20

PHYS 1444 Section 501 Lecture #20 PHYS 1444 Section 501 Lecture #0 Monday, Apr. 17, 006 Transformer Generalized Faraday s Law Inductance Mutual Inductance Self Inductance Inductor Energy Stored in the Magnetic Field 1 Announcements Quiz

More information

Tutorial #2: Simulating Transformers in Multisim. In this tutorial, we will discuss how to simulate two common types of transformers in Multisim.

Tutorial #2: Simulating Transformers in Multisim. In this tutorial, we will discuss how to simulate two common types of transformers in Multisim. SCHOOL OF ENGINEERING AND APPLIED SCIENCE DEPARTMENT OF ELECTRICAL AND COMPUTER ENGINEERING ECE 2115: ENGINEERING ELECTRONICS LABORATORY Tutorial #2: Simulating Transformers in Multisim INTRODUCTION In

More information

PHYS 1441 Section 001 Lecture #22 Wednesday, Nov. 29, 2017

PHYS 1441 Section 001 Lecture #22 Wednesday, Nov. 29, 2017 PHYS 1441 Section 001 Lecture #22 Chapter 29:EM Induction & Faraday s Law Transformer Electric Field Due to Changing Magnetic Flux Chapter 30: Inductance Mutual and Self Inductance Energy Stored in Magnetic

More information

Electronic Instrumentation

Electronic Instrumentation 10/15/01 1 Electronic Instrumentation Experiment 3 Part A: Making an Inductor Part B: Measurement of Inductance Part C: imulation of a Transformer Part D: Making a Transformer Review RC and Resonance How

More information

University of Pittsburgh

University of Pittsburgh University of Pittsburgh Experiment #11 Lab Report Inductance/Transformers Submission Date: 12/04/2017 Instructors: Dr. Minhee Yun John Erickson Yanhao Du Submitted By: Nick Haver & Alex Williams Station

More information

PHYS 1442 Section 004 Lecture #15

PHYS 1442 Section 004 Lecture #15 PHYS 1442 Section 004 Lecture #15 Monday March 17, 2014 Dr. Andrew Brandt Chapter 21 Generator Transformer Inductance 3/17/2014 1 PHYS 1442-004, Dr. Andrew Brandt Announcements HW8 on Ch 21-22 will be

More information

Session Eleven: An On-Line Technique to Detect Winding Deformation within Power Transformers

Session Eleven: An On-Line Technique to Detect Winding Deformation within Power Transformers Session Eleven: An On-Line Technique to Detect Winding Deforation within Power Transforers A. Abu-Siada Senior Lecturer, Curtin University Abstract Frequency Response Analysis (FRA) has been growing in

More information

AP Physics C. Alternating Current. Chapter Problems. Sources of Alternating EMF

AP Physics C. Alternating Current. Chapter Problems. Sources of Alternating EMF AP Physics C Alternating Current Chapter Problems Sources of Alternating EMF 1. A 10 cm diameter loop of wire is oriented perpendicular to a 2.5 T magnetic field. What is the magnetic flux through the

More information

A.C. FUNDA- MENTALS. Learning Objectives

A.C. FUNDA- MENTALS. Learning Objectives C H A P T E R Learning Objectives Generation of Alternating Voltages and Currents Alternate Method for the Equations of Alternating Voltages and currents Siple Wavefors Cycle Different Fors of E.M.F. Equation

More information

Chapter 13 Magnetically Coupled Circuits. Chapter Objectives:

Chapter 13 Magnetically Coupled Circuits. Chapter Objectives: Chapter 13 Magnetically Coupled Circuits Chapter Objectives: Understand magnetically coupled circuits. Learn the concept of mutual inductance. Be able to determine energy in a coupled circuit. Learn how

More information

Spring 2000 EE361: MIDTERM EXAM 1

Spring 2000 EE361: MIDTERM EXAM 1 NAME: STUDENT NUMBER: Spring 2000 EE361: MIDTERM EXAM 1 This exam is open book and closed notes. Assume f=60 hz and use the constant µ o =4π 10-7 wherever necessary. Be sure to show all work clearly. 1.

