Electromagnetic Induction and Electromagnetic Waves!

Slides:



Advertisements
Similar presentations
Electromagnetic Induction
Advertisements

Chapter 30. Induction and Inductance
F=BqvsinQ for a moving charge F=BIlsinQ for a current
Chapter 31 Faraday’s Law 31.1 Faraday’s Law of Induction
Magnetism and Electromagnetic Induction
Copyright © 2010 Pearson Education, Inc. Lecture Outline Chapter 23 Physics, 4 th Edition James S. Walker.
Generators & Motors Textbook Sections 23-6 – Physics.
Copyright © 2007, Pearson Education, Inc., Publishing as Pearson Addison-Wesley. Magnets and the magnetic field Electric currents create magnetic fields.
Phy 213: General Physics III Chapter 30: Induction & Inductance Lecture Notes.
Magnetism July 2, Magnets and Magnetic Fields  Magnets cause space to be modified in their vicinity, forming a “ magnetic field ”.  The magnetic.
Electromagnetic Induction
Physics 24-Winter 2003-L181 Electromagnetic Induction Basic Concepts Faraday’s Law (changing magnetic flux induces emf) Lenz’s Law (direction of induced.
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.
Biot-Savart Law The Field Produced by a Straight Wire.
AP Physics C Montwood High School R. Casao
Physics 121 Practice Problem Solutions 11 Faraday’s Law of Induction
Physics 121: Electricity & Magnetism – Lecture 11 Induction I Dale E. Gary Wenda Cao NJIT Physics Department.
Electromagnetic Induction
CHAPTER 20, SECTION 1 ELECTRICITY FROM MAGNETISM.
Electromagnetic Induction ….the grand finale…. Need to include pictures of Itaipu and Three Gorges Dam!!!!!
Electromagnetic Induction Objective: TSW understand and apply the concept of magnetic flux in order to explain how induced emfs are created and calculate.
AP Physics Chapter 20 Electromagnetic Induction. Chapter 20: Electromagnetic Induction 20.1:Induced Emf’s: Faraday’s Law and Lenz’s Law : Omitted.
Induction and Inductance Chapter 30 Magnetic Flux.
1 Faraday’s Law Chapter Ampere’s law Magnetic field is produced by time variation of electric field.
Induced EMF. EMF EMF - It is potential difference and is measured in volts (V ).
Announcements WebAssign HW Set 7 due this Friday
Electromagnetic Induction
Lecture Outline Chapter 20 College Physics, 7 th Edition Wilson / Buffa / Lou © 2010 Pearson Education, Inc.
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.
Chapter 21 Electromagnetic Induction and Faraday’s Law.
AP Physics B Summer Course 年 AP 物理 B 暑假班 M Sittig Ch 22: Magnetism.
General electric flux definition
Magnetic Induction Chapter Induced currents
Chapter 31 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.
Induced Voltages and Inductance
1 Electromagnetic Induction Chapter Induction A loop of wire is connected to a sensitive ammeter When a magnet is moved toward the loop, the ammeter.
Presentation is prepared by: Guided By: Meet Patel(13BEEEM052) Prof. Krishna Chauhan Jaydev Kubavat(13BEEEG049) Electrical Engg. Dept. Mayur Patel(13BEEEM053)
Chapter 21 Magnetic Induction. Electric and magnetic forces both act only on particles carrying an electric charge Moving electric charges create a magnetic.
Faraday’s Law and Induction
Announcements Clicker quizzes NO LONGER GRADED!
Magnetic Flux and Faraday’s Law of Induction
My Chapter 20 Lecture Outline.
Magnetism and its applications.
Induced Voltages and Inductance
Chapter 20 Electromagnetic Induction. Electricity and magnetism Generators, motors, and transformers.
Chapter 25 Electromagnetic Induction. Objectives 25.1 Explain how a changing magnetic field produces an electric current 25.1 Define electromotive force.
Unit 9: Part 2 Electromagnetic Induction and Waves.
Faraday’s Law of Induction.  = -N  B /  t –  : induced potential (V) – N: # loops –  B : magnetic flux (Webers, Wb) – t: time (s)
Chapter 31 Faraday’s Law. Faraday’s Law of Induction – Statements The emf induced in a circuit is directly proportional to the time rate of change of.
Generators & Motors Textbook Sections 23-6 – Physics.
Chapter 30 Lecture 30: Faraday’s Law and Induction: I.
 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.
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.
Magnetism Unit 12. Magnets Magnet – a material in which the spinning electrons of its atom are aligned with one another Magnet – a material in which the.
Magnets and Electromagnetism Chapter Outline 1.Magnets, magnetic poles, and magnetic force. 2.Magnetic effects of electric current. 3.Magnetic effects.
Magnets and Electromagnetism Chapter Outline 1.Magnets, magnetic poles, and magnetic force. 2.Magnetic effects of electric current. 3.Magnetic effects.
Electromagnetism.  A moving charge creates a magnetic field  Electric current (I) is moving electrons, so a current-carrying wire creates a magnetic.
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 – The production of an emf (the energy per unit charge supplied by a source of electric current) in a conducting circuit by.
Magnetic Induction 1Physics is Life. Objectives To learn how magnetic fields can produce currents in conductors To understand how this effect is applied.
Chapter 29:Electromagnetic Induction and Faraday’s Law
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?
Electromagnetism.
Electromagnetic induction
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?
Chapter 31 Faraday’s Law 31.1 Faraday’s Law of Induction
Chapter 31 Faraday’s Law 31.1 Faraday’s Law of Induction
Presentation transcript:

Electromagnetic Induction and Electromagnetic Waves! Chapter 20

Emf Recall that Emf stands for “electromotive force” which is a voltage (potential difference) capable of creating an electrical current. Emf is measured in Volts!

Magnetic Flux Magnetic flux is the magnetic field that passes through a given area. Magnetic flux is similar to ‘magnetic field density’ – it gives the number of magnetic field lines passing through a given area. Magnetic flux depends on the magnetic field and the area of the wire loop.

Magnetic Flux Flux can be increased by increasing the density of magnetic field lines, or by increasing the area. Φ = BAcos θ [Tm2] = [Weber] = [Wb]

Changing Magnetic Flux Shape of area doesn’t matter. Orientation does matter.

Changing Magnetic Flux Motion of the magnet changes flux Also motion of the wire changes flux

Faraday’s Law / Lenz’s Law A current (voltage) is induced in a wire when magnetic flux is changing! (Faraday) The current induced opposes the change in magnetic flux! (Lenz)

Faraday’s Law for Induced Emf Emf = -N(ΔΦ/Δt) Where N gives the number of turns in a wire loop and Φ = BAcos θ

Example The south end of a bar magnet is pulled far away from a small wire coil. Looking from behind the coil towards the south end of the magnet, what is the direction of induced current? Clockwise or counterclockwise?

Example In rural areas where electric power lines carry electricity to big cities, it is possible to generate small electric currents by means of induction in a conducting loop. The overhead high tension power lines carry currents that periodically reverse direction 60 times per second (60 Hz). How would you orient the plane of a conducting loop to maximize induced current if current in the power lines run north-south.

Example: Electrical instruments can be damaged if they are in a rapidly changing magnetic field. If the induced currents are large enough, they could damage the instrument. Consider a computer speaker that is near an electromagnet. Suppose the electromagnet reverses direction every (1/120) s and exposes the speaker to a magnetic field of 1.0 mT. Assume the speaker coil consists of 100 circular loops of radius 3.00cm with a resistance of 1.00 Ω. Calculate the magnitude of the average induced Emf. Will it damage the speaker?

Homework Read Sections 20.1 and 20.1 Do # 2 – 6, 9, 11- 13, 16- 18, 20, 21, 24, 28

Example An external force does work to move the bar; the work is converted to electrical energy. Since there is a magnetic field present, flux changes. What is the direction of induced current in the resistor? If the bar is 20cm long and pulled at a steady speed of 10 cm/s, what is the induce current if B = 0.25 T and R = 5.0 Ω

Electric Generator A generator is a device that converts mechanical energy to electrical energy. Φ = BAcos θ Emf = -N(ΔΦ/Δt) For uniform circular motion, θ = ωt So Φ = BAcos ωt

Electric Generator Φ = BAcosωt Emf = -N(ΔΦ/Δt) = -N(ΔBAcosωt)/Δt In the generator, B and A are constant Emf = -NBA(Δcosωt/Δt) Emf = (NBAω) sinωt Recall ω = 2πf

Generator If natural processes can create a turning motion, then current can be generated from the turning motion!

Motor A motor is a device that converts electrical energy into mechanical energy. Current sets up a magnetic field in the coil; the magnetic field aligns with the magnet Brushes then reverse the current and the coil rotates to align again. The process continues because every half turn, the brushes switch the current.

Electromagnetic Waves Vibrating electric charges create a varying electric field and a varying magnetic field. This variation in electric and magnetic fields is known as an electromagnetic wave. Consider an electron moving up and down in an antenna…

Electromagnetic Waves Electromagnetic waves are varying electric and magnetic fields. The travel in vacuum at the speed of light, and have a characteristic frequency (and wavelength). The frequency of the wave depends on the frequency of vibration of the oscillating charge. Electromagnetic waves transfer energy and have no mass!

Electromagnetic Spectrum

Homework Read and record example 20.5 on page 665. Read carefully pages 672 – 677. Do # 32, 35, 42, 43, 44, 70 – 73, 78, 79, 82, 84 page 684