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Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field
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Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

Dec 15, 2015

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Page 1: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

Copyright © 2009 Pearson Education, Inc.

Chapter 21Electric Charge and

Electric Field

Page 2: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

Copyright © 2009 Pearson Education, Inc.

• Static Electricity; Electric Charge and Its Conservation

• Electric Charge in the Atom

• Insulators and Conductors

• Induced Charge; the Electroscope

• Coulomb’s Law

• The Electric Field

• Electric Field Calculations for Continuous Charge Distributions

Units of Chapter 21

Page 3: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

Copyright © 2009 Pearson Education, Inc.

• Field Lines

• Electric Fields and Conductors

• Motion of a Charged Particle in an Electric Field

• Electric Dipoles

• Electric Forces in Molecular Biology: DNA

• Photocopy Machines and Computer Printers Use Electrostatics

Units of Chapter 21

Page 4: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

Copyright © 2009 Pearson Education, Inc.

Objects can be charged by rubbing

21-1 Static Electricity; Electric Charge and Its Conservation

Page 5: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

Copyright © 2009 Pearson Education, Inc.

Charge comes in two types, positive and negative; like charges repel and opposite charges attract.

21-1 Static Electricity; Electric

Charge and Its Conservation

Page 6: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

ConcepTest 21.1aConcepTest 21.1a Electric Charge IElectric Charge I

1) one is positive, the other

is negative

2) both are positive

3) both are negative

4) both are positive or both

are negative

Two charged balls are Two charged balls are

repelling each other as repelling each other as

they hang from the ceiling. they hang from the ceiling.

What can you say about What can you say about

their charges?their charges?

Page 7: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

ConcepTest 21.1aConcepTest 21.1a Electric Charge IElectric Charge I

The fact that the balls repel each

other can tell you only that they

have the same chargesame charge, but you do

not know the sign. So they can

be either both positive or both

negative.

1) one is positive, the other

is negative

2) both are positive

3) both are negative

4) both are positive or both

are negative

Two charged balls are Two charged balls are

repelling each other as repelling each other as

they hang from the ceiling. they hang from the ceiling.

What can you say about What can you say about

their charges?their charges?

Follow-up:Follow-up: What does the picture look like if the two balls are oppositely What does the picture look like if the two balls are oppositely charged? What about if both balls are neutral?charged? What about if both balls are neutral?

Page 8: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

1) have opposite charges

2) have the same charge

3) all have the same charge

4) one ball must be neutral (no charge)

From the picture, From the picture,

what can you what can you

conclude about conclude about

the charges?the charges?

ConcepTest 21.1bConcepTest 21.1b Electric Charge IIElectric Charge II

Page 9: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

1) have opposite charges

2) have the same charge

3) all have the same charge

4) one ball must be neutral (no charge)

From the picture, From the picture,

what can you what can you

conclude about conclude about

the charges?the charges?

The GREEN and PINK balls must

have the same charge, since they

repel each other. The YELLOW

ball also repels the GREEN, so it

must also have the same charge

as the GREEN (and the PINK).

ConcepTest 21.1bConcepTest 21.1b Electric Charge IIElectric Charge II

Page 10: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

Copyright © 2009 Pearson Education, Inc.

Electric charge is conserved – the arithmetic sum of the total charge cannot change in any interaction.

21-1 Static Electricity; Electric Charge and Its Conservation

Page 11: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

Copyright © 2009 Pearson Education, Inc.

Atom:

Nucleus (small, massive, positive charge)

Electron cloud (large, very low density, negative charge)

21-2 Electric Charge in the Atom

Page 12: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

Copyright © 2009 Pearson Education, Inc.

Polar molecule: neutral overall, but charge not evenly distributed

21-2 Electric Charge in the Atom

Page 13: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

Copyright © 2009 Pearson Education, Inc.

Conductor:

Charge flows freely

Metals

Insulator:

Almost no charge flows

Most other materials

Some materials are semiconductors.

21-3 Insulators and Conductors

Page 14: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

Copyright © 2009 Pearson Education, Inc.

Metal objects can be charged by conduction:

21-4 Induced Charge; the Electroscope

Page 15: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

Copyright © 2009 Pearson Education, Inc.

They can also be charged by induction, either while connected to ground or not:

21-4 Induced Charge; the Electroscope

Page 16: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

Copyright © 2009 Pearson Education, Inc.

