Physics 102: Lecture 11 Generators and Transformers
|
|
- Basil Murphy
- 5 years ago
- Views:
Transcription
1 Physics 102: Lecture 11 Generators and Transormers Physics 102: Lecture 11, Slide 1
2 Reiew: Magnetic Flux & Induction B Flux: Induced oltage: = B A cos() is angle between normal and B ε = Φ Δt = Φ Φ i t t i Last lecture Today Physics 102: Lecture 11, Slide 2 3 things can change : 1. Area o loop 2. Magnetic ield B 3. Angle between normal and B
3 Generators and EMF A loop o wire is rotated (ex: by a steam engine turbine) in a uniorm B ield d normal normal a B B c b = B A cos() Loop normal rotates relatie to B ield => changes => changes => em in loop => oltage generated! Physics 102: Lecture 11, Slide 3
4 Reiew (Phys 101): Rotation Variables,,, T Velocity (): How ast a point moes. Units: usually m/s Angular Frequency ( ): How ast something rotates. Units: radians / sec Physics 102: Lecture 11, Slide 4 = / r Frequency ( ): How ast something rotates. Units: rotations / sec = Hz Period (T): How much time one ull rotation takes. Units: usually seconds r = / 2 T = 1 / = 2 /
5 Generator: lux t = 0, = AB (max) n B t > 0, < AB t = T/4, = 0 t > T/4, < 0 t = T/2, = AB (min) AB t -AB = B A cos() = B A cos( t) Physics 102: Lecture 11, Slide 5
6 Generator: EMF t = 0, ~const, e = 0 ε = Φ Δt B n t > 0,, e > 0 t = T/4,, e (max) t > T/4,, e > 0 t = T/2, ~const, e = 0 AB t AB e t -AB T - AB T = B A cos( t) Physics 102: Lecture 11, Slide 6 e = B A sin( t)
7 Comparison: Flux s. EMF Flux is maximum Most lines thru loop EMF is minimum Just beore: lines enter rom let Just ater: lines enter rom let No change! Physics 102: Lecture 11, Slide 7 Flux is minimum Zero lines thru loop EMF is maximum Just beore: lines enter rom top. Just ater: lines enter rom bottom. Big change!
8 ACT: Generators and EMF x A B C At which time does the loop hae the greatest em (greatest / t)? Physics 102: Lecture 11, Slide 8
9 ACT: EMF direction In which direction does the current low in wire a-b at the moment shown? d a Side iew a B B b c n b n A) B) EMF = 0 C) Physics 102: Lecture 11, Slide 9
10 Generators and Torque e = A B sin() F Voltage! Connect loop to resistance R use I=V/R: I = A B sin() / R I t B Recall: t = A B I sin() = A 2 B 2 sin 2 ()/R F Direction: use RHR1 n Torque, due to current and B ield, tries to slow spinning loop down. Must supply external torque to keep it spinning at constant Physics 102: Lecture 11, Slide 10
11 Generator A generator consists o a square coil o wire with 40 turns, each side is 0.2 meters long, and it is spinning with angular elocity = 2.5 radians/second in a uniorm magnetic ield B=0.15 T. Calculate the maximum EMF and torque i the resistie load is 4W. e = NA B sin() = = t = NI A B sin() x = = = Physics 102: Lecture 11, Slide 11 Note: Em is maximum at =90 Note: Torque is maximum at =90
12 In a hydropower plant, that torque is supplied by alling water. The power plant deliers AC (alternating current) power to your house: the oltage and current switch directions at =60 Hz (more next lecture). At your house: 120 V. There is a big challenge getting electric current to your house: P = I 2 R! Physics 102: Lecture 11, Slide 12
13 Power Transmission A generator produces 1.2 Giga watts o power, which it transmits to a town 7 miles away through power lines with a total resistance 0.01 ohms. How much power is lost in the lines i the energy is transmitted at 120 Volts? P = IV Power deliered by generator through lines I = P/V = 1.2x10 9 W/120 V = 10,000,000 Amps in lines! P = I 2 R Power lost in lines = 10,000,000 2 (.01) = 1.0 Giga Watt Lost in Lines! Large current is the problem. Since P=IV, use high oltage and low current to delier power. I V = 12,000 Volts, lose Giga Watts! Physics 102: Lecture 11, Slide 13
14 Transormers make it possible to distribute electrical power at high oltage and step-down to low oltage at your house. 500,000 V Low current 240 / 120 V High current Physics 102: Lecture 11, Slide 14
15 Transormers Key to Modern electrical system Transorm between high and low oltages Very eicient Nikola Tesla Physics 102: Lecture 11, Slide 15
