W13D3 More Patterns

39
W13D3 More Patterns Fields, Patterns, Maxwell’s Equations and Begin Induction/Faraday’s Law 2049 SCALE-UP EASY!

description

Easy!. W13D3 More Patterns. Fields, Patterns, Maxwell’s Equations and Begin Induction/Faraday’s Law 2049 SCALE-UP. Calender. THE EVAN SHOW. Field Patterns From Last Time. “Curly Field” No diverging source. Diverging Field Point Sources. - PowerPoint PPT Presentation

Transcript of W13D3 More Patterns

Page 1: W13D3  More Patterns

W13D3 More PatternsFields, Patterns, Maxwell’s Equations and Begin Induction/Faraday’s Law2049SCALE-UP

EASY!

Page 2: W13D3  More Patterns

CalenderMonday Wednesday Friday Saturday

14

Chapter 22Gauss

16 (Read rest of chapter)2 WebAssignsChapter 22Gauss

18QUIZ

Chapter 22Lentz & More

21

Chapter 23Faraday

23QUIZ

Chapter 23Faraday

HOLIDAY

28

Chapter 23Faraday

30

Chapter 24EM

2Chapter 24 EMOptional Exam

(22-24)

3

FINAL EXAM

Page 3: W13D3  More Patterns

THE EVAN SHOW

Page 4: W13D3  More Patterns

Field Patterns From Last Time

“Curly Field”No diverging source

Diverging FieldPoint Sources

Electrostatic Fields Magnetic Fields

Page 5: W13D3  More Patterns

Maxwell’s Equations

0

0 .

0

? =Faraday's Law of Induction - Next Topic

(One additional term)

inside

inside path

qdA

dA

d

d I

E n

B •n

E l

B l

Page 6: W13D3  More Patterns

A puzzlement ..

enclosedid 0 sB

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

Page 7: W13D3  More Patterns

Consider the poor little capacitor…

i i

CHARGING OR DISCHARGING …. HOW CAN CURRENTFLOW THROUGH THE GAP

In a FIELD description??

Page 8: W13D3  More Patterns

Through Which Surface Do we measure the current for Ampere’s Law?

I=0

Page 9: W13D3  More Patterns

In the gap… DISPLACEMENT CURRENT

dtd

dtdqI

ntDisplaceme

Idtdq

Letdtdq

dtd

qEA

Ed

d

E

E

0

0

0

2

Current

gap)(in

1

S through FLUX ELECTRIC The

Page 10: W13D3  More Patterns

0

0 . 0

0

? =Faraday's Law of Induction - Next Topic

( + )

inside

Einside path

qdA

dA

d

dd I

dt

E n

B •n

E l

B l

Page 11: W13D3  More Patterns

NEXT

Fix the Last Maxwell Equation

? =Faraday's Law of Induction - d E l

Page 12: W13D3  More Patterns
Page 13: W13D3  More Patterns

The Coil and the Magnet

Coil

Galvanometer

Page 14: W13D3  More Patterns

Magnetic Flux M

Integral over a SURFACE

Page 15: W13D3  More Patterns

What’s Happening Here??

A

Page 16: W13D3  More Patterns

Observation

Meter Deflects

There must be an emf around the loops!

VariablesDirectionPolarityPitchVelocity

Page 17: W13D3  More Patterns

Down the Hatch

Aluminum Pipe

Page 18: W13D3  More Patterns

Down the Hatch

B

Aluminum Pipe

N

S

Induced Current

NREPEL!!

There must bean Electric Fieldin the metal thatis pushing the current!!

Page 19: W13D3  More Patterns

You said that there is a conducting loop.You said that there is therefore a current induced around the loop if the flux through the loop changes.But the beginning and end point of the loop are the same so how can there be a voltage difference around the loop?Or a current???‘tis a puzzlement!

HEY BINDELL – WAIT A SECOND …….

Page 20: W13D3  More Patterns
Page 21: W13D3  More Patterns

REMEMBER when I said E Fields start and end on CHARGES???

DID I LIE??

Page 22: W13D3  More Patterns

Electric fields that are created by static charges must start on a (+) charge and end on a (–) charge as I said previously.Electric Fields created by changing magnetic fields (NON-Coulombic) can actually be shaped in loops.

The truth

BUT WAIT, YOU STILL LIE!

Page 23: W13D3  More Patterns

Why do you STILL think I am a liar?

Because you said that an emf is a voltage so if I put a voltmeter from one point on the loop around to the same point, I will get ZERO

volts, won’t I? How can there be a current??

Page 24: W13D3  More Patterns

Yes … butthis doesn’t make

me a liar!Let Me Explain.

Page 25: W13D3  More Patterns

Is the WORK that an external agent has to do to move a unit charge from one point to another.But we also have (neglecting the sign):

The POTENTIAL between two points

sEV

s

Page 26: W13D3  More Patterns

So, consider the following:

E

Conductor

x x x x x x xx x x x x x xx x x x x x xx x x x x x xx x x x x x xx x x x x x x

zeroREemf

sEsEemf

2

Page 27: W13D3  More Patterns

THEREFORE WHAT WILL A VOLTMETER READ FROM A to A?

E

Conductor

x x x x x x xx x x x x x xx x x x x x xx x x x x x xx x x x x x xx x x x x x x

A

A The emfB ZeroC Can’t tell

Page 28: W13D3  More Patterns

How Big is the emf?

temf loopthe

Through

Faraday’s Law

Michael Faraday (1791-1867)

MINUS????

Page 29: W13D3  More Patterns

Q: Which way does E point?A: The way that you don’t want it to point! (Lenz’s Law).

Lenz’s Law Explains the (-) sign!

Page 30: W13D3  More Patterns

Push a magnet into a coil of two wires and a current is produced via an emf.

In this case, 2 coils, each have the SAME emf so we add..Ohm’s Law still works, so

coilRemfi

tNemf

Page 31: W13D3  More Patterns

Faraday’s Experiments

??

Page 32: W13D3  More Patterns

Insert Magnet into Coil

Page 33: W13D3  More Patterns

Remove Coil from Field Region

Page 34: W13D3  More Patterns

That’s Strange …..

These two coils are perpendicular to each other

Page 35: W13D3  More Patterns

All Involve Changing The Magnetic

Flux through the Loops

Page 36: W13D3  More Patterns

Remember the Definition of TOTAL ELECTRIC FLUX through a CLOSED surface:

dA

is surface aLEAVING FieldElectric theofFlux Total

outE

surface EE d

nE

Page 37: W13D3  More Patterns

Magnetic FluxApplies to an OPEN SURFACE only.“Quantity” of magnetism that goes through a

surface.

AB dBsurface

Page 38: W13D3  More Patterns

In the figure below a 120-turn coil of radius 1.8 cm and resistance 6.8 W is coaxial with a solenoid with 209 turns/cm and diameter 3.2 cm. The solenoid current drops from 1.5 A to zero in time interval Δt = 25 ms. What current is induced in the coil during Δt?

0.0224 A

Page 39: W13D3  More Patterns

DONE