physics for scientists and engineers ii, summer semester 2009 1 lecture 20: july 10 th 2009 physics...

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Physics for Scientists and Engineers II , Summer Semester 2009 1 Lecture 20: July 10 th 2009 Physics for Scientists and Engineers II

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Physics for Scientists and Engineers II , Summer Semester 2009

1

Lecture 20: July 10th 2009

Physics for Scientists and Engineers II

Physics for Scientists and Engineers II , Summer Semester 2009

2

Transmission line economics

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Physics for Scientists and Engineers II , Summer Semester 2009

3

Transmission line economics – using transformers

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TR

21 NNer transformup-Step

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12 N,Nformer down trans-Step

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Physics for Scientists and Engineers II , Summer Semester 2009

4

Example: Problem 43 in Chapter 33

line?ion transmissin thepower of loss theisWhat

500KV toup dtransforme50.4V

power of5.00MW transmit toNeed

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Physics for Scientists and Engineers II , Summer Semester 2009

5

Example: Problem 43 in Chapter 33

:ansformerWithout tr

ed? transmittbecan much How be.cannot This

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Physics for Scientists and Engineers II , Summer Semester 2009

6

Example: Problem 43 in Chapter 33

.R when load toed transferrispower maximum that thefound we

wherebattery, a of resistance internal with as principle same BTW, d).transmitte

becan power lesseven casesother allIn .R when ONLY is this(and

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Physics for Scientists and Engineers II , Summer Semester 2009

7

The 500000 Volt Tesla Coil – featuring Adam Beehler succesfully trying to not electrocute himself

Physics for Scientists and Engineers II , Summer Semester 2009

8

Chapter 34: Electromagnetic Waves

carriers) chargeby (createdcurrent conduction a isdt

dqI where,B

law? sAmpere'Remember

0 Isd

Capacitor plates

1S1S

I

IPPath

. through passes none through passescurrent conduction a whileHowever,

path. same by the bound are and both but through passesonly I :Problem

21

211

SS

SSS

Physics for Scientists and Engineers II , Summer Semester 2009

9

General Form of Ampere’s Law

flux. electric theis and

space. free ofty permittivi where, I

:currentnt displaceme a defined He fields. electric varying-time

include tolaw sAmpere' dGeneralize :MaxellClark James

situation. for this inadequateclearly is,B

00d

0

AdE

dt

d

Isd

E

E

B

:Law) Maxwell-(Ampere

Law sAmpere' of form General

0000 dt

dIIIsd E

d

Physics for Scientists and Engineers II , Summer Semester 2009

10

Calculating displacement current: Example

2S

1S

I

I

Idt

dqq

dt

d

EAdt

d

dt

dIsd

IIsd

Ed

000

00

000002

001

0B:S Surface

0B:S Surface

Physics for Scientists and Engineers II , Summer Semester 2009

11

Major Point

B

:Law) Maxwell-(Ampere

Law sAmpere' of form General

0000 dt

dIIIsd E

d

Magnetic fields are produced both by conduction currents andby time-varying electric fields.

Physics for Scientists and Engineers II , Summer Semester 2009

12

Example: Chapter 34, Problem 1

AIdt

d

Cs

Nm

NmC

AI

dt

dq

dt

d

dt

d

A

E

E

E

100.01

I (b)

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qEA

qE :Capacitor Plate

plates. ebetween thcurrent nt displaceme theb) and

plates ebetween thflux electric of change of rate time thea) Find 4.00mm. is separation plate

The side.each on cm 5.00 plates square hasthat capacitor a charging iscurrent A -0.100A

000d

210

2

212000

00

Physics for Scientists and Engineers II , Summer Semester 2009

13

A Complete Description of All Classical Electromagnetic Interactions in a Vacuum

law Maxwell-Ampere B

law sFaraday'sdE

magnetismin law sGauss'0AdB

law sGauss'AdE

space freein Equations sMaxwell'

0000

0

dt

dIIIsd

dt

d

q

Ed

B

law force Lorentz BvqEqF

Physics for Scientists and Engineers II , Summer Semester 2009

14

Maxwell’s Prediction

law Maxwell-Ampere B

law sFaraday'sdE

magnetismin law sGauss'0AdB

law sGauss'0AdE

0I and 0q when space freein Equations sMaxwell'

00 dt

dsd

dt

d

E

B

Can be combined Result: Wave equations for electric and magnetic fields

Solution of wave equations shows that electric and magnetic field waves travel(“electromagnetic radiation”) with the speed of light, leading Maxwell to predict that light is a form of electromagnetic radiation.

Physics for Scientists and Engineers II , Summer Semester 2009

15

Hertz’s Experiment

Hertz showed with this apparatus that electro-magnetic waves exist.

Physics for Scientists and Engineers II , Summer Semester 2009

16

Hertz’s Experiment

Details of the apparatus:

How it works: Battery charges the capacitor in the primary circuit on the left. The interrupter periodically creates a short circuit across that capacitor and alternating charging and discharging of capacitor occurs. A large periodic change of flux occurs in the primary winding. The secondary winding picks up this large flux change and transforms the primary voltage fluctuation into a much higher voltage fluctuation in the secondary circuit. The secondary circuit is tuned (LC) creating a very large voltage across the spark balls. High electric fieldsoccur between the spark balls, causing a sudden charge transfer (spark). The electric fieldbreaks down but is then built up again. This fluctuating electric field induces a fluctuatingmagnetic field (Ampere-Maxwell law), which in turn creates a fluctuating electric field (Faraday’s law)….. electromagnetic radiation, which is then picked up by the detection ringcausing it to spark across it’s spark gaps (detection ring is also tuned to the same frequency).

Physics for Scientists and Engineers II , Summer Semester 2009

17

Hertz’s Experiment

Other experiments by Hertz:

em wave generator

metal plate reflectsem wave.

Standingem wave

Nodes can be detected wavelength can be determined

light. visibleof speed thec, vresult was The . using

calculated becan waveem theof speed theknow, isfrequency Since

fv

Physics for Scientists and Engineers II , Summer Semester 2009

18

Plane versus Spherical Waves

Let’s first look at mechanical waves: Imagine looking down on a pond. Someone throws rocks into the middle ofThe pond, creating spherical waves in two dimensions.

Direction of wave propagation

If instead, the person throws very long metal bars into the pond,plane waves are created.

Metalbar

All parts of the wave front have the samephase.

Physics for Scientists and Engineers II , Summer Semester 2009

19

Plane Electromagnetic Waves

Plane linearly polarized electromagnetic waves with propagation in x-direction.

y

zx

Properties:1)Wherever in the yz plane em wave comes from, it propagates in the x-direction. (all “rays” of this wave are parallel).2) All em waves coming from different parts of the yz plane are all in phase.3) Electric and magnetic waves oscillate perpendicular to each other (take this by faith for now).4) Electric field is in the same direction (here in y-direction) “linearly polarized”.5) Magnetic field is in the same direction (here in z-direction) “linearly polarized”.6) And B are only function of x and t and do not depend on y and z E(x,t), B(x,t).

E

B

cc

E

B