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Chapter 22 Patterns of Fields in Space Electric flux Gauss’s law Ampere’s law Maxwell equations
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Chapter 22

Feb 24, 2016

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Chaman ahirwar

Chapter 22. Patterns of Fields in Space. Electric flux Gauss’s law Ampere’s law Maxwell equations. Patterns of Fields in Space. What is in the box?. vertical charged plate?. no charges?. Patterns of Fields in Space. Box versus open surface. …no clue…. Seem to be able to tell - PowerPoint PPT Presentation
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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