More information

New Characteristics Analysis Considering Transmission Distance and Load Variation in Wireless Power Transfer via Magnetic Resonant Coupling

New Characteristics Analysis Considering Transmission Distance and Load Variation in Wireless Power Transfer via Magnetic Resonant Coupling New Characteristics nalysis Considering Transission Distance and oad Variation in Wireless Power Transfer via Magnetic Resonant Coupling Masaki Kato, Takehiro ura, Yoichi Hori The Departent of dvanced

More information

Transformers. Objectives

Transformers. Objectives Transformers Objectives Explain mutual inductance Describe how a transformer is constructed and how it works Explain how a step-up transformer works Explain how a step-down transformer works Discuss the

More information

An induced emf is the negative of a changing magnetic field. Similarly, a self-induced emf would be found by

An induced emf is the negative of a changing magnetic field. Similarly, a self-induced emf would be found by This is a study guide for Exam 4. You are expected to understand and be able to answer mathematical questions on the following topics. Chapter 32 Self-Induction and Induction While a battery creates an

More information

Properties of Inductor and Applications

Properties of Inductor and Applications LABORATORY Experiment 3 Properties of Inductor and Applications 1. Objectives To investigate the properties of inductor for different types of magnetic material To calculate the resonant frequency of a

More information

Design of a Microcontroller Based Automatic Voltage Stabilizer with Toroidal Transformer

Design of a Microcontroller Based Automatic Voltage Stabilizer with Toroidal Transformer Design of a Microcontroller Based utoatic Voltage Stabilizer with Toroidal Transforer Thet Htun ung Departent of Electrical Power Engineering Mandalay Technological University Myanar bstract- Every electrical

More information

ANALYSIS OF MUTUAL INDUCTANCE AND COUPLING FACTOR OF INDUCTIVELY COUPLED COILS FOR WIRELESS ELECTRICITY

ANALYSIS OF MUTUAL INDUCTANCE AND COUPLING FACTOR OF INDUCTIVELY COUPLED COILS FOR WIRELESS ELECTRICITY VO., NO. 3, JUY 7 IN 89-668 6-7 Asian Research Publishing Network (ARPN. All rights reserved. ANAYI OF MUTUA INDUCTANCE AND COUPING FACTOR OF INDUCTIVEY COUPED COI FOR WIREE EECTRICITY Chandrasekharan

More information

A Decoupling Structure of Controllable Reactor of Transformer Type

A Decoupling Structure of Controllable Reactor of Transformer Type TELKOMNIKA Indonesian Journal of Electrical Engineering Vol., No., January 5, pp. ~ 5 DOI:.59/telkonika.vi.67 A Decoupling Structure of Controllable Reactor of Transforer Type Yu He*, Huatai Chen Power

More information

#8A RLC Circuits: Free Oscillations

#8A RLC Circuits: Free Oscillations #8A RL ircuits: Free Oscillations Goals In this lab we investigate the properties of a series RL circuit. Such circuits are interesting, not only for there widespread application in electrical devices,

More information

13. Magnetically Coupled Circuits

13. Magnetically Coupled Circuits 13. Magnetically Coupled Circuits The change in the current flowing through an inductor induces (creates) a voltage in the conductor itself (self-inductance) and in any nearby conductors (mutual inductance)

More information

DESIGN OF TRANSFORMER BASED CMOS ACTIVE INDUCTANCES

DESIGN OF TRANSFORMER BASED CMOS ACTIVE INDUCTANCES roceedings of the 5th WSEAS Int. Conf. on Microelectronics, Nanoelectronics, Optoelectronics, rague, Czech epublic, March -4, 6 (pp64-69) DESIGN OF TANSFOME BASED CMOS ACTIVE INDUCTANCES G.SCANDUA, C.CIOFI

More information

Electronic Instrumentation

Electronic Instrumentation 10/1/014 1 Electronic Instrumentation Experiment 3 Part A: Making an Inductor Part B: Measurement of Inductance Part C: imulation of a Transformer Part D: Making a Transformer Inductors & Transformers

More information

EXPERIMENTAL VERIFICATION OF SINUSOIDAL APPROXIMATION IN ANALYSIS OF THREE-PHASE TWELVE-PULSE OUTPUT VOLTAGE TYPE RECTIFIERS

EXPERIMENTAL VERIFICATION OF SINUSOIDAL APPROXIMATION IN ANALYSIS OF THREE-PHASE TWELVE-PULSE OUTPUT VOLTAGE TYPE RECTIFIERS th INTERNATIONAL SYPOSIU on POWER ELECTRONICS - Ee 9 XV eđunarodni sipoziju Energetska elektronika Ee 9 NOVI SAD, REPUBLIC OF SERBIA, October 8 th - th, 9 EXPERIENTAL VERIFICATION OF SINUSOIDAL APPROXIATION

