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Electromagnetism & Optics and wave phenomena. Physics 1220/1320. Lecture Magnetism, chapter 27-32. Electromagnetic Induction. Field strength, Shape, Location, Orientation If any of these change, I is induced. Faraday’s Law. F B =int[ B •d A ] For uniform B: F B = B • A. - PowerPoint PPT Presentation
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Physics 1220/1320 Electromagnetism & Optics and wave phenomena Lecture Magnetism, chapter 27-32
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Page 1: Physics 1220/1320

Physics 1220/1320

Electromagnetism&

Optics and wave phenomena

Lecture Magnetism, chapter 27-32

Page 2: Physics 1220/1320

Electromagnetic Induction

Field strength,Shape,Location,Orientation

- If any of these change, I is induced

Page 3: Physics 1220/1320
Page 4: Physics 1220/1320

Faraday’s Law

FB=int[B•dA]

For uniform B:FB= B•A

Page 5: Physics 1220/1320

Direction of Induced EMFNote: only CHANGE in flux causes the emf, not the presence of flux

http://www.uwsp.edu/physastr/kmenning/flash/AF_3101.swf

Page 6: Physics 1220/1320

A second way to determine direction:Lenz’s Law

Page 7: Physics 1220/1320

MutualInductance

Units: henry[H] = [Wb/A] = [Vs/A] = [J/A2]

Page 8: Physics 1220/1320

SelfInductance

Page 9: Physics 1220/1320

For M = 240 mH and N2 =5 turns, what needs N1 to be if L = 1cmand A= 1cm2?

Page 10: Physics 1220/1320

Magnetic Field Energy

Page 11: Physics 1220/1320

Energy stored in an inductor:

What L is needed to store 1 kWh energyin coil with 1A, 1kA, 1mA?

L = 2U/I2

Page 12: Physics 1220/1320

What is the effect of L on a circuit?a- The R-L Circuit

i = E/R (1-e-(R/L)t)

i = I0 e-(R/L)t

During discharge:

Loop rule: E – iR – L di/dt = 0

Page 13: Physics 1220/1320

The L-C Circuit

Page 14: Physics 1220/1320

We find that instead of the exponential behavior of the RLcircuit, in the LC circuit i oscillates!

Loop rule: -L di/dt – q/C = 0 or d2q/dt2 + 1/LC q = 0

‘harmonic oscillator’q = Q cos(wt+f)i = dq/dt = - wQ sin(wt+f)

From further analogybetween mechanic oscillatorslike springs, we find:

Page 15: Physics 1220/1320

Ex 30.35 C 60mF charged by connecting 12V battery.Then C disconnected from battery and hooked up to L=1.5H

a) w and T of oscillations?

b) Initial charge on C?

c) How much energy initially in C?

d) Charge on C after 23 ms?

Signs on plates are opposite to those at t=0e) i in L at that time?

Page 16: Physics 1220/1320

Finally, the LRC series circuit:

Page 17: Physics 1220/1320

Ex 30.41 L=0.285H, C= 0.46 mF, w’= (6LC)-0.5

What is R?

Group Task

LCLCLR

LCLCLR

LCL

R

LC 6

112

6

114

6

1

4

1 222

22

. 4.45F)10(4.60H)6(0.285

1

F)10(4.60H)(0.285

1)H285.0(2

44

R

Page 18: Physics 1220/1320

Alternating Currents (AC)v = V cos wt

i2 = I2 cos2 wtNote: cos2wt = ½ (1+ cos2wt) i2 = I2 ½ (1+cos2wt)The average of cos(anything) is zero<i2>avg = I2/2 and <i>= irms = I/20.5

Page 19: Physics 1220/1320

Ex PC: 2.7A from 120V 60Hz

a) Average current – zero

b) Average of square of current is not zero:

c) Current amplitude I

Page 20: Physics 1220/1320

Resistance, Reactance

vR = VR cos wt = iR = (IR) cos wt

Page 21: Physics 1220/1320

In other words: that little trick createsan ohm-like equation

with ‘inductive reactance’ XL = wL

Page 22: Physics 1220/1320

Similarly, with ‘capacitive reactance’ XC = 1/wC

Page 23: Physics 1220/1320
Page 24: Physics 1220/1320

The LRC Series Circuit

2 cases: XL > XC or XC > XL

‘Same ohm-trick’ “Impedance”

Page 25: Physics 1220/1320

i in phase with VR

Page 26: Physics 1220/1320
Page 27: Physics 1220/1320

Power in Ac Circuits:

Page 28: Physics 1220/1320

Resonance in AC Circuits

Page 29: Physics 1220/1320
Page 30: Physics 1220/1320

So far, we have avoided a complication in ourunderstanding of circuitry:

It turns out that Ampere’s lawis ____________

:

Page 31: Physics 1220/1320

The hindsight approach for electromagnetism is to start with theMaxwell Equations: (here in their less useful integral form)

Page 32: Physics 1220/1320

http://scienceworld.wolfram.com/physics/MaxwellEquations.html

In their more useful differential form, they become:

divergence,        curl,

Page 33: Physics 1220/1320

In sum, it turns out that all radiation propagates in form of electromagneticwaves, where E and B are just two aspects of the same thing: A movingelectric charge which creates a dipole moment.

Page 34: Physics 1220/1320

A general description of such a propagating wave is:

For waves in (through) matter , we get correction factors:

The energy and momentum of these waves can be described by acharacteristic vector:

Page 35: Physics 1220/1320

A whole set of phenomena we are familiar withboil down to being em-waves:

Page 36: Physics 1220/1320

In modern physics, much attention is paid to the factthat this view (‘classical physics’) of the world breaksdown in the realm of the very small and the very large.

Classical Physics is not abandoned altogether, it’s fieldof relevance is simply found to be limited. It exists as a limiting case of GR and QP as a macroscopic approximation of the true behaviors. In its realm, CP gives remarkably precise information.

Page 37: Physics 1220/1320

Quantum Physics

recognizes that the distinction between matterand energy is artificial

for light, a famous paradox occurs, the wave-particleduality, ie it can be shown that light must be bothat the same time (so called ‘two-slit’ experiment)

General Relativity

recognizes that there is an absolute maximum speed,the speed of lightand that space itself is curved bythe presence of heavy objects (so the Euclidian statement that a straight line is the

shortest distance between two points is ultimately not true (albeit very close to reality for distances not very much larger than lightyears).

Much of the effort in Modern Physics is devoted to find newexotic phenomena in materials which exploit QP (most recently:nano science and modern optics (quantum computation, dataencryption, teleportation). A great unknown is the ‘how to’ of unifying the two great theories of physics, QP and GR.


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