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,

Slides:



Advertisements
Similar presentations
Oscillations in an LC Circuit
Advertisements

Chapter 32 Inductance.
Inductance Self-Inductance RL Circuits Energy in a Magnetic Field
Dale E. Gary Wenda Cao NJIT Physics Department
Chapter 30.
AP Electricity Quiz Review
Which of the two cases shown has the smaller equivalent resistance between points a and b? Q Case #1 2. Case #2 3. the equivalent resistance is.
Inductors1 ELECTROMAGNETIC INDUCTION All conductors that carry a current produce a magnetic field As the magnet is moved in and out of a coil of wire in.
Capacitors and/or TV (not Emf). 1. An empty capacitor does not resist the flow of current, and thus acts like a wire. 2. A capacitor that is full of charge.
2. the intensity of light bulb A increases.
O Aim of the lecture  Inductors Behaviour in circuits Energy storage  Comparison with Capacitors V vs i Energy  Use in Circuits LR time constant sparks.
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)
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.
3/12/03 Minute Paper How does the capacitor behave if it is already charged when you turn a switch to connect it to a load? You take a long time with minute.
RL Circuits PH 203 Professor Lee Carkner Lecture 21.
Delay is very useful for other circuit No Sudden Change in voltage, i.e. voltage has to change continuously! Large RC inputoutput Rectifying circuit: convert.
PHY 232 Spring 2002 Prof. S. Billinge Class 10. PHY 232 Spring 2002 Prof. S. Billinge Announcements.
Announcements Assignment 1 due now. Assignment 2 posted, due on Thursday.
Physics 4 Inductance Prepared by Vince Zaccone
Shantanu Dutt ECE Dept. UIC
Complete the activity on charging and discharging capacitors located under Activities on the website sites.google.com/site/sienaphys140spring2011/activities/char.
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,
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.
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)
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.
Fundamentals of Electric Circuits Chapter 7
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)
Self-Inductance and Circuits LC circuits. 0 1τ 2τ 3τ 4τ 63% ε /R I t Recall: RC circuit, increasing current.
Exam review Inductors, EM oscillations
Chapter 30 Inductance. Inductor and Inductance Capacitor: store electric energy Inductor: store magnetic energy Measure how effective it is at trapping.
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.
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)
Direct Current Circuits A current is maintained in a closed circuit by an emf (electromotive force) Battery. An emf forces electrons to move against the.
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.
Lesson 10 Calculation of Inductance LR circuits
Phys102 Lecture 10 & 11 DC Circuits Key Points EMF and Terminal Voltage Resistors in Series and in Parallel Circuits Containing Resistor and Capacitor.
RC 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.
Response of First Order RL and RC
Halliday/Resnick/Walker Fundamentals of Physics 8th edition
Physics 6B Inductors and AC circuits Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB.
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
Inductance and Capacitance Response of First Order RL and RC
Ing shap e Wav 1.
Concept Questions with Answers 8.02 W12D2
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.
Topics to be Discussed Steady State and Transient Response.
AC circuits Physics /27/2018 Lecture IX.
University Physics Chapter 14 INDUCTANCE.
Shantanu Dutt ECE Dept. UIC
Chapter 31B - Transient Currents and Inductance
LC Circuits.
Presentation transcript:

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, so V L =0 In a dc circuit, inductor behaves like a short circuit

Inductor & Capacitor in DC Circuit If there is a sudden change in current or Voltage occurs in a circuit such as close or open a switch, then InductorCapacitor Current (i L ) must be continuous, i.e. i + =i - Voltage (V c ) must be continous, i.e. V + =V - At t>>  Short circuit Open circuit Magnetic field energy stored in an inductor: Power supplied by battery Dissipated power Work stored

Concept Check A battery is connected to a solenoid. When the switch is opened, the light bulb 1.Remain off 2.Goes off 3.Slowly dims out 4.Keeps burning as brightly as it did before the switch was opened. 5.Flares up brightly, then dims and goes out Answer 5

LC Circuit a)Charged C connected L V max =q max /C, i = 0, di/dt: max U E =q max 2 /2C, max U B =Li 2 /2=0 b) U=U B +U E c) i max, q=0, U B max

LC oscillation V max =q max /C, i=0 U E =q max 2 /2C, max U B =Li 2 /2=0 Speed of charging depends on L, C U E =q 2 /2C, U B =Li 2 /2 q=0, i max U E =q 2 /2C=0 U B =Li max 2 /2, max V max =q max /C, i=0 U E =q max 2 /2C, max U B =Li 2 /2=0 The charge starts to flow back the other way, resulting opposite current

LC oscillation

The oscillations continuous indefinitely in the absence of loss (R=0) The V c (or charges) is out of phase with i, i.e. V c max. at i=0, vice versa. LC circuit  Oscillating block-spring systems q Displacement: x i=dq/dtv=dx/dt L m C 1/k U B =Li 2 /2U k =mv 2 /2 U E =q 2 /2CU=kx 2 /2

LC oscillation Circuit

Concept Check Which Circuit takes the least time to fully discharge the capacitors during the oscillation (a) Answer: (b) has smaller C eq, thus smaller T, fast discharge (b)

Example: RC circuit 33-19P, In an oscillating LC circuit, L=3.0 mH and C=2.60  F. At t=0 the charge on the capacitor is zero and the current is 2.00 A. (a) what is the maximum charge that will appear on the capacitor? (b) In terms of the period T of the oscillation, how much time will elapse after t=0 until the energy stored in the capacitor will be increasing at its greatest rate? c) What is this greatest rate at which energy is transferred to the capacitor?

Damped and Forced Oscillations Damped OscillationForced Oscillation