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Induction. Fall 2006. Magnetic Flux. For a CLOSED Surface we might expect this to be equal to some constant times the enclosed poles … but there ain’t no such thing!. CLOSED SURFACE. Examples. S N. A puzzlement . Let’s apply this to the gap of a capacitor.

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induction

Induction

Fall 2006

Induction - Fall 2006

magnetic flux
Magnetic Flux

For a CLOSED Surface we might expect this to be equal to some constant times the

enclosed poles … but there ain’t no such thing!

CLOSED SURFACE

Induction - Fall 2006

examples
Examples

S N

Induction - Fall 2006

a puzzlement
A puzzlement ..

Let’s apply this to the gap of a capacitor.

Induction - Fall 2006

consider the poor little capacitor
Consider the poor little capacitor…

i

i

?

CHARGING OR DISCHARGING …. HOW CAN CURRENT

FLOW THROUGH THE GAP

In a FIELD description??

Induction - Fall 2006

through which surface do we measure the current for ampere s law
Through Which Surface Do we measure the current for Ampere’s Law?

I=0

Huh??

Induction - Fall 2006

in the gap displacement current
In the gap… DISPLACEMENT CURRENT

Fixes the Problem!

Induction - Fall 2006

slide8

Let\'s DO the Demo !

Induction - Fall 2006

slide9

OK

Let\'s take a look.

Induction - Fall 2006

from the demo
From The Demo ..

A changing magnetic field INDUCES

a current in a circuit loop.

Induction - Fall 2006

faraday s experiments
Faraday’s Experiments

?

?

Induction - Fall 2006

insert magnet into coil
Insert Magnet into Coil

Induction - Fall 2006

remove coil from field region
Remove Coil from Field Region

Induction - Fall 2006

that s strange
That’s Strange …..

These two coils are perpendicular to each other

Induction - Fall 2006

magnetic flux f b
Magnetic Flux:FB
  • Similar Definition with a special difference!

Faraday\'s Law

Induction - Fall 2006

magnetic flux1
Magnetic Flux
  • Applies to an OPEN SURFACE only.
  • “Quantity” of magnetism that goes through a surface.

surface

Induction - Fall 2006

consider a loop

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Consider a Loop
  • Magnetic field passing through the loop is CHANGING.
  • FLUX is changing.
  • There must be an emf developed around the loop.
    • A current develops (as we saw in demo)
  • Work has to be done to move a charge completely around the loop.

Induction - Fall 2006

faraday s law michael faraday

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Faraday’s Law (Michael Faraday)
  • Again, for a current to flow around the circuit, there must be an emf.
  • (An emf is a voltage)
  • The voltage is found to increase as the rate of change of flux increases.

Induction - Fall 2006

faraday s law michael faraday1

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Faraday’s Law (Michael Faraday)

We will get to the minus sign in a short time.

Induction - Fall 2006

faraday s law the minus sign

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Faraday’s Law (The Minus Sign)

Using the right hand rule, we

would expect the direction

of the current to be in the

direction of the arrow shown.

Induction - Fall 2006

faraday s law more on the minus sign

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Faraday’s Law (More on the Minus Sign)

The minus sign means that the current goes the other way.

This current will produce a magnetic field that would be coming OUT of the page.

The Induced Current therefore creates a magnetic field that OPPOSES the attempt to INCREASE the magnetic field! This is referred to as Lenz’s Law.

Induction - Fall 2006

how much work

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How much work?

emf

Faraday\'s Law

A magnetic field and an electric field are

intimately connected.)

Induction - Fall 2006

the strange world of dr lentz

The Strange World of Dr. Lentz

Induction - Fall 2006

magnetic flux2
MAGNETIC FLUX
  • This is an integral over an OPEN Surface.
  • Magnetic Flux is a Scalar
  • The UNIT of FLUX is the weber
    • 1 weber = 1 T-m2

Induction - Fall 2006

we finally stated
We finally stated

FARADAY’s LAW

Induction - Fall 2006

from the equation
From the equation

Lentz

Lentz

Induction - Fall 2006

flux can change
Flux Can Change
  • If B changes
  • If the AREA of the loop changes
  • Changes cause emf s and currents and consequently there are connections between E and B fields
  • These are expressed in Maxwells Equations

Induction - Fall 2006

three of maxwell s four equations next course just a preview
Three of Maxwell’s Four Equations(Next Course .. Just a Preview!)

Ampere’s Law

Gauss

Faraday

Induction - Fall 2006

slide30
The Flux into the page begins to increase.

An emf is induced around a loop

A current will flow

That current will create a new magnetic field.

THAT new field will change the magnetic flux.

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Another View Of That damned minus sign again …..SUPPOSE that B begins to INCREASE its MAGNITUDE INTO THE PAGE

Induction - Fall 2006

lenz s law

Lenz’s Law

Induced Magnetic Fields always FIGHT to stop what you are trying to do!

i.e... Murphy’s Law for Magnets

Induction - Fall 2006

example of nasty lenz
Example of Nasty Lenz

The induced magnetic field opposes the

field that does the inducing!

Induction - Fall 2006

don t hurt yourself
Don’t Hurt Yourself!

The current i induced in the loop has the direction

such that the current’s magnetic field Bi opposes the

change in the magnetic field B inducing the current.

Induction - Fall 2006

slide35

Let’s do the

Lentz Warp

again !

Induction - Fall 2006

lenz s law1

OR

The toast will always fall buttered side down!

Lenz’s Law

An induced current has a direction

such that the magnetic field due to

the current opposes the change in

the magnetic flux that induces the

current. (The result of the negative sign!) …

Induction - Fall 2006

an example
An Example
  • The field in the diagram
  • creates a flux given by
  • FB=6t2+7tin milliWebers
  • and t is in seconds.
  • What is the emf when
  • t=2 seconds?
  • (b) What is the direction
  • of the current in the
  • resistor R?

Induction - Fall 2006

this is an easy one
This is an easy one …

Direction? B is out of the screen and increasing.

Current will produce a field INTO the paper

(LENZ). Therefore current goes clockwise and R

to left in the resistor.

Induction - Fall 2006

slide39

Figure 31-36 shows two parallel loops of wire having a common axis. The smaller loop (radius r) is above the larger loop (radius R) by a distance x >>R. Consequently, the magnetic field due to the currenti in the larger loop is nearly constant throughout the smaller loop. Suppose that x is increasing at the constant rate of dx/dt = v. (a) Determine the magnetic flux through the area bounded by the smaller loop as a function of x. (Hint: See Eq. 30-29.) In the smaller loop, find (b) the induced emf and (c) the direction of the induced current.

v

Induction - Fall 2006

slide40

q

B is assumed to be constant through the center of the small loop and caused by the large one.

Induction - Fall 2006

the calculation of b z

q

The calculation of Bz

Induction - Fall 2006

more work

dx/dt=v

More Work

In the small loop:

Induction - Fall 2006

what happens here
What Happens Here?
  • Begin to move handle as shown.
  • Flux through the loop decreases.
  • Current is induced which opposed this decrease – current tries to re-establish the B field.

Induction - Fall 2006

moving the bar
moving the bar

Induction - Fall 2006

moving the bar takes work
Moving the Bar takes work

v

Induction - Fall 2006

what about a solid loop
What about a SOLID loop??

Energy is LOST

BRAKING SYSTEM

METAL

Pull

Eddy Currents

Induction - Fall 2006

slide48

Inductors

Back to Circuits for a bit ….

Induction - Fall 2006

definition
Definition

Current in loop produces a magnetic field

in the coil and consequently a magnetic flux.

If we attempt to change the current, an emf

will be induced in the loops which will tend to

oppose the change in current.

This this acts like a “resistor” for changes in current!

Induction - Fall 2006

remember faraday s law
Remember Faraday’s Law

Lentz

Induction - Fall 2006

look at the following circuit
Look at the following circuit:
  • Switch is open
  • NO current flows in the circuit.
  • All is at peace!

Induction - Fall 2006

close the circuit
Close the circuit…
  • After the circuit has been close for a long time, the current settles down.
  • Since the current is constant, the flux through the coil is constant and there is no Emf.
  • Current is simply E/R (Ohm’s Law)

Induction - Fall 2006

close the circuit1
Close the circuit…
  • When switch is first closed, current begins to flow rapidly.
  • The flux through the inductor changes rapidly.
  • An emf is created in the coil that opposes the increase in current.
  • The net potential difference across the resistor is the battery emf opposed by the emf of the coil.

Induction - Fall 2006

close the circuit2
Close the circuit…

Induction - Fall 2006

moving right along
Moving right along …

Induction - Fall 2006

definition of inductance l
Definition of Inductance L

UNIT of Inductance = 1 henry = 1 T- m2/A

FB is the flux near the center of one of the coils

making the inductor

Induction - Fall 2006

consider a solenoid
Consider a Solenoid

l

n turns per unit length

Induction - Fall 2006

slide58
So….

Depends only on geometry just like C and

is independent of current.

Induction - Fall 2006

inductive circuit
Inductive Circuit
  • Switch to “a”.
  • Inductor seems like a short so current rises quickly.
  • Field increases in L and reverse emf is generated.
  • Eventually, i maxes out and back emf ceases.
  • Steady State Current after this.

i

Induction - Fall 2006

the big induction
THE BIG INDUCTION
  • As we begin to increase the current in the coil
  • The current in the first coil produces a magnetic field in the second coil
  • Which tries to create a current which will reduce the field it is experiences
  • And so resists the increase in current.

Lenz with an ATTITUDE!

Induction - Fall 2006

back to the real world

i

Back to the real world…

Switch to “a”

Induction - Fall 2006

solution
Solution

Induction - Fall 2006

switch position b
Switch position “b”

Induction - Fall 2006

slide64

Max Current Rate of

increase = max emf

VR=iR

~current

Induction - Fall 2006

slide65

Solve the loop equation.

Induction - Fall 2006

important question
IMPORTANT QUESTION
  • Switch closes.
  • No emf
  • Current flows for a while
  • It flows through R
  • Energy is conserved (i2R)

WHERE DOES THE ENERGY COME FROM??

Induction - Fall 2006

for an answer return to the big c

E=e0A/d

+dq

+q

-q

For an answerReturn to the Big C
  • We move a charge dq from the (-) plate to the (+) one.
  • The (-) plate becomes more (-)
  • The (+) plate becomes more (+).
  • dW=Fd=dq x E x d

Induction - Fall 2006

the calc
The calc

The energy is in

the FIELD !!!

Induction - Fall 2006

what about power
What about POWER??

power

to

circuit

power

dissipated

by resistor

Must be dWL/dt

Induction - Fall 2006

slide70
So

Energy

stored

in the

Capacitor

Induction - Fall 2006

where is the energy
WHERE is the energy??

l

Induction - Fall 2006

remember the inductor
Remember the Inductor??

?????????????

Induction - Fall 2006

slide73
So …

Induction - Fall 2006

slide74

ENERGY IN THEFIELD TOO!

Induction - Fall 2006

important conclusion
IMPORTANT CONCLUSION
  • A region of space that contains either a magnetic or an electric field contains electromagnetic energy.
  • The energy density of either is proportional to the square of the field strength.

Induction - Fall 2006

slide76

END OF TOPIC

Induction - Fall 2006

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