Exam I Solutions p

advertisement

Physics 54 !

Summer 2012

Exam I

Solutions

Part A. Multiple choice questions. Check the best answer. Each question carries a value of 4 points.

1.

!

A small dipole with moment p oriented as shown is near a fixed positive point charge Q . If the dipole is released from rest in this configuration:

!

p will rotate clockwise and then be repelled by Q .

Q

!

p will rotate counter-clockwise and then be repelled by Q .

!

p will rotate clockwise and then be attracted by Q .

!

p will rotate counter-clockwise then be attracted by Q .

p

!

2.

!

Two hollow spheres have the same dimensions and carry the same total charge + Q . Sphere A is a conductor; sphere B is a non-conductor with charge distributed uniformly throughout the material. Consider each case separately as an isolated sphere, taking

V

( ∞ ) = 0 . The potential at the center of the sphere:

A B

!

Is the same for both cases.

!

Is equal to the potential at the outer surface for both cases.

!

Is greater for case A .

!

Is greater for case B .

[The potential continues to increase as we cross the charged material in the nonconducting sphere, while for the conductor the potential remains constant inside the outer surface.]

1

Physics 54 !

Summer 2012

3.

!

Two point charges of equal magnitude are fixed at points on the x -axis. There is a point on that axis between the charges where V

= 0 (taking as usual

V

( ∞ ) = 0 ).

!

There is a point on the finite x -axis where E

= 0 .

!

There is another point on the finite x -axis where V

= 0 .

!

The potential energy of the charges is negative. {Opposite sign charges.]

!

None of the above is true.

!

!

4.

!

In the situation shown, a parallel plate capacitor is fully charged and remains connected to the battery. A conducting plate is inserted into the gap between the plates, partially filling the gap. Which of the following is NOT true?

!

The capacitance increases.

!

!

It makes no difference where the conducting plate is located vertically between the plates.

!

The E-field in the gaps between the capacitor plates is unchanged.

[It increases because the charge increases.]

!

The charge on the capacitor plates increases.

!

!

Part B. True-false questions. Check T or F depending on whether the statement is true or false. Each question carries a value of 3 points.

5.

!

The total charge in a closed system cannot be changed by any means.

T F

6.

!

If a point charge Q is surrounded by a hollow metal container, the total charge on the inner surface of the container is – Q regardless of the shape of the container.

T F

7.

!

Removing dielectric material from between the plates of a charged and isolated capacitor results in an increase in the energy stored by the capacitor.

T F [ C decreases so U increases.]

2

Physics 54 !

Summer 2012

Part C. Problems. Work problem in space provided, using extra sheets if needed. Explain your method clearly. Problems carry the point values shown.

1.

!

Two dipoles, consisting of charges ± q separated by distance d , oriented as shown, are a distance x apart.

x a.

!

Write the potential energy in terms of the given quantities (omitting the energy of the charges within each dipole).

b.

!

Use the binomial approximation to find the formula for this energy when

x

>> d . Write it in terms of the dipole moment

p

= qd .

c.

!

If the dipoles are released from rest, will they attract or repel each other?

How do you know?

[15 points] a.

!

The opposite charge pairs are at distance x apart. The same charge pairs are at distance

x

2 + d

2

apart. Thus we have

U = − 2 k q

2 x

+ 2 k x

2 q

2

+ d

2

= − 2 kq

2

1 x

− x

2

1

+ d

2

.

b.

!

The 2nd term in ( ) can be written as

1 x find U ≈ − k

( qd )

2 x

3

= − k p x

2

3

.

(

⋅ 1 + ( d / x )

2

) − 1/2

1 x

(

1 − 1

2

( d / x )

2

)

, so we c.

!

Since U is negative the system is bound. They will attract each other.

3

!

Physics 54 !

Summer 2012

2.

!

A parallel plate capacitor has half the region between its plates filled with a dielectric material as shown. The plates have area A and are separated by distance d . The potential of the positive plate is

V 0

and that of the negative plate is zero. Take κ = 2 .

+ a.

!

Let the E-field in the empty gap be

E 1

and that in the dielectric

E 2

. What is the ratio

E 2

/ E

1

?

x b.

!

What are

E 1

and

E 2

in terms of the given quantities?

[Express

V 0

in terms of the E-fields.] c.

!

Plot carefully the potential between the plates V vs. x , with x

= 0 at the positive plate. [What is the potential at

x

= d /2 ?]

− d.

!

Find the stored energy. [What are the energy densities in the two regions?]

[20 points] a.

!