More information

Inductors & Resonance

Inductors & Resonance Inductors & Resonance The Inductor This figure shows a conductor carrying a current. A magnetic field is set up around the conductor as concentric circles. If a coil of wire has a current flowing through

More information

Chapter 2-1 Transformers

Chapter 2-1 Transformers Principles of Electric Machines and Power Electronics Chapter 2-1 Transformers Third Edition P. C. Sen Transformer application 1: power transmission Ideal Transformer Assumptions: 1. Negligible winding

More information

Chapter 6. POWER AMPLIFIERS

Chapter 6. POWER AMPLIFIERS hapter 6. OWER AMFERS An aplifying syste usually has several cascaded stages. The input and interediate stages are sall signal aplifiers. Their function is only to aplify the input signal to a suitable

More information

Review: Lecture 9. Instantaneous and Average Power. Effective or RMS Value. Apparent Power and Power Factor. Complex Power. Conservation of AC Power

Review: Lecture 9. Instantaneous and Average Power. Effective or RMS Value. Apparent Power and Power Factor. Complex Power. Conservation of AC Power Review: Lecture 9 Instantaneous and Average Power p( t) VmI m cos ( v i ) VmI m cos ( t v i ) Maximum Average Power Transfer Z L R L jx Effective or RMS Value I rms I m L R P * TH Apparent Power and Power

More information

Research Article Novel Design for Reduction of Transformer Size in Dynamic Voltage Restorer

Research Article Novel Design for Reduction of Transformer Size in Dynamic Voltage Restorer Research Journal of Applied Sciences, Engineering and Technology 8(19): 057-063, 014 DOI:10.1906/rjaset.8.1198 ISSN: 040-7459; e-issn: 040-7467 014 Maxwell Scientific Publication Corp. Subitted: April

More information

11. AC-resistances of capacitor and inductors: Reactances.

11. AC-resistances of capacitor and inductors: Reactances. 11. AC-resistances of capacitor and inductors: Reactances. Purpose: To study the behavior of the AC voltage signals across elements in a simple series connection of a resistor with an inductor and with

More information

Unit-02 Basic Electricity I

Unit-02 Basic Electricity I Unit-0 Basic Electricity Objective: n this experient, we would like to get you ailiar with the theore, structure and use o ultieter and learn the easureent o Alternating Current (AC) / Direct Current (DC)

More information

Table of Contents. Table of Figures. Table of Tables

Table of Contents. Table of Figures. Table of Tables Abstract The aim of this report is to investigate and test a transformer and check if it is good to use by doing the following tests continuity test, insulation test, polarity test, open circuit test,

More information

EE2022 Electrical Energy Systems

EE2022 Electrical Energy Systems EE0 Electrical Energy Systems Lecture : Transformer and Per Unit Analysis 7-0-0 Panida Jirutitijaroen Department of Electrical and Computer Engineering /9/0 EE0: Transformer and Per Unit Analysis by P.

More information

Compensated Single-Phase Rectifier

Compensated Single-Phase Rectifier Copensated Single-Phase Rectifier Jānis DoniĦš Riga Technical university jdonins@gail.co Abstract- Paper describes ethods of rectified DC pulsation reduction adding a ensation node to a single phase rectifier.

More information

HÉDIO TATIZAWA 1, ERASMO SILVEIRA NETO 2, GERALDO F. BURANI 1, ANTÔNIO A. C. ARRUDA 1, KLEIBER T. SOLETTO 1, NELSON M. MATSUO 1

HÉDIO TATIZAWA 1, ERASMO SILVEIRA NETO 2, GERALDO F. BURANI 1, ANTÔNIO A. C. ARRUDA 1, KLEIBER T. SOLETTO 1, NELSON M. MATSUO 1 Application of odelling and coputer siulation for the developent of a test setup for calibration of power quality easureent transducers for high voltage networks HÉDIO TATIZAWA 1, ERASMO SILVEIRA NETO

More information

86 chapter 2 Transformers

86 chapter 2 Transformers 86 chapter 2 Transformers Wb 1.2x10 3 0 1/60 2/60 3/60 4/60 5/60 6/60 t (sec) 1.2x10 3 FIGURE P2.2 2.3 A single-phase transformer has 800 turns on the primary winding and 400 turns on the secondary winding.

