Chapter 30 Inductance. Inductor and Inductance Capacitor: store electric energy Inductor: store magnetic energy Measure how effective it is at trapping.

Slides:



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

-Mutual Inductance -LC Circuit
The current through the inductor can be considered a sum of the current in the circuit and the induced current. The current in the circuit will be constant,
Mutual Inductance(sec. 30.1) Self-inductance and inductors(sec. 30.2) Magnetic field energy(sec. 30.3) RL circuit(sec. 30.4) LC circuit (sec. 30.5) RLC.
Physics 1402: Lecture 21 Today’s Agenda Announcements: –Induction, RL circuits Homework 06: due next MondayHomework 06: due next Monday Induction / AC.
Physics 1502: Lecture 22 Today’s Agenda Announcements: –RL - RV - RLC circuits Homework 06: due next Wednesday …Homework 06: due next Wednesday … Induction.
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.
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.
Physics 4 Inductance Prepared by Vince Zaccone
Physics for Scientists and Engineers II, Summer Semester Lecture 17: July 1 st 2009 Physics for Scientists and Engineers II.
Ch. 32 Self Inductance Inductance A
Fall 2008 Physics 121 Practice Problem Solutions 13 Electromagnetic Oscillations AC Circuits Contents: 121P13 - 2P, 3P, 9P, 33P, 34P, 36P, 49P, 51P, 60P,
Physics 2102 Inductors, RL circuits, LC circuits Physics 2102 Gabriela González.
Lectures (Ch. 30) Inductance and Self-inductunce
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.
Electromagnetic Induction
Fall 2008Physics 231Lecture 10-1 Chapter 30 Inductance.
Inductance Self-Inductance A
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.
RL and LC Circuits Capacitor and Inductors in Series Resistors and Inductors in Series.
Chapter 32 Inductance. Joseph Henry 1797 – 1878 American physicist First director of the Smithsonian Improved design of electromagnet Constructed one.
1 Chapter 16 Capacitors and Inductors in Circuits.
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.
30. Inductance Self & Mutual Inductance Inductance: unit : H (henry)
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.
Chapter 24 Inductance and
© 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 32 Inductance.
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 32 Inductance L and the stored magnetic energy RL and LC circuits RLC circuit.
Exam review Inductors, EM oscillations
1 Electromagnetic Induction We introduced motional emf and Faraday’s Law through these two examples: Today we will the discussion about Faraday’s Law of.
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.
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.
L C LC Circuits 0 0 t V V C L t t U B U E Today... Oscillating voltage and current Transformers Qualitative descriptions: LC circuits (ideal inductor)
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 30 Inductance, Electromagnetic Oscillations, and AC Circuits.
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.
Lecture 10 Induction Applications Chapter 20.6  20.8 Outline Self-Inductance RL Circuits Energy Stored in a Magnetic Field.
Lesson 10 Calculation of Inductance LR circuits
Physics 1202: Lecture 15 Today’s Agenda Announcements: –Lectures posted on: –HW assignments, solutions.
Chapter 36 Inductance Capacitance Electric energy Magnetic energy Inductance.
Thursday August 2, PHYS 1444 Ian Howley PHYS 1444 Lecture #15 Thursday August 2, 2012 Ian Howley Dr. B will assign final (?) HW today(?) It is due.
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.
EM OSCILLATION & AC. LC oscillation.
Lecture 19-1 RL Circuits – Starting Current 2. Loop Rule: 3. Solve this differential equation τ=L/R is the inductive time constant 1.Switch to e at t=0.
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.
Copyright © 2009 Pearson Education, Inc. Chapter 30 Inductance, Electromagnetic Oscillations, and AC Circuits.
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.
Copyright © 2009 Pearson Education, Inc. Chapter 29 Electromagnetic Induction and Faraday’s Law.
For vacuum and material with constant susceptibility M 21 is a constant and given by Inductance We know already: changing magnetic flux creates an emf.
Inductance of a solenoid
Mutual Inductance Mutual inductance: a changing current in one coil will induce a current in a second coil: And vice versa; note that the constant M, known.
Induction and Inductance
Coils sharing the same magnetic flux, BA
Moving conductor – eddy currents
AC circuits Physics /27/2018 Lecture IX.
University Physics Chapter 14 INDUCTANCE.
Chapter 30 Inductance.
Chapter 30 Induction and Inductance
Presentation transcript:

Chapter 30 Inductance

Inductor and Inductance Capacitor: store electric energy Inductor: store magnetic energy Measure how effective it is at trapping magnetic energy

Inductance of a solenoid l

Self-Induction Always resists the change in current

The sign of ξ L If ξ L is positive, then the induced emf points in the same direction as the current. If ξ L is negative, then the induced emf points in the opposite direction as the current.

RL Circuits (“charging”)

Example

“Discharging”

Energy in an inductor

Magnetic and Electric energy density

Mutual Inductance Coil 2 with respect to 1:

Coil 1 with respect to 2:

Example Note that this equation is only true for a flat coil, not true for solenoid (which you will derive in the homework)

Reminder: Magnetic and Electric energy

Electromagnetic Oscillations

Energy conservation

Going around the loop

Simple Harmonic Oscillator This is the same equation as all other simple harmonic oscillators

Solution

MasteringPhysics In HW 30, the question “Oscillations in an LC circuit” Part C, use instead: Reason: They wanted you to look at the magnitude of the current only, and without the minus sign I would have been negative.

Energy

Energy conservation

Damped Oscillations Energy is dissipated by the resistor Going around the loop:

Solution (damped)

(Natural) Frequency, Period, etc…