16 Transormers Key to eicient power distribution Changing current in primary creates changing lux in primary and secondary. iron V p = N p ΔΦ Δt V s = N s ΔΦ Δt V s V p = N s N p Same / t e ~ N s > N p : V s > V p step up V p N s < N p : V s < V p step down N P (primary) V s N S (secondary) R Energy conseration! Physics 102: Lecture 11, Slide 16 I p V p = I s V s I s I p = N p N s
17 CheckPoint 3.1 The good news is you are going on a trip to France. The bad news is that in France the outlets hae 240 olts. You remember rom P102 that you need a transormer, so you wrap 100 turns around the primary. How many turns should you wrap around the secondary i you need 120 olts out to run your hair dryer? iron 1) 50 2) 100 3) 200 e ~ V p V s R N P (primary) N S (secondary) Physics 102: Lecture 11, Slide 17
18 ACT: Transormers iron V p V s R A 12 Volt battery is connected to a transormer transormer that has a 100 turn primary coil, and 200 turn secondary coil. What is the oltage across the secondary ater the battery has been connected or a long time? N P (primary) N S (secondary) A) V s = 0 B) V s = 6 C) V s = 12 D) V s = 24 Physics 102: Lecture 11, Slide 18
19 Questions to Think About In a transormer the side with the most turns always has the larger peak oltage. (T/F) In a transormer the side with the most turns always has the larger peak current. (T/F) In a transormer the side with the most turns always dissipates the most power. (T/F) Which o the ollowing changes will increase the peak oltage deliered by a generator Increase the speed it is spinning. Increase the area o the loop. Increase the strength o the magnetic ield. Physics 102: Lecture 11, Slide 19
Physics 102: Lecture 10. Faraday s Law. Changing Magnetic Fields create Electric Fields. Physics 102: Lecture 10, Slide 1
Physics 102: Lecture 10 Faraday s Law Changing Magnetic Fields create Electric Fields Physics 102: Lecture 10, Slide 1 Last Two Lectures Magnetic fields Forces on moing charges and currents Torques on
More information13. Faraday s Law. S. G. Rajeev. March 3, 2009
13. Faraday s Law S. G. Rajeev March 3, 009 1 Electromotive Force If a coil moves (or rotates) near a magnet, a current in induced on it, even if it is not connected to a battery. That means an electric
More informationElectromagnetism 03/12/2010. Electromagnetism Canada s Triumph Accelerator. Putting it All Together. Hydrogen Minus. Initial Acceleration
Electromagnetism Canada s Triumph Accelerator Putting it All Together Hydrogen Minus Electromagnetism Initial Acceleration Electrostatic Circular Motion Magnetic Steering iltering Magnetic lux Magnetic
More informationFaraday s Law. Physics 102: Lecture 10. Exam 1 tonight. All you need is a #2 pencil, calculator, and your ID. CHEATING we will prosecute!
Physics 102: Lecture 10 Faraday s Law Changing Magnetic Fields create Electric Fields Exam 1 tonight Be sure to bring your ID and go to correct room All you need is a #2 pencil, calculator, and your ID
More informationChapter 21 Lecture Notes
Chapter 21 Lecture Notes Physics 2424 - Strauss Formulas: Φ = BA cosφ E = -N Φ/ t Faraday s Law E = Bvl E = NABω sinωt M = (N 2 Φ 2 )/I 1 E 2 = -M I 1 / t L = NΦ/I E = -L I/ t L = µ 0 n 2 A l Energy =
More informationPhysics 102: Lecture 05 Circuits and Ohm s Law
Physics 102: Lecture 05 Circuits and Ohm s Law Physics 102: Lecture 5, Slide 1 Summary of Last Time Capacitors Physical C = ke 0 A/d C=Q/V Series 1/C eq = 1/C 1 + 1/C 2 Parallel C eq = C 1 + C 2 Energy
More informationTRANSFORMERS B O O K P G
TRANSFORMERS B O O K P G. 4 4 4-449 REVIEW The RMS equivalent current is defined as the dc that will provide the same power in the resistor as the ac does on average P average = I 2 RMS R = 1 2 I 0 2 R=
More informationBook Page cgrahamphysics.com Transformers
Book Page 444-449 Transformers Review The RMS equivalent current is defined as the dc that will provide the same power in the resistor as the ac does on average P average = I 2 RMS R = 1 2 I 0 2 R= V RMS
More informationPhysics 11b Lecture #13
Physics 11b Lecture #13 Faraday s Law S&J Chapter 31 Midterm #2 Midterm #2 will be on April 7th by popular vote Covers lectures #8 through #14 inclusive Textbook chapters from 27 up to 32.4 There will
More informationSelf-Inductance. Φ i. Self-induction. = (if flux Φ 1 through 1 loop. Tm Vs A A. Lecture 11-1