More information

General Smith Chart Matching

General Smith Chart Matching General Sith Chart Matching Table of Contents I. General Ipedance Matching II. Ipedance Transforation for Power Aplifiers III. Ipedance Matching with a Sith Chart IV. Inputs V. Network Eleents VI. S-Paraeter

More information

Walchand Institute of Technology. Basic Electrical and Electronics Engineering. Transformer

Walchand Institute of Technology. Basic Electrical and Electronics Engineering. Transformer Walchand Institute of Technology Basic Electrical and Electronics Engineering Transformer 1. What is transformer? explain working principle of transformer. Electrical power transformer is a static device

More information

Exam 3 Review Session

Exam 3 Review Session Exam 3 Review Session I will hold a review for Exam 3 which covers Chapters 27, 28, 29 and 30, on Wednesday November 7 th at 7:15pm in MPHY 205. Exam 3 will be given in class on Thursday, November 8 th.

More information

Chapter Moving Charges and Magnetism

Chapter Moving Charges and Magnetism 100 Chapter Moving Charges and Magnetism 1. The power factor of an AC circuit having resistance (R) and inductance (L) connected in series and an angular velocity ω is [2013] 2. [2002] zero RvB vbl/r vbl

More information

The SI unit of inductance is the henry, defined as:

The SI unit of inductance is the henry, defined as: Inductors A coil of wire, or solenoid, can be used in a circuit to store energy in the magnetic field. We define the inductance of a solenoid having N turns, length l and cross-section area A as: The SI

More information

Clamping of Switch Peak Voltage with Diode and Transformer at Output of Class E Amplifier for Renewable Energy Applications

Clamping of Switch Peak Voltage with Diode and Transformer at Output of Class E Amplifier for Renewable Energy Applications adashi Suetsugu et al., Vol.3, No., 013 Claping of Switch Peak Voltage with Diode and ransforer at Output of Class E Aplifier for enewable Energy Applications adashi Suetsugu*, Xiuqin Wei * *Departent

More information

CH 1. Large coil. Small coil. red. Function generator GND CH 2. black GND

CH 1. Large coil. Small coil. red. Function generator GND CH 2. black GND Experiment 6 Electromagnetic Induction "Concepts without factual content are empty; sense data without concepts are blind... The understanding cannot see. The senses cannot think. By their union only can

More information

Experiment 7: Frequency Modulation and Phase Locked Loops October 11, 2006

Experiment 7: Frequency Modulation and Phase Locked Loops October 11, 2006 Experient 7: Frequency Modulation and Phase ocked oops October 11, 2006 Frequency Modulation Norally, we consider a voltage wave for with a fixed frequency of the for v(t) = V sin(ω c t + θ), (1) where

More information

Core Technology Group Application Note 1 AN-1

Core Technology Group Application Note 1 AN-1 Measuring the Impedance of Inductors and Transformers. John F. Iannuzzi Introduction In many cases it is necessary to characterize the impedance of inductors and transformers. For instance, power supply

More information

PROBLEMS. Figure13.74 For Prob Figure13.72 For Prob Figure13.75 For Prob Figure13.73 For Prob Figure13.76 For Prob

PROBLEMS. Figure13.74 For Prob Figure13.72 For Prob Figure13.75 For Prob Figure13.73 For Prob Figure13.76 For Prob CHAPTER 13 Magnetically Coupled Circuits 571 13.9 In order to match a source with internal impedance of 500 to a 15- load, what is needed is: (a) step-up linear transformer (b) step-down linear transformer

More information

Parameter Identification of Transfer Functions Using MATLAB

Parameter Identification of Transfer Functions Using MATLAB Paraeter Identification of Transfer Functions Using MATLAB Mato Fruk, Goran Vujisić, Toislav Špoljarić Departent of Electrical Engineering The Polytechnic of Zagreb Konavoska, Zagreb, Croatia ato.fruk@tvz.hr,

More information

Electromagnetic Induction - A

Electromagnetic Induction - A Electromagnetic Induction - A APPARATUS 1. Two 225-turn coils 2. Table Galvanometer 3. Rheostat 4. Iron and aluminum rods 5. Large circular loop mounted on board 6. AC ammeter 7. Variac 8. Search coil

More information

Transformers. Dr. Gamal Sowilam

Transformers. Dr. Gamal Sowilam Transformers Dr. Gamal Sowilam OBJECTIVES Become familiar with the flux linkages that exist between the coils of a transformer and how the voltages across the primary and secondary are established. Understand

More information

Switching Transients of Low Cost Two Speed Drive for Single-Phase Induction Machine

Switching Transients of Low Cost Two Speed Drive for Single-Phase Induction Machine Switching Transients of Low Cost Two Speed Drive for Single-Phase Induction Machine L. Woods, A. Hoaifar, F. Fatehi M. Choat, T. Lipo CA&T State University University of Wisconsin-Madison Greensboro, C

More information

WIPL-D Pro: What is New in v12.0?

