chapter 23: electric potential section 23-1: potential difference

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Chapter 23: Electric Potential Section 23-1: Potential Difference

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Page 1: Chapter 23: Electric Potential Section 23-1: Potential Difference

Chapter 23: Electric Potential

Section 23-1: Potential Difference

Page 2: Chapter 23: Electric Potential Section 23-1: Potential Difference

The voltage between the cathode and the screen of a television set is 22 kV. If we assume a speed of zero for an electron as it leaves the cathode, what is its speed just

before it hits the screen?

A. 8.8 × 107 m/s

B. 2.8 × 106 m/s

C. 6.2 × 107 m/s

D. 7.7 × 1015 m/s

E. 5.3 × 107 m/s

Page 3: Chapter 23: Electric Potential Section 23-1: Potential Difference

The voltage between the cathode and the screen of a television set is 22 kV. If we assume a speed of zero for an electron as it leaves the cathode, what is its speed just

before it hits the screen?

A. 8.8 × 107 m/s

B. 2.8 × 106 m/s

C. 6.2 × 107 m/s

D. 7.7 × 1015 m/s

E. 5.3 × 107 m/s

Page 4: Chapter 23: Electric Potential Section 23-1: Potential Difference

The electric field in a region is given by E = 2x2 i + 3y j where the units are in V/m. What is the change in electric potential from the origin to (x, y) = (2, 0) m?

a. 8 V

b. –8 V

c. –16/3 V

d. –24/3 V

e. 11 V

Page 5: Chapter 23: Electric Potential Section 23-1: Potential Difference

The electric field in a region is given by E = 2x2 i + 3y j where the units are in V/m. What is the change in electric potential from the origin to (x, y) = (2, 0) m?

A. 8 V

B. –8 V

C. –16/3 V

D. –24/3 V

E. 11 V

Page 6: Chapter 23: Electric Potential Section 23-1: Potential Difference

A lithium nucleus with a charge of +3e and a mass of 7 u, and an alpha particle with a charge of +2e and a mass of 4 u, are at rest. They could be

accelerated to the same kinetic energy by

A. accelerating them through the same electrical potential difference.

B. accelerating the alpha particle through V volts and the lithium nucleus through 2V/3 volts.

C. accelerating the alpha particle through V volts and the lithium nucleus through 7V/4 volts.

D. accelerating the alpha particle through V volts and the lithium nucleus through 7V/6 volts.

E. none of these procedures.

Page 7: Chapter 23: Electric Potential Section 23-1: Potential Difference

A lithium nucleus with a charge of +3e and a mass of 7 u, and an alpha particle with a charge of +2e and a mass of 4 u, are at rest. They could be

accelerated to the same kinetic energy by

A. accelerating them through the same electrical potential difference.

B. accelerating the alpha particle through V volts and the lithium nucleus through 2V/3 volts.

C. accelerating the alpha particle through V volts and the lithium nucleus through 7V/4 volts.

D. accelerating the alpha particle through V volts and the lithium nucleus through 7V/6 volts.

E. none of these procedures.

Page 8: Chapter 23: Electric Potential Section 23-1: Potential Difference

The concept of difference in electric potential is most closely associated with

A. the mechanical force on an electron.

B. the number of atoms in one gram-atom.

C. the charge on one electron.

D. the resistance of a certain specified column of mercury.

E. the work per unit quantity of electric charge.

Page 9: Chapter 23: Electric Potential Section 23-1: Potential Difference

The concept of difference in electric potential is most closely associated with

A. the mechanical force on an electron.

B. the number of atoms in one gram-atom.

C. the charge on one electron.

D. the resistance of a certain specified column of mercury.

E. the work per unit quantity of electric charge.

Page 10: Chapter 23: Electric Potential Section 23-1: Potential Difference

Charges Q and q (Q ≠ q), separated by a distance d, produce a potential VP = 0 at point P. This means that

A. no force is acting on a test charge placed at point P.

B. Q and q must have the same sign.

C. the electric field must be zero at point P.

D. the net work in bringing Q to distance d from q is zero.

E. the net work needed to bring a charge from infinity to point P is zero.

Page 11: Chapter 23: Electric Potential Section 23-1: Potential Difference

Charges Q and q (Q ≠ q), separated by a distance d, produce a potential VP = 0 at point P. This means that

