Physics 121 Practice Problem Solutions 12 Inductance

Slides:



Advertisements
Similar presentations
AP Physics C Montwood High School R. Casao
Advertisements

Chapter 32 Inductance.
Unit 5 Day 11: RL Circuits Series RL Circuit Layout Current and Voltage Response vs. Time when V 0 is applied Current & Voltage Response vs. Time during.
PHY1013S INDUCTANCE Gregor Leigh
Fisica Generale - Alan Giambattista, Betty McCarty Richardson Copyright © 2008 – The McGraw-Hill Companies s.r.l. 1 Chapter 20: Electromagnetic Induction.
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.
Inductors. Stored energy. LR 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,
Physics 1402: Lecture 21 Today’s Agenda Announcements: –Induction, RL circuits Homework 06: due next MondayHomework 06: due next Monday Induction / AC.
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.
Transient Analysis Transient Analysis.
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.
Department of Electrical & Electronics Engineering ELE 1001: Basic Electrical Technology Lecture 5 Inductor.
Physics 4 Inductance Prepared by Vince Zaccone
© 2012 Pearson Education, Inc. { Chapter 30 Inductance.
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.
Induction and Inductance When a bar magnet moves towards the loop, there is a deflection on the ammeter and when the magnet is moved away, there is also.
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.
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. Joseph Henry 1797 – 1878 American physicist First director of the Smithsonian Improved design of electromagnet Constructed one.
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
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.
Copyright © 2009 Pearson Education, Inc. Chapter 33 Inductance, Electromagnetic Oscillations, and AC Circuits.
Self-Inductance, RL Circuits
Inductance and Magnetic Energy Chapter 32 Mutual Inductance Self-Inductance Inductors in Circuits Magnetic Energy.
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.
Exam review Inductors, EM oscillations
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.
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.
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.
Copyright © 2009 Pearson Education, Inc. Chapter 32: Inductance, Electromagnetic Oscillations, and AC Circuits.
Review 1.
Inductance and AC Circuits. Mutual Inductance Self-Inductance Energy Stored in a Magnetic Field LR Circuits LC Circuits and Electromagnetic Oscillations.
R-L Circuits. R-L Circuits? What does the “L” stand for? Good Question! “L” stands for the self-inductance of an inductor measured in Henrys (H). So…What.
P212c31: 1 Chapter31: Inductance Currents create magnetic fields Changing currents create changing magnetic fields Changing magnetic fields induce EMF’s.
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.
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.
Lecture 10 Induction Applications Chapter 20.6  20.8 Outline Self-Inductance RL Circuits Energy Stored in a Magnetic Field.
Self-Inductance and Circuits Inductors in circuits RL circuits.
Lesson 12 Inductors Transient Analysis
Halliday/Resnick/Walker Fundamentals of Physics
Self Inductance and RL Circuits
Inductance CHAPTER OUTLINE 32.1 Self-Inductance 32.3 Energy in a Magnetic Field Chapter 32.
Copyright © 2009 Pearson Education, Inc. Chapter 30 Inductance, Electromagnetic Oscillations, and AC Circuits.
Inductance of a solenoid
Chapter 30 Inductance, Electromagnetic Oscillations, and AC Circuits
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
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.
11/13/2018.
Topics to be Discussed Steady State and Transient Response.
Self-Inductance and Circuits
Physics 014 Induction.
Chapter 32 Inductance 32-1 Self-Inductance 32-3 Energy of a Magnetic Field.
Chapter 32 Inductance 32-1 Self-Inductance 32-3 Energy of a Magnetic Field.
Chapter 32 Inductance 32-1 Self-Inductance 32-3 Energy of a Magnetic Field.
Chapter 30 Inductance.
Chapter 31B - Transient Currents and Inductance
Presentation transcript:

Physics 121 Practice Problem Solutions 12 Inductance Contents: 121P11 - 40P, 42P, 45P, 46P, 47P, 48P, 49P, 51P, 53P, 54P, 55P Inductors and Inductance Self-Inductance RL Circuits – Current Growth RL Circuits – Current Decay Energy Stored in a Magnetic Field Energy Density of a Magnetic Field Mutual Inductance

PROBLEM 121P11-40P*: At a given instant the current and self-induced emf in an inductor are directed as indicated the figure . (a) Is the current increasing or decreasing? (b) The induced emf is 17 V and the rate of change of the current is 25 kA/s; find the inductance.

PROBLEM 121P11-42P: The current i through a 4 PROBLEM 121P11-42P: The current i through a 4.6 H inductor varies with time t as shown by the graph in the figure. The inductor has a resistance of 12 W. Find the magnitude of the induced emf during the time intervals (a) t = 0 to t = 2 ms, (b) t = 2 ms to t = 5 ms, (c) t = 5 ms to t = 6 ms. (Ignore the behavior at the ends of the intervals.)

PROBLEM 121P11-45P: In terms of tL, how long must we wait for the current in an RL circuit to build up to within 0.100% of its equilibrium value?

PROBLEM 121P11-46P*: The current in an RL circuit builds up to one-third of its steady-state value in 5.00 s. Find the inductive time constant.

PROBLEM 121P11-47P. : The current in an RL circuit drops from 1 PROBLEM 121P11-47P*: The current in an RL circuit drops from 1.0 A to 10 mA in the first second following removal of the battery from the circuit. If L is 10 H, find the resistance R in the circuit.

Problem 121P11-48 Consider the RL circuit of the sketch. In terms of the battery emf , (a) what is the self-induced emf L when the switch has just been closed on a, and (b) what is L when t = 2.0tL? (c) In terms of tL, when will L be just one-half the battery emf ? R

Problem 121P11-49 PROBLEM 121P11-49: A solenoid having an inductance of 6.30 mH is connected in series with a 1.20 kW resistor. (a) If a 14.0 V battery is switched across the pair, how long will it take for the current through the resistor to reach 80.0% of its final value? (b) What is the current through the resistor at time t = 1.0 tL?

PROBLEM 121P11-51: At time t = 0, a 45.0 V potential difference is suddenly applied to a coil with L = 50.0 mH and R = 180 W. At what rate is the current increasing at t = 1.20 ms?

PROBLEM 121P11-53: In the figure, = 100 V, R1 = 10. 0 W, R2 = 20 PROBLEM 121P11-53: In the figure, = 100 V, R1 = 10.0 W, R2 = 20.0 W, R3 = 30.0 W, and L = 2.00 H. Find the values of i1 and i2 (a) immediately after the closing of switch S, (b) a long time later, (c) immediately after the reopening of switch S, and (d) a long time after the reopening.

PROBLEM 121P11-54: In the circuit shown below , = 10 V, R1 = 5 PROBLEM 121P11-54: In the circuit shown below , = 10 V, R1 = 5.0 W, R2 = 10 W, and L = 5.0 H. For the two separate conditions (I) switch S just closed and (II) switch S closed for a long time, calculate (a) the current i1 through R1, (b) the current i2 through R2, (c) the current i through the switch, (d) the potential difference across R2, (e) the potential difference across L, and (f) the rate of change di2/dt.

PROBLEM 121P11-55P: In the circuit shown below, switch S is closed at time t = 0. Thereafter, the constant current source, by varying its emf, maintains a constant current i out of its upper terminal. (a) Derive an expression for the current through the inductor as a function of time. (b) Show that the current through the resistor equals the current through the inductor at time t = (L/R) ln 2.