WIPL-D Pro: What is New in v12.0? WIPL-D Pro: What is New in v12.0? Iproveents/new features introduced in v12.0 are: 1. Extended - Extree Liits a. Extreely LOW contrast aterials b. Extended resolution for radiation pattern c. Extreely

More information

Isolation System with Wireless Power Transfer for Multiple Gate Driver Supplies of a Medium Voltage Inverter

Isolation System with Wireless Power Transfer for Multiple Gate Driver Supplies of a Medium Voltage Inverter Isolation Syste with Wireless Power Transfer for Multiple Gate Driver Supplies of a Mediu Voltage Inverter Keisuke Kusaka, Koji Orikawa and Jun-ichi Itoh Dept. of Energy and Environental Nagaoka University

More information

ET 304A Laboratory Tutorial-Circuitmaker For Transient and Frequency Analysis

ET 304A Laboratory Tutorial-Circuitmaker For Transient and Frequency Analysis ET 304A Laboratory Tutorial-Circuitmaker For Transient and Frequency Analysis All circuit simulation packages that use the Pspice engine allow users to do complex analysis that were once impossible to

More information

Name: Lab Partner: Section: The purpose of this lab is to study induction. Faraday s law of induction and Lenz s law will be explored. B = B A (8.

Name: Lab Partner: Section: The purpose of this lab is to study induction. Faraday s law of induction and Lenz s law will be explored. B = B A (8. Chapter 8 Induction - Faraday s Law Name: Lab Partner: Section: 8.1 Purpose The purpose of this lab is to study induction. Faraday s law of induction and Lenz s law will be explored. 8.2 Introduction It

More information

PESIT Bangalore South Campus Hosur road, 1km before Electronic City, Bengaluru -100 Department of Electronics & Communication Engineering

PESIT Bangalore South Campus Hosur road, 1km before Electronic City, Bengaluru -100 Department of Electronics & Communication Engineering CONTINUOUS INTERNAL EVALUATION TEST -1 Date : 27/2/2018 Marks:60 Subject & Code : Basic Electrical Engineering, 17ELE25 Section: A,B,C,D,E Time : 8:30 am 11:30 a.m Name of faculty: Mrs. Dhanashree Bhate,

More information

In this lecture. Electromagnetism. Electromagnetism. Oersted s Experiment. Electricity & magnetism are different aspects of the same basic phenomenon:

In this lecture. Electromagnetism. Electromagnetism. Oersted s Experiment. Electricity & magnetism are different aspects of the same basic phenomenon: In this lecture Electromagnetism Electromagnetic Effect Electromagnets Electromechanical Devices Transformers Electromagnetic Effect Electricity & magnetism are different aspects of the same basic phenomenon:

More information

Question & its Answer

Question & its Answer Iportant Instructions to exainers: 1) The answers should be exained by keywords and not as word-to-word as given in the odel answer schee. 2) The odel answer and the answer written by candidate ay vary

More information

EXPERIMENT 9 Problem Solving: First-order Transient Circuits

EXPERIMENT 9 Problem Solving: First-order Transient Circuits EXPERIMENT 9 Problem Solving: First-order Transient Circuits I. Introduction In transient analyses, we determine voltages and currents as functions of time. Typically, the time dependence is demonstrated

More information

Magnetics. Important relationships. Magnetic quantities Analogies to electrical quantities

Magnetics. Important relationships. Magnetic quantities Analogies to electrical quantities Mor M. Peretz, Switch-Mode Power Supplies [3-1] Faraday s and Amper s laws Permeability Inductor Reluctance model Air gap Current crowding Inductor design Skin effect, proximity effect Losses Transformer

More information

Smarter Balanced Assessment Consortium Claims, Targets, and Standard Alignment for Math