Lecture - Self-Inductance As current i through coil increases, magnetic flux through itself increases. This in turn induces back emf in the coil itself When current i is decreasing, emf is induced again
More informationLenz s Law (Section 22.5)
Lenz s Law (Section 22.5) : Thursday, 25 of February 7:00 9:00 pm Rooms: Last Name Room (Armes) Seats A - F 201 122 G - R 200 221 S - Z 205 128 2016-02-21 Phys 1030 General Physics II (Gericke) 1 1) Charging
More informationChapter 20: Electromagnetic Induction. PHY2054: Chapter 20 1
Chapter 20: Electromagnetic Induction PHY2054: Chapter 20 1 Electromagnetic Induction Magnetic flux Induced emf Faraday s Law Lenz s Law Motional emf Magnetic energy Inductance RL circuits Generators and
More informationVoltage (AC) period, T
33-1 (SJP, Phys 1120) AC Voltage and Current: Batteries produce a steady, fixed voltage, called DC, or direct current. (We should probably call them DV, direct voltage, but never mind) The power company
More informationInformation for Physics 1201 Midterm I Wednesday, February 20
My lecture slides are posted at http://www.physics.ohio-state.edu/~humanic/ Information for Physics 1201 Midterm I Wednesday, February 20 1) Format: 10 multiple choice questions (each worth 5 points) and
More informationPreview of Period 17: Induction Motors and Transformers
Preview of Period 17: Induction Motors and Transformers 17.1 Induced Current How can we use induce current in a wire? 17.2 Generators How is electricity generated? 17.3 AC and DC Induced Current Is the
More informationELECTROMAGNETIC OSCILLATIONS AND ALTERNATING CURRENT
Chapter 31: ELECTROMAGNETIC OSCILLATIONS AND ALTERNATING CURRENT 1 A charged capacitor and an inductor are connected in series At time t = 0 the current is zero, but the capacitor is charged If T is the
More informationPhysics 212. Lecture 9. Electric Current
Physics 212 Lecture 9 Electric Current Exam Here, Tuesday, June 26, 8 9:30 AM Will begin at 7:30 for those who must leave by 9. Office hours 1-7 PM, Rm 232 Loomis Bring your ID! Physics 212 Lecture 9,
More informationLast time. Ampere's Law Faraday s law
Last time Ampere's Law Faraday s law 1 Faraday s Law of Induction (More Quantitative) The magnitude of the induced EMF in conducting loop is equal to the rate at which the magnetic flux through the surface
More informationAlternating Currents. The power is transmitted from a power house on high voltage ac because (a) Electric current travels faster at higher volts (b) It is more economical due to less power wastage (c)
More information1 Fig. 3.1 shows the variation of the magnetic flux linkage with time t for a small generator. magnetic. flux linkage / Wb-turns 1.
1 Fig. 3.1 shows the variation of the magnetic flux linkage with time t for a small generator. 2 magnetic 1 flux linkage / 0 10 2 Wb-turns 1 2 5 10 15 t / 10 3 s Fig. 3.1 The generator has a flat coil
More informationPhysics 6B Summer 2007 Final
Physics 6B Summer 2007 Final Question 1 An electron passes through two rectangular regions that contain uniform magnetic fields, B 1 and B 2. The field B 1 is stronger than the field B 2. Each field fills
More informationElectroMagnetic Induction
ElectroMagnetic Induction Physics 1 What is E/M Induction? Electromagnetic Induction is the process of using magnetic fields to produce voltage, and in a complete circuit, a current. Michael Faraday first
More informationExam 2 Solutions. PHY2054 Spring Prof. Paul Avery Prof. Pradeep Kumar Mar. 18, 2014
Exam 2 Solutions Prof. Paul Avery Prof. Pradeep Kumar Mar. 18, 2014 1. A series circuit consists of an open switch, a 6.0 Ω resistor, an uncharged 4.0 µf capacitor and a battery with emf 15.0 V and internal
More informationCh. 23 Electromagnetic Induction, AC Circuits, And Electrical Technologies
Ch. 23 Electromagnetic Induction, AC Circuits, And Electrical Technologies Induced emf - Faraday s Experiment When a magnet moves toward a loop of wire, the ammeter shows the presence of a current When
More information1. An isolated stationary point charge produces around it. a) An electric field only. b) A magnetic field only. c) Electric as well magnetic fields.
