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- q +q s p We can define a vector called the dipole moment ( 电电 ). Magnitude: Direction: from the negative (-) charge to the positive (+) charge. qs p NOTE: This p has nothing to do with momentum!

We can define a vector called the dipole moment ( 电矩 )

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We can define a vector called the dipole moment ( 电矩 ). NOTE : This p has nothing to do with momentum!. +q. -q. s. Magnitude: Direction : from the negative (-) charge to the positive (+) charge. http://phet.colorado.edu/en/simulation/balloons. - PowerPoint PPT Presentation

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Page 1: We can define a vector called the  dipole moment ( 电矩 )

-q +q

s

p

We can define a vector called the dipole moment (电矩 ).

Magnitude:

Direction: from the negative (-) charge to the positive (+) charge.

qsp

NOTE: This p has nothing to do with momentum!

Page 2: We can define a vector called the  dipole moment ( 电矩 )

304

1

r

pE

30

axis

2

4

1

r

pE

p

Page 3: We can define a vector called the  dipole moment ( 电矩 )

http://phet.colorado.edu/en/simulation/balloons

Page 4: We can define a vector called the  dipole moment ( 电矩 )

http://phet.colorado.edu/en/simulation/balloons

Page 5: We can define a vector called the  dipole moment ( 电矩 )

Why does the charged balloon stick to the neutral wall?

http://phet.colorado.edu/en/simulation/balloons

Page 6: We can define a vector called the  dipole moment ( 电矩 )

Neutral atom

+-

Page 7: We can define a vector called the  dipole moment ( 电矩 )

The atom becomes polarized.

++-

Page 8: We can define a vector called the  dipole moment ( 电矩 )

The atom becomes polarized.

++-

Page 9: We can define a vector called the  dipole moment ( 电矩 )

We can approximate the polarized atom as a dipole.

+ +-chargeE

p

chargeEp

This is the polarizability, which is different for every material.

Page 10: We can define a vector called the  dipole moment ( 电矩 )

The dipole makes an electric field at the charge.

+ +-chargeE

p

chargeEp

dipoleE

What is the force on the charge?

Page 11: We can define a vector called the  dipole moment ( 电矩 )

+ +-chargeE

p

dipoleE

rr

qE ˆ

4

12

0charge

Page 12: We can define a vector called the  dipole moment ( 电矩 )

+ +-chargeE

p

dipoleE

rr

qE ˆ

4

12

0charge

3

charge

03

0dipole

2

4

12

4

1

r

E

r

pE

Substitute…

Page 13: We can define a vector called the  dipole moment ( 电矩 )

+ +-chargeE

p

dipoleE

rr

qE ˆ

4

12

0charge

rr

qE ˆ

2

4

15

2

0dipole

Substitute…

Page 14: We can define a vector called the  dipole moment ( 电矩 )

+ +-chargeE

p

dipoleE

rr

qEqF ˆ

2

4

15

22

0dipolecharge

The charge is attracted to the polarized atom, no matter if the charge is positive or negative!

Page 15: We can define a vector called the  dipole moment ( 电矩 )

Wall

Balloon------

--

+ -

+ -

+ -

+ -

+ -

+ -

+ -

+ -

+ -

+ -

(1) The charges on the balloon polarize the wall.

Page 16: We can define a vector called the  dipole moment ( 电矩 )

Wall

Balloon------

--

+ -

+ -

+ -

+ -

+ -

+ -

+ -

+ -

+ -

+ -

(2) The polarized atoms in the wall attract the balloon.

Page 17: We can define a vector called the  dipole moment ( 电矩 )

The wall and the balloon are both insulators (绝缘材料 , or 电价值 ).

In an insulator, the charges are not free to move around. Atoms can be polarized, but they do not change their position.

A material in which charges are free to move around is called a conductor (导体 ).

Page 18: We can define a vector called the  dipole moment ( 电矩 )

Example: Salt water (ionic solution 离子溶液 )

At equilibrium, the net field in a conductor must be zero.

The ions move with a speed v = uE, where u is called the mobility.

Page 19: We can define a vector called the  dipole moment ( 电矩 )

Example: A metalIn a metal, one or two electrons from every atom is free to move around. They form a sea of electrons.

appliedE

onpolarizatiE

The metal becomes polarized.

Page 20: We can define a vector called the  dipole moment ( 电矩 )

Example: A metalIn a metal, one or two electrons from every atom is free to move around. They form a sea of electrons.

Net field inside is zero.

The metal becomes polarized.

Page 21: We can define a vector called the  dipole moment ( 电矩 )

We will prove these later, using Gauss’ Law

Page 22: We can define a vector called the  dipole moment ( 电矩 )

Permanent dipoles in an electric field

+

-

Water is a permanent dipole

OH

H

Page 23: We can define a vector called the  dipole moment ( 电矩 )

E+-

p

F

F

In a uniform field, the net force on a dipole is zero:

0 FF

Page 24: We can define a vector called the  dipole moment ( 电矩 )

E+-

p

F

F

But the net torque around the dipole’s COM is not zero:

Ep

Page 25: We can define a vector called the  dipole moment ( 电矩 )

E+

- p

F

F

This torque will rotate the dipole until it is parallel with the field.

Page 26: We can define a vector called the  dipole moment ( 电矩 )

E+

- p

F

F

The dipole-field system has a potential energy:

EpU

dipole

Page 27: We can define a vector called the  dipole moment ( 电矩 )

Water

Balloon------

--

+-

+-

+-

+-

+-

+-

+-

+ -

+-

+-

Page 28: We can define a vector called the  dipole moment ( 电矩 )

Water

Balloon------

--

+ -

+ -

+ -

+ -

+ -

+ -+

-

+ -

+ -

+ -

Water is polarized by rotating the molecules.