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

Size: px
Start display at page:

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

Transcription

1 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 unit of inductance is the henry, defined as: 1 henry = 1 H = 1 Wb/A = 1 T m2/a A coil of wire used in a circuit for the purpose of inductance is called an inductor. The circuit symbol for an ideal inductor is. Slide

2 Potential Difference Across an Inductor The figure above shows a steady current into the left side of an inductor. The solenoid s magnetic field passes through the coils, establishing a flux. Slide

3 Potential Difference Across an Inductor In the figure, the current into the solenoid is increasing. This creates an increasing flux to the left. Therefore the induced magnetic field must point to the right. The induced emf V L must be opposite to the current into the solenoid: Slide

4 Potential Difference Across an Inductor In the figure, the current into the solenoid is decreasing. To oppose the decrease in flux, the induced emf V L is in the same direction as the input current. The potential difference across an inductor, measured along the direction of the current, is: Slide

5 Potential Difference Across an Inductor Slide

6 QuickCheck Which current is changing more rapidly? A. Current I 1. B. Current I 2. C. They are changing at the same rate. D. Not enough information to tell. Slide

7 Example 1 - What is the potential difference across a 10 mh inductor if the current through the inductor drops from 150 ma to 50 ma in 10 μs? Does the potential increase or decrease along the direction of the current? Slide

8 Energy in Inductors and Magnetic Fields As current passes through an inductor, the electric power is: P elec is negative because the current is losing energy. That energy is being transferred to the inductor, which is storing energy U L at the rate: We can find the total energy stored in an inductor by integrating: Slide

9 Energy in Inductors and Magnetic Fields Inside a solenoid, the magnetic field strength is B = μ 0 NI/l. The inductor s energy can be related to B: But Al is the volume inside the solenoid. Dividing by Al, the magnetic field energy density (energy per m 3 ) is: Slide

10 Energy in Electric and Magnetic Fields Slide

11 Example 2 - How much energy is stored in a 3.0-cmdiameter, 12-cm-long solenoid that has 200 turns of wire and carries a current of 0.80 A? Slide

12 LC Circuits The figure shows a capacitor with initial charge Q 0, an inductor, and a switch. The switch has been open for a long time, so there is no current in the circuit. At t 0, the switch is closed. How does the circuit respond? The charge and current oscillate in a way that is analogous to a mass on a spring. Slide

13 LC Circuits: Step A Slide

14 LC Circuits: Step B Slide

15 LC Circuits: Step C Slide

16 LC Circuits: Step D Slide

17 LC Circuits An LC circuit is an electric oscillator. The letters on the graph correspond to the four steps in the previous slides. The charge on the upper plate is Q Q 0 cosωt and the current through the inductor is I I max sinωt, where: Slide

18 QuickCheck If the top circuit has an oscillation frequency of 1000 Hz, the frequency of the bottom circuit is A. 500 Hz. B. 707 Hz. C Hz. D Hz. Slide

19 LC Circuits A cell phone is actually a very sophisticated two-way radio that communicates with the nearest base station via high-frequency radio waves roughly 1000 MHz. As in any radio or communications device, the transmission frequency is established by the oscillating current in an LC circuit. Slide

20 Example 3 - An electric oscillator is made with a 0.10 μf capacitor and a 1.0 mh inductor. The capacitor is initially charged to 5.0 V. What is the maximum current through the inductor as the circuit oscillates? Slide

21 LR Circuits The figure shows an inductor and resistor in series. Initially there is a steady current I 0 being driven through the LR circuit by an external battery. At t 0, the switch is closed. How does the circuit respond? The current through the circuit decays exponentially, with a time constant L/R. Slide

22 LR Circuits Slide

23 QuickCheck What is the battery current immediately after the switch has closed? A. 0 A B. 1 A C. 2 A D. Undefined Slide

24 QuickCheck What is the battery current immediately after the switch has been closed for a very long time? A. 0 A B. 1 A C. 2 A D. Undefined Slide

25 Problem Example 4 - What is the current out of the battery immediately after the switch is closed? What is the current out of the battery after the switch has been closed a long time?