Nonconductors won’t become charged by conduction or induction, but will experience charge separation:

21-4 Induced Charge; the Electroscope

Page 17: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

ConcepTest 21.2aConcepTest 21.2a Conductors IConductors I

1) positive

2) negative

3) neutral

4) positive or neutral

5) negative or neutral

A metal ball hangs from the ceiling

by an insulating thread. The ball is

attracted to a positive-charged rod

held near the ball. The charge of

the ball must be:

Page 18: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

Clearly, the ball will be attracted if its

charge is negativenegative. However, even if

the ball is neutralneutral, the charges in the

ball can be separated by inductioninduction

(polarization), leading to a net

attraction.

1) positive

2) negative

3) neutral

4) positive or neutral

5) negative or neutral

A metal ball hangs from the ceiling

by an insulating thread. The ball is

attracted to a positive-charged rod

held near the ball. The charge of

the ball must be:

Remember the ball is a conductor!

ConcepTest 21.2aConcepTest 21.2a Conductors IConductors I

Follow-up:Follow-up: What happens if the What happens if the metal ballmetal ball is replaced by a is replaced by a plastic ballplastic ball??

Page 19: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

Copyright © 2009 Pearson Education, Inc.

The electroscope can be used for detecting charge.

21-4 Induced Charge; the Electroscope

Page 20: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

Copyright © 2009 Pearson Education, Inc.

The electroscope can be charged either by conduction or by induction.

21-4 Induced Charge; the Electroscope

Page 21: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

Copyright © 2009 Pearson Education, Inc.

The charged electroscope can then be used to determine the sign of an unknown charge.

21-4 Induced Charge; the Electroscope

Page 22: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

Two neutral conductors are connected

by a wire and a charged rod is brought

near, but does not touch. The wire is

taken away, and then the charged rod

is removed. What are the charges on

the conductors?

ConcepTest 21.2bConcepTest 21.2b Conductors IIConductors II1) 0 0

2) + –

3) – +

4) + +

5) – –

0 0

? ?

Page 23: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

While the conductors are connected, positive positive

charge will flow from the blue to the green charge will flow from the blue to the green

ball due to polarizationball due to polarization. Once disconnected,

the charges will remain on the separate charges will remain on the separate

conductorsconductors even when the rod is removed.

Two neutral conductors are connected

by a wire and a charged rod is brought

near, but does not touch. The wire is

taken away, and then the charged rod

is removed. What are the charges on

the conductors?

ConcepTest 21.2bConcepTest 21.2b Conductors IIConductors II1) 0 0

2) + –

3) – +

4) + +

5) – –

0 0

? ?Follow-up:Follow-up: What will happen when the What will happen when the

conductors are reconnected with a wire?conductors are reconnected with a wire?

Page 24: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

Copyright © 2009 Pearson Education, Inc.

Experiment shows that the electric force between two charges is proportional to the product of the charges and inversely proportional to the distance between them.

21-5 Coulomb’s Law

Page 25: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

Copyright © 2009 Pearson Education, Inc.

Coulomb’s law:

This equation gives the magnitude of the force between two charges.

21-5 Coulomb’s Law

Page 26: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

Copyright © 2009 Pearson Education, Inc.

The force is along the line connecting the charges, and is attractive if the charges are opposite, and repulsive if they are the same.

21-5 Coulomb’s Law

Page 27: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

QQ QQF1 = 3 N F2 = ?

1) 1.0 N

2) 1.5 N

3) 2.0 N

4) 3.0 N

5) 6.0 N

What is the magnitude What is the magnitude

of the force of the force FF22??

ConcepTest 21.3aConcepTest 21.3a Coulomb’s Law ICoulomb’s Law I

Page 28: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

The force F2 must have the same magnitudesame magnitude as F1. This is

due to the fact that the form of Coulomb’s law is totally

symmetric with respect to the two charges involved. The

force of one on the other of a pair is the same as the reverseforce of one on the other of a pair is the same as the reverse.

Note that this sounds suspiciously like Newton’s 3rd law!!Note that this sounds suspiciously like Newton’s 3rd law!!

QQ QQF1 = 3 N F2 = ?

1) 1.0 N

2) 1.5 N

3) 2.0 N

4) 3.0 N

5) 6.0 N

What is the magnitude What is the magnitude

of the force of the force FF22??

