Self-Inductance and Circuits LC circuits. 0 1τ 2τ 3τ 4τ 63% ε /R I t Recall: RC circuit, increasing current.

Slides:



Advertisements
Similar presentations
Oscillations in an LC Circuit
Advertisements

A) LC circuits and Oscillation Frequency
Chapter 32 Inductance.
Inductance Self-Inductance RL Circuits Energy in a Magnetic Field
-Mutual Inductance -LC Circuit
1 Chapter 24--Examples. 2 Problem In the figure to the left, a potential difference of 20 V is applied across points a and b. a) What is charge on each.
Self-Inductance and Circuits
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,
LC Oscillators PH 203 Professor Lee Carkner Lecture 22.
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.
Alternating Current Circuits
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 Circuit t=0, i=0  R/L Switch to position a Switch to position b Initially, i change is max, thus largest V L. After t>>  all voltage is on R, di/dt=0,
Physics 2113 Jonathan Dowling
Physics 4 Inductance Prepared by Vince Zaccone
© 2012 Pearson Education, Inc. { Chapter 30 Inductance.
Ch. 31: Electrical Oscillations, LC Circuits, Alternating Current
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 for Scientists and Engineers, 6e Chapter – 32 Inductance.
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.
-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.
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.
Chapter 22 Alternating-Current Circuits and Machines.
Chapter 32 Inductance.
ARRDEKTA INSTITUTE OF TECHNOLOGY GUIDED BY GUIDED BY Prof. R.H.Chaudhary Prof. R.H.Chaudhary Asst.prof in electrical Asst.prof in electrical Department.
RC, RLC circuit and Magnetic field RC Charge relaxation RLC Oscillation Helmholtz coils.
RL and LC Circuits Capacitor and Inductors in Series Resistors and Inductors in Series.
Copyright © 2009 Pearson Education, Inc. Chapter 30 Inductance, Electromagnetic Oscillations, and AC Circuits.
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.
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 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.
Wednesday, Nov. 16, 2005PHYS , Fall 2005 Dr. Jaehoon Yu 1 PHYS 1444 – Section 003 Lecture #20 Wednesday, Nov. 16, 2005 Dr. Jaehoon Yu Self Inductance.
Copyright © 2009 Pearson Education, Inc. Chapter 33 Inductance, Electromagnetic Oscillations, and AC Circuits.
Chapter 32 Inductance.
Class 34 Today we will: learn about inductors and inductance
Chapter 32 Inductance L and the stored magnetic energy RL and LC circuits RLC circuit.
Exam review Inductors, EM oscillations
The Ups and Downs of Circuits The End is Near! Quiz – Nov 18 th – Material since last quiz. (Induction) Exam #3 – Nov 23 rd – WEDNESDAY LAST CLASS –
LC CURCUIT LC CURCUIT PRESENTED TO PRESENTED TO SIR TARIQ SIR TARIQ PRESENTED BY PRESENTED BY JAMEELA JAMEELA ROLL NO ROLL NO
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.
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)
Review 1.
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.
Physics 212 Lecture 19, Slide 1 Physics 212 Lecture 19 LC and RLC Circuits.
Lecture 41: WED 02 DEC Final Exam Review I Physics 2113 Jonathan Dowling.
Lesson 10 Calculation of Inductance LR circuits
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.
EM OSCILLATION & AC. LC oscillation.
AQA Physics Gravitational Fields, Electric Fields and Capacitance Section 9 Charging and Discharging a Capacitor.
Copyright © 2009 Pearson Education, Inc. Chapter 30 Inductance, Electromagnetic Oscillations, and AC Circuits.
Physics 6B Inductors and AC circuits Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB.
Copyright © 2009 Pearson Education, Inc. Chapter 29 Electromagnetic Induction and Faraday’s Law.
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.
Concept Questions with Answers 8.02 W15D2
Concept Questions with Answers 8.02 W12D2
Physics 2113 Jonathan Dowling
Ch. 31.1–4: Electrical Oscillations, LC Circuits, Alternating Current
University Physics Chapter 14 INDUCTANCE.
LC Circuits.
Presentation transcript:

Self-Inductance and Circuits LC circuits

0 1τ 2τ 3τ 4τ 63% ε /R I t Recall: RC circuit, increasing current

I t 0τ τ 2τ 3τ 4τ 0.37 I 0 IoIo Recall: RC circuit, decreasing current

Question: What happens if we put a capacitor in the circuit, along with R, or L, or both?

LC circuits The switch is closed at t =0; Find I (t). C L I + - A capacitor is connected to an inductor in an LC circuit Assume the capacitor is initially charged and then the switch is closed Assume no resistance and no energy losses to radiation

Oscillations in an LC Circuit, 1 The capacitor is fully charged –The energy U in the circuit is stored in the electric field of the capacitor –The energy is equal to Q 2 max /2C –The current in the circuit is zero –No energy is stored in the inductor The switch is closed

Oscillations in an LC Circuit, 2 The current is equal to the rate at which the charge changes on the capacitor (dQ/dt) –As the capacitor discharges, the energy stored in the electric field decreases –Since there is now a current, some energy is stored in the magnetic field of the inductor –Energy is transferred from the electric field to the magnetic field

Oscillations in an LC Circuit, 3 The capacitor becomes fully discharged –It stores no energy –All of the energy is now stored in the magnetic field of the inductor –This energy is equal to ½ LI 2 –The current reaches its maximum value The current now decreases in magnitude, recharging the capacitor with its plates having opposite their initial polarity

Oscillations in an LC Circuit, 4 Eventually the capacitor becomes fully charged and the cycle repeats The energy continues to oscillate between the inductor and the capacitor The total energy stored in the LC circuit remains constant in time and equals:

LC Circuit Analogy to Spring-Mass System The kinetic energy (½ mv 2 ) of the spring is analogous to the magnetic energy (½ L I 2 ) stored in the inductor The potential energy ½kx 2 stored in the spring is analogous to the electric potential energy ½CV max 2 stored in the capacitor At any point in the cycle, energy is shared between the electric and magnetic fields

LC circuits The switch is closed at t =0; Find I (t). C L I Which can be written as (remember, P=VI): + - Looking at the energy loss in each component of the circuit gives us: E L +E C =0

Solution

Charge and Current in an LC Circuit The charge on the capacitor oscillates between Q max and –Q max The current in the inductor oscillates between I max and –I max Q and I are 90 o out of phase with each other –So when Q is a maximum, I is zero, etc.

Energy in an LC Circuit – Graphs The energy continually oscillates between the energy stored in the electric and magnetic fields When the total energy is stored in one field, the energy stored in the other field is zero

Example 1: A 1.00-μF capacitor is charged by a 40.0-V power supply. The fully charged capacitor is then discharged through a 10.0-mH inductor. Find the maximum current in the resulting oscillations.

Example 2: An LC circuit consists of a 3.30-H inductor and an 840-pF capacitor, initially carrying a 105-μC charge. The switch is open for t < 0 and then closed at t = 0. Compute the following quantities at t = 2.00 ms: a) the energy stored in the capacitor b) the energy stored in the inductor c) the total energy in the circuit.

Solution

Example 3: The switch in the figure below is connected to point a for a long time. After the switch is thrown to point b, what are a) the frequency of oscillation of the LC circuit, b) the maximum charge that appears on the capacitor, c) the maximum current in the inductor d) the total energy the circuit possesses at t = 3.00 s?

Solution

Notes About Real LC Circuits In actual circuits, there is always some resistance Therefore, there is some energy transformed to internal energy The total energy in the circuit continuously decreases as a result of these processes