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

Inductance. Chapter 30. PowerPoint Lectures for University Physics, Thirteenth Edition Hugh D. Young and Roger A. Freedman. Lectures by Wayne Anderson

Inductance. Chapter 30. PowerPoint Lectures for University Physics, Thirteenth Edition Hugh D. Young and Roger A. Freedman. Lectures by Wayne Anderson Chapter 30 Inductance PowerPoint Lectures for University Physics, Thirteenth Edition Hugh D. Young and Roger A. Freedman Lectures by Wayne Anderson Goals for Chapter 30 To learn how current in one coil

More information

Inductance. Chapter 30. PowerPoint Lectures for University Physics, Thirteenth Edition Hugh D. Young and Roger A. Freedman. Lectures by Wayne Anderson

Inductance. Chapter 30. PowerPoint Lectures for University Physics, Thirteenth Edition Hugh D. Young and Roger A. Freedman. Lectures by Wayne Anderson Chapter 30 Inductance PowerPoint Lectures for University Physics, Thirteenth Edition Hugh D. Young and Roger A. Freedman Lectures by Wayne Anderson Goals for Chapter 30 To learn how current in one coil

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

Physics 202 Midterm Exam 3 Nov 30th, 2011

Physics 202 Midterm Exam 3 Nov 30th, 2011 Physics 202 Midterm Exam 3 Nov 30th, 2011 Name: Student ID: Section: TA (please circle): Daniel Crow Scott Douglas Yutao Gong Taylor Klaus Aaron Levine Andrew Loveridge Jason Milhone Hojin Yoo Instructions:

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

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

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

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

EE 42/100 Lecture 16: Inductance. Rev B 3/15/2010 (8:55 PM) Prof. Ali M. Niknejad

EE 42/100 Lecture 16: Inductance. Rev B 3/15/2010 (8:55 PM) Prof. Ali M. Niknejad A. M. Niknejad University of California, Berkeley EE 100 / 42 Lecture 16 p. 1/23 EE 42/100 Lecture 16: Inductance ELECTRONICS Rev B 3/15/2010 (8:55 PM) Prof. Ali M. Niknejad University of California, Berkeley

More information

PHYSICS WORKSHEET CLASS : XII. Topic: Alternating current

PHYSICS WORKSHEET CLASS : XII. Topic: Alternating current PHYSICS WORKSHEET CLASS : XII Topic: Alternating current 1. What is mean by root mean square value of alternating current? 2. Distinguish between the terms effective value and peak value of an alternating

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

Electromagnetic Oscillations and Currents. March 23, 2014 Chapter 30 1

Electromagnetic Oscillations and Currents. March 23, 2014 Chapter 30 1 Electromagnetic Oscillations and Currents March 23, 2014 Chapter 30 1 Driven LC Circuit! The voltage V can be thought of as the projection of the vertical axis of the phasor V m representing the time-varying

More information

Physics 115. Inductors, Capacitors, and RLC circuits. General Physics II. Session 34

Physics 115. Inductors, Capacitors, and RLC circuits. General Physics II. Session 34 Physics 115 General Physics II Session 34 Inductors, Capacitors, and RLC circuits R. J. Wilkes Email: phy115a@u.washington.edu Home page: http://courses.washington.edu/phy115a/ 06/05/13 1 Lecture Schedule

More information

Alternating Current. Slide 1 / 69. Slide 2 / 69. Slide 3 / 69. Topics to be covered. Sources of Alternating EMF. Sources of alternating EMF

Alternating Current. Slide 1 / 69. Slide 2 / 69. Slide 3 / 69. Topics to be covered. Sources of Alternating EMF. Sources of alternating EMF Slide 1 / 69 lternating urrent Sources of alternating EMF Transformers ircuits and Impedance Topics to be covered Slide 2 / 69 LR Series ircuits Resonance in ircuit Oscillations Sources of lternating EMF

More information

Alternating Current. Slide 2 / 69. Slide 1 / 69. Slide 3 / 69. Slide 4 / 69. Slide 6 / 69. Slide 5 / 69. Topics to be covered

Alternating Current. Slide 2 / 69. Slide 1 / 69. Slide 3 / 69. Slide 4 / 69. Slide 6 / 69. Slide 5 / 69. Topics to be covered Slide 1 / 69 lternating urrent Sources of alternating EMF ircuits and Impedance Slide 2 / 69 Topics to be covered LR Series ircuits Resonance in ircuit Oscillations Slide 3 / 69 Sources of lternating EMF

More information

Exam 3 Solutions. ! r, the ratio is ( N ) ( ) ( )( ) 2. PHY2054 Spring Prof. Pradeep Kumar Prof. Paul Avery Prof. Yoonseok Lee Mar.

Exam 3 Solutions. ! r, the ratio is ( N ) ( ) ( )( ) 2. PHY2054 Spring Prof. Pradeep Kumar Prof. Paul Avery Prof. Yoonseok Lee Mar. PHY054 Spring 009 Prof. Pradeep Kumar Prof. Paul Avery Prof. Yoonseok Lee Mar. 7, 009 Exam 3 Solutions 1. Two coils (A and B) made out of the same wire are in a uniform magnetic field with the coil axes

More information

RC_Circuits RC Circuits Lab Q1 Open the Logger Pro program RC_RL_Circuits via the Logger Launcher icon on your desktop. RC Circuits Lab Part1 Part 1: Measuring Voltage and Current in an RC Circuit 1. 2.

