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Winter wk 8 – Thus.24.Feb.05

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Winter wk 8 – Thus.24.Feb.05. Review Ch.30 – Faraday and Lenz laws Ch.32: Maxwell Equations ! Gauss: q E Ampere: I B Faraday: dB/dt E (applications) Maxwell: dE/dt B Magnetism in matter. Energy Systems, EJZ. Gauss: charge q  E field. No magnetic charges. - PowerPoint PPT Presentation
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Winter wk 8 – Thus.24.Feb.05 Review Ch.30 – Faraday and Lenz laws Ch.32: Maxwell Equations! •Gauss: q E •Ampere: I B •Faraday: dB/dt E (applications) •Maxwell: dE/dt B Magnetism in matter Energy Systems, EJZ
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Page 1: Winter wk 8 – Thus.24.Feb.05

Winter wk 8 – Thus.24.Feb.05

Review Ch.30 – Faraday and Lenz laws

Ch.32: Maxwell Equations!

• Gauss: q E

• Ampere: I B

• Faraday: dB/dt E (applications)

• Maxwell: dE/dt B

Magnetism in matter

Energy Systems, EJZ

Page 2: Winter wk 8 – Thus.24.Feb.05

Gauss: charge q E field

0

E dA encE

q

B dA 0B ��������������

No magnetic charges

Practice: P2 (p.883)

Page 3: Winter wk 8 – Thus.24.Feb.05

Ampere: current I B field

0 encB ds i ����������������������������

Page 4: Winter wk 8 – Thus.24.Feb.05

Faraday: dB/dt E field

Bd

dt

B dAd

E dsdt

����������������������������

Page 5: Winter wk 8 – Thus.24.Feb.05

Lenz’s law tells DIRECTION of

Induced emf opposes change in flux:

Induced current Ii creates an induced field Bi to oppose any change in the external flux.

In what direction does current flow, in each diagram?

Bd

dt

Page 6: Winter wk 8 – Thus.24.Feb.05

Practice with Lenz’s law

In what direction does current flow, in each loop

Page 7: Winter wk 8 – Thus.24.Feb.05

Generators & Transformers

cos sind

BA t NBA tdt

N

1 2

1 2

2

1

1 1 2 2

2

1

:

________

________

B

B

d

dtshared flux

d V V

dt N N

V

V

Power I V I V

I

I

V N

Page 8: Winter wk 8 – Thus.24.Feb.05

AC power depends on transformers

Step-up transformer: higher voltage, lower current

Step-down: lower voltage, higher current

Page 9: Winter wk 8 – Thus.24.Feb.05

Induced magnetic fields: dE/dt B

BdE ds

dt

����������������������������

Recall Faraday: changing magnetic flux E field

Symmetry: changing electric flux B

0 0Ed

B dsdt

����������������������������

Practice: P 5, 10 (p.884)

Page 10: Winter wk 8 – Thus.24.Feb.05

Ampere-Maxwell Law

What can cause a magnetic field B?

Ampere: Current IB:

Maxwell: changing EB: 0 0Ed

B dsdt

����������������������������

0 enci B ds ����������������������������

0 0 0E

enc

dB ds i

dt

����������������������������

Page 11: Winter wk 8 – Thus.24.Feb.05

Practice with magnetic induction

Q1 (p.882): Is E increasing or decreasing?

Q2: Which loop has the greatest magnetic circulation?

Page 12: Winter wk 8 – Thus.24.Feb.05

Maxwell Eqns EM waves

Next week we will combine the Maxwell equations to

• Derive electromagnetic waves

• Derive the speed of light

Page 13: Winter wk 8 – Thus.24.Feb.05

Magnetism in matter

Earth’s B field is due to currents in the molten outer core

Electron spin ~ current loop magnetic moment =IA

Magnetic materials have regions of aligned electron spin

Probs. 67, 72, 73


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