Chapter 24 Electric Fields 第二十四章 電場. Action at a distance q1q1 q1q1 q2q2 q2q2.

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Chapter 24 Electric Fields 第第第第第 第第
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Transcript of Chapter 24 Electric Fields 第二十四章 電場. Action at a distance q1q1 q1q1 q2q2 q2q2.

Page 1: Chapter 24 Electric Fields 第二十四章 電場. Action at a distance q1q1 q1q1 q2q2 q2q2.

Chapter 24 Electric Fields

第二十四章 電場

Page 2: Chapter 24 Electric Fields 第二十四章 電場. Action at a distance q1q1 q1q1 q2q2 q2q2.

Action at a distance

1 212 212

21

ˆkq q

F rr

q1

q1

q2

q2

21r̂

9 2 29.0 10 /k Nm C

Page 3: Chapter 24 Electric Fields 第二十四章 電場. Action at a distance q1q1 q1q1 q2q2 q2q2.

Another point of view -- Fields

1 212 212

21

ˆkq q

F rr

)( 212112 rEqF

rr

qr

r

kqrE ˆ

4

1ˆ)(

22

022

2

where E2 is the electric field generated by charge q2 and r is a position vector from the position of q2 to any point in space.

22120 /10854.8 NmC

Page 4: Chapter 24 Electric Fields 第二十四章 電場. Action at a distance q1q1 q1q1 q2q2 q2q2.

Electric field lines

Page 5: Chapter 24 Electric Fields 第二十四章 電場. Action at a distance q1q1 q1q1 q2q2 q2q2.

Electric field linesThe concept of electric field lines was originally due to Faraday who envisioned that the space around a charge is filled with “lines of force”.

The field lines are originated from positive charges and terminated at negative charges, and they are unbroken in vacuum.

Page 6: Chapter 24 Electric Fields 第二十四章 電場. Action at a distance q1q1 q1q1 q2q2 q2q2.

The relationship between the electrical field and field lines

Electric field lines with arrows indicate the local field directions, and their density in a plane perpendicular to the local field represents the magnitude of the local field.

Suppose that there are N field lines originated from a positive charge q, then we have the density of field lines given by N / 4πr2 at a distance r from the charge.

Note that if N = q / ε0 then we recover E = q / 4πε0 r2.

Page 7: Chapter 24 Electric Fields 第二十四章 電場. Action at a distance q1q1 q1q1 q2q2 q2q2.

Field lines repel each other

Page 8: Chapter 24 Electric Fields 第二十四章 電場. Action at a distance q1q1 q1q1 q2q2 q2q2.

Field lines are smooth

Page 9: Chapter 24 Electric Fields 第二十四章 電場. Action at a distance q1q1 q1q1 q2q2 q2q2.
Page 10: Chapter 24 Electric Fields 第二十四章 電場. Action at a distance q1q1 q1q1 q2q2 q2q2.

The electric field due to a point charge

)(4

13

0i

i

ii rr

rr

qE

)(...)()()( 21 rErErErE n

Page 11: Chapter 24 Electric Fields 第二十四章 電場. Action at a distance q1q1 q1q1 q2q2 q2q2.

Sample problem

What is the electric field at point P?

Page 12: Chapter 24 Electric Fields 第二十四章 電場. Action at a distance q1q1 q1q1 q2q2 q2q2.

Sample problem

What is the electric field at point P?

Page 13: Chapter 24 Electric Fields 第二十四章 電場. Action at a distance q1q1 q1q1 q2q2 q2q2.

The electric field due to an electric dipole

x

y

-a a

P

3 30

( )4

r r r rqE

r r r r

r

r

r

ˆr ax

ˆr ax

Electric dipole moment:

ˆ( ) 2p q r r qax

2p qa

Page 14: Chapter 24 Electric Fields 第二十四章 電場. Action at a distance q1q1 q1q1 q2q2 q2q2.

The electric field due to an electric dipole

Along x-axis: ˆr xx

For 2 2 2

0

21

4 ( )

x pE

x a

For 2 2

2 2 20

1 ( )

4 ( )

a x pE

a a x

30

1 2

4

pE

x

:ax

:ax

:ax

Page 15: Chapter 24 Electric Fields 第二十四章 電場. Action at a distance q1q1 q1q1 q2q2 q2q2.

The electric field due to an electric dipole

In y-z plane: ˆ ˆr yy zz

2 2 2 3/ 20

1

4 ( )

pE

y z a

30

1

4

pE

r

Note that 2

1E

r for net charge 0

3

1E

r for net charge 0

but net dipole moment 0

:ar

Page 16: Chapter 24 Electric Fields 第二十四章 電場. Action at a distance q1q1 q1q1 q2q2 q2q2.

Electric field due to a line of charge

Page 17: Chapter 24 Electric Fields 第二十四章 電場. Action at a distance q1q1 q1q1 q2q2 q2q2.

Electric field due to a line of charge

Page 18: Chapter 24 Electric Fields 第二十四章 電場. Action at a distance q1q1 q1q1 q2q2 q2q2.

Electric field due to a line of charge

Page 19: Chapter 24 Electric Fields 第二十四章 電場. Action at a distance q1q1 q1q1 q2q2 q2q2.

Electric field due to a line of charge

Page 20: Chapter 24 Electric Fields 第二十四章 電場. Action at a distance q1q1 q1q1 q2q2 q2q2.

Electric field due to a charge disk

Page 21: Chapter 24 Electric Fields 第二十四章 電場. Action at a distance q1q1 q1q1 q2q2 q2q2.

A point charge in an electric field

F qE

Millikan oil-drop experiment (1910-1913)

Page 22: Chapter 24 Electric Fields 第二十四章 電場. Action at a distance q1q1 q1q1 q2q2 q2q2.

Cathode-ray tube

Page 23: Chapter 24 Electric Fields 第二十四章 電場. Action at a distance q1q1 q1q1 q2q2 q2q2.

Deflecting charge particles

Page 24: Chapter 24 Electric Fields 第二十四章 電場. Action at a distance q1q1 q1q1 q2q2 q2q2.

A dipole in an electric field

2

306.2 10H Op Cm

Page 25: Chapter 24 Electric Fields 第二十四章 電場. Action at a distance q1q1 q1q1 q2q2 q2q2.

A dipole in an electric fieldThere is no net force on a dipole.

But there is a torque.

sin ( )( sin )

sin

qEa qE a

pE

p E

Page 26: Chapter 24 Electric Fields 第二十四章 電場. Action at a distance q1q1 q1q1 q2q2 q2q2.

Potential energy of a dipole in a uniform electric field

cosU pE

ˆ ˆ( ) sinU

pE

Page 27: Chapter 24 Electric Fields 第二十四章 電場. Action at a distance q1q1 q1q1 q2q2 q2q2.

Home work

Question ( 問題 ): 6, 8, 19

Exercise ( 練習題 ): 5, 10, 16

Problem ( 習題 ): 8, 18, 31, 32