More information

ELECTROMAGNETIC INDUCTION AND ALTERNATING CURRENT (Assignment)

ELECTROMAGNETIC INDUCTION AND ALTERNATING CURRENT (Assignment) ELECTROMAGNETIC INDUCTION AND ALTERNATING CURRENT (Assignment) 1. In an A.C. circuit A ; the current leads the voltage by 30 0 and in circuit B, the current lags behind the voltage by 30 0. What is the

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

Chapter 24. Alternating Current Circuits

Chapter 24. Alternating Current Circuits Chapter 24 Alternating Current Circuits Objective of Lecture Generators and Motors Inductance RL Circuits (resistance and inductance) Transformers AC REMINDER: WORK ON THE EXAMPLES Read physics in perspective

More information

RC and RL Circuits Prelab

RC and RL Circuits Prelab RC and RL Circuits Prelab by Dr. Christine P. Cheney, Department of Physics and Astronomy, 401 Nielsen Physics Building, The University of Tennessee, Knoxville, Tennessee 37996-1200 2018 by Christine P.

More information

12/6/2011. Electromagnetic Induction. Electromagnetic Induction and Electromagnetic Waves. Checking Understanding. Magnetic Flux. Lenz s Law.

12/6/2011. Electromagnetic Induction. Electromagnetic Induction and Electromagnetic Waves. Checking Understanding. Magnetic Flux. Lenz s Law. Electromagnetic Induction and Electromagnetic Waves Topics: Electromagnetic induction Lenz s law Faraday s law The nature of electromagnetic waves The spectrum of electromagnetic waves Electromagnetic

More information

Chapter 6: Alternating Current. An alternating current is an current that reverses its direction at regular intervals.

Chapter 6: Alternating Current. An alternating current is an current that reverses its direction at regular intervals. Chapter 6: Alternating Current An alternating current is an current that reverses its direction at regular intervals. Overview Alternating Current Phasor Diagram Sinusoidal Waveform A.C. Through a Resistor

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

CHAPTER 6: ALTERNATING CURRENT

CHAPTER 6: ALTERNATING CURRENT CHAPTER 6: ALTERNATING CURRENT PSPM II 2005/2006 NO. 12(C) 12. (c) An ac generator with rms voltage 240 V is connected to a RC circuit. The rms current in the circuit is 1.5 A and leads the voltage by

More information

SIDDHARTH GROUP OF INSTITUTIONS :: PUTTUR (AUTONOMOUS) Siddharth Nagar, Narayanavanam Road QUESTION BANK (DESCRIPTIVE) UNIT I INTRODUCTION

SIDDHARTH GROUP OF INSTITUTIONS :: PUTTUR (AUTONOMOUS) Siddharth Nagar, Narayanavanam Road QUESTION BANK (DESCRIPTIVE) UNIT I INTRODUCTION SIDDHARTH GROUP OF INSTITUTIONS :: PUTTUR (AUTONOMOUS) Siddharth Nagar, Narayanavanam Road 517583 QUESTION BANK (DESCRIPTIVE) Subject with Code : Electrical Circuits(16EE201) Year & Sem: I-B.Tech & II-Sem

More information

MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics 8.02 Spring 2005 Experiment 10: LR and Undriven LRC Circuits

MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics 8.02 Spring 2005 Experiment 10: LR and Undriven LRC Circuits MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics 8.0 Spring 005 Experiment 10: LR and Undriven LRC Circuits OBJECTIVES 1. To determine the inductance L and internal resistance R L of a coil,

More information

Experiment 9: AC circuits

Experiment 9: AC circuits Experiment 9: AC circuits Nate Saffold nas2173@columbia.edu Office Hour: Mondays, 5:30PM-6:30PM @ Pupin 1216 INTRO TO EXPERIMENTAL PHYS-LAB 1493/1494/2699 Introduction Last week (RC circuit): This week:

More information

Experiment 7: Undriven & Driven RLC Circuits

Experiment 7: Undriven & Driven RLC Circuits MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics 8.02 Spring 2006 OBJECTIVES Experiment 7: Undriven & Driven RLC Circuits 1. To explore the time dependent behavior of RLC Circuits, both driven

More information

Introduction. Inductors in AC Circuits.