ConcepTest 21.3aConcepTest 21.3a Coulomb’s Law ICoulomb’s Law I

Page 29: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

ConcepTest 21.3bConcepTest 21.3b Coulomb’s Law IICoulomb’s Law II

1) 3/4 N

2) 3.0 N

3) 12 N

4) 16 N

5) 48 N

If we increase one charge to If we increase one charge to 44QQ, ,

what is the magnitude ofwhat is the magnitude of F F11??

44QQ QQF1 = ? F2 = ?

QQ QQF1 = 3 N F2 = ?

Page 30: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

ConcepTest 21.3bConcepTest 21.3b Coulomb’s Law IICoulomb’s Law II

Originally we had:

F1 = k(Q)(Q)/r2 = 3 N

Now we have:

F1 = k(4Q)(Q)/r2

which is 4 times bigger4 times bigger than before.

1) 3/4 N

2) 3.0 N

3) 12 N

4) 16 N

5) 48 N

If we increase one charge to If we increase one charge to 44QQ, ,

what is the magnitude of what is the magnitude of FF11??

44QQ QQF1 = ? F2 = ?

QQ QQF1 = 3 N F2 = ?

Follow-up:Follow-up: Now what is the magnitude of Now what is the magnitude of FF22??

Page 31: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

1) 9F

2) 3F

3) F

4) 1/3F

5) 1/9F

The force between two charges

separated by a distance d is F. If

the charges are pulled apart to a

distance 3d, what is the force on

each charge?

QQFF

QFF

dd

QQ??

QQ??

33dd

ConcepTest 21.3cConcepTest 21.3c Coulomb’s Law IIICoulomb’s Law III

Page 32: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

Originally we had:

Fbefore = k(Q)(Q)/d2 = F

Now we have:

Fafter = k(Q)(Q)/(3d)2 = 1/9F

1) 9F

2) 3F

3) F

4) 1/3F

5) 1/9F

The force between two charges

separated by a distance d is F. If

the charges are pulled apart to a

distance 3d, what is the force on

each charge?

QQFF

QFF

dd

QQ??

QQ??

33dd

ConcepTest 21.3cConcepTest 21.3c Coulomb’s Law IIICoulomb’s Law III

Follow-up:Follow-up: What is the force if the original distance is halved? What is the force if the original distance is halved?

Page 33: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

Copyright © 2009 Pearson Education, Inc.

Unit of charge: coulomb, C.

The proportionality constant in Coulomb’s law is then:

k = 8.99 x 109 N·m2/C2.

Charges produced by rubbing are typically around a microcoulomb:

1 μC = 10-6 C.

21-5 Coulomb’s Law

Page 34: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

Copyright © 2009 Pearson Education, Inc.

Charge on the electron:

e = 1.602 x 10-19 C.

Electric charge is quantized in units of the electron charge.

21-5 Coulomb’s Law

Page 35: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

Copyright © 2009 Pearson Education, Inc.

The proportionality constant k can also be written in terms of ε0, the permittivity of free space:

21-5 Coulomb’s Law

Page 36: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

Copyright © 2009 Pearson Education, Inc.

21-5 Coulomb’s Law

Conceptual Example 21-1: Which charge exerts the greater force?

Two positive point charges, Q1 = 50 μC and Q2 = 1 μC, are separated by a distance . Which is larger in magnitude, the force that Q1 exerts on Q2 or the force that Q2 exerts on Q1?

Page 37: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

Copyright © 2009 Pearson Education, Inc.

21-5 Coulomb’s LawExample 21-2: Three charges in a line.

Three charged particles are arranged in a line, as shown. Calculate the net electrostatic force on particle 3 (the -4.0 μC on the right) due to the other two charges.

Page 38: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

ConcepTest 21.4aConcepTest 21.4a Electric Force IElectric Force I

1) yes, but only if QQ00 is positiveis positive

2) yes, but only if QQ00 is negativeis negative

3) yes, independent of the sign

(or value) of QQ00

4) no, the net force can never

be zero

Two balls with charges Two balls with charges ++QQ and and +4+4QQ

are fixed at a separation distance are fixed at a separation distance

of of 33RR. Is it possible to place . Is it possible to place

another charged ball another charged ball QQ00 on the line on the line

between the two charges such that between the two charges such that

the net force on the net force on QQ00 will be zero? will be zero?

3R

+Q +4Q

Page 39: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

ConcepTest 21.4aConcepTest 21.4a Electric Force IElectric Force I

1) yes, but only if QQ00 is positiveis positive

2) yes, but only if QQ00 is negativeis negative

3) yes, independent of the sign (or value) of QQ00

4) no, the net force can never

be zero

Two balls with charges Two balls with charges ++QQ and and +4+4QQ

are fixed at a separation distance are fixed at a separation distance

of of 33RR. Is it possible to place . Is it possible to place

another charged ball another charged ball QQ00 on the line on the line

between the two charges such that between the two charges such that

the net force on the net force on QQ00 will be zero? will be zero?

3R

+Q +4Q

A positive charge would be repelled

by both charges, so a point where

these two repulsive forces cancel

can be found. A negative charge

would be attracted by both, and the

same argument holds.

Follow-up:Follow-up: What happens if both charges are + What happens if both charges are +QQ? ? Where would the Where would the FF = 0 point be in this case? = 0 point be in this case?

Page 40: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

3R

+Q –– 4Q

Two balls with charges Two balls with charges ++QQ and and ––44QQ

are fixed at a separation distance are fixed at a separation distance

of of 33RR. Is it possible to place . Is it possible to place

another charged ball another charged ball QQ00 anywhereanywhere

on the line such that the net force on the line such that the net force

on on QQ00 will be zero? will be zero?

ConcepTest 21.4cConcepTest 21.4c Electric Force IIIElectric Force III

1) yes, but only if QQ00 is positiveis positive

2) yes, but only if QQ00 is negativeis negative

3) yes, independent of the sign

(or value) of QQ00

4) no, the net force can never

be zero

Page 41: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

3R

+Q –– 4Q

A charge (positive or negative) can

be placed to the leftto the left of the +Q charge,

such that the repulsive force from the

+Q charge cancels the attractive

force from –4Q.

Two balls with charges Two balls with charges ++QQ and and ––44QQ

are fixed at a separation distance are fixed at a separation distance

of of 33RR. Is it possible to place . Is it possible to place

another charged ball another charged ball QQ00 anywhereanywhere

on the line such that the net force on the line such that the net force

on on QQ00 will be zero? will be zero?

ConcepTest 21.4cConcepTest 21.4c Electric Force IIIElectric Force III

1) yes, but only if QQ00 is positiveis positive

2) yes, but only if QQ00 is negativeis negative

3) yes, independent of the sign

(or value) of QQ00

4) no, the net force can never

be zero

Follow-up:Follow-up: What happens if one charge is + What happens if one charge is +QQ and the other is and the other is ––QQ??

Page 42: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

Copyright © 2009 Pearson Education, Inc.

21-5 Coulomb’s LawExample 21-3: Electric force using vector components.

Calculate the net electrostatic force on charge Q3 shown in the figure due to the charges Q1 and Q2.

Page 43: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

Copyright © 2009 Pearson Education, Inc.

21-5 Coulomb’s Law

Conceptual Example 21-4: Make the force on Q3 zero.

In the figure, where could you place a fourth charge, Q4 = -50 μC, so that the net force on Q3 would be zero?

Page 44: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

Which of the arrows best

represents the direction

of the net force on charge

+Q due to the other two

charges?

+2Q

+4Q

+Q

1 23

4

5d

d

ConcepTest 21.6ConcepTest 21.6 Forces in 2DForces in 2D

Page 45: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

The charge +2Q repels +Q toward the

right. The charge +4Q repels +Q

upward, but with a stronger force.

Therefore, the net force is up and to net force is up and to

the right, but mostly upthe right, but mostly up.

+2Q

+4Q

+Q

1 23

4

5d

d

+2Q

+4Q

ConcepTest 21.6ConcepTest 21.6 Forces in 2DForces in 2D

Which of the arrows best

represents the direction

of the net force on charge

+Q due to the other two

charges?

Follow-up:Follow-up: What would happen if What would happen if the yellow charge were +3the yellow charge were +3QQ??

Page 46: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

Copyright © 2009 Pearson Education, Inc.

The electric field is defined as the force on a small charge, divided by the magnitude of the charge:

21-6 The Electric Field

Page 47: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

Copyright © 2009 Pearson Education, Inc.

21-6 The Electric Field

An electric field surrounds every charge.

Page 48: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

Copyright © 2009 Pearson Education, Inc.

For a point charge:

21-6 The Electric Field

Page 49: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

1) 44EE00

2) 22EE00

3) EE00

4) 1/21/2EE00

5) 1/44EE00

You are sitting a certain distance from You are sitting a certain distance from

a point charge, and you measure an a point charge, and you measure an

electric field of electric field of EE00. If the charge is . If the charge is

doubleddoubled and your distance from the and your distance from the

charge is also charge is also doubleddoubled, what is the , what is the

electric field strength now?electric field strength now?

ConcepTest 21.7ConcepTest 21.7 Electric FieldElectric Field

Page 50: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

Remember that the electric field is: E = kQ/r2.

Doubling the chargeDoubling the charge puts a factor of 2factor of 2 in the

numerator, but doubling the distancedoubling the distance puts a factor factor

of 4of 4 in the denominator, because it is distance

squared!! Overall, that gives us a factor of 1/2factor of 1/2.

1) 44EE00

2) 22EE00

3) EE00

4) 1/21/2EE00

5) 1/44EE00

You are sitting a certain distance from You are sitting a certain distance from

a point charge, and you measure an a point charge, and you measure an

electric field of electric field of EE00. If the charge is . If the charge is

doubleddoubled and your distance from the and your distance from the

charge is also charge is also doubleddoubled, what is the , what is the

electric field strength now?electric field strength now?

ConcepTest 21.7ConcepTest 21.7 Electric FieldElectric Field

Follow-up:Follow-up: If your distance is doubled, what must you do to If your distance is doubled, what must you do to the charge to the charge to maintain the same maintain the same EE field field at your new position? at your new position?

Page 51: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

Copyright © 2009 Pearson Education, Inc.

Force on a point charge in an electric field:

21-6 The Electric Field

Page 52: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

Copyright © 2009 Pearson Education, Inc.

21-6 The Electric Field

Example 21-6: Electric field of a single point charge.

Calculate the magnitude and direction of the electric field at a point P which is 30 cm to the right of a point charge Q = -3.0 x 10-6 C.

Page 53: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

Copyright © 2009 Pearson Education, Inc.

21-6 The Electric FieldExample 21-7: E at a point between two charges.Two point charges are separated by a distance of 10.0 cm. One has a charge of -25 μC and the other +50 μC. (a) Determine the direction and magnitude of the electric field at a point P between the two charges that is 2.0 cm from the negative charge. (b) If an electron (mass = 9.11 x 10-31 kg) is placed at rest at P and then released, what will be its initial acceleration (direction and magnitude)?

Page 54: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

Copyright © 2009 Pearson Education, Inc.

21-6 The Electric Field

Example 21-8: above two point charges.

Calculate the total electric field (a) at point A and (b) at point B in the figure due to both charges, Q1 and Q2.

E

Page 55: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

What is the electric field at What is the electric field at

the center of the square?the center of the square?

43

2 1

-2 C

-2 C

5) E = 0

ConcepTest 21.9aConcepTest 21.9a Superposition ISuperposition I

Page 56: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

For the upper charge, the E field vector at the center

of the square points toward that charge. For the

lower charge, the same thing is true. Then the vector

sum of these two E field vectors points to the leftpoints to the left.

What is the electric field at What is the electric field at

the center of the square?the center of the square?

43

2 1

-2 C

-2 C

5) E = 0

ConcepTest 21.9aConcepTest 21.9a Superposition ISuperposition I

Follow-up:Follow-up: What if the lower charge were +2 C? What if the lower charge were +2 C? What if both charges were +2 C? What if both charges were +2 C?

Page 57: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

Copyright © 2009 Pearson Education, Inc.

Problem solving in electrostatics: electric forces and electric fields

1. Draw a diagram; show all charges, with signs, and electric fields and forces with directions.

2. Calculate forces using Coulomb’s law.

3. Add forces vectorially to get result.

4. Check your answer!

21-6 The Electric Field

Page 58: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

Copyright © 2009 Pearson Education, Inc.

• Two kinds of electric charge – positive and negative.

• Charge is conserved.

• Charge on electron:

e = 1.602 x 10-19 C.

• Conductors: electrons free to move.

• Insulators: nonconductors.

Summary of Chapter 21 Sec. 1-6

Page 59: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

Copyright © 2009 Pearson Education, Inc.

• Charge is quantized in units of e.

• Objects can be charged by conduction or induction.

• Coulomb’s law:

•Electric field is force per unit charge:

Summary of Chapter 21 Sec. 1-6

Page 60: Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.

Copyright © 2009 Pearson Education, Inc.

• Electric field of a point charge:

Summary of Chapter 21 Sec. 1-6