1. An isolated stationary point charge produces around it. a) An electric field only. b) A magnetic field only. c) Electric as well magnetic fields. 2. An isolated moving point charge produces around it.
More informationLecture 11 th & 12 th week March April
Lecture 11 th & 12 th week March 27-29-31. April 03. 2017. Chapter 14 Magnetism: Are you attracted or repelled? Where does magnetism come from? What use is magnetism? Post pictures and notes on refrigerators
More informationFaraday's Law F-1. Faraday's Law (in words): An induced emf (E) is created by changing magnetic field.
F-1 Faraday's Law Faraday's Law is one of 4 basic equations of the theory of electromagnetism, called Maxwell's Equations. We have said before that charges makes electric fields. This is the truth, but
More informationPHYSICS. Chapter 30 Lecture FOR SCIENTISTS AND ENGINEERS A STRATEGIC APPROACH 4/E RANDALL D. KNIGHT
PHYSICS FOR SCIENTISTS AND ENGINEERS A STRATEGIC APPROACH 4/E Chapter 30 Lecture RANDALL D. KNIGHT Chapter 30 Electromagnetic Induction IN THIS CHAPTER, you will learn what electromagnetic induction is
More informationAC vs. DC Circuits. Constant voltage circuits. The voltage from an outlet is alternating voltage
Circuits AC vs. DC Circuits Constant voltage circuits Typically referred to as direct current or DC Computers, logic circuits, and battery operated devices are examples of DC circuits The voltage from
More informationMotional EMF & Lenz law
Phys 102 Lecture 13 Motional EMF & Lenz law 1 Physics 102 recently Basic principles of magnetism Lecture 10 magnetic fields & forces Lecture 11 magnetic dipoles & current loops Lecture 12 currents & magneticfields
More informationMutual Inductance. The field lines flow from a + charge to a - change
Capacitors Mutual Inductance Since electrical charges do exist, electric field lines have a starting point and an ending point. For example, if you have a + and a - change, the field lines would look something
More informationPhysics 1402: Lecture 19 Today s Agenda
Physics 1402: Lecture 19 Today s Agenda Announcements: Midterm 1 aailable Homework 06 next Friday Induction Faraday's Law d 1 Induction Effects ar magnet moes through coil Current induced in coil Change
More informationGen. Phys. II Exam 2 - Chs. 21,22,23 - Circuits, Magnetism, EM Induction Mar. 5, 2018
Gen. Phys. II Exam 2 - Chs. 21,22,23 - Circuits, Magnetism, EM Induction Mar. 5, 2018 Rec. Time Name For full credit, make your work clear. Show formulas used, essential steps, and results with correct
More informationAgenda for Today. Elements of Physics II. Forces on currents
Forces on currents Physics 132: Lecture e 14 Elements of Physics II Agenda for Today Currents are moving charges Torque on current loop Torque on rotated loop Currents create B-fields Adding magnetic fields
More informationGeneral Physics (PHY 2140)
General Physics (PHY 2140) Lecture 10 6/12/2007 Electricity and Magnetism Induced voltages and induction Self-Inductance RL Circuits Energy in magnetic fields AC circuits and EM waves Resistors, capacitors
More informationChapter 15 Magnetism and Electromagnetic Induction 15.1 Magnetic Force on a Current-Carrying Wire Homework # 125
Magnetism and Electromagnetic nduction 15.1 Magnetic Force on a Current-Carrying Wire Homework # 125 01. A wire carrying a 2.45-A current wire passes through a 1.60-T magnetic field. What is the force
More informationPhysics 2112 Unit 18
Physics 2112 Unit 18 Today s Concepts: A) Induction B) Circuits Electricity & Magnetism ecture 18, Slide 1 Where we are.. Just finished introducing magnetism Will now apply magnetism to AC circuits Unit
More informationPhysics 7B-1 (A/B) Professor Cebra. Winter 2010 Lecture 2. Simple Circuits. Slide 1 of 20
Physics 7B-1 (A/B) Professor Cebra Winter 2010 Lecture 2 Simple Circuits Slide 1 of 20 Conservation of Energy Density In the First lecture, we started with energy conservation. We divided by volume (making
More informationElectron Theory of Charge. Electricity. 1. Matter is made of atoms. Refers to the generation of or the possession of electric charge.
Electricity Refers to the generation of or the possession of electric charge. There are two kinds of electricity: 1. Static Electricity the electric charges are "still" or static 2. Current Electricity
More informationElectricity Test Review
Electricity Test Review Definitions; Series Circuit, Parallel Circuit, Equivalent Resistance, Fuse, Circuit Breaker, kilowatt hour, load, short circuit, dry cell, wet cell, fuel cells, solar cells, fossil
More informationChapter In Fig , the magnetic flux through the loop increases according to the relation Φ B. =12.0t
Chapter 30 30.1 In Fig. 30-37, the magnetic lux through the loop increases according to the relation = 6.0t 2 + 7.0t where the lux is in milliwebers and t is in seconds. (a) What is the magnitude o the
More informationElectromagnetic Oscillations and Alternating Current. 1. Electromagnetic oscillations and LC circuit 2. Alternating Current 3.
Electromagnetic Oscillations and Alternating Current 1. Electromagnetic oscillations and LC circuit 2. Alternating Current 3. RLC circuit in AC 1 RL and RC circuits RL RC Charging Discharging I = emf R
More informationInduction_P1. 1. [1 mark]
Induction_P1 1. [1 mark] Two identical circular coils are placed one below the other so that their planes are both horizontal. The top coil is connected to a cell and a switch. The switch is closed and
More informationPhysics 2220 Fall 2010 George Williams THIRD MIDTERM - REVIEW PROBLEMS
Physics 2220 Fall 2010 George Williams THIRD MIDTERM - REVIEW PROBLEMS Solution sets are available on the course web site. A data sheet is provided. Problems marked by "*" do not have solutions. 1. An
More informationElements of Physics II. Agenda for Today. Induced EMF. Force on moving charges Induced Current Magnetic Flux Area Vector. Physics 201: Lecture 1, Pg 1
Induced EMF Physics 132: Lecture e 21 Elements of Physics II Agenda for Today Force on moving charges Induced Current Magnetic Flux Area Vector Physics 201: Lecture 1, Pg 1 Atomic Magnets A plausible explanation
More informationPhysics 1502: Lecture 25 Today s Agenda
Physics 1502: Lecture 25 Today s Agenda Announcements: Midterm 2: NOT Nov. 6 Following week Homework 07: due Friday net week AC current esonances Electromagnetic Waves Mawell s Equations - evised Energy
More informationInduction and Inductance
Welcome Back to Physics 1308 Induction and Inductance Michael Faraday 22 September 1791 25 August 1867 Announcements Assignments for Tuesday, November 6th: - Reading: Chapter 30.6-30.8 - Watch Videos:
More informationElectricity (& Magnetism)
EA Notes (Scen 101), Tillery Chapter 6 Electricity (& Magnetism) Introduction First five chapters are "Newtonian Physics", mechanical explanations based on Newton's Laws applied to explain the motion of
More informationPhys 102 Lecture 12 Currents & magnetic fields
Phys 102 Lecture 12 Currents & magnetic fields 1 Today we will... Learn how magnetic fields are created by currents Use specific examples Long straight wire Current loop Solenoid Apply these concepts Electromagnets
More informationElectricity & Magnetism Lecture 9: Electric Current
Electricity & Magnetism Lecture 9: Electric Current Today s Concept: Electric Current Electricity & Magne8sm Lecture 9, Slide 1 Battery and Bulb Which current flow model is correct? Figure 22-5: Four alternative
More informationRevision Compare Between. Application
evision Compare etween Points of Comparison Series Connection Parallel Connection Drawing otal resistance ( ) = + + 3 3 Potential Difference () = + + 3 = = = 3 Electric Current (I) I = I = I = I 3 I =
More informationElements of Physics II. Agenda for Today. Induced EMF. Force on moving charges Induced Current Magnetic Flux Area Vector. Physics 201: Lecture 1, Pg 1
Induced EMF Physics 132: Lecture e 21 Elements of Physics II Agenda for Today Force on moving charges Induced Current Magnetic Flux Area Vector Physics 201: Lecture 1, Pg 1 Clicker Question 11: A rectangular
More informationChapter 31 Electromagnetic Oscillations and Alternating Current LC Oscillations, Qualitatively
Chapter 3 Electromagnetic Oscillations and Alternating Current LC Oscillations, Qualitatively In the LC circuit the charge, current, and potential difference vary sinusoidally (with period T and angular
More informationYou MUST TAKE THE FINAL, even if you are a senior!!! If you are sick that day, you will have to make it up before you are allowed to graduate!
LAHS Physics 2006-2007 End-of-Year Final Review Problems Your End-of-Year Physics Final covers the material in Physics during semester two. Juniors and Seniors will take Finals on the SAME Senior Final
More informationYour comments. Having taken ece 110 made it easy for me to grasp most of the concepts.
Your comments Having taken ece 110 made it easy for me to grasp most of the concepts. God I can go to bed now. Oh wait I can't cuz EXAM??!?!!111 I know that this course has to move at a fast pace and that
More informationa) (4 pts) What is the magnitude and direction of the acceleration of the electron?
PHYSCS 22 Fall 2010 - MDTERM #3 SHOW ALL WORK & REASONNG FOR FULL PONTS Question 1. (5 pts): Accurately show or state the direction of the force that is felt by the following charges or currents. +q -q
More informationLecture 30: WED 04 NOV
Physics 2113 Jonathan Dowling Lecture 30: WED 04 NOV Induction and Inductance II Fender Stratocaster Solenoid Pickup F a r a d a y ' s E x p e r i m e n t s I n a s e r i e s o f e x p e r i m e n t s,
More informationPhysics 1302W.400 Lecture 33 Introductory Physics for Scientists and Engineering II
Physics 1302W.400 Lecture 33 Introductory Physics for Scientists and Engineering II In today s lecture, we will discuss generators and motors. Slide 30-1 Announcement Quiz 4 will be next week. The Final
More informationPhysics 102 Exam 2 Spring Last Name: First Name Network-ID
Last Name: First Name Network-ID Discussion Section: Discussion TA Name: Turn off your cell phone and put it out of sight. Keep your calculator on your own desk. Calculators cannot be shared. This is a
More informationChapter 3: Electric Current and Direct-Current Circuit
Chapter 3: Electric Current and Direct-Current Circuit n this chapter, we are going to discuss both the microscopic aspect and macroscopic aspect of electric current. Direct-current is current that flows
More informationApplication Of Faraday s Law
Application Of Faraday s Law Dr Miguel Cavero September 2, 2014 Application Of Faraday s Law September 2, 2014 1 / 23 The PHYS120 Exam will be divided into three sections as follows: Section A: Short Questions
More informationThis Week. 10/1/2015 Physics 214 Fall
This Week Magnetism: Are you attracted or repelled? Where does magnetism come from? What use is magnetism? Post pictures and notes on refrigerators Electrical motors turn electricity into work Generators
More informationChapter 23 Magnetic Flux and Faraday s Law of Induction
Chapter 23 Magnetic Flux and Faraday s Law of Induction Recall: right hand rule 2 10/28/2013 Units of Chapter 23 Induced Electromotive Force Magnetic Flux Faraday s Law of Induction Lenz s Law Mechanical
More informationFaraday s Law; Inductance
This test covers Faraday s Law of induction, motional emf, Lenz s law, induced emf and electric fields, eddy currents, self-inductance, inductance, RL circuits, and energy in a magnetic field, with some
More information21 MAGNETIC FORCES AND MAGNETIC FIELDS
CHAPTER 1 MAGNETIC FORCES AND MAGNETIC FIELDS ANSWERS TO FOCUS ON CONCEPTS QUESTIONS 1 (d) Right-Hand Rule No 1 gives the direction of the magnetic force as x for both drawings A and B In drawing C, the
More informationClosed loop of moving charges (electrons move - flow of negative charges; positive ions move - flow of positive charges. Nucleus not moving)
Unit 2: Electricity and Magnetism Lesson 3: Simple Circuits Electric circuits transfer energy. Electrical energy is converted into light, heat, sound, mechanical work, etc. The byproduct of any circuit
More informationChapter 22. Induction
Chapter 22 Induction Induced emf A current can be produced by a changing magnetic field First shown in an experiment by Michael Faraday A primary coil is connected to a battery A secondary coil is connected
More informationLecture 21. Resonance and power in AC circuits. Physics 212 Lecture 21, Slide 1
Physics 1 ecture 1 esonance and power in A circuits Physics 1 ecture 1, Slide 1 I max X X = w I max X w e max I max X X = 1/w I max I max I max X e max = I max Z I max I max (X -X ) f X -X Physics 1 ecture
More informationFundamentals of Electric Circuits, Second Edition - Alexander/Sadiku
Chapter 3, Problem 9(8). Find V x in the network shown in Fig. 3.78. Figure 3.78 Chapter 3, Solution 9(8). Consider the circuit below. 2 Ω 2 Ω -j 8 30 o I j 4 j 4 I 2 -j2v For loop, 8 30 = (2 j4)i ji 2
More informationYour Comments. I have three midterms this week; specifically, two tomorrow. I am studying for chemistry and calculus tonight.
Your Comments I wish we had a day off for exams that would be fantastic WE SHOULD NOT HAE HAD CLASS TODAY!!!!! BOOOOOOOo!!! I have three midterms this week; specifically, two tomorrow. I am studying for
More informationPhysics 240 Fall 2005: Exam #3. Please print your name: Please list your discussion section number: Please list your discussion instructor:
Physics 240 Fall 2005: Exam #3 Please print your name: Please list your discussion section number: Please list your discussion instructor: Form #1 Instructions 1. Fill in your name above 2. This will be
More informationFirst Name: Last Name: Section: n 1. March 26, 2003 Physics 202 EXAM 2
First Name: Last Name: Section: n 1 March 26, 2003 Physics 202 EXAM 2 Print your name and section clearly on all five pages. (If you do not know your section number, write your TA s name.) Show all work
More informationNotes on Electricity (Circuits)
A circuit is defined to be a collection of energy-givers (batteries) and energy-takers (resistors, light bulbs, radios, etc.) that form a closed path (or complete path) through which electrical current
More information18 - ELECTROMAGNETIC INDUCTION AND ALTERNATING CURRENTS ( Answers at the end of all questions ) Page 1
( Answers at the end of all questions ) Page ) The self inductance of the motor of an electric fan is 0 H. In order to impart maximum power at 50 Hz, it should be connected to a capacitance of 8 µ F (
More informationGeneral Physics (PHY 2140)
General Physics (PHY 40) eminder: Exam this Wednesday 6/3 ecture 0-4 4 questions. Electricity and Magnetism nduced voltages and induction Self-nductance Circuits Energy in magnetic fields AC circuits and
More informationSlide 1 / 50. Electromagnetic Induction and Faraday s Law
Slide 1 / 50 Electromagnetic Induction and Faraday s Law Slide 2 / 50 Electromagnetic Induction and Faraday s Law Induced EMF Faraday s Law of Induction Lenz s Law EMF Induced in a Moving Conductor Changing
More informationSlide 1 / 50. Slide 2 / 50. Slide 3 / 50. Electromagnetic Induction and Faraday s Law. Electromagnetic Induction and Faraday s Law.
Electromagnetic Induction and Faraday s Law Slide 1 / 50 Electromagnetic Induction and Faraday s Law Slide 2 / 50 Induced EMF Faraday s Law of Induction Lenz s Law EMF Induced in a Moving Conductor Changing
More informationr where the electric constant
0. Coulomb s law a) Explain the concepts of electrons, protons, charged objects, charged up, gaining charge, losing charge, grounding and charge conservation. b) Describe the motion of point charges when
More informationP202 Practice Exam 2 Spring 2004 Instructor: Prof. Sinova
P202 Practice Exam 2 Spring 2004 Instructor: Prof. Sinova Name: Date: (5)1. How many electrons flow through a battery that delivers a current of 3.0 A for 12 s? A) 4 B) 36 C) 4.8 10 15 D) 6.4 10 18 E)
More informationElectromagnetic Induction Faraday s Law Lenz s Law Self-Inductance RL Circuits Energy in a Magnetic Field Mutual Inductance
Lesson 7 Electromagnetic Induction Faraday s Law Lenz s Law Self-Inductance RL Circuits Energy in a Magnetic Field Mutual Inductance Oscillations in an LC Circuit The RLC Circuit Alternating Current Electromagnetic
More informationGreek Letter Omega Ω = Ohm (Volts per Ampere)
) What is electric current? Flow of Electric Charge 2) What is the unit we use for electric current? Amperes (Coulombs per Second) 3) What is electrical resistance? Resistance to Electric Current 4) What
More informationRLC Circuit (3) We can then write the differential equation for charge on the capacitor. The solution of this differential equation is
RLC Circuit (3) We can then write the differential equation for charge on the capacitor The solution of this differential equation is (damped harmonic oscillation!), where 25 RLC Circuit (4) If we charge
More informationGeneral Physics - E&M (PHY 1308) - Lecture Notes. General Physics - E&M (PHY 1308) Lecture Notes
General Physics - E&M (PHY 1308) Lecture Notes Lecture 021: Self-Inductance and Inductors SteveSekula, 12 April 2011 (created 7 November 2010) Goals of this Lecture no tags Understand "self-inductance"
More informationPhysics 212. Motional EMF
Physics 212 Lecture 16 Motional EMF Conductors moing in field nduced emf!! Physics 212 Lecture 16, Slide 1 Music Who is the Artist? A) Gram Parsons ) Tom Waits C) Elis Costello D) Townes Van Zandt E) John
More informationDemo: Solenoid and Magnet. Topics. Chapter 22 Electromagnetic Induction. EMF Induced in a Moving Conductor
Topics Chapter 22 Electromagnetic Induction EMF Induced in a Moving Conductor Magnetic Flux EMF Induced in a Moving Conductor Demo: Solenoid and Magnet v 1 EMF Induced in a Moving Conductor q Work done
More informationFerromagnetism. we saw that with the propane torch on Thursday
Announcements l Help room hours (1248 BPS) Ian La Valley(TA) Mon 4-6 PM Tues 12-3 PM Wed 6-9 PM Fri 10 AM-noon l LON-CAPA #7 due Oct. 25 l Final Exam Tuesday Dec 11 7:45-9:45 AM Ferromagnetism l What makes
More informationChapter 18. Direct Current Circuits
Chapter 18 Direct Current Circuits Sources of emf The source that maintains the current in a closed circuit is called a source of emf Any devices that increase the potential energy of charges circulating
More informationInformation for Makeup exam is posted on the course website.
Information for Makeup exam is posted on the course website. Three resistors are connected to a 6-V battery as shown. The internal resistance of the battery is negligible. What is the current through the
More informationMEP 382: Design of Applied Measurement Systems Lecture 3: DC & AC Circuit Analysis
Faculty of Engineering MEP 38: Design of Applied Measurement Systems Lecture 3: DC & AC Circuit Analysis Outline oltage and Current Ohm s Law Kirchoff s laws esistors Series and Parallel oltage Dividers
More informationChapter 19 Lecture Notes
Chapter 19 Lecture Notes Physics 2424 - Strauss Formulas: R S = R 1 + R 2 +... C P = C 1 + C 2 +... 1/R P = 1/R 1 + 1/R 2 +... 1/C S = 1/C 1 + 1/C 2 +... q = q 0 [1-e -t/(rc) ] q = q 0 e -t/(rc τ = RC
More informationCHAPTER 5: ELECTROMAGNETIC INDUCTION
CHAPTER 5: ELECTROMAGNETIC INDUCTION PSPM II 2005/2006 NO. 5 5. An AC generator consists a coil of 30 turns with cross sectional area 0.05 m 2 and resistance 100 Ω. The coil rotates in a magnetic field
More informationiclicker Quiz a) True b) False
iclicker Quiz (1) I have completed at least 50% of the reading and studyguide assignments associated with the lecture, as indicated on the course schedule. a) True b) False Note on Monday is fee late day
More informationMagnetostatics III. P.Ravindran, PHY041: Electricity & Magnetism 1 January 2013: Magntostatics
Magnetostatics III Magnetization All magnetic phenomena are due to motion of the electric charges present in that material. A piece of magnetic material on an atomic scale have tiny currents due to electrons
More informationPhysics 2135 Exam 2 October 20, 2015
Exam Total / 200 Physics 2135 Exam 2 October 20, 2015 Printed Name: Rec. Sec. Letter: Five multiple choice questions, 8 points each. Choose the best or most nearly correct answer. 1. A straight wire segment
More informationGeneral Physics - E&M (PHY 1308) - Lecture Notes. General Physics - E&M (PHY 1308) Lecture Notes
General Physics - E&M (PHY 1308) Lecture Notes Lecture 029: Forms of Induction and Self-Inductance SteveSekula, 8 November 2010 (created 7 November 2010) Goals of this Lecture no tags Further understand
More informationPHYS 1444 Section 003. Lecture #12
Chapter 5 Power PHYS 1444 Section 003 Alternating Current Microscopic Current Chapter 6 EMF and Terminal Voltage Lecture #1 Tuesday October 9, 01 Dr. Andrew Brandt Resistors in Series and Parallel Energy
More informationPhysics 115. Induction Induced currents. General Physics II. Session 30
Physics 115 General Physics II Session 30 Induction Induced currents R. J. Wilkes Email: phy115a@u.washington.edu Home page: http://courses.washington.edu/phy115a/ 1 Lecture Schedule Today 5/23/14 2 Physics
More informationYour Comments. THIS IS SOOOO HARD. I get the concept and mathematical expression. But I do not get links among everything.
Your omments THIS IS SOOOO HAD. I get the concept and mathematical expression. But I do not get links among everything. ery confusing prelecture especially what happens when switches are closed/opened
More informationYour Comments. I don't understand how to find current given the velocity and magnetic field. I only understand how to find external force
Your Comments CONFUSED! Especially with the direction of eerything The rotating loop checkpoint question is incredibly difficult to isualize. All of this is pretty confusing, but 'm especially confused
More information