Introduction. Inductors in AC Circuits. Module 3 AC Theory What you ll learn in Module 3. Section 3.1 Electromagnetic Induction. Magnetic Fields around Conductors. The Solenoid. Section 3.2 Inductance & Back e.m.f. The Unit of Inductance. Factors

More information

Chapter 6: Alternating Current

Chapter 6: Alternating Current hapter 6: Alternating urrent 6. Alternating urrent.o 6.. Define alternating current (A) An alternating current (A) is the electrical current which varies periodically with time in direction and magnitude.

More information

not to be republished NCERT ALTERNATING CURRENT Chapter Seven MCQ 1

not to be republished NCERT ALTERNATING CURRENT Chapter Seven MCQ 1 hapter Seven ALTERNATING URRENT MQ 1 7.1 If the rms current in a 50 Hz ac circuit is 5 A, the value of the current 1/300 seconds after its value becomes zero is (a) 5 2 A (b) 5 3/2 A (c) 5/6 A (d) 5/ 2

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

Lab 7 - Inductors and LR Circuits

Lab 7 - Inductors and LR Circuits Lab 7 Inductors and LR Circuits L7-1 Name Date Partners Lab 7 - Inductors and LR Circuits The power which electricity of tension possesses of causing an opposite electrical state in its vicinity has been

More information

y 2irfCj Resonance in AC Circuits Summary v v The rms current in an LRC series circuit is given by (see Eqs , 21-15, 21-llb, and 21-12b):

y 2irfCj Resonance in AC Circuits Summary v v The rms current in an LRC series circuit is given by (see Eqs , 21-15, 21-llb, and 21-12b): -* Resonance in AC Circuits The rms current in an LRC series circuit is given by (see Eqs. 21-14, 21-15, 21-llb, and 21-12b): -'rms v v

More information

ANADOLU UNIVERSITY FACULTY OF ENGINEERING AND ARCHITECTURE DEPARTMENT OF ELECTRICAL AND ELECTRONICS ENGINEERING

ANADOLU UNIVERSITY FACULTY OF ENGINEERING AND ARCHITECTURE DEPARTMENT OF ELECTRICAL AND ELECTRONICS ENGINEERING ANADOLU UNIVERSITY FACULTY OF ENGINEERING AND ARCHITECTURE DEPARTMENT OF ELECTRICAL AND ELECTRONICS ENGINEERING EEM 206 ELECTRICAL CIRCUITS LABORATORY EXPERIMENT#3 RESONANT CIRCUITS 1 RESONANT CIRCUITS

More information

Level 3 Physics, 2017

Level 3 Physics, 2017 91526 915260 3SUPERVISOR S Level 3 Physics, 2017 91526 Demonstrate understanding of electrical systems 2.00 p.m. Monday 20 November 2017 Credits: Six Achievement Achievement with Merit Achievement with

More information

GSEB QUESTION PAPER PHYSICS

GSEB QUESTION PAPER PHYSICS GSEB QUESTION PAPER PHYSICS Time : 3 Hours Maximum Marks: 100 Instructions : 1. There are four sections and total 60 questions in this question paper. 2. Symbols used in this question paper have their

More information

15. the power factor of an a.c circuit is.5 what will be the phase difference between voltage and current in this

15. the power factor of an a.c circuit is.5 what will be the phase difference between voltage and current in this 1 1. In a series LCR circuit the voltage across inductor, a capacitor and a resistor are 30 V, 30 V and 60 V respectively. What is the phase difference between applied voltage and current in the circuit?

More information

Goals. Introduction. To understand the use of root mean square (rms) voltages and currents.

Goals. Introduction. To understand the use of root mean square (rms) voltages and currents. Lab 10. AC Circuits Goals To show that AC voltages cannot generally be added without accounting for their phase relationships. That is, one must account for how they vary in time with respect to one another.

More information

Physics 202 Midterm Exam 3 April 25, 2012

Physics 202 Midterm Exam 3 April 25, 2012 ID CODE: C Physics 202 Midterm Exam 3 April 25, 2012 Name:... Student ID:... Section:... TA (please circle): Deepak Agarwal Nicholas Brewer Raghvendra Chaubey Todd Garon Yutao Gong Andrew Loveridge Abhishek

More information

Level 3 Physics, 2018

Level 3 Physics, 2018 91526 915260 3SUPERVISOR S Level 3 Physics, 2018 91526 Demonstrate understanding of electrical systems 2.00 p.m. Tuesday 20 November 2018 Credits: Six Achievement Achievement with Merit Achievement with

More information

Chapter 30 Inductance, Electromagnetic. Copyright 2009 Pearson Education, Inc.

