Thur. Nov. 5, 2009Physics 208, Lecture 191 From last time… Faraday: Motional EMF Moving conductor generates electric potential difference to cancel motional.

Slides:



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

PHY1013S INDUCTANCE Gregor Leigh
CHAPTER 32 inductance 32.1 Self-Inductance 32.3 Energy in a Magnetic Field.
Chapter Review.
Physics 1304: Lecture 13, Pg 1 Faraday’s Law and Lenz’s Law ~ B(t) i.
© 2007 Pearson Prentice Hall This work is protected by United States copyright laws and is provided solely for the use of instructors in teaching their.
Copyright © 2010 Pearson Education, Inc. Lecture Outline Chapter 23 Physics, 4 th Edition James S. Walker.
Walker, Chapter 23 Magnetic Flux and Faraday’s Law of Induction
Electromagnetic Induction
Copyright © 2009 Pearson Education, Inc. Lecture 9 – Electromagnetic Induction.
Physics 121: Electricity & Magnetism – Lecture 11 Carsten Denker NJIT Physics Department Center for Solar–Terrestrial Research.
Magnetism Lenz’s Law 1 Examples Using Lenz’s Law.
Electromagnetism Physics 100 Chapt 15 Michael Faraday.
RL Circuits Physics 102 Professor Lee Carkner Lecture 21.
Physics 24-Winter 2003-L181 Electromagnetic Induction Basic Concepts Faraday’s Law (changing magnetic flux induces emf) Lenz’s Law (direction of induced.
RL Circuits Physics 102 Professor Lee Carkner Lecture 22.
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.
Electromagnetic Induction
Chapter 29:Electromagnetic Induction and Faraday’s Law
AP Physics C Montwood High School R. Casao
Induction and Inductance Chapter 30 Magnetic Flux.
Magnetic Flux and Faraday’s Law of Induction. Questions 1.What is the name of the disturbance caused by electricity moving through matter? 2.How does.
Electromagnetic Induction
Self-Inductance, RL Circuits
Physics 2112 Unit 18 Today’s Concepts: A) Induction B) RL Circuits Electricity & Magnetism Lecture 18, Slide 1.
Inductance and Magnetic Energy Chapter 32 Mutual Inductance Self-Inductance Inductors in Circuits Magnetic Energy.
Induction: Faraday’s Law
Physics 2102 Lecture 18 Ch30: Inductors & Inductance II Physics 2102 Jonathan Dowling Nikolai Tesla.
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)
Chapter 20 Self-Inductance LR Circuits Motional EMF.
Chapter 32 Inductance L and the stored magnetic energy RL and LC circuits RLC circuit.
AP Physics C III.E – Electromagnetism. Motional EMF. Consider a conducting wire moving through a magnetic field.
Motional EMF This is the emf induced in a conductor moving through a magnetic field. Examples on sheet 10 To change the magnetic flux we can change: 1.the.
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.
Lecture 27: FRI 20 MAR Inductors & Inductance Ch.30.7–9 Inductors & Inductance Physics 2102 Jonathan Dowling Nikolai Tesla.
Induced Voltage and 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 As the source current.
MAGNETIC INDUCTION MAGNETUIC FLUX: FARADAY’S LAW, INDUCED EMF:
Lecture 19: THU 25 MAR 2010 Ch30. Ch30.5–9 Induction and Inductance II Induction and Inductance II Physics 2102 Jonathan Dowling.
Magnetic Flux and Faraday’s Law of Induction
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.
My Chapter 20 Lecture Outline.
Faraday’s Law and Inductance. Faraday’s Law A moving magnet can exert a force on a stationary charge. Faraday’s Law of Induction Induced emf is directly.
Electro- magnetic Induction Lecture 3 AP Physics.
Induction - Faraday’s Law Sections Physics 1161: Lecture 12 Changing Magnetic Fields create Electric Fields.
Lecture 10 Induction Applications Chapter 20.6  20.8 Outline Self-Inductance RL Circuits Energy Stored in a Magnetic Field.
Inductors ? circuit diagram symbol.
Self Inductance and RL Circuits
1 28 magnetic induction. 2 3 induced currents due to magnetic force qv x B.
AP Physics C III.E – Electromagnetism. Motional EMF. Consider a conducting wire moving through a magnetic field.
Lecture 30: WED 05 NOV Induction and Inductance II Physics 2113 Jonathan Dowling Fender Stratocaster Solenoid Pickup.
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.
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.
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.
From last time… Faraday: Lenz: induced currents oppose change in flux
Eddy Current A current induced in a solid conducting object, due to motion of the object in an external magnetic field. The presence of eddy current in.
From last time… Faraday: Inductance: flux = (inductance) x (current)
11/13/2018.
Last lecture Motional EMF
Faraday’s Law Discovered in 1830s by Michael Faraday and Joseph Henry. Faraday was a poor boy and worked as a lab assistant and eventually took over the.
I2 is decreasing in magnitude I2 is constant
Induction and Inductance III
Chapter 32 Inductance 32-1 Self-Inductance 32-3 Energy of a Magnetic Field.
Induction and Inductance III
Chapter 32 Inductance 32-1 Self-Inductance 32-3 Energy of a Magnetic Field.
Induction and Inductance III
Chapter 32 Inductance 32-1 Self-Inductance 32-3 Energy of a Magnetic Field.
Presentation transcript:

Thur. Nov. 5, 2009Physics 208, Lecture 191 From last time… Faraday: Motional EMF Moving conductor generates electric potential difference to cancel motional EMF Changing flux generates EMF

Motional EMF Charges in metal feel magnetic force Tue. Nov. 2, 2009Physics 208, Lecture 182 Charges move, build up at ends of metal Equilibrium: electric force cancels magnetic force

Tue. Nov. 2, 2009Physics 208, Lecture 183 Question Two identical bars are moving through a vertical magnetic field. Bar (a) is moving vertically and bar (b) is moving horizontally. Which of following statements is true? A. motional emf exists for (a), but not (b) B. motional emf exists for (b), but not (a) C. motional emf exists for both (a) and (b) D. motional emf exists for neither (a) nor (b)

B(t) Coil in magnetic field Uniform B-field increasing in time Flux in z-direction increasing in time Thur. Nov. 5, 2009Physics 208, Lecture 194 Lenz’ law: Induced EMF would produce current to oppose change in flux Induced current

B(t) But no equilibrium current Charges cannot flow out end Build up at ends, makes Coulomb electric field Cancels Faraday electric field End result No current flowing Electric potential difference from one end to other Opposes Faraday EMF ΔV = - EMF Thur. Nov. 5, 2009Physics 208, Lecture 195 Increasing with time Compare motional EMF

Thur. Nov. 5, 2009Physics 208, Lecture 196 Coil can generate it’s own flux Uniform field inside solenoid Change current -> change flux N turns Wire turns Surface for flux

Thur. Nov. 5, 2009Physics 208, Lecture 197 ‘Self’-flux in a solenoid Flux through one turn  =Flux through entire solenoid N=# of turns, =length of solenoid inductance

Thur. Nov. 5, 2009Physics 208, Lecture 198 Inductance: a general result Flux = (Inductance) X (Current) Change in Flux = (Inductance) X (Change in Current)

Thur. Nov. 5, 2009Physics 208, Lecture 199 Question The current through a solenoid is doubled. The inductance of the solenoid A.Doubles B.Halves C.Stays the same Inductance is a geometrical property, like capacitance

Thur. Nov. 5, 2009Physics 208, Lecture 1910 Question A solenoid is stretched to twice its length while keeping the same current and same cross-sectional area. The inductance A.Increases B.Decreases C.Stays the same Field, hence flux, have decreased for same current

Fixed current through ideal inductor For fixed resistor value Current through inductor I = V batt /R Flux through inductor = LI Constant current -> Flux through inductor doesn’t change No induced EMF Voltage across inductor = 0 Thur. Nov. 5, 2009Physics 208, Lecture 1911 V batt R L I Ideal inductor: coil has zero resistance

V batt R L I VbVb VaVa Try to change current You increase R in time: Current through inductor starts to decrease Flux LI through inductor starts to decrease Faraday electric fields in inductor wires Induces current to oppose flux decrease Drive charges to ends of inductor Charges produce Coulomb electric field Electric potential diff Thur. Nov. 5, 2009Physics 208, Lecture 1912 time R(t)R(t)

Thur. Nov. 5, 2009Physics 208, Lecture 1913 Question The potential at a is higher than at b. Which of the following could be true? A) I is from a to b, steady B) I is from a to b, increasing C) I is from a to b, decreasing D) I is from b to a, increasing E) I is from b to a, decreasing e,.g. current from a to b: current increases, flux to right increases. sign of induced emf such that it would induce current to produce flux to left to oppose change in flux. Electric potential difference opposite to induced EMF, so V a >V B

Thur. Nov. 5, 2009Physics 208, Lecture 1914 Energy stored in ideal inductor Constant current (uniform charge motion) No work required to move charge through inductor Increasing current: Work required to move charge across induced EMF Energy is stored in inductor: Total stored energy Energy stored in inductor

Thur. Nov. 5, 2009Physics 208, Lecture 1915 Magnetic energy density Energy stored in inductor Solenoid inductance Energy stored in solenoid B solenoid Energy density

Thur. Nov. 5, 2009Physics 208, Lecture 1916 Question A solenoid is stretched to twice its length while keeping the same current and same cross-sectional area. The stored energy A.Increases B.Decreases C.Stays the same B decreases by 2 Energy density decr by 4 Volume increases by 2

Thur. Nov. 5, 2009Physics 208, Lecture 1917 Inductor circuit Induced EMF extremely high Breaks down air gap at switch Air gap acts as resistor

Question Here is a snapshot of an inductor circuit at a particular time. What is the behavior of the current? Thur. Nov. 5, 2009Physics 208, Lecture 1918 I VbVb VaVa A.Increasing B.Decreasing C.Nonzero Constant D.Must be zero E.Need more info

Thur. Nov. 5, 2009Physics 208, Lecture 1919 Perfect inductors in circuits Constant current flowing All Voltage drops = 0 I I? Voltage needed to drive current thru resistor -IR +  V L = 0 + -

Thur. Nov. 5, 2009Physics 208, Lecture 1920 RL circuits Current decreases in time Slow for large inductance (inductor fights hard, tries to keep constant current) Slow for small resistance (little inductor voltage needed to drive current) I? + - Time constant

Thur. Nov. 5, 2009Physics 208, Lecture 1921 RL circuits I(t) + - Time constant