l22 ch30 ind e inductors

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PHYS.1440 Lecture 22 A.Danylov Department of Physics and Applied Physics Lecture 22 Chapter 30 Induced Electric Field Physics II This fool said some nonsense that the electric field can be produced from the magnetic field. Course website: https://sites.uml.edu/andriy-danylov/teaching/physics-ii/

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Page 1: L22 Ch30 Ind E Inductors

PHYS.1440Lecture22 A.DanylovDepartmentofPhysicsandAppliedPhysics

Lecture 22

Chapter 30

Induced Electric Field

Physics II

This fool said some nonsense that the electric field can be

produced from the magnetic field.

Course website:https://sites.uml.edu/andriy-danylov/teaching/physics-ii/

Page 2: L22 Ch30 Ind E Inductors

PHYS.1440Lecture22 A.DanylovDepartmentofPhysicsandAppliedPhysics

Applications of Faraday’s Law

(some leftovers from the previous class)

Page 3: L22 Ch30 Ind E Inductors

PHYS.1440Lecture22 A.DanylovDepartmentofPhysicsandAppliedPhysics

Applications (Faraday’s Law)

How Electric guitar works?

• Presence of a permanent magnet makes the guitar wire a magnet.

• When the magnetic guitar wire vibrates, it changes the magnetic flux in the coil.

• This flux induces a current in the coil which exactly follow the vibrations of the guitar wire.

• This current is fed to the amplifier and we can hear the sound of vibration of the guitar wire. 

How Microphone works?

• When a sound wave strikes the diaphragm, a coil fixed to the diaphragm vibrates over a stationary bar magnet, changing the flux in the coil and induced an emf in the coil which is then amplified and sent to speakers.

Page 4: L22 Ch30 Ind E Inductors

PHYS.1440Lecture22 A.DanylovDepartmentofPhysicsandAppliedPhysics

Applications (An Alternating-Current Generator)

Page 5: L22 Ch30 Ind E Inductors

PHYS.1440Lecture22 A.DanylovDepartmentofPhysicsandAppliedPhysics

Generators

A generator is a device that transforms mechanical energy into electric energy.

A generator inside a hydroelectric dam uses electromagnetic induction to convert the mechanical energy of a spinning turbine into electric energy.

Hydroelectric Power Plant Working Animation (start at 1 min)

Page 6: L22 Ch30 Ind E Inductors

PHYS.1440Lecture22 A.DanylovDepartmentofPhysicsandAppliedPhysics

Induced Electric Field

Let’s reformulate Faraday’s Law in terms of Φ

Page 7: L22 Ch30 Ind E Inductors

PHYS.1440Lecture22 A.DanylovDepartmentofPhysicsandAppliedPhysics

Induced Electric FieldConsider a conducting loop in an increasing uniform magnetic field.

CCW

So,accordingtoLenz’slaw,thereisaninducedcurrentinthecounterclockwisedirection.Ifthereisacurrent,theremustbesomethingthatactsonthechargecarrierstomakethemmove,(I)soweinferthattheremustbeaninducedelectricfieldtangenttotheloopatallpoints

sdEVVVf

iif

Let’s calculate ∆V or Ɛ (emf) over the closed loop:

dtdsdE m

General form

of Faraday’s law

From Eq.26.3: sdEV

Fromtheotherside,Faraday’slaw:

Combiningthemwecanget

TheconductingloopisnotnecessarytogenerateE.(Theelectricfieldarisewhetherornotcircuitsarepresent).

Thus,(II)thespaceisfilledwithaninducedelectricfield.

Thislawimpliesthatachangingmagneticfluxwillinduceaninducedelectricfield

YoucanusetheloopwasusedasaprobesystemtoconvinceourselvesthattherewastheEfield

Page 8: L22 Ch30 Ind E Inductors

PHYS.1440Lecture22 A.DanylovDepartmentofPhysicsandAppliedPhysics

Two types of the electric field

Coulomb electric field : Induced electric field:Thus, now we know two types of electric field:

1) E is produced by changing B, not by charges

2) Induced el. field lines form closed loops

3) Induced E is nonconservative

1) E is produced by charges2) Coulomb el. field lines start/stop on 

charges

3) Coulomb E is conservative

dtdsdE m

0 sdE

Amazing! A changing magnetic field produces an electric field!!!

BAABm

Let’s look at the special case, when A=const and θ=0. HowcanwefindadirectionoftheinducedE?

‐ Imagine a conducting loop in thespace and use Lenz’s rule to find Iinddirection and that is Eind direction.

Page 9: L22 Ch30 Ind E Inductors

ConcepTest Faraday’s Law

Themagneticfieldisdecreasing.Whichistheinducedelectricfield?

E. There’s no induced field in this case.

Thefieldisthesamedirectionasinducedcurrentwouldflowiftherewerealoopinthefield.CCWImagine a loop CCW

Bind behaveslikeFlorence Nightingale

Page 10: L22 Ch30 Ind E Inductors

PHYS.1440Lecture22 A.DanylovDepartmentofPhysicsandAppliedPhysics

Let’s apply Faraday’s lawIn a solenoid

EB

Eternal dance

Page 11: L22 Ch30 Ind E Inductors

PHYS.1440Lecture22 A.DanylovDepartmentofPhysicsandAppliedPhysics

Induced Electric Field in a Solenoid

The current through the solenoidcreates an upward pointing magneticfield.As the current is increasing, B isincreasing, so it must induce an electricfield.

So, the induced current is clockwise.The induced electric field musttherefore be clockwise around themagnetic field lines.

EB

Eternal dance

HowcanwefindadirectionoftheinducedE?

‐ Imagine a conducting loop in thesolenoid and use Lenz’s rule to find Iinddirection and that is Eind direction.

Page 12: L22 Ch30 Ind E Inductors

PHYS.1440Lecture22 A.DanylovDepartmentofPhysicsandAppliedPhysics

Induced Electric Field in a Solenoid

Page 13: L22 Ch30 Ind E Inductors

PHYS.1440Lecture22 A.DanylovDepartmentofPhysicsandAppliedPhysics

Lecture 23

Chapter 30

Inductors

Physics II

Again, a violent resistance of a system to an attempt

to make some changes

Course website:https://sites.uml.edu/andriy-danylov/teaching/physics-ii/

Page 14: L22 Ch30 Ind E Inductors

PHYS.1440Lecture22 A.DanylovDepartmentofPhysicsandAppliedPhysics

Today we are going to discuss:

Chapter 30:

Section 30.8

Page 15: L22 Ch30 Ind E Inductors

PHYS.1440Lecture22 A.DanylovDepartmentofPhysicsandAppliedPhysics

InductorsInductors (solenoids) store potential energy in

a form of a magnetic field.

Ugh!It’s just energy

Page 16: L22 Ch30 Ind E Inductors

PHYS.1440Lecture22 A.DanylovDepartmentofPhysicsandAppliedPhysics

Inductance (definition)Consider a solenoid of N turns with current I.

The total magnetic flux is I

Φ ~

The coefficient of proportionality is called inductance, L

The SI unit of inductance is the henry, defined as:1 henry = 1 H = 1 Wb/A = 1 T m2/A

The circuit symbol for an ideal inductor is .

The solenoid’s magnetic field passes through the coils, establishing a flux.

Page 17: L22 Ch30 Ind E Inductors

PHYS.1440Lecture22 A.DanylovDepartmentofPhysicsandAppliedPhysics

Let’s find solenoid inductance

Consider a solenoid of N turns with current I.

Recall (your take-home quiz)

Φ

You see, solenoid inductance depends only on its geometry

Φ Φ ∙ ∥

Page 18: L22 Ch30 Ind E Inductors

PHYS.1440Lecture22 A.DanylovDepartmentofPhysicsandAppliedPhysics

Thank you