Chapter 30 Inductance, Electromagnetic. Copyright 2009 Pearson Education, Inc. Chapter 30 Inductance, Electromagnetic Oscillations, and AC Circuits 30-7 AC Circuits with AC Source Resistors, capacitors, and inductors have different phase relationships between current and voltage

More information

(c) In the process of part (b), must energy be supplied to the electron, or is energy released?

(c) In the process of part (b), must energy be supplied to the electron, or is energy released? (1) A capacitor, as shown, has plates of dimensions 10a by 10a, and plate separation a. The field inside is uniform, and has magnitude 120 N/C. The constant a equals 4.5 cm. (a) What amount of charge is

More information

Physics Jonathan Dowling. Lecture 35: MON 16 NOV Electrical Oscillations, LC Circuits, Alternating Current II

Physics Jonathan Dowling. Lecture 35: MON 16 NOV Electrical Oscillations, LC Circuits, Alternating Current II hysics 2113 Jonathan Dowling Lecture 35: MON 16 NOV Electrical Oscillations, LC Circuits, Alternating Current II Damped LCR Oscillator Ideal LC circuit without resistance: oscillations go on forever; ω

More information

RESIT EXAM: WAVES and ELECTROMAGNETISM (AE1240-II) 10 August 2015, 14:00 17:00 9 pages

RESIT EXAM: WAVES and ELECTROMAGNETISM (AE1240-II) 10 August 2015, 14:00 17:00 9 pages Faculty of Aerospace Engineering RESIT EXAM: WAVES and ELECTROMAGNETISM (AE140-II) 10 August 015, 14:00 17:00 9 pages Please read these instructions first: 1) This exam contains 5 four-choice questions.

More information

Series and Parallel Resonant Circuits

Series and Parallel Resonant Circuits Series and Parallel Resonant Circuits Aim: To obtain the characteristics of series and parallel resonant circuits. Apparatus required: Decade resistance box, Decade inductance box, Decade capacitance box

More information

University of Jordan School of Engineering Electrical Engineering Department. EE 219 Electrical Circuits Lab

University of Jordan School of Engineering Electrical Engineering Department. EE 219 Electrical Circuits Lab University of Jordan School of Engineering Electrical Engineering Department EE 219 Electrical Circuits Lab EXPERIMENT 4 TRANSIENT ANALYSIS Prepared by: Dr. Mohammed Hawa EXPERIMENT 4 TRANSIENT ANALYSIS

More information

total j = BA, [1] = j [2] total

total j = BA, [1] = j [2] total Name: S.N.: Experiment 2 INDUCTANCE AND LR CIRCUITS SECTION: PARTNER: DATE: Objectives Estimate the inductance of the solenoid used for this experiment from the formula for a very long, thin, tightly wound

More information

Exercises of resistors 1. Calculate the resistance of a 10 m long Copper wire with diameter d = 1.0 mm.

Exercises of resistors 1. Calculate the resistance of a 10 m long Copper wire with diameter d = 1.0 mm. Exercises of resistors 1. Calculate the resistance of a 10 m long Copper wire with diameter d = 1.0 mm. 2. Calculate the resistances of following equipment: using 220V AC a) a 1000 W electric heater b)

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

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

Inductance in DC Circuits

Inductance in DC Circuits Inductance in DC Circuits Anurag Srivastava Concept: Inductance is characterized by the behavior of a coil of wire in resisting any change of electric current through the coil. Arising from Faraday's law,

More information

z z" z v 2 ft = 2k ft. 328 Concepts of Physics The energy dissipated in 1000 s = P * 1000 s

z z z v 2 ft = 2k ft. 328 Concepts of Physics The energy dissipated in 1000 s = P * 1000 s 38 Concepts of Physics. A series AC circuit contains an inductor ( mh), a capacitor ( (JF), a resistor ( ft) and an AC source of V, Hz. Find the energy dissipated in the circuit in s. Solution : The time

More information

Goals. Introduction. To understand the use of root mean square (rms) voltages and currents.

Goals. Introduction. To understand the use of root mean square (rms) voltages and currents. Lab 10. AC Circuits Goals To show that AC voltages cannot generally be added without accounting for their phase relationships. That is, one must account for how they vary in time with respect to one another.