A. no force is acting on a test charge placed at point P.

B. Q and q must have the same sign.

C. the electric field must be zero at point P.

D. the net work in bringing Q to distance d from q is zero.

E. the net work needed to bring a charge from infinity to point P is zero.

Page 12: Chapter 23: Electric Potential Section 23-1: Potential Difference

When +2.0 C of charge moves at constant speed from a point with zero potential to a point with potential +6.0 V, the amount of work done is

A. 2 J.

B. 3 J.

C. 6 J.

D. 12 J.

E. 24 J.

Page 13: Chapter 23: Electric Potential Section 23-1: Potential Difference

When +2.0 C of charge moves at constant speed from a point with zero potential to a point with potential +6.0 V, the amount of work done is

A. 2 J.

B. 3 J.

C. 6 J.

D. 12 J.

E. 24 J.

Page 14: Chapter 23: Electric Potential Section 23-1: Potential Difference

The electron volt is a unit of

A. capacitance.

B. charge.

C. energy.

D. momentum.

E. potential.

Page 15: Chapter 23: Electric Potential Section 23-1: Potential Difference

The electron volt is a unit of

A. capacitance.

B. charge.

C. energy.

D. momentum.

E. potential.

Page 16: Chapter 23: Electric Potential Section 23-1: Potential Difference

Two parallel horizontal plates are spaced 0.40 cm apart in air. You introduce an oil droplet of mass 4.9 × 10–17 kg between the plates. If the droplet carries two electronic charges and if there were no air buoyancy, you could hold the droplet motionless between the plates if you kept the potential difference between them at

A. 60 V.

B. 12 V.

C. 3.0 V.

D. 0.12 kV.

E. 6.0 V.

Page 17: Chapter 23: Electric Potential Section 23-1: Potential Difference

Two parallel horizontal plates are spaced 0.40 cm apart in air. You introduce an oil droplet of mass 4.9 × 10–17 kg between the plates. If the droplet carries two electronic charges and if there were no air buoyancy, you could hold the droplet motionless between the plates if you kept the potential difference between them at

A. 60 V.

B. 12 V.

C. 3.0 V.

D. 0.12 kV.

E. 6.0 V.

Page 18: Chapter 23: Electric Potential Section 23-1: Potential Difference

Two parallel metal plates 5.0 cm apart have a potential difference between them of 75 V. The electric force on a positive charge of 3.2 × 10–19 C at a point midway between the plates is approximately

A. 4.8 × 10–18 N.

B. 2.4 × 10–17 N.

C. 1.6 × 10–18 N.

D. 4.8 × 10–16 N.

E. 9.6 × 10–17 N.

Page 19: Chapter 23: Electric Potential Section 23-1: Potential Difference

Two parallel metal plates 5.0 cm apart have a potential difference between them of 75 V. The electric force on a positive charge of 3.2 × 10–19 C at a point midway between the plates is approximately

A. 4.8 × 10–18 N.

B. 2.4 × 10–17 N.

C. 1.6 × 10–18 N.

D. 4.8 × 10–16 N.

E. 9.6 × 10–17 N.

Page 20: Chapter 23: Electric Potential Section 23-1: Potential Difference

The electrostatic potential as a function of distance along a certain line in space is shown in graph (1). Which of the curves in graph (2) is most likely to represent the electric field as a function of distance along the same line?

Page 21: Chapter 23: Electric Potential Section 23-1: Potential Difference

The electrostatic potential as a function of distance along a certain line in space is shown in graph (1). Which of the curves in graph (2) is most likely to represent the electric field as a function of distance along the same line?

Page 22: Chapter 23: Electric Potential Section 23-1: Potential Difference

Which of the points shown in the diagram are at the same potential?

a. 2 and 5

b. 2, 3, and 5

c. 1 and 4

d. 1 and 5

e. 2 and 4

Page 23: Chapter 23: Electric Potential Section 23-1: Potential Difference

Which of the points shown in the diagram are at the same potential?