Smarter Balanced Assessment Consortium Claims, Targets, and Standard Alignment for Math Sarter Balanced Assessent Consortiu Clais, s, Stard Alignent for Math The Sarter Balanced Assessent Consortiu (SBAC) has created a hierarchy coprised of clais targets that together can be used to ake stateents

More information

CHAPTER 9. Sinusoidal Steady-State Analysis

CHAPTER 9. Sinusoidal Steady-State Analysis CHAPTER 9 Sinusoidal Steady-State Analysis 9.1 The Sinusoidal Source A sinusoidal voltage source (independent or dependent) produces a voltage that varies sinusoidally with time. A sinusoidal current source

More information

Bucking Coils produce Energy Gain Cyril Smith, 2015

Bucking Coils produce Energy Gain Cyril Smith, 2015 Bucking Coils produce Energy Gain Cyril Smith, 015 1. Introduction There are many claims of overunity for systems that employ bucking coils. These are coils mounted on a common core and connected in series

More information

ECE 241L Fundamentals of Electrical Engineering. Experiment 8 A-C Transformer, Magnetization & Hysteresis

ECE 241L Fundamentals of Electrical Engineering. Experiment 8 A-C Transformer, Magnetization & Hysteresis ECE 241L Fundamentals of Electrical Engineering Experiment 8 A-C Transformer, Magnetization & Hysteresis A. Objectives: I. Measure leakage inductance and resistance loss II. Measure magnetization inductance

More information

Ignition and monitoring technique for plasma processing of multicell superconducting radio frequency cavities

Ignition and monitoring technique for plasma processing of multicell superconducting radio frequency cavities Ignition and onitoring technique for plasa processing of ulticell superconducting radio frequency cavities Marc Doleans Oak Ridge ational Laboratory, Oak Ridge, Tennessee 3783, USA E ail: doleans@ornl.gov

More information

1 K Hinds 2012 TRANSFORMERS

1 K Hinds 2012 TRANSFORMERS 1 K Hinds 2012 TRANSFORMERS A transformer changes electrical energy of a given voltage into electrical energy at a different voltage level. It consists of two coils which are not electrically connected,

More information

29 th International Physics Olympiad

29 th International Physics Olympiad 29 th International Physics Olympiad Reykjavik, Iceland Experimental competition Monday, July 6th, 1998 Time available: 5 hours Read this first: Use only the pen provided. 1. Use only the front side of

More information

Alternating current circuits- Series RLC circuits

Alternating current circuits- Series RLC circuits FISI30 Física Universitaria II Professor J.. ersosimo hapter 8 Alternating current circuits- Series circuits 8- Introduction A loop rotated in a magnetic field produces a sinusoidal voltage and current.

More information

N I N LI I. I t. (Note how L is independent of the current I.)

N I N LI I. I t. (Note how L is independent of the current I.) UNIT- IV MAGNETICALLY COUPLED CIRCUITS Magnetically Coupled Circuits: Self inductance - Mutual inductance - Dot rule - Coefficient of coupling - Analysis of multi winding coupled circuits - Series, Parallel

More information

10 Electromagnetic Interactions

10 Electromagnetic Interactions Lab 10 Electromagnetic Interactions What You Need To Know: The Physics Electricity and magnetism are intrinsically linked and not separate phenomena. A changing magnetic field can create an electric field

More information

13 th Asian Physics Olympiad India Experimental Competition Wednesday, 2 nd May 2012

13 th Asian Physics Olympiad India Experimental Competition Wednesday, 2 nd May 2012 13 th Asian Physics Olympiad India Experimental Competition Wednesday, nd May 01 Please first read the following instructions carefully: 1. The time available is ½ hours for each of the two experimental

More information

APPLICATION NOTE - 018

APPLICATION NOTE - 018 APPLICATION NOTE - 018 Power Transformers Background Power Transformers are used within an AC power distribution systems to increase or decrease the operating voltage to achieve the optimum transmission

More information

Experiment 6. Electromagnetic Induction and transformers

Experiment 6. Electromagnetic Induction and transformers Experiment 6. Electromagnetic Induction and transformers 1. Purpose Confirm the principle of electromagnetic induction and transformers. 2. Principle The PASCO scientific SF-8616 Basic Coils Set and SF-8617

More information

Estimation of Inductance for Sine and Cosine Shape Spiral Coils

Estimation of Inductance for Sine and Cosine Shape Spiral Coils Estiation of Inductance for Sine and Cosine Sape Spiral Coils A. Darwin Jose Raju Assistant Professor, St. Xavier s Catolic College of Engineering, Nagercoil, Tail Nadu, India S. Solai anoar Professor,