More information

AC Sources and Phasors

AC Sources and Phasors AC Sources and Phasors Circuits powered by a sinusoidal emf are called AC circuits, where AC stands for alternating current. Steady-current circuits are called DC circuits, for direct current. The instantaneous

More information

Physics for Scientists & Engineers 2 2 = 1 LC. Review ( ) Review (2) Review (3) e! Rt. cos "t + # ( ) q = q max. Spring Semester 2005 Lecture 30 U E

Physics for Scientists & Engineers 2 2 = 1 LC. Review ( ) Review (2) Review (3) e! Rt. cos t + # ( ) q = q max. Spring Semester 2005 Lecture 30 U E Review hysics for Scientists & Engineers Spring Semester 005 Lecture 30! If we have a single loop RLC circuit, the charge in the circuit as a function of time is given by! Where q = q max e! Rt L cos "t

More information

Flyback Converter for High Voltage Capacitor Charging

Flyback Converter for High Voltage Capacitor Charging Flyback Converter for High Voltage Capacitor Charging Tony Alfrey (tonyalfrey at earthlink dot net) A Flyback Converter is a type of switching power supply that may be used to generate an output voltage

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

Lab 9 - INTRODUCTION TO AC CURRENTS AND VOLTAGES

Lab 9 - INTRODUCTION TO AC CURRENTS AND VOLTAGES 145 Name Date Partners Lab 9 INTRODUCTION TO AC CURRENTS AND VOLTAGES V(volts) t(s) OBJECTIVES To learn the meanings of peak voltage and frequency for AC signals. To observe the behavior of resistors in

More information

Lab 1. Resonance and Wireless Energy Transfer Physics Enhancement Programme Department of Physics, Hong Kong Baptist University

Lab 1. Resonance and Wireless Energy Transfer Physics Enhancement Programme Department of Physics, Hong Kong Baptist University Lab 1. Resonance and Wireless Energy Transfer Physics Enhancement Programme Department of Physics, Hong Kong Baptist University 1. OBJECTIVES Introduction to the concept of resonance Observing resonance

More information

No Brain Too Small PHYSICS

No Brain Too Small PHYSICS ELECTRICITY: AC QUESTIONS No Brain Too Small PHYSICS MEASURING IRON IN SAND (2016;3) Vivienne wants to measure the amount of iron in ironsand mixtures collected from different beaches. The diagram below

More information

Chapt ha e pt r e r 11 Inductors

Chapt ha e pt r e r 11 Inductors Chapter 11 Inductors The Basic Inductor When a length of wire is formed onto a coil, it becomes a basic inductor Magnetic lines of force around each loop in the winding of the coil effectively add to the

More information

AC Circuits INTRODUCTION DISCUSSION OF PRINCIPLES. Resistance in an AC Circuit

AC Circuits INTRODUCTION DISCUSSION OF PRINCIPLES. Resistance in an AC Circuit AC Circuits INTRODUCTION The study of alternating current 1 (AC) in physics is very important as it has practical applications in our daily lives. As the name implies, the current and voltage change directions

More information

1. If the flux associated with a coil varies at the rate of 1 weber/min,the induced emf is

1. If the flux associated with a coil varies at the rate of 1 weber/min,the induced emf is 1. f the flux associated with a coil varies at the rate of 1 weber/min,the induced emf is 1 1. 1V 2. V 60 3. 60V 4. Zero 2. Lenz s law is the consequence of the law of conservation of 1. Charge 2. Mass

More information

Laboratory Exercise 6 THE OSCILLOSCOPE

Laboratory Exercise 6 THE OSCILLOSCOPE Introduction Laboratory Exercise 6 THE OSCILLOSCOPE The aim of this exercise is to introduce you to the oscilloscope (often just called a scope), the most versatile and ubiquitous laboratory measuring

More information

Lab 6 - Inductors and LR Circuits

Lab 6 - Inductors and LR Circuits Lab 6 Inductors and LR Circuits L6-1 Name Date Partners Lab 6 - Inductors and LR Circuits The power which electricity of tension possesses of causing an opposite electrical state in its vicinity has been

More information

Electric Circuit Fall 2017 Lab10. LABORATORY 10 RLC Circuits. Guide. Figure 1: Voltage and current in an AC circuit.

Electric Circuit Fall 2017 Lab10. LABORATORY 10 RLC Circuits. Guide. Figure 1: Voltage and current in an AC circuit. LABORATORY 10 RLC Circuits Guide Introduction RLC circuit When an AC signal is input to a RLC circuit, voltage across each element varies as a function of time. The voltage will oscillate with a frequency

More information

A.C. Circuits -- Conceptual Solutions

A.C. Circuits -- Conceptual Solutions A.C. Circuits -- Conceptual Solutions 1.) Charge carriers in a DC circuit move in one direction only. What do charge carriers do in an AC circuit? Solution: The voltage difference between the terminals

More information

Look over Chapter 31 sections 1-4, 6, 8, 9, 10, 11 Examples 1-8. Look over Chapter 21 sections Examples PHYS 2212 PHYS 1112

Look over Chapter 31 sections 1-4, 6, 8, 9, 10, 11 Examples 1-8. Look over Chapter 21 sections Examples PHYS 2212 PHYS 1112 PHYS 2212 Look over Chapter 31 sections 1-4, 6, 8, 9, 10, 11 Examples 1-8 PHYS 1112 Look over Chapter 21 sections 11-14 Examples 16-18 Good Things To Know 1) How AC generators work. 2) How to find the

More information

Lecture 16 Date: Frequency Response (Contd.)

