Lecture 10 Induction Applications Chapter 20.6  20.8 Outline Self-Inductance RL Circuits Energy Stored in a Magnetic Field.

Slides:



Advertisements
Similar presentations
Inductance Self-Inductance RL Circuits Energy in a Magnetic Field
Advertisements

Inductors and Inductance A capacitor can be used to produce a desired electric field. Similarly, an inductor (symbol ) can be used to produce a desired.
RL Circuits Physics 102 Professor Lee Carkner Lecture 22.
Electromagnetic Induction
Self Inductance. Solenoid Flux  Coils of wire carrying current generate a magnetic field. Strong field inside solenoidStrong field inside solenoid 
Induced EMF and Inductance 1830s Michael Faraday Joseph Henry.
Dr. Jie ZouPHY Chapter 32 Inductance. Dr. Jie ZouPHY Outline Self-inductance (32.1) Mutual induction (32.4) RL circuits (32.2) Energy in a.
RL Circuits PH 203 Professor Lee Carkner Lecture 21.
Physics 121: Electricity & Magnetism – Lecture 11 Carsten Denker NJIT Physics Department Center for Solar–Terrestrial Research.
G L Pollack and D R Stump Electromagnetism Electromagnetic Induction Faraday’s law If a magnetic field changes in time there is an induced electric.
Ch. 30 Inductance AP Physics. Mutual Inductance According to Faraday’s law, an emf is induced in a stationary circuit whenever the magnetic flux varies.
Physics 2102 Inductors, RL circuits, LC circuits Physics 2102 Gabriela González.
Physics 2102 Lecture 19 Ch 30: Inductors and RL Circuits Physics 2102 Jonathan Dowling Nikolai Tesla.
-Self Inductance -Inductance of a Solenoid -RL Circuit -Energy Stored in an Inductor AP Physics C Mrs. Coyle.
Self-Inductance When the switch is closed, the current does not immediately reach its maximum value Faraday’s law can be used to describe the effect.
Unit 5: Day 8 – Mutual & Self Inductance
AP Physics C Montwood High School R. Casao
INDUCTANCE. When the current in a loop if wire changes with time, an emf is induced in the loop according to Faraday’s law. The self- induced emf is Ɛ.
Chapter 32 Inductance.
Chapter 32 Inductance. Joseph Henry 1797 – 1878 American physicist First director of the Smithsonian Improved design of electromagnet Constructed one.
Chapter 30 Inductance. Self Inductance When a time dependent current passes through a coil, a changing magnetic flux is produced inside the coil and this.
1 Faraday’s Law Chapter Ampere’s law Magnetic field is produced by time variation of electric field.
Inductance and AC Circuits. Mutual Inductance Self-Inductance Energy Stored in a Magnetic Field LR Circuits LC Circuits and Electromagnetic Oscillations.
© 2005 Pearson Prentice Hall This work is protected by United States copyright laws and is provided solely for the use of instructors in teaching their.
Chapter 32 Inductance. Self-inductance  A time-varying current in a circuit produces an induced emf opposing the emf that initially set up the time-varying.
Chapter 32 Inductance. Introduction In this chapter we will look at applications of induced currents, including: – Self Inductance of a circuit – Inductors.
Copyright © 2009 Pearson Education, Inc. Chapter 33 Inductance, Electromagnetic Oscillations, and AC Circuits.
Chapter 10 Inductance. 2 Objectives –After completing this chapter, the student should be able to: Explain the principles of inductance. Identify the.
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.
15/25/2016 General Physics (PHY 2140) Lecture 18  Electricity and Magnetism Induced voltages and induction Generators and motors Self-induction Chapter.
Inductance and Magnetic Energy Chapter 32 Mutual Inductance Self-Inductance Inductors in Circuits Magnetic Energy.
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 32 Inductance.
Physics 121 Practice Problem Solutions 12 Inductance
Chapter 20 Induced Voltages and Inductance. General Physics Inductors & RL Circuits Sections 5–8.
Lecture 18-1 Ways to Change Magnetic Flux Changing the magnitude of the field within a conducting loop (or coil). Changing the area of the loop (or coil)
Copyright © 2012 Pearson Education Inc. PowerPoint ® Lectures for University Physics, Thirteenth Edition – Hugh D. Young and Roger A. Freedman Lectures.
Chapter 22: Electromagnetic Induction Essential Concepts and Summary.
Chapter 32 Inductance L and the stored magnetic energy RL and LC circuits RLC circuit.
Exam review Inductors, EM oscillations
AP Physics C III.E – Electromagnetism. Motional EMF. Consider a conducting wire moving through a magnetic field.
Lecture 27: FRI 20 MAR Inductors & Inductance Ch.30.7–9 Inductors & Inductance Physics 2102 Jonathan Dowling Nikolai Tesla.
Chapter 30 Inductance. Inductor and Inductance Capacitor: store electric energy Inductor: store magnetic energy Measure how effective it is at trapping.
Induced Voltage and Inductance
When the switch is closed, the current does not immediately reach its maximum value Faraday’s law can be used to describe the effect As the source current.
Self Inductance. A variable power supply is connected to a loop. The current in the loop creates a magnetic field. What happens when the power supply.
Chapter 32 Inductance. Joseph Henry 1797 – 1878 American physicist First director of the Smithsonian Improved design of electromagnet Constructed one.
Chapter 32 Inductance. Self-inductance Some terminology first: Use emf and current when they are caused by batteries or other sources Use induced emf.
Slide 1Fig 32-CO, p Slide 2  As the source current increases with time, the magnetic flux through the circuit loop due to this current also increases.
INDUCTANCE. When the current in a loop if wire changes with time, an emf is induced in the loop according to Faraday’s law. The self- induced emf is Ɛ.
Copyright © 2009 Pearson Education, Inc. Chapter 32: Inductance, Electromagnetic Oscillations, and AC Circuits.
21 Electromagnetic Induction. Induction Experimental.
My Chapter 20 Lecture Outline.
Electro- magnetic Induction Lecture 3 AP Physics.
9. Inductance M is a geometrical factor! L is a geometrical factor!
Chapter 28 Inductance; Magnetic Energy Storage. Self inductance 2 Magnetic flux Φ B ∝ current I Electric currentmagnetic fieldEMF (changing) Phenomenon.
CHAPTER 32 : INDUCTANCE Source = source emf and source current Induced = emfs and currents caused by a changing magnetic field. S R I I 1st example Consider.
23.5 Self-Induction When the switch is closed, the current does not immediately reach its maximum value Faraday’s Law can be used to describe the effect.
Chapter 30 Lecture 31: Faraday’s Law and Induction: II HW 10 (problems): 29.15, 29.36, 29.48, 29.54, 30.14, 30.34, 30.42, Due Friday, Dec. 4.
Copyright © 2012 Pearson Education Inc. PowerPoint ® Lectures for University Physics, Thirteenth Edition – Hugh D. Young and Roger A. Freedman Lectures.
Self Inductance and RL Circuits
Inductance CHAPTER OUTLINE 32.1 Self-Inductance 32.3 Energy in a Magnetic Field Chapter 32.
Chapter 6 Inductance. 23/15/2016 N S S v change Review example Determine the direction of current in the loop for bar magnet moving down. Initial flux.
1 28 magnetic induction. 2 3 induced currents due to magnetic force qv x B.
AP Physics C III.E – Electromagnetism. Motional EMF. Consider a conducting wire moving through a magnetic field.
Chapter 30: Induction and Inductance This chapter covers the following topics: -Faraday’s law of induction -Lenz’s Law -Electric field induced by a changing.
Physics 014 Induction.
Chapter 32 Inductance 32-1 Self-Inductance 32-3 Energy of a Magnetic Field.
Chapter 31B - Transient Currents and Inductance
Chapter 32 Inductance 32-1 Self-Inductance
Presentation transcript:

Lecture 10 Induction Applications Chapter 20.6  20.8 Outline Self-Inductance RL Circuits Energy Stored in a Magnetic Field

Self-Inductance Faraday’s law prevents the current in a circuit to reach the maximum value immediately. The magnetic flux through the loop increases together with the current. As a result, an induced emf appears and opposes the change in magnetic flux. The opposing emf results in a gradual increase of the current. The effect is called self-inductance. I R B

Magnitude of Self-Inductance The self-induced emf is proportional to the time rate of change of the current.  I ℇ =  L   t L is called inductance ℇ =  N  B /  t The SI unit of inductance is henry 1 H = 1 V s / A N  B /  t = L  I /  t  L = N  B /  I = N  B /I

RL Circuits Solenoids or closely wrapped coils have a large inductance and are called inductors.inductors For a circuits with a resistor ℇ  IR = 0 and  V=  IR. Resistance is a measure of opposition to the current. Inductance is a measure of opposition to the rate of change in current ( ℇ =  L  I /  t). For a circuit with both a resistor and an inductor, the current is unable to reach its maximum value instantaneously. We can define a time constant for such a circuit as  = L/R.circuit

Problem with an RL Circuit Problem: A circuit has a 10-V battery, a 5-  resistor, and a 20-mH inductor. Find the circuit time constant and the current after 1 time constant.  = L/R =  2 H / 5  = 0.04 s I = ℇ/ R (1  e  Rt/L ) t =   1  e  1 = I = ℇ /R = V / 5  = 1.26 A

Energy Stored in a Magnetic Field The battery has to do work to produce a current. This work is energy stored by the inductor in its magnetic field. The energy stored by an inductor is similar to that of a capacitor. L I 2 PE L =  2 C  V 2 PE C =  2

Summary Self-inductance is a phenomenon of opposing to a change in current in electric circuits due to appearance of the magnetic field. Inductor is an element with a large inductance. Energy stored by an inductor is similar to that stored by a capacitor.