More information

A NEW APPROACH TO UNGROUNDED FAULT LOCATION IN A THREE-PHASE UNDERGROUND DISTRIBUTION SYSTEM USING COMBINED NEURAL NETWORKS & WAVELET ANALYSIS

A NEW APPROACH TO UNGROUNDED FAULT LOCATION IN A THREE-PHASE UNDERGROUND DISTRIBUTION SYSTEM USING COMBINED NEURAL NETWORKS & WAVELET ANALYSIS A NEW APPROACH TO UNGROUNDED FAULT LOCATION IN A THREE-PHASE UNDERGROUND DISTRIBUTION SYSTEM USING COMBINED NEURAL NETWORKS & WAVELET ANALYSIS Jaal Moshtagh University of Bath, UK oshtagh79@yahoo.co Abstract

More information

Transformer circuit calculations

Transformer circuit calculations Transformer circuit calculations This worksheet and all related files are licensed under the Creative Commons Attribution License, version 1.0. To view a copy of this license, visit http://creativecommons.org/licenses/by/1.0/,

More information

AC CIRCUITS. Part 1: Inductance of a Coil. THEORY: If the current in a resistor R, a capacitor C, and/or an inductor L is given by:

AC CIRCUITS. Part 1: Inductance of a Coil. THEORY: If the current in a resistor R, a capacitor C, and/or an inductor L is given by: AC CIRCUITS OBJECTIVE: To study the effect of alternating currents on various electrical quantities in circuits containing resistors, capacitors and inductors. Part 1: Inductance of a Coil THEORY: If the

More information

By Gill ( ) PDF created with FinePrint pdffactory trial version

By Gill (  ) PDF created with FinePrint pdffactory trial version By Gill (www.angelfire.com/al4/gill ) 1 Introduction One of the main reasons of adopting a.c. system instead of d.c. for generation, transmission and distribution of electrical power is that alternatin

More information

Study of Inductive and Capacitive Reactance and RLC Resonance

Study of Inductive and Capacitive Reactance and RLC Resonance Objective Study of Inductive and Capacitive Reactance and RLC Resonance To understand how the reactance of inductors and capacitors change with frequency, and how the two can cancel each other to leave

More information

L It indicates that g m is proportional to the k, W/L ratio and ( VGS Vt However, a large V GS reduces the allowable signal swing at the drain.

L It indicates that g m is proportional to the k, W/L ratio and ( VGS Vt However, a large V GS reduces the allowable signal swing at the drain. Field-Effect Transistors (FETs) 3.9 MOSFET as an Aplifier Sall-signal equivalent circuit odels Discussions about the MOSFET transconductance W Forula 1: g = k n ( VGS Vt ) L It indicates that g is proportional

More information

Design Consideration of Half-Bridge LLC Resonant Converter

Design Consideration of Half-Bridge LLC Resonant Converter Design Consideration of Halfbridge LLC Resonant Converter 13 JPE 71 Design Consideration of HalfBridge LLC Resonant Converter HangSeok Choi airchild Korea Seiconductor, Korea ABSTRACT LLC resonant converters

More information

Electrical Theory 2 Lessons for Fall Semester:

Electrical Theory 2 Lessons for Fall Semester: Electrical Theory 2 Lessons for Fall Semester: Lesson 1 Magnetism Lesson 2 Introduction to AC Theory Lesson 3 Lesson 4 Capacitance and Capacitive Reactance Lesson 5 Impedance and AC Circuits Lesson 6 AC

More information

B.Tech II SEM Question Bank. Electronics & Electrical Engg UNIT-1

B.Tech II SEM Question Bank. Electronics & Electrical Engg UNIT-1 UNIT-1 1. State & Explain Superposition theorem & Thevinin theorem with example? 2. Calculate the current in the 400Ωm resistor of below figure by Superposition theorem. 3. State & Explain node voltage

More information

Dual-Band Channel Measurements for an Advanced Tyre Monitoring System

Dual-Band Channel Measurements for an Advanced Tyre Monitoring System Dual-Band Channel Measureents for an Advanced Tyre Monitoring Syste Gregor Lasser and Christoph F. Mecklenbräuker Vienna University of Technology Institute of Counications and Radio-Frequency Engineering

More information