Lecture 16 Date: Frequency Response (Contd.) Lecture 16 Date: 03.10.2017 Frequency Response (Contd.) Bode Plot (contd.) Bode Plot (contd.) Bode Plot (contd.) not every transfer function has all seven factors. To sketch the Bode plots for a generic

More information

Chapter 33. Alternating Current Circuits

Chapter 33. Alternating Current Circuits Chapter 33 Alternating Current Circuits Alternating Current Circuits Electrical appliances in the house use alternating current (AC) circuits. If an AC source applies an alternating voltage to a series

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

PART B. t (sec) Figure 1

PART B. t (sec) Figure 1 Code No: R16128 R16 SET 1 I B. Tech II Semester Regular Examinations, April/May 217 ELECTRICAL CIRCUIT ANALYSIS I (Electrical and Electronics Engineering) Time: 3 hours Max. Marks: 7 Note: 1. Question

More information

Experiment 13: LR Circuit

Experiment 13: LR Circuit 012-05892A AC/DC Electronics Laboratory Experiment 13: LR Circuit Purpose Theory EQUIPMENT NEEDED: Computer and Science Workshop Interface Power Amplifier (CI-6552A) (2) Voltage Sensor (CI-6503) AC/DC

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

Physics 132 Quiz # 23

Physics 132 Quiz # 23 Name (please (please print) print) Physics 132 Quiz # 23 I. I. The The current in in an an ac ac circuit is is represented by by a phasor.the value of of the the current at at some time time t t is is

More information

Activity P51: LR Circuit (Power Output, Voltage Sensor)

Activity P51: LR Circuit (Power Output, Voltage Sensor) Activity P51: LR Circuit (Power Output, Voltage Sensor) Concept DataStudio ScienceWorkshop (Mac) ScienceWorkshop (Win) Circuits P51 LR Circuit.DS (See end of activity) (See end of activity) Equipment Needed

More information

Lab #4: Measuring Q by the Ringdown Method Physics 426

Lab #4: Measuring Q by the Ringdown Method Physics 426 Name: I. INTRODUCTION See Part V, Tuned LRC Circuits. In this lab exercise, we will be working with the setup shown below in Figure 1. Function generator in squarewave mode (to CH. 1 (to CH. 2 Figure 1.

More information

The G4EGQ RAE Course Lesson 4A AC theory

The G4EGQ RAE Course Lesson 4A AC theory AC. CIRCUITS This lesson introduces inductors into our AC. circuit. We then look at the result of having various combinations of capacitance, inductance and resistance in the same circuit. This leads us

More information

Inductance, capacitance and resistance

Inductance, capacitance and resistance Inductance, capacitance and resistance As previously discussed inductors and capacitors create loads on a circuit. This is called reactance. It varies depending on current and frequency. At no frequency,

More information

Solution: All electromagnetic waves in vacuum, regardless of their wavelength or frequency, travel at the speed of light, c.

Solution: All electromagnetic waves in vacuum, regardless of their wavelength or frequency, travel at the speed of light, c. 1. Two electromagnetic waves travel through empty space. Wave A as a wavelength of 700 nm (red light), while Wave B has a wavelength of 400 nm (blue light). Which statement is true? A) Wave A travels faster

More information

UNIT-04 ELECTROMAGNETIC INDUCTION & ALTERNATING CURRNT

UNIT-04 ELECTROMAGNETIC INDUCTION & ALTERNATING CURRNT UNIT-04 ELECTROMAGNETIC INDUCTION & ALTERNATING CURRNT.MARK QUESTIONS:. What is the magnitude of the induced current in the circular loop-a B C D of radius r, if the straight wire PQ carries a steady current

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

CHAPTER 22: Electromagnetic Waves. Answers to Questions

CHAPTER 22: Electromagnetic Waves. Answers to Questions CHAPTR : lectromagnetic Waves Answers to Questions. If the direction of travel for the M wave is north and the electric field oscillates east-west, then the magnetic field must oscillate up and down. For

