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There will be one last homework assigned today. It will not be due until the day of the final, Dec...

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There will be one last homework assigned today. It will not be due until the day of the final, Dec 13. I will also put some practice problems on line today. There will be a problem solving session tomorrow, Nov 30. I will not be here next week. The last lecture will be given by another professor. However, you may email with questions. The final is Dec 13 at 2 PM. Remember that it will be 40% comprehensive and 60% on material covered since the last exam. You will be allowed two 8 ½ X 11 sheets of paper for notes (both sides) and it is open book. I will have a review session the day before the final. Look at your schedule and think about when you would like to have it. I am available all day.
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Page 1: There will be one last homework assigned today. It will not be due until the day of the final, Dec 13. I will also put some practice problems on line today.

There will be one last homework assigned today. It will not be due until the day of the final, Dec 13.

I will also put some practice problems on line today.

There will be a problem solving session tomorrow, Nov 30.

I will not be here next week. The last lecture will be given by another professor. However, you may email with questions.

The final is Dec 13 at 2 PM. Remember that it will be 40% comprehensive and 60% on material covered since the last exam. You will be allowed two 8 ½ X 11 sheets of paper for notes (both sides) and it is open book.

I will have a review session the day before the final. Look at your schedule and think about when you would like to have it. I am available all day. We will discuss this on Thursday.

Page 2: There will be one last homework assigned today. It will not be due until the day of the final, Dec 13. I will also put some practice problems on line today.

Motional emf – conductor moving in a constant magnetic field

FB = qvB will move charges

until compensated by the electric

field of end accumulations

qvB = qE = qV / l

V = Bvl

B Blx

dxBl Blv

dt

Page 3: There will be one last homework assigned today. It will not be due until the day of the final, Dec 13. I will also put some practice problems on line today.

2 2resistor

/

( ) /

I Blv R

P I R Blv R

Generators as Energy Converters

2

Who does the work?

We! - By moving the bar:

( ) /

Energy conserved

appliedP Fv IBlv Blv R Generator does not produce electric energyout of nowhere – it is supplied by whatever entity that keeps the rod moving. All it does is to convert it to a different form, namely toelectric energy (current)

Page 4: There will be one last homework assigned today. It will not be due until the day of the final, Dec 13. I will also put some practice problems on line today.

20

:emf Total

:element Small

)(

:bar Rotating

2lBdrr

lB

drBvd

rrv

2

0

2

)/(

)/exp(

)(

:force magnetic

by the ddecelerate

relax illvelocity w

push, initialAfter

BlmR

tvv

vR

BlIBl

dt

dvm

Motion does not necessarily

mean changing magnetic flux!

Page 5: There will be one last homework assigned today. It will not be due until the day of the final, Dec 13. I will also put some practice problems on line today.

Significance of the minus sign – Lenz’s Law

Induced current has such direction that its own flux opposes the change of the external

magnetic flux

Magnetic field of the induced current wants to decrease the total flux

Magnetic field of the induced current wants to increase the total flux

Correspondingly, magnetic forces oppose the motion – consistently with conservation of

energy!

Lenz’s Law – the direction of any magnetic induction effect as to oppose the cause of the effect

Lenz’s Law – a direct consequence of the energy conservation principle

Page 6: There will be one last homework assigned today. It will not be due until the day of the final, Dec 13. I will also put some practice problems on line today.

Finding the direction of the induced current

Page 7: There will be one last homework assigned today. It will not be due until the day of the final, Dec 13. I will also put some practice problems on line today.

Induced Electric Fields

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BE

BBv

BvF

F

BvEF

d

t

q

q

B

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Page 8: There will be one last homework assigned today. It will not be due until the day of the final, Dec 13. I will also put some practice problems on line today.

Electric field around a solenoid with alternating current

Current : I(t) = Imax cos(ωt)

Magnetic field inside the solenoid :

B(t) = μ0nI(t) (outside B = 0)

Flux through the surface bounded by the path :

ΦB (t) = B(t) ⋅πR2

Electric field circulation around the path :

E ⋅ds = E ⋅2πr = −dΦB

dt∫ = μ0nImaxπR

2ω sin(ωt)

Outside : E(r, t) =μ0nImaxR

2rsin(ωt)

Inside (R → r) : E(r, t) =μ0nImaxrω

2sin(ωt)

Page 9: There will be one last homework assigned today. It will not be due until the day of the final, Dec 13. I will also put some practice problems on line today.

NO! - field? thishave circuit to real a need weDo

ativenonconserv and )(dependent - timeisit now

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changingby generated field electric The

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tdA

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E

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nB

nB

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Page 10: There will be one last homework assigned today. It will not be due until the day of the final, Dec 13. I will also put some practice problems on line today.

We cannot change magnitude of the velocity of a charged particle

in a static magnetic field B

BUT

We can do it in a time-varying magnetic field B(t) – the resulting

electric field E(t) will do the job

And that’s indeed how particles are accelerated in betatrons!

Page 11: There will be one last homework assigned today. It will not be due until the day of the final, Dec 13. I will also put some practice problems on line today.

Magnetospheric and Ionospheric Current SystemsMagnetospheric and Ionospheric Current Systems

Several current systems exist in the magnetosphere: magnetopause current, neutral sheet current, ring current, etc…

These currents close partially within the magnetosphere and partially through ionospheric currents via field-aligned currents or Birkeland currents

-magnetic field lines act like current carrying wires

During geomagnetic storms, can be very intense

- cause ground induced currents

Page 12: There will be one last homework assigned today. It will not be due until the day of the final, Dec 13. I will also put some practice problems on line today.

Geomagnetically Induced Currents (GICs)Geomagnetically Induced Currents (GICs)Ionospheric currents

• flow at ~100 km• experience large spatiotemporal variations reflected in variations of the Earth's geomagnetic field• as consequence of Faraday's law of induction, an electric field at the surface of the Earth is induced• surface electric field causes electrical currents, known as geomagnetically induced currents (GIC), to flow in any conducting structure, for example, a power or pipeline grid grounded in the Earth

Conducting networks include electrical power transmission grids, oil and gas pipelines, undersea communication cables, telephone and telegraph networks and railways.

Can cause problems, such as increased corrosion of pipeline steel and damaged high-voltage power transformers

Page 13: There will be one last homework assigned today. It will not be due until the day of the final, Dec 13. I will also put some practice problems on line today.

Known since the mid-1800s:• electrical telegraph systems could sometimes run without power during geomagnetic storms, described at the time as operating on the "celestial battery”• other times completely inoperative.

The Great Storm of 1859• great Auroras of August 28 and September 4 lit up the skies of nearly every major city on the planet.

Communication between two telegraph operators:

- Boston operator (to Portland operator): "Please cut off your battery [power source] entirely for fifteen minutes."- Portland operator: "Will do so. It is now disconnected."- Boston: "Mine is disconnected, and we are working with the auroral current. How do you receive my writing?"- Portland: "Better than with our batteries on. - Current comes and goes gradually."

Historical EventsHistorical Events

Page 14: There will be one last homework assigned today. It will not be due until the day of the final, Dec 13. I will also put some practice problems on line today.

Historical EventsHistorical EventsMarch 24, 1940

• First reported effects on power systems, with voltage dips, large swings in reactive power, and tripping of transformer banks, reported from power companies in the US and Canada • Effects also observed on the telephone and telegraph systems in US

March13, 1989• severe geomagnetic storm • aurora seen as far south as Florida and Cuba• caused the collapse of the Hydro-Québec power grid in a matter of seconds as equipment protection relays tripped in a cascading sequence of events.• six million people left without power for nine hours• eventual cost – $2 billion

Gas pipelines• currents cause the normal corrosion of pipelines to be accelerated• modern pipelines protected from long-term current flows by a weak counter current of a few amperes - applied so that the pipeline has a net, negative potential relative to ground.

- auroral currents change polarity in minutes, rendering this 'cathodic protection' useless

Page 15: There will be one last homework assigned today. It will not be due until the day of the final, Dec 13. I will also put some practice problems on line today.

Eddy Currents

When magnetic field is on, currents (eddy currents) are induced in conductors so that the pendulum slows down or stops

Page 16: There will be one last homework assigned today. It will not be due until the day of the final, Dec 13. I will also put some practice problems on line today.
Page 17: There will be one last homework assigned today. It will not be due until the day of the final, Dec 13. I will also put some practice problems on line today.

Displacement Current

0 enclB dl I 0

0 0( ) EA

q C Ed EAd

0E

cddq

idt dt

0 displacement currentEd

di

dt

Page 18: There will be one last homework assigned today. It will not be due until the day of the final, Dec 13. I will also put some practice problems on line today.

tcc

Ej

Bj

B0

2

0

2

1

20

0 c

“displacement current” of the electric field

flux as opposed to conduction

current

!fields! magnetic gcirculatin torise give

toofields electric changingbut currentsonly Not

:tiongeneraliza sMaxwell'

esconsequenc reaching-farwith

result ain gculminatin theory ofy consistenc theof

analysis oreticalpurely the a of examplegreat a is

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000

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sB

Page 19: There will be one last homework assigned today. It will not be due until the day of the final, Dec 13. I will also put some practice problems on line today.

The Reality of Displacement Current

D ci i

2

0 2

02

0

2

inside the capacitor2

outside capacitor2

D

c

c

rB dl rB i

Rr

B iR

B ir

Field in the region outside of the capacitor existsas if the wire were continuous within the capacitor


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