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.

Slides:



Advertisements
Similar presentations
Electromagnetic Induction
Advertisements

Electromagnetic Induction Inductors. Problem A metal rod of length L and mass m is free to slide, without friction, on two parallel metal tracks. The.
Fisica Generale - Alan Giambattista, Betty McCarty Richardson Copyright © 2008 – The McGraw-Hill Companies s.r.l. 1 Chapter 20: Electromagnetic Induction.
Physics 1304: Lecture 13, Pg 1 Faraday’s Law and Lenz’s Law ~ B(t) i.
Lenz’s Law AP Physics C Montwood High School R. Casao.
Chapter 22 Electromagnetic Induction Induced Emf and Induced Current There are a number of ways a magnetic field can be used to generate an electric.
Lecture 20 Discussion. [1] A rectangular coil of 150 loops forms a closed circuit with a resistance of 5 and measures 0.2 m wide by 0.1 m deep, as shown.
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.
Copyright © 2009 Pearson Education, Inc. Lecture 9 – Electromagnetic Induction.
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.
Physics 24-Winter 2003-L181 Electromagnetic Induction Basic Concepts Faraday’s Law (changing magnetic flux induces emf) Lenz’s Law (direction of induced.
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.
Electromagnetic Induction
Electromagnetic Induction What’s Next? Electromagnetic Induction Faraday’s Discovery Electromotive Force Magnetic Flux Electric Generators Lenz’s Law.
Induction and Inductance Chapter 30 Magnetic Flux.
Lect. 15: Faraday’s Law and Induction
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.
Electromagnetic Induction
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
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.
Chapter 29 Electromagnetic Induction and Faraday’s Law
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 31 Faraday’s Law. Introduction This section we will focus on the last of the fundamental laws of electromagnetism, called Faraday’s Law of Induction.
Chapter 20 Self-Inductance LR Circuits Motional EMF.
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.
MAGNETIC INDUCTION MAGNETUIC FLUX: FARADAY’S LAW, INDUCED EMF:
Faraday’s Law of Induction
Electromagnetic Induction What do we know? Hans Christian Oersted showed that moving charges create a magnetic field.
Induction II. Law of Induction The magnitude of the induced emf in a circuit is equal to the rate at which the magnetic flux through the circuit is.
Announcements Clicker quizzes NO LONGER GRADED!
Electromagnetic Induction (EMI) AP Physics. Electromagnetic Induction (EMI) A changing magnetic field can induce a current in a circuit called the induced.
Magnetic Flux and Faraday’s Law of Induction
My Chapter 20 Lecture Outline.
Unit 5 Day 2: Induced EMF in a Moving Conductor Induced EMF in a Moving Conductor in a Magnetic Field Force Required to Move a Moving Conductor in a Uniform.
What is the direction of the induced current?
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.
Faraday’s Law.
Magnetism #2 Induced EMF Ch.20. Faraday’s Law of Induction We now know that a current carrying wire will produce its own magnetic field with the lines.
Physics 102: Lecture 10, Slide 1 Faraday’s Law Physics 102: Lecture 10 Changing Magnetic Fields create Electric Fields Last Two Lectures Magnetic fields.
Slide 1Fig 31-CO, p.967. Slide 2 The focus of our studies in electricity and magnetism so far has been the electric fields produced by stationary charges.
Copyright © 2009 Pearson Education, Inc. Chapter 29 Electromagnetic Induction and Faraday’s Law.
Chapter 22 Electromagnetic Induction Induced Emf and Induced Current There are a number of ways a magnetic field can be used to generate an electric.
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
Problem 4 A metal wire of mass m can slide without friction on two parallel, horizontal, conducting rails. The rails are connected by a generator which.
Finally! Flux! Electromagnetic Induction. Objectives.
AP Physics ST Motional emf Lenz’s Law ireference.ca.
AP Physics Summer Institute Free-Response-Questions MAGNETISM.
Physics 212 Lecture 17, Slide 1 Physics 212 Lecture 17 Faraday’s Law.
EMF Induced in a Moving Conductor (“Motional EMF”)
Faraday’s Law.
Electromagnetic induction
Electromagnetic Induction

I2 is decreasing in magnitude I2 is constant
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.
Electromagnetic Induction
Phys102 Lecture 18/19 Electromagnetic Induction and Faraday’s Law
EMF Induced in a Moving Conductor (“Motional EMF”)
Induction An induced current is produced by a changing magnetic field There is an induced emf associated with the induced current A current can be produced.
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 Flux () is related to the number of magnetic field lines passing through a surface B N S B Magnetic Flux =  = B A cos  SI unit = 1 Weber.
Electromagnetic Induction
Faraday’s Law.
Induction and Inductance Chapter 30
Chapter 31 Faraday’s Law 31.1 Faraday’s Law of Induction
Presentation transcript:

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 the power switch, on the left, up. Next, store your student number in the clicker. You only have to do this once. Press the * button to enter the setup menu. Press the up arrow button to get to ID Press the big green arrow key Press the T button, then the up arrow to get a U Enter the rest of your BU ID. Press the big green arrow key.