More information

Experiment 18: Driven RLC Circuit

Experiment 18: Driven RLC Circuit MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics 8. Spring 3 Experiment 8: Driven LC Circuit OBJECTIVES To measure the resonance frequency and the quality factor of a driven LC circuit INTODUCTION

More information

Resonant Frequency of the LRC Circuit (Power Output, Voltage Sensor)

Resonant Frequency of the LRC Circuit (Power Output, Voltage Sensor) 72 Resonant Frequency of the LRC Circuit (Power Output, Voltage Sensor) Equipment List Qty Items Part Numbers 1 PASCO 750 Interface 1 Voltage Sensor CI-6503 1 AC/DC Electronics Laboratory EM-8656 2 Banana

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

Project: Electromagnetic Ring Launcher

Project: Electromagnetic Ring Launcher Project: Electromagnetic Ring Launcher Introduction: In science museums and physics-classrooms an experiment is very commonly demonstrated called the Jumping Ring or Electromagnetic Ring Launcher. The

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

General Physics (PHY 2140)

General Physics (PHY 2140) General Physics (PHY 2140) Lecture 11 Electricity and Magnetism AC circuits and EM waves Resonance in a Series RLC circuit Transformers Maxwell, Hertz and EM waves Electromagnetic Waves 6/18/2007 http://www.physics.wayne.edu/~alan/2140website/main.htm

More information

Lab 9 - AC Filters and Resonance

Lab 9 - AC Filters and Resonance Lab 9 AC Filters and Resonance L9-1 Name Date Partners Lab 9 - AC Filters and Resonance OBJECTIES To understand the design of capacitive and inductive filters. To understand resonance in circuits driven

More information

The Tuned Circuit. Aim of the experiment. Circuit. Equipment and components. Display of a decaying oscillation. Dependence of L, C and R.

The Tuned Circuit. Aim of the experiment. Circuit. Equipment and components. Display of a decaying oscillation. Dependence of L, C and R. The Tuned Circuit Aim of the experiment Display of a decaying oscillation. Dependence of L, C and R. Circuit Equipment and components 1 Rastered socket panel 1 Resistor R 1 = 10 Ω, 1 Resistor R 2 = 1 kω

More information

Electricity and Magnetism Transformers and Alternating Current

Electricity and Magnetism Transformers and Alternating Current Electricity and Magnetism Transformers and Alternating Current Lana Sheridan De Anza College Mar 16, 2018 Last time mutual inductance LC circuits and oscillations Overview LC circuits, mechanical analogy

More information

ALTERNATING CURRENT. Lesson-1. Alternating Current and Voltage

ALTERNATING CURRENT. Lesson-1. Alternating Current and Voltage esson- ATENATING UENT Alternating urrent and oltage An alternating current or voltage is that variation of current or voltage respectively whose magnitude and direction vary periodically and continuously

More information

Radio Frequency Electronics

Radio Frequency Electronics Radio Frequency Electronics Preliminaries II Guglielmo Giovanni Maria Marconi Thought off by many people as the inventor of radio Pioneer in long-distance radio communications Shared Nobel Prize in 1909

More information

Exercise 1: Inductors

Exercise 1: Inductors Exercise 1: Inductors EXERCISE OBJECTIVE When you have completed this exercise, you will be able to describe the effect an inductor has on dc and ac circuits by using measured values. You will verify your

More information

KINGS COLLEGE OF ENGINEERING DEPARTMENT OF ELECTRICAL AND ELECTRONICS ENGINEERING QUESTION BANK UNIT I BASIC CIRCUITS ANALYSIS PART A (2-MARKS)

KINGS COLLEGE OF ENGINEERING DEPARTMENT OF ELECTRICAL AND ELECTRONICS ENGINEERING QUESTION BANK UNIT I BASIC CIRCUITS ANALYSIS PART A (2-MARKS) KINGS COLLEGE OF ENGINEERING DEPARTMENT OF ELECTRICAL AND ELECTRONICS ENGINEERING QUESTION BANK YEAR / SEM : I / II SUBJECT CODE & NAME : EE 1151 CIRCUIT THEORY UNIT I BASIC CIRCUITS ANALYSIS PART A (2-MARKS)

More information

DC and AC Circuits. Objective. Theory. 1. Direct Current (DC) R-C Circuit

DC and AC Circuits. Objective. Theory. 1. Direct Current (DC) R-C Circuit [International Campus Lab] Objective Determine the behavior of resistors, capacitors, and inductors in DC and AC circuits. Theory ----------------------------- Reference -------------------------- Young

More information