E 2

/ E

1

= 1/ κ = 1/2 .

b.

!

We have

V 0

= E

1

⋅ ( d /2) + E

2

( d /2) . Using (a) we find E

1

=

4 V

0

3 d

and E

2

=

2 V

0

3 d

.

c.

!

See plot. The potential at

x

= d /2 is

2

3

V

0

. d.

!

We have u e

(1) = 1

2

ε

0

E

2

1 in each region is

A

= 8

9

ε

0

( V

0

/ d )

2

and u e

(2) = 1

2

κε

0

E

2

2

⋅ ( d /2) so we find U = ( Ad /2) ⋅ [ u e

=

(1) + u

4

9

ε

0

( V

0

/ d )

2

. The volume e

(2)] = 2

3

ε

0

A d

⋅ V

0

2

.

!

V 0

V

2

3

V

0

!

d

/2

4

d

x

Physics 54 !

Summer 2012

3.

!

In the cases shown, a conducting sphere of radius a is surrounded by a larger concentric conducting shell of radius b and negligible thickness.

Case 1 Case 2

Case 1. Charge + Q is placed on the inner sphere only.

Case 2. Charge +Q is placed on the outer shell only.

a.

In each case, sketch lines of the E-field, in the gap between the conductors and in the space outside the shell.

b.

!

In each case, find the potential on both conductors (taking

V

( ∞ ) = 0 ).

c.

!

Compare the energy stored in the field in the two cases. [Which is larger?] d.

!

Suppose a thin conducting wire is connected between the sphere and the shell. What difference would that make to your answers?

[20 points] a.

!

See drawing above. In Case 2 the charge is only on the outer surface of the shell.

b.

!

For r

V

> b the situation is like a point charge Q at the center in both cases, so

( b ) = kQ / b . In Case 2 the potential is constant at this value for r

< b . For Case 1 we have V ( a ) − V ( b ) = −

b a kQ r

2 dr = kQ

⎝⎜

1 a

1 b

⎠⎟

. Since V ( b ) = kQ b

we find V ( a ) = kQ a

.

[The negligible thickness of the shell makes it this simple.] c.

!

The energy stored outside the outer shell is the same in both cases. In Case 2 that is the total energy stored. But in Case 1 there is also energy between the sphere and the shell, so the total energy is greater in that case.

d.

!

No difference in Case 2, because the two conductors are already at the same potential. In Case 1 the charge on the inner sphere would cancel with the charge on the inner surface of the shell, making this case like Case 2.

5

Physics 54 !

Summer 2012

4.

!

A parallel plate capacitor has plates of area A separated by distance x , so it has capacitance

C

= ε

0

A / x . It is charged to potential V by a battery, which remains connected to it. An external agent changes the distance between the plates from initial value

x 1

to final value

x 2

, changing the capacitance from

C 1 to

C 2

, and changing the stored energy by the amount Δ U = 1

2

( C

2

− C

1

) ⋅ V

2

.

a.

!

When the distance between the plates is x , what is the charge

Q

( x ) ?

b.

!

The force of attraction between the plates is the charge on one plate times the E-field created by the other. [Each plate creates half the total field in the gap.] Write this force in terms of

Q

( x ) and then use your answer to (a) to put it in terms of x .

c.

!

Show that the work done by the external agent is equal to −Δ U .

d.

!

Find the initial and final charges, and show that the work done by the battery while the charge changes is equal to 2 Δ U .

!

[20 points] a. !

Q ( x ) = C ( x ) ⋅ V =

ε

0

A x

⋅ V .

b.

!

The field due to one plate alone is E

= σ

/ 2

ε

0

=

Q / 2 A

ε

0

. The force is thus

F

= QE = Q

2

/2 A ε

0

. Substituting from (a) we have F ( x ) =

ε

0

AV

2

2

1 x

2

.

c.

!

W =

x

2 x

1

F ( x ) dx =

ε

0

AV

2

2

⎝⎜

1 x

1

1

⎞ x

2

⎠⎟

= 1

2

( C

1

− C

2

) ⋅ V

2

. This is −Δ U as claimed.

d.

!

The initial and final charges are supplied by the battery is

Q 1

Δ Q = ( C

2

= C

1

V and

Q 2

− C

1

) V

= C

2

V , so the amount of charge

. the work done to put this charge on the capacitor is

W batt

= Δ Q ⋅ V = ( C

2

− C

1

) ⋅ V

2 = 2 Δ U , as claimed.

6

Physics 54 !

Median = 63

SD = 11

Summer 2012

7

Download