A. 2 and 5

B. 2, 3, and 5

C. 1 and 4

D. 1 and 5

E. 2 and 4

Page 24: Chapter 23: Electric Potential Section 23-1: Potential Difference

Which point in the electric field in the diagram is at the highest potential?

a. 1

b. 2

c. 3

d. 4

e. 5

Page 25: Chapter 23: Electric Potential Section 23-1: Potential Difference

Which point in the electric field in the diagram is at the highest potential?

A. 1

B. 2

C. 3

D. 4

E. 5

Page 26: Chapter 23: Electric Potential Section 23-1: Potential Difference

Which point in the electric field in the diagram is at the lowest potential?

a. 1

b. 2

c. 3

d. 4

e. 5

Page 27: Chapter 23: Electric Potential Section 23-1: Potential Difference

Which point in the electric field in the diagram is at the lowest potential?

A. 1

B. 2

C. 3

D. 4

E. 5

Page 28: Chapter 23: Electric Potential Section 23-1: Potential Difference

The figure shows two plates A and B. Plate A has a potential of 0 V and plate B a potential of 100 V. The dotted lines represent equipotential lines of 25, 50, and 75 V. A positive test charge of 1.6 × 10–19 C at point x is transferred to point z. The electric potential energy

gained or lost by the test charge is A. 8 × 10–18 J, gained. B. 8 × 10–18 J, lost. C. 24 × 10–18 J, gained. D. 24 × 10–8 J, lost. E. 40 × 10–8 J, gained.

Page 29: Chapter 23: Electric Potential Section 23-1: Potential Difference

The figure shows two plates A and B. Plate A has a potential of 0 V and plate B a potential of 100 V. The dotted lines represent equipotential lines of 25, 50, and 75 V. A positive test charge of 1.6 × 10–19 C at point x is transferred to point z. The electric potential energy

gained or lost by the test charge is A. 8 × 10–18 J, gained. B. 8 × 10–18 J, lost. C. 24 × 10–18 J, gained. D. 24 × 10–8 J, lost. E. 40 × 10–8 J, gained.

Page 30: Chapter 23: Electric Potential Section 23-1: Potential Difference

Chapter 23: Electric Potential

Section 23-2: Potential Due to a System of Point Charges

Page 31: Chapter 23: Electric Potential Section 23-1: Potential Difference

Charges +Q and –Q are arranged at the corners of a square as shown. When the magnitude of the electric field E and the electric potential V are determined at P, the center of the square, we find that

A. E ≠ 0 and V > 0.

B. E = 0 and V = 0.

C. E = 0 and V > 0.

D. E ≠ 0 and V < 0.

E. None of these is correct.

Page 32: Chapter 23: Electric Potential Section 23-1: Potential Difference

Charges +Q and –Q are arranged at the corners of a square as shown. When the magnitude of the electric field E and the electric potential V are determined at P, the center of the square, we find that

A. E ≠ 0 and V > 0.

B. E = 0 and V = 0.

C. E = 0 and V > 0.

D. E ≠ 0 and V < 0.

E. None of these is correct.

Page 33: Chapter 23: Electric Potential Section 23-1: Potential Difference

Q

200V 00V a b c

Q

Two equal positive charges are placed in an external electric field. The equipotential lines shown are at 100 V intervals. The potential for line c is

A. 100 V.

B. 100 V.

C. 200 V.

D. 200 V.

E. zero

Page 34: Chapter 23: Electric Potential Section 23-1: Potential Difference

Q

200V 00V a b c

Q

Two equal positive charges are placed in an external electric field. The equipotential lines shown are at 100 V intervals. The potential for line c is

A. 100 V.

B. 100 V.

C. 200 V.

D. 200 V.

E. zero

Page 35: Chapter 23: Electric Potential Section 23-1: Potential Difference

Two equal positive charges are placed in an external electric field. The equipotential lines shown are at 100 V intervals. The work required to move a third charge, q = e, from the 100 V line to b is

A. 100 eV.

B. 100 eV.

C. 200 eV.

D. 200 eV.

E. zeroQ

200V 00V a b c

Q

Page 36: Chapter 23: Electric Potential Section 23-1: Potential Difference

Two equal positive charges are placed in an external electric field. The equipotential lines shown are at 100 V intervals. The work required to move a third charge, q = e, from the 100 V line to b is

A. 100 eV.

B. 100 eV.

C. 200 eV.

D. 200 eV.

E. zeroQ

200V 00V a b c

Q

Page 37: Chapter 23: Electric Potential Section 23-1: Potential Difference

The potential at a point due to a unit positive point charge is found to be V. If the distance between the charge and the point is tripled, the potential becomes

A. V/3.

B. 3V.

C. V/9.

D. 9V.

E. 1/V 2 .

Page 38: Chapter 23: Electric Potential Section 23-1: Potential Difference

The potential at a point due to a unit positive point charge is found to be V. If the distance between the charge and the point is tripled, the potential becomes

A. V/3.

B. 3V.

C. V/9.

D. 9V.

E. 1/V 2 .

Page 39: Chapter 23: Electric Potential Section 23-1: Potential Difference

The electric field for a charge distribution is E = 0 for

r < 1 m, and for .

A. 4000 V.

B. 2000 V.

C. 1000 V.

D. Zero.

E. Cannot be determined precisely.

E (

10 V

/m)

3

r (m)0 1 2 3 4

0

1

2

3

4

rr

E ˆmV4000

2

m 1r

Use the reference point V = 0 as r infinity. The potential for r < 1 m is

Page 40: Chapter 23: Electric Potential Section 23-1: Potential Difference

The electric field for a charge distribution is E = 0 for

r < 1 m, and for .

A. 4000 V.

B. 2000 V.

C. 1000 V.

D. Zero.

E. Cannot be determined precisely.

E (

10 V

/m)

3

r (m)0 1 2 3 4

0

1

2

3

4

rr

E ˆmV4000

2

m 1r

Use the reference point V = 0 as r infinity. The potential for r < 1 m is

Page 41: Chapter 23: Electric Potential Section 23-1: Potential Difference

The electric field for a charge distribution is E = 0 for

r < 1 m, and for .

A. 4000 eV.

B. 2000 eV.

C. 1000 eV.

D. −4000 eV.

E. Zero

E (

10 V

/m)

3

r (m)0 1 2 3 4

0

1

2

3

4

rr

E ˆmV4000

2

m 1r

Use the reference point V = 0 as r infinity. The work required to move a charge, q = e from infinity to r = 2 m is

Page 42: Chapter 23: Electric Potential Section 23-1: Potential Difference

The electric field for a charge distribution is E = 0 for

r < 1 m, and for .

A. 4000 eV.

B. 2000 eV.

C. 1000 eV.

D. −4000 eV.

E. Zero

E (

10 V

/m)

3

r (m)0 1 2 3 4

0

1

2

3

4

rr

E ˆmV4000

2

m 1r

Use the reference point V = 0 as r infinity. The work required to move a charge, q = e from infinity to r = 2 m is

Page 43: Chapter 23: Electric Potential Section 23-1: Potential Difference

Chapter 23: Electric Potential

Section 23-3: Computing the Electric Field from the Potential, and Concept

Checks 23-1 and 23-2

Page 44: Chapter 23: Electric Potential Section 23-1: Potential Difference

In what direction can you move relative to an electric field so that the electric potential does not change?

A. parallel to the electric field

B. perpendicular to the electric field

Page 45: Chapter 23: Electric Potential Section 23-1: Potential Difference

In what direction can you move relative to an electric field so that the electric potential does not change?

A. parallel to the electric field

B. perpendicular to the electric field

Page 46: Chapter 23: Electric Potential Section 23-1: Potential Difference

In what direction can you move relative to an electric field so that the electric potential increases at the greatest rate?

A. in the direction of the electric field

B. opposite to the direction of the electric field

C. perpendicular to the electric field

Page 47: Chapter 23: Electric Potential Section 23-1: Potential Difference

In what direction can you move relative to an electric field so that the electric potential increases at the greatest rate?

A. in the direction of the electric field

B. opposite to the direction of the electric field

C. perpendicular to the electric field

Page 48: Chapter 23: Electric Potential Section 23-1: Potential Difference

The figure depicts a uniform electric field. Along which direction is there no change in the electric potential?

Page 49: Chapter 23: Electric Potential Section 23-1: Potential Difference

The figure depicts a uniform electric field. Along which direction is there no change in the electric potential?

Page 50: Chapter 23: Electric Potential Section 23-1: Potential Difference

The figure depicts a uniform electric field. Along which direction is the increase in the electric potential a maximum?

Page 51: Chapter 23: Electric Potential Section 23-1: Potential Difference

The figure depicts a uniform electric field. Along which direction is the increase in the electric potential a maximum?

Page 52: Chapter 23: Electric Potential Section 23-1: Potential Difference

The electric potential in a region of space is given by V = 2xy + 3y2 in units of V. The electric field, in V/m, in this region is

above. theof None E.

ˆ)62(ˆ2 D.

)ˆ3ˆ(2 C.

)ˆ3ˆ(2 B.

ˆ)62(ˆ2 A.

jyxiy

jiy

jiy

jyxiy

Page 53: Chapter 23: Electric Potential Section 23-1: Potential Difference

The electric potential in a region of space is given by V = 2xy + 3y2 in units of V. The electric field, in V/m, in this region is

above. theof None E.

ˆ)62(ˆ2 D.

)ˆ3ˆ(2 C.

)ˆ3ˆ(2 B.

ˆ)62(ˆ2 A.

jyxiy

jiy

jiy

jyxiy

Page 54: Chapter 23: Electric Potential Section 23-1: Potential Difference

If the potential V of an array of charges versus the distance from the charges is as shown in graph 1, which graph A, B, C, D, or E shows the electric field E as a function of distance r?

Page 55: Chapter 23: Electric Potential Section 23-1: Potential Difference

If the potential V of an array of charges versus the distance from the charges is as shown in graph 1, which graph A, B, C, D, or E shows the electric field E as a function of distance r?

Page 56: Chapter 23: Electric Potential Section 23-1: Potential Difference

Which of the following statements is true?

A. The gradient of the potential must have a larger magnitude at a place where the electric field is stronger.

B. The gradient of the potential must have a smaller magnitude at a place where the electric field is stronger.

C. The potential must be larger at a place where the electric field is stronger.

D. The potential must be smaller at a place where the electric field is stronger.

Page 57: Chapter 23: Electric Potential Section 23-1: Potential Difference

Which of the following statements is true?

A. The gradient of the potential must have a larger magnitude at a place where the electric field is stronger.

B. The gradient of the potential must have a smaller magnitude at a place where the electric field is stronger.

C. The potential must be larger at a place where the electric field is stronger.

D. The potential must be smaller at a place where the electric field is stronger.

Page 58: Chapter 23: Electric Potential Section 23-1: Potential Difference

Chapter 23: Electric Potential

Section 23-4: Calculations of V for Continuous Charge Distributions

Page 59: Chapter 23: Electric Potential Section 23-1: Potential Difference

Which graph A, B, C, D, or E that best represents the electric potential of a uniformly charged spherical shell as a function of the distance from the center of the shell?

Page 60: Chapter 23: Electric Potential Section 23-1: Potential Difference

Which graph A, B, C, D, or E that best represents the electric potential of a uniformly charged spherical shell as a function of the distance from the center of the shell?

Page 61: Chapter 23: Electric Potential Section 23-1: Potential Difference

Which graph A, B, C, D, or E best represents the electric potential near an infinite plane of charge?

Page 62: Chapter 23: Electric Potential Section 23-1: Potential Difference

Which graph A, B, C, D, or E best represents the electric potential near an infinite plane of charge?

Page 63: Chapter 23: Electric Potential Section 23-1: Potential Difference

Chapter 23: Electric Potential

Section 23-5: Equipotential Surfaces

Page 64: Chapter 23: Electric Potential Section 23-1: Potential Difference

Which of the following statements regarding potential is true?

a. The units of potential are N/C.

b. Potential is a vector quantity.

c. Equipotential surfaces are at right angles to lines of electric force.

d. Potential differences can be measured directly with a ballistic galvanometer.

e. Equipotential surfaces for an isolated point charge are cubes concentric with the charge.

Page 65: Chapter 23: Electric Potential Section 23-1: Potential Difference

Which of the following statements regarding potential is true?

A. The units of potential are N/C.

B. Potential is a vector quantity.

C. Equipotential surfaces are at right angles to lines of electric force.

D. Potential differences can be measured directly with a ballistic galvanometer.

E. Equipotential surfaces for an isolated point charge are cubes concentric with the charge.

Page 66: Chapter 23: Electric Potential Section 23-1: Potential Difference

The vector that best represents the direction of the electric field intensity at point x on the 20 V equipotential line is

correct. is theseof None E.

4 D.

3 C.

2 B.

1 A.

Page 67: Chapter 23: Electric Potential Section 23-1: Potential Difference

The vector that best represents the direction of the electric field intensity at point x on the 20 V equipotential line is

correct. is theseof None E.

4 D.

3 C.

2 B.

1 A.

Page 68: Chapter 23: Electric Potential Section 23-1: Potential Difference

The vector that best represents the direction of the electric field intensity at point x on the 200 V equipotential line is

correct. is theseof None E.

4 D.

3 C.

2 B.

1 A.

Page 69: Chapter 23: Electric Potential Section 23-1: Potential Difference

The vector that best represents the direction of the electric field intensity at point x on the 200 V equipotential line is

correct. is theseof None E.

4 D.

3 C.

2 B.

1 A.

Page 70: Chapter 23: Electric Potential Section 23-1: Potential Difference

Two charged metal spheres are connected by a wire. Sphere A is larger than sphere B, as shown. The magnitude of the electric potential of sphere A

a. is greater than that at the surface of sphere B.

b. is less than that at the surface of sphere B.

c. is the same as that at the surface of sphere B.

Page 71: Chapter 23: Electric Potential Section 23-1: Potential Difference

Two charged metal spheres are connected by a wire. Sphere A is larger than sphere B, as shown. The magnitude of the electric potential of sphere A

A. is greater than that at the surface of sphere B.

B. is less than that at the surface of sphere B.

C. is the same as that at the surface of sphere B.

Page 72: Chapter 23: Electric Potential Section 23-1: Potential Difference

The potential on the surface of a solid conducting sphere of radius r = 20 cm is 100 V. The potential at r = 10 cm is

A. 100 V.

B. 50 V.

C. 25 V.

D. Zero.

E. Cannot be determined.

Page 73: Chapter 23: Electric Potential Section 23-1: Potential Difference

The potential on the surface of a solid conducting sphere of radius r = 20 cm is 100 V. The potential at r = 10 cm is

A. 100 V.

B. 50 V.

C. 25 V.

D. Zero.

E. Cannot be determined.

Page 74: Chapter 23: Electric Potential Section 23-1: Potential Difference

When a small, positively charged metal ball comes in contact with the interior of a positively charged metal shell,

a. the charge on the ball becomes negative.

b. the amount of positive charge on the ball increases.

c. the positive charge on the shell decreases.

d. the charge on the shell and on the ball reach the same value.

e. the ball loses all of its excess charge.

Page 75: Chapter 23: Electric Potential Section 23-1: Potential Difference

When a small, positively charged metal ball comes in contact with the interior of a positively charged metal shell,

A. the charge on the ball becomes negative.

B. the amount of positive charge on the ball increases.

C. the positive charge on the shell decreases.

D. the charge on the shell and on the ball reach the same value.

E. the ball loses all of its excess charge.

Page 76: Chapter 23: Electric Potential Section 23-1: Potential Difference

A solid conducting sphere of radius ra is placed concentrically inside a conducting spherical shell of inner radius rb1 and outer radius rb2. The inner sphere carries a charge Q while the outer sphere does not carry any net charge. The potential for rb1 r rb2 is

zero E.

D.

C.

B.

A.

2

1

r

kQ

r

kQ

r

kQ

r

kQ

b

b

a

Page 77: Chapter 23: Electric Potential Section 23-1: Potential Difference

A solid conducting sphere of radius ra is placed concentrically inside a conducting spherical shell of inner radius rb1 and outer radius rb2. The inner sphere carries a charge Q while the outer sphere does not carry any net charge. The potential for rb1 r rb2 is

zero E.

D.

C.

B.

A.

2

1

r

kQ

r

kQ

r

kQ

r

kQ

b

b

a

Page 78: Chapter 23: Electric Potential Section 23-1: Potential Difference

A metal ball of charge +Q is lowered into an isolated, uncharged metal shell and allowed to rest on the bottom of the shell. When the charges reach equilibrium,

A. the outside of the shell has a charge of –Q and the ball has a charge of +Q.

B. the outside of the shell has a charge of +Q and the ball has a charge of +Q.

C. the outside of the shell has a charge of zero and the ball has a charge of +Q.

D. the outside of the shell has a charge of +Q and the ball has zero charge.

E. the outside of the shell has a charge of +Q and the ball has a charge of –Q.

Page 79: Chapter 23: Electric Potential Section 23-1: Potential Difference

A metal ball of charge +Q is lowered into an isolated, uncharged metal shell and allowed to rest on the bottom of the shell. When the charges reach equilibrium,

A. the outside of the shell has a charge of –Q and the ball has a charge of +Q.

B. the outside of the shell has a charge of +Q and the ball has a charge of +Q.

C. the outside of the shell has a charge of zero and the ball has a charge of +Q.

D. the outside of the shell has a charge of +Q and the ball has zero charge.

E. the outside of the shell has a charge of +Q and the ball has a charge of –Q.

Page 80: Chapter 23: Electric Potential Section 23-1: Potential Difference

We give the same charge to a metal sphere of radius R and a metal cone of radius R and height 2R. The shaded regions in the figure are of equal area. Which region has the greatest surface charge density?

a. 1

b. 2

c. 3

d. 4

e. All have equal charge densities.

Page 81: Chapter 23: Electric Potential Section 23-1: Potential Difference

We give the same charge to a metal sphere of radius R and a metal cone of radius R and height 2R. The shaded regions in the figure are of equal area. Which region has the greatest surface charge density?

A. 1

B. 2

C. 3

D. 4

E. All have equal charge densities.

Page 82: Chapter 23: Electric Potential Section 23-1: Potential Difference

An electric charge q is placed on an isolated metal sphere of radius r1. If an uncharged sphere of radius r2 (with r2 > r1) is then connected to the first sphere, the spheres will have equal

A. and like charges on their surfaces.

B. electric fields.

C. potentials.

D. capacitances.

E. but opposite charges on their surfaces.

Page 83: Chapter 23: Electric Potential Section 23-1: Potential Difference

An electric charge q is placed on an isolated metal sphere of radius r1. If an uncharged sphere of radius r2 (with r2 > r1) is then connected to the first sphere, the spheres will have equal

A. and like charges on their surfaces.

B. electric fields.

C. potentials.

D. capacitances.

E. but opposite charges on their surfaces.

Page 84: Chapter 23: Electric Potential Section 23-1: Potential Difference

Dielectric breakdown occurs in the air at an electric field strength of Emax = 3.0 106 V/m. What is the maximum surface charge density that can be placed on a spherical conductor of radius 1.5 m before breakdown?

A. 2.7 10–5 C/m2

B. 1.2 10–5 C/m2

C. 8.1 10–5 C/m2

D. 8.6 10–6 C/m2

E. 1.8 10–5 C/m2

Page 85: Chapter 23: Electric Potential Section 23-1: Potential Difference

Dielectric breakdown occurs in the air at an electric field strength of Emax = 3.0 106 V/m. What is the maximum surface charge density that can be placed on a spherical conductor of radius 1.5 m before breakdown?

A. 2.7 10–5 C/m2

B. 1.2 10–5 C/m2

C. 8.1 10–5 C/m2

D. 8.6 10–6 C/m2

E. 1.8 10–5 C/m2

Page 86: Chapter 23: Electric Potential Section 23-1: Potential Difference

Chapter 23: Electric Potential

Section 23-6: Electrostatic Potential Energy

Page 87: Chapter 23: Electric Potential Section 23-1: Potential Difference

Which of the curves on the graph represents the electrostatic potential energy of a small negative charge plotted as a function of its distance from a positive point charge?

Page 88: Chapter 23: Electric Potential Section 23-1: Potential Difference

Which of the curves on the graph represents the electrostatic potential energy of a small negative charge plotted as a function of its distance from a positive point charge?

Page 89: Chapter 23: Electric Potential Section 23-1: Potential Difference

Which of the following statements is false?

A. The total work required to assemble a collection of discrete charges is the electrostatic potential energy of the system.

B. The potential energy of a pair of positively charged bodies is positive.

C. The potential energy of a pair of oppositely charged bodies is positive.

D. The potential energy of a pair of oppositely charged bodies is negative.

E. The potential energy of a pair of negatively charged bodies is negative.

Page 90: Chapter 23: Electric Potential Section 23-1: Potential Difference

Which of the following statements is false?

A. The total work required to assemble a collection of discrete charges is the electrostatic potential energy of the system.

B. The potential energy of a pair of positively charged bodies is positive.

C. The potential energy of a pair of oppositely charged bodies is positive.

D. The potential energy of a pair of oppositely charged bodies is negative.

E. The potential energy of a pair of negatively charged bodies is negative.

Page 91: Chapter 23: Electric Potential Section 23-1: Potential Difference

The work required to bring a positively charged body from very far away is greatest for which point?

Page 92: Chapter 23: Electric Potential Section 23-1: Potential Difference

The work required to bring a positively charged body from very far away is greatest for which point?

Page 93: Chapter 23: Electric Potential Section 23-1: Potential Difference

The electrostatic potential energy of a positively charged body is greatest at which point?

Page 94: Chapter 23: Electric Potential Section 23-1: Potential Difference

The electrostatic potential energy of a positively charged body is greatest at which point?

Page 95: Chapter 23: Electric Potential Section 23-1: Potential Difference

Three charges are brought from infinity and placed at the corner of an equilateral triangle. Which of the following statements is true?

A. The work required to assemble the charges is always positive.

B. The electrostatic potential energy of the system is always positive.

C. The electrostatic potential energy does not depend on the order the charges are placed at the corners.

D. The work required to assemble the charges depends on which charge is placed at which corner.

E. The electrostatic potential energy depends on which charge is placed at which corner.

Page 96: Chapter 23: Electric Potential Section 23-1: Potential Difference

Three charges are brought from infinity and placed at the corner of an equilateral triangle. Which of the following statements is true?

A. The work required to assemble the charges is always positive.

B. The electrostatic potential energy of the system is always positive.

C. The electrostatic potential energy does not depend on the order the charges are placed at the corners.

D. The work required to assemble the charges depends on which charge is placed at which corner.

E. The electrostatic potential energy depends on which charge is placed at which corner.

Page 97: Chapter 23: Electric Potential Section 23-1: Potential Difference

Calculate the work done to bring a charge,Q = 1 mC, from infinity and place it at a distance R = 10 cm along the axis of a thin uniformly charged ring with linear charge density λ = 10 C/m and radius R.

A. 564 J

B. 282 J

C. 127 J

D. 399 J

E. zero

QR

R

from infinity

Page 98: Chapter 23: Electric Potential Section 23-1: Potential Difference

Calculate the work done to bring a charge,Q = 1 mC, from infinity and place it at a distance R = 10 cm along the axis of a thin uniformly charged ring with linear charge density λ = 10 C/m and radius R.

A. 564 J

B. 282 J

C. 127 J

D. 399 J

E. zero

QR

R

from infinity

Page 99: Chapter 23: Electric Potential Section 23-1: Potential Difference

Calculate the work done to bring a charge, Q = 1 mC, from infinity and place it at a distance R = 10 cm along the axis of a uniformly charged disk with surface charge density σ = 10 C/m2 and radius R.

A. 78.9 J

B. 23.4 J

C. 56.5 J

D. 97.8 J

E. zero

QR

R

from infinity

Page 100: Chapter 23: Electric Potential Section 23-1: Potential Difference

Calculate the work done to bring a charge, Q = 1 mC, from infinity and place it at a distance R = 10 cm along the axis of a uniformly charged disk with surface charge density σ = 10 C/m2 and radius R.

A. 78.9 J

B. 23.4 J

C. 56.5 J

D. 97.8 J

E. zero

QR

R

from infinity