Motional emf Motional emf is the voltage induced across a conductor moving through a magnetic field. If a metal rod of length L moves at velocity v through a magnetic field B, the motional emf is: as long as the velocity, field, and length are mutually perpendicular. In which direction do positive charges deflect, if they move with a metal rod to the right in a magnetic field directed into the page?

Motional emf In which direction do positive charges deflect, if they move with a metal rod to the right in a magnetic field directed into the page? Use the right-hand rule associated with. Positive charges deflect up, and negative charges deflect down.

Acting like a battery The moving rod can act like a battery if we connect it up in a circuit, like so. The rod is placed on a pair of conducting rails that are separated by a distance L. The rails are connected at the left end by a resistor of resistance R - assume the resistance of the rod and rails is negligible compared to R. There is a uniform magnetic field of magnitude B directed into the page.

Direction of the induced current? If the rod (in red) is moved to the right, will there be an induced current? If so, in what direction is it? 1. Clockwise 2. Counterclockwise 3. There is no induced current

Apply the pictorial method BeforeAfter The simulation draws the Before and After pictures for us. To oppose the change, the loop needs to create field lines out of the page, requiring a counterclockwise induced current.

Acting like a battery The rod is initially at rest, but is then subjected to a constant force F directed right. Neglect friction between the rod and the rails. What happens? 1. The bar experiences a constant acceleration, and the speed increases at a constant rate 2. The changing flux gives rise to another force in the same direction as F that accelerates the bar even faster than F would by itself. 3. The changing flux gives rise to another force opposite in direction to F that causes the bar to reach a terminal (constant) velocity 4. The changing flux gives rise to another force opposite in direction to F that causes the bar to come to rest

Acting like a battery The faster the rod goes, the larger the current induced in the loop consisting of rod, rail, resistor, rail. This current gives rise to a force of magnitude ILB opposing the applied force F. When the forces are equal and opposite, there is no net force, so the rod continues to move at a constant velocity. F ILB

Eddy currents An eddy current is a swirling current set up in a conductor in response to a changing magnetic field. By Lenz's law, the swirling current sets up a magnetic field opposing the change. In a conductor, electrons swirl in a plane perpendicular to the magnetic field. Eddy currents cause energy to be lost. More accurately, eddy currents transform more useful forms of energy, such as kinetic energy, into heat, which is generally much less useful. In many applications the loss of useful energy is not particularly desirable, but there are some practical applications such as train brakes.

Eddy current application: train brakes During braking, the metal wheels are exposed to a magnetic field from an electromagnet, generating eddy currents in the wheels. The magnetic interaction between the applied field and the eddy currents acts to slow the wheels down. The faster the wheels are spinning, the stronger the effect, meaning that as the train slows the braking force is reduced, producing a smooth stopping motion. Draw a set of pictures for the green region, to show the direction of the induced current in the green region as it enters the magnetic field.

Eddy current application: train brakes During braking, the metal wheels are exposed to a magnetic field from an electromagnet, generating eddy currents in the wheels. The magnetic interaction between the applied field and the eddy currents acts to slow the wheels down. The faster the wheels are spinning, the stronger the effect, meaning that as the train slows the braking force is reduced, producing a smooth stopping motion. In which direction is the force on this induced current?

Eddy current application: train brakes During braking, the metal wheels are exposed to a magnetic field from an electromagnet, generating eddy currents in the wheels. The magnetic interaction between the applied field and the eddy currents acts to slow the wheels down. The faster the wheels are spinning, the stronger the effect, meaning that as the train slows the braking force is reduced, producing a smooth stopping motion.

Eddy current question To stop (or slow down) the train, an electromagnet is turned on, passing a magnetic field through sections of the train's wheels. The eddy currents set up in the wheels act to slow the train down. What would happen if the direction of the magnetic field was reversed? 1. The train would still slow down. 2. The train would speed up.

Eddy current question If the field goes the other way, the eddy currents also reverse direction. Reversing both the field and the current gives a force ( F = ILB ) in the same direction – the train still slows down.

Whiteboard