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© 2012 Pearson Education, Inc. { { Chapter 23 Chapter 23 Electric Potential (cont.) Electric Potential (cont.)

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Chapter 23. Electric Potential (cont.). Q23.5. The electric potential energy of two point charges approaches zero as the two point charges move farther away from each other. - PowerPoint PPT Presentation

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Page 1: Chapter 23

© 2012 Pearson Education, Inc.

{{Chapter 23Chapter 23

Electric Potential (cont.)Electric Potential (cont.)

Page 2: Chapter 23

© 2012 Pearson Education, Inc.

Q23.5

A. positive.

B. negative.

C. zero.

D. unknown – there is not enough information given to decide.

Charge #1

Charge #2

Charge #3

+q

+q

–qx

y

The electric potential energy of two point charges approaches zero as the two point charges move farther away from each other.

If the three point charges shown here lie at the vertices of an equilateral triangle, the electric potential energy of the system of three charges is

Page 3: Chapter 23

© 2012 Pearson Education, Inc.

A. positive.

B. negative.

C. zero.

D. unknown – there is not enough information given to decide.

The electric potential energy of two point charges approaches zero as the two point charges move farther away from each other.

If the three point charges shown here lie at the vertices of an equilateral triangle, the electric potential energy of the system of three charges is

A23.5

Charge #1

Charge #2

Charge #3

+q

+q

–qx

y

Page 4: Chapter 23

© 2012 Pearson Education, Inc.

A. positive.

B. negative.

C. zero.

D. unknown – there is not enough information given to decide.

The electric potential energy of two point charges approaches zero as the two point charges move farther away from each other.

If the three point charges shown here lie at the vertices of an equilateral triangle, the electric potential energy of the system of three charges is

Q23.6

Charge #1

Charge #2

Charge #3

+q

–q

–qx

y

Page 5: Chapter 23

© 2012 Pearson Education, Inc.

A. positive.

B. negative.

C. zero.

D. unknown – there is not enough information given to decide.

The electric potential energy of two point charges approaches zero as the two point charges move farther away from each other.

If the three point charges shown here lie at the vertices of an equilateral triangle, the electric potential energy of the system of three charges is

A23.6

Charge #1

Charge #2

Charge #3

+q

–q

–qx

y

Page 6: Chapter 23

© 2012 Pearson Education, Inc.

The electric potential due to a point charge approaches zero as you move farther away from the charge.

If the three point charges shown here lie at the vertices of an equilateral triangle, the electric potential at the center of the triangle is

Q23.7

A. positive.

B. negative.

C. zero.

D. unknown – there is not enough information given to decide.

Charge #1

Charge #2

Charge #3

+q

+q

–qx

y

Page 7: Chapter 23

© 2012 Pearson Education, Inc.

The electric potential due to a point charge approaches zero as you move farther away from the charge.

If the three point charges shown here lie at the vertices of an equilateral triangle, the electric potential at the center of the triangle is

A23.7

A. positive.

B. negative.

C. zero.

D. unknown – there is not enough information given to decide.

Charge #1

Charge #2

Charge #3

+q

+q

–qx

y

Page 8: Chapter 23

© 2012 Pearson Education, Inc.

The electric potential due to a point charge approaches zero as you move farther away from the charge.

If the three point charges shown here lie at the vertices of an equilateral triangle, the electric potential at the center of the triangle is

Q23.8

A. positive.

B. negative.

C. zero.

D. unknown – there is not enough information given to decide.

Charge #1

Charge #2

Charge #3

+q

–q

–qx

y

Page 9: Chapter 23

© 2012 Pearson Education, Inc.

The electric potential due to a point charge approaches zero as you move farther away from the charge.

If the three point charges shown here lie at the vertices of an equilateral triangle, the electric potential at the center of the triangle is

A23.8

A. positive.

B. negative.

C. zero.

D. unknown – there is not enough information given to decide.

Charge #1

Charge #2

Charge #3

+q

–q

–qx

y

Page 10: Chapter 23

© 2012 Pearson Education, Inc.

Consider a point P in space where the electric potential is zero. Which statement is correct?

Q23.9

A. A point charge placed at P would feel no electric force.

B. The electric field at points around P is directed toward P.

C. The electric field at points around P is directed away from P.

D. none of the above can possibly be true

E. not enough information given to decide

Page 11: Chapter 23

© 2012 Pearson Education, Inc.

Consider a point P in space where the electric potential is zero. Which statement is correct?

A23.9

A. A point charge placed at P would feel no electric force.

B. The electric field at points around P is directed toward P.

C. The electric field at points around P is directed away from P.

D. none of the above can possibly be true

E. not enough information given to decide

Page 12: Chapter 23

© 2012 Pearson Education, Inc.

Equipotential surfaces and field linesEquipotential surfaces and field lines• An An equipotential surfaceequipotential surface is a surface on which the is a surface on which the

electric potential is the same at every point.electric potential is the same at every point.• Figure 23.23 below shows the equipotential Figure 23.23 below shows the equipotential

surfaces and electric field lines for assemblies of surfaces and electric field lines for assemblies of point charges.point charges.

• Field lines and equipotential surfaces are always Field lines and equipotential surfaces are always mutually perpendicular.mutually perpendicular.

Page 13: Chapter 23

© 2012 Pearson Education, Inc.

Equipotentials and conductorsEquipotentials and conductors• When all charges are at rest:When all charges are at rest:

the surface of a conductor is always an equipotential the surface of a conductor is always an equipotential surface.surface.

the electric field just outside a conductor is always the electric field just outside a conductor is always perpendicular to the surface (see figures below).perpendicular to the surface (see figures below).

the entire solid volