Faraday’s Law Physics 102: Lecture 10 Changing Magnetic Fields create Electric Fields Exam II Exam 1 tonight Be sure to bring your ID and go to correct.

Slides:



Advertisements
Similar presentations
Electromagnetism.
Advertisements

F=BqvsinQ for a moving charge F=BIlsinQ for a current
Q29.1 A circular loop of wire is in a region of spatially uniform magnetic field. The magnetic field is directed into the plane of the figure. If the magnetic.
Chapter 31 Faraday’s Law 31.1 Faraday’s Law of Induction
Physics 1304: Lecture 13, Pg 1 Faraday’s Law and Lenz’s Law ~ B(t) i.
Phys 102 – Lecture 13 Motional EMF & Lenz’ law.
Physics 4 Magnetic Induction Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB.
Lenz’s Law AP Physics C Montwood High School R. Casao.
Generators & Motors Textbook Sections 23-6 – Physics.
Faraday’s Law PH 203 Professor Lee Carkner Lecture 19.
Magnetic Fields Faraday’s Law
Faraday’s Law - Induction Textbook Sections Physics 1161: PreLecture 14 Changing Magnetic Fields create Electric Fields.
Physics 24-Winter 2003-L181 Electromagnetic Induction Basic Concepts Faraday’s Law (changing magnetic flux induces emf) Lenz’s Law (direction of induced.
ConcepTest Clicker Questions College Physics, 7th Edition
Two questions: (1) How to find the force, F on the electric charge, Q excreted by the field E and/or B? (2) How fields E and/or B can be created? Gauss’s.
Announcements  Homework for tomorrow… Ch. 33: CQ 4, Probs. 10, 12, & 14 CQ1: CCW CQ2: push against resistive force 33.2: 0.10 T, out of page 33.3: 2.3.
Motors Physics 102 Professor Lee Carkner Lecture 21.
Physics 121: Electricity & Magnetism – Lecture 11 Induction I Dale E. Gary Wenda Cao NJIT Physics Department.
Remember?  An electron is moving downward with a velocity, v, in a magnetic field directed within the page, determine direction of force.
Magnetic Flux and Faraday’s Law of Induction
Induced EMF. EMF EMF - It is potential difference and is measured in volts (V ).
When a coil of wire and a bar magnet are moved in relation to each other, an electric current is produced. This current is produced because the strength.
Today’s Concept: Faraday’s Law Lenz’s Law
Chapter 20 Induced Voltages and Inductance. Faraday’s Experiment A primary coil is connected to a battery and a secondary coil is connected to an ammeter.
Induction: Faraday’s Law
Magnetic Induction Chapter Induced currents
1 Chapter 30: Induction and Inductance Introduction What are we going to talk about in chapter 31: A change of magnetic flux through a conducting loop.
Chapter 31 Faraday’s Law.
1 W09D2: Faraday’s Law: The Best Law in the Entire Universe Today’s Reading Assignment Course Notes: Sections
Chapter 20 Induced Voltages and Inductance. Faraday’s Experiment – Set Up A current can be produced by a changing magnetic field First shown in an experiment.
Chapter 3: Faraday’s Law. 2.1 Induced EMF and magnetic flux  Two circuits are not connected: no current?  However, closing the switch we see that the.
Faraday’s Law Sections Physics 1161: Lecture 14 Changing Magnetic Fields create Electric Fields.
Chapter 21 Magnetic Induction. Electric and magnetic forces both act only on particles carrying an electric charge Moving electric charges create a magnetic.
Fall 2008Physics 231Lecture 9-1 Electromagnetic Induction.
Induced Voltage and Inductance
Faraday's Law dS B.
A circular loop of wire is in a region of spatially uniform magnetic field. The magnetic field is directed into the plane of the figure. If the magnetic.
Faraday’s Law of Induction
Induced Voltages and Inductance
Chapter 20 Electromagnetic Induction. Electricity and magnetism Generators, motors, and transformers.
Chapter 22 Electromagnetic Induction Magnetic Fields Produced by Currents The direction of the magnetic field due to a current-carrying wire can.
Using the “Clicker” If you have a clicker now, and did not do this last time, please enter your ID in your clicker. First, turn on your clicker by sliding.
Magnetic Induction. Key Points about Induction  If the current in the primary circuit is constant, then the current in the secondary circuit is zero.
Generators & Motors Textbook Sections 23-6 – Physics.
ConcepTest 23.1a Magnetic Flux I In order to change the magnetic flux through the loop, what would you have to do? 1) drop the magnet 2) move the magnet.
Physics 102: Lecture 10, Slide 1 Faraday’s Law Physics 102: Lecture 10 Changing Magnetic Fields create Electric Fields Exam 1 tonight Be sure to bring.
Physics 102: Lecture 10, Slide 1 Faraday’s Law Physics 102: Lecture 10 Changing Magnetic Fields create Electric Fields Last Two Lectures Magnetic fields.
Induction - Faraday’s Law Sections Physics 1161: Lecture 12 Changing Magnetic Fields create Electric Fields.
 B = BA Cos  Example 1.1 A coil consists of 200 turns of wire. Each turn is a square of side 18 cm, and a uniform magnetic field directed.
1) drop the magnet 2) move the magnet upward
Devil physics The baddest class on campus IB Physics
GeneratorsGenerators and Transformers Today’s lecture will cover Textbook Sections 20.2, 20.6 Physics 102: Lecture 11.
1 Magnetic flux [weber Wb], defines the amount of magnetic field (B [Tesla]) which travels perpendicular to an area A [m 2 ] Symbol: Ф Unit: Weber Wb A.
Right-hand Rule 2 gives direction of Force on a moving positive charge Right-Hand Rule Right-hand Rule 1 gives direction of Magnetic Field due to current.
ElectroMagnetic Induction. What is E/M Induction? Electromagnetic Induction is the process of using magnetic fields to produce voltage, and in a complete.
PHY 102: Lecture Induced EMF, Induced Current 7.2 Motional EMF
Magnetic Induction 1Physics is Life. Objectives To learn how magnetic fields can produce currents in conductors To understand how this effect is applied.
Finally! Flux! Electromagnetic Induction. Objectives.
5/20/16 Oregon State University PH 213, Class #241 Changing Magnetic Flux: Faraday’s Law Mathematically, we can express the motion-induced voltage in a.
Faraday’s Law.
Changing Magnetic Fields create Electric Fields
General Physics (PHY 2140) Lecture 17 Electricity and Magnetism
General Review Electrostatics Magnetostatics Electrodynamics
Changing Magnetic Fields create Electric Fields
Active Figure 31.1 (a) When a magnet is moved toward a loop of wire connected to a sensitive ammeter, the ammeter deflects as shown, indicating that a.
Changing Magnetic Fields create Electric Fields
Changing Magnetic Fields create Electric Fields
ConcepTest Clicker Questions College Physics, 7th Edition
Changing Magnetic Fields create Electric Fields
Chapter 31 Faraday’s Law 31.1 Faraday’s Law of Induction
Presentation transcript:

Faraday’s Law Physics 102: Lecture 10 Changing Magnetic Fields create Electric Fields Exam II Exam 1 tonight Be sure to bring your ID and go to correct roomcorrect room All you need is pencil/pen and calculator –No cell phones –No IPods, etc.

Last Two Lectures Magnetic fields Forces on moving charges and currents Magnetic field due to –Long straight wire –Solenoid

Today: Faraday’s Law Key to EVERYTHING in E+M –Generating electricity –Microphones, Speakers and Tape Decks –Amplifiers –Computer disks and card readers –Ground Fault Interrupters 7

Motional EMF, Preflight 10.1 F = q v B sin(  ) + v Potential Difference  = F d/q EMF = q v B sin(  ) L/q = v B L B L v Only 22% got this correct on the preflight!! Velocity Moving + charge feels force downwards: Moving + charge still feels force downwards: B 10 F

Preflight 10.2 Which bar has the larger motional emf? a b v v E = v B L sin(  )  is angle between v and B Case a:  = 0, so E = 0 Case b:  = 90, so E = v B L 52% got this correct. 12 “A is parallel, b is perpendicular”

Motional EMF circuit Direction of Current Direction of force (F=ILB sin(  )) on bar due to magnetic field I =  /R Magnitude of current Clockwise (+ charges go down thru bar, up thru bulb) To left, slows down Moving bar acts like battery  = vBL B -+-+ V What changes if B points into page? = vBL/R 15 DEMO: 371

Motional EMF circuit I =  /R = vBL/R Still to left, slows down Moving bar acts like battery  = vBL B + - V x x x x x x x x x x x x x x x x x Direction of Current Direction of force (F=ILB sin(  )) on bar due to magnetic field Magnitude of current Counter-Clockwise (+ charges go up thru bar, down thru bulb) 18

Preflight 10.4 Increase Stay the Same Decrease Suppose the magnetic field is reversed so that it now points OUT of the page instead of IN as shown in the figure. To keep the bar moving at the same speed, the force supplied by the hand will have to: F=ILB sin(  )) B and v still perpendicular (  =90), so F=ILB just like before! 32% 52% 16% 19

Preflight 10.5 True False Suppose the magnetic field is reversed so that it now points OUT of the page instead of IN as shown in the figure. To keep the bar moving to the right, the hand will have to supply a force in the opposite direction. Current flows in the opposite direction, so force from the B field remains the same! 51% 49% 20

Magnetic Flux Count number of field lines through loop. Uniform magnetic field, B, passes through a plane surface of area A. A Magnetic flux  = B A Magnetic flux   B A cos(  )  is angle between normal and B 22 B A  normal B Note: The flux can be negative (if field lines go thru loop in opposite direction)

Preflight 10.7 Compare the flux through loops a and b. 1)  a >  b 2)  a <  b a b n n B  A = B A cos(0) = BA  B = B A cos(90) = 0 68% 32% 24 “more lines pass through its surface in that position.”

Faraday’s Law (EMF Magnitude) Emf = Change in magnetic Flux/Time Since  = B A cos(  3 things can change  1.Area of loop 2.Magnetic field B 3.Angle  between A and B 26

28 Lenz’s Law (EMF Direction) Emf opposes change in flux EMF does NOT oppose B field, or flux! EMF opposes the CHANGE in flux If flux increases: New EMF makes new field opposite original field If flux decreases: New EMF makes new field same as original field demo: 1093

ACT: Change Area 1 v v 3 Which loop has the greatest induced EMF at the instant shown above? L W E 1 = BvL E 3 = BvW 1 moves right - gets 4 more field lines. 2 moves down - gets 0 more field lines. 3 moves down - only gets 2 more lines. 2 v E 2 = 0 1 is gaining flux fastest! 35

Change Area II V t=0  0 =BLW t  t =BL(W+vt) L W V W vt EMF Direction: B is out of page and  is increasing so EMF creates B field (inside loop) going into page. I 38 EMF Magnitude:  = B A cos(  )

ACT: Change B As current is increasing in the solenoid, what direction will current be induced in ring? 1)Same as solenoid 2)Opposite of solenoid 3)No current 40 SNSN  Solenoid current (counter-clockwise)  B-field (upwards) =>  Flux thru loop EMF will create opposite B-field (downwards) Induced loop current must be clockwise Demo 157

ACT: Change B II SNSN Flux from magnet is down. Induced current creates flux up - opposite original. So flux from magnet must be increasing. Magnet must be falling down N S 42 Which way is the magnet moving if it is inducing a current in the loop as shown? 1)Up 2)Down Demo 371

ACT: Change B II (cont’d) If I reduce the resistance in the wire, the magnet will fall 1)faster 2)slower 3)at the same speed SNSN N S Decreasing R, increases I. Increases opposing field, which makes magnet fall slower. 42

Change  A flat coil of wire has A=0.2 m 2 and R=10 . At time t=0, it is oriented so the normal makes an angle  0 =0 w.r.t. a constant B field of 0.12 T. The loop is rotated to an angle of  =30 o in 0.5 seconds. Calculate the induced EMF. n B A   i = B A cos(0)  f = B A cos(30)  = 6.43x10 -3 Volts 44 What direction is the current induced?  upwards and decreasing. New field will be in same direction (opposes change). Current must be counter clockwise. Demo 68, 371

Magnetic Flux Examples A conducting loop is inside a solenoid (B=  o nI). What happens to the flux through the loop when you… Increase area of solenoid? Increase area of loop? Increase current in solenoid? Rotate loop slightly? Nothing Increases   B A cos(  ) Increases Decreases 48

Magnetic Flux II Increase area of solenoid Increase area of loop Increase current in solenoid Increases Nothing Increases 50 A solenoid (B=  o nI) is inside a conducting loop. What happens to the flux through the loop when you…   B A cos(  )

Good Luck Tonight! 50