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Page 1: Chapter 22

Chapter 22

Patterns of Fields in Space

• Electric flux• Gauss’s law• Ampere’s law• Maxwell equations

Page 2: Chapter 22

What is in the box?

no charges? vertical charged plate?

Patterns of Fields in Space

Page 3: Chapter 22

Box versus open surface

Seem to be able to tellif there are charges inside

…no clue…

Gauss’s law: If we know the field distribution on closed surface we can tell what is inside.

Patterns of Fields in Space

Page 4: Chapter 22

0

ˆ

inside

surface

qAnE

0

ˆ

insideqdAnE

Symmetry makes it simple!

Gauss’s Law

Page 5: Chapter 22

Symmetry: Field must be perpendicular to surfaceEleft=Eright

0

ˆ

inside

surface

qAnE

2EAbox Q / A Abox

0

E Q / A 20

The Electric Field of a Large Plate

Page 6: Chapter 22

Symmetry: 1. Field should be radial2. The same at every location

on spherical surface

0

ˆ

inside

surface

qAnE

A. Outer sphere:

0

24

QrE 204

1rQE

B. Inner sphere:

0

2 04

rE 0E

The Electric Field of a Uniform Spherical Shell of Charge

Page 7: Chapter 22

0

ˆ

inside

surface

qAnE

Is Gauss’s law still valid?

Can we find E using Gauss’s law?

The Electric Field of a Uniform Cube

Page 8: Chapter 22

Gauss’s Law for Electric Dipole

Page 9: Chapter 22

Can we have excess charge inside in steady state?

0

ˆ

inside

surface

qAnE

surfacerightsurfaceleft

AnEAnE__

ˆˆ

00

insideq

Gauss’s Law: Circuits

Page 10: Chapter 22

Gauss’s Law: Junction Between Two Different Metal Wires

i1=i2

n1Au1E1 = n2Au2E2

E2 n1u1

n2u2

E1 E1

0

ˆ

inside

surface

qAnE

There is negative charge along the interface!

qinside 0 (E1A E2A) 0

n2<n1u2<u1

Page 11: Chapter 22

Magnet Cut in Half & Pulled Apart

No magnetic monopole! Try to cut a magnet down to a single pole, just get smaller magnets

No magnetic Charge!

Page 12: Chapter 22

Dipoles:Electric field: ‘+’ and ‘–’ charges can be separatedMagnetic field: no monopoles

Suppose magnetic dipole consists of two magnetic monopoles, each producing a magnetic field similar to the electric field.One cannot separate them total magnetic ‘charge’ is zero.

0

ˆ

inside

surface

qAnE

Gauss’s law for magnetism0ˆ

surface

AnB

0ˆ AnBor

Gauss’s Law for Magnetism

Page 13: Chapter 22

Patterns of Magnetic Field in Space

Is there current passing through these regions?

There must be a relationship between the measurements of the magnetic field along a closed path and current flowing through the enclosed area.

Ampere’s law

Page 14: Chapter 22

Quantifying the Magnetic Field Pattern

rIBwire

24

0

Curly character – introduce: ldB

dlrIldB 2

40

rrI

224

0

IldB 0

Similar to Gauss’s law (Q/0)

Page 15: Chapter 22

All the currents in the universe contribute to Bbut only ones inside the path result in nonzero path integral

Ampere’s law is almost equivalent to the Biot-Savart law:but Ampere’s law is relativistically correct

Ampère’s Law

pathinsideIldB _0

Page 16: Chapter 22

pathinsideIldB _0

Can B have an out of plane component?

Is it always parallel to the path?

rBldB 2

IrB 02

rIB 2

40

for thick wire: (the same as for thin wire)

Would be hard to derive using Biot-Savart law

Ampere’s Law: A Long Thick Wire

Page 17: Chapter 22

pathinsideIldB _0

Number of wires: (N/L)d

What is on sides? ldB

B outside is very small

BdldB

Bd 0I N / L dLINB 0

(solenoid)

Uniform: same B no matter where is the path

Ampere’s Law: A Solenoid

Page 18: Chapter 22

Three equations:

Gauss’s law for electricity

Gauss’s law for magnetism

Ampere’s law for magnetism pathinsideIldB _0

0

ˆ

insideqdAnE

Is anything missing?

‘Ampere’s law for electricity’ ldE

0 ldE

(incomplete)

Maxwell’s Equations

0ˆ AnB

Page 19: Chapter 22

0

ˆ

insideqdAnE

0 ldE

pathinsideIldB _0

Gauss’s law for electricity

Gauss’s law for magnetism

Incomplete version of Faraday’s law

Ampere’s law(Incomplete Ampere-Maxwell law)

First two: integrals over a surfaceSecond two: integrals along a path

Incomplete: no time dependence

Maxwell’s Equations (incomplete)

0ˆ AnB


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