Exam review Inductors, EM oscillations

Slides:



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

Chapter 30.
Chapter 31B - Transient Currents and Inductance
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,
Ch 32 Inductance 32.1 Self Inductance L = N B /I  L = -L(dI/dt) Units: Tm 2 /A = Henry Solenoid P32.4 (p.916) P32.3 (p.916)
Electromagnetic Induction
Let us examine this LC circuit mathematically. To do this let us examine the energy of the system. Conservation of Energy 2 nd order differential equation.
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.
RL Circuits PH 203 Professor Lee Carkner Lecture 21.
PHYS 270 – SUPPL. #8 DENNIS PAPADOPOULOS FEBRUARY 19,
Self-inductance and inductors(sec. 30.2) Magnetic field energy(sec. 30.3) RL circuit(sec. 30.4) LC circuit (sec. 30.5) RLC series circuit (sec. 30.6) Inductance.
Ch. 32 Self Inductance Inductance A
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.
Lectures (Ch. 30) Inductance and Self-inductunce
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.
1 W12D2 RC, LR, and Undriven RLC Circuits; Experiment 4 Today’s Reading Course Notes: Sections , 11.10, ; Expt. 4: Undriven RLC Circuits.
Fall 2008Physics 231Lecture 10-1 Chapter 30 Inductance.
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.
RL and LC Circuits Capacitor and Inductors in Series Resistors and Inductors in Series.
1 Chapter 16 Capacitors and Inductors in Circuits.
30. Inductance Self & Mutual Inductance Inductance: unit : H (henry)
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. 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.
Inductance and Magnetic Energy Chapter 32 Mutual Inductance Self-Inductance Inductors in Circuits Magnetic Energy.
Physics 121 Practice Problem Solutions 12 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.
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.
Chapter 32 Inductance. Self-inductance Some terminology first: Use emf and current when they are caused by batteries or other sources Use induced emf.
Self Inductance Consider a solenoid with n turns/m, length l, current i, and cross sectional area A. l A There is a magnetic field inside the solenoid,
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.
Lab 7: RLC Resonant Circuits Only 5 more labs to go!! C L When we connect a charged capacitor to an inductor oscillations will occur in the charge of the.
Copyright © 2009 Pearson Education, Inc. Admin: Assignment 8 is complete Assignment 9 is posted 2 more AC analysis problems RC circuits Due Monday (May.
Unit 5: Day 9 – Energy Stored in a Magnetic Field of an Inductor Power delivered by an inductor Work done to increase the current in an inductor The energy.
P212c31: 1 Chapter31: Inductance Currents create magnetic fields Changing currents create changing magnetic fields Changing magnetic fields induce EMF’s.
9. Inductance M is a geometrical factor! L is a geometrical factor!
Self Inductance Consider a solenoid L, connect it to a battery Area A, length  l, N turns What happens as you close the switch? Lenz’s law – loop resists.
Copyright © 2012 Pearson Education Inc. PowerPoint ® Lectures for University Physics, Thirteenth Edition – Hugh D. Young and Roger A. Freedman Lectures.
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
Chapter 36 Inductance Capacitance Electric energy Magnetic energy Inductance.
Wednesday, Apr. 19, 2006PHYS , Spring 2006 Dr. Jaehoon Yu 1 PHYS 1444 – Section 501 Lecture #21 Wednesday, Apr. 19, 2006 Dr. Jaehoon Yu Energy.
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.
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.
Copyright © 2009 Pearson Education, Inc. Chapter 30 Inductance, Electromagnetic Oscillations, and AC Circuits.
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.
Inductance and Capacitance Response of First Order RL and RC
Coils sharing the same magnetic flux, BA
The figure shows an {image} circuit with a switch and a 440-volt battery. What is the current in the circuit and the potential difference between points.
Moving conductor – eddy currents
AC circuits Physics /27/2018 Lecture IX.
Physics 014 Induction.
Induction and Inductance III
9. Inductance M is a geometrical factor! L is a geometrical factor!
Induction and Inductance III
Chapter 30 Inductance.
Chapter 31B - Transient Currents and Inductance
Ch. 31 Self Inductance Inductance A
Presentation transcript:

Exam review Inductors, EM oscillations Physics 2102 Gabriela González Physics 2102 Exam review Inductors, EM oscillations

Exam review Q1: 75.7 P1: 61.6 Q2: 67.2 Q3: 79.2 P2: 58.2 P3:52.2

Inductors Inductance definition: L=NFB/I Solenoid inductance: L=m0n2Al Induced emf (voltage) across an inductor is E=-L di/dt In an RL circuit, we can “charge” the inductor with a battery until there is a constant current, or “discharge” the inductor through the resistor. Time constant is L/R. An inductor stores magnetic potential energy: UB=Li2/2 Energy density stored in a magnetic field is uB=B2/2m0

EM oscillations An LC combination produces an electrical oscillator, the natural frequency of oscillator is w=1/LC Total energy in circuit is conserved: switches between energy stored in capacitor (electric energy) and in inductor (magnetic energy). If a resistor is included in the circuit, the total energy decays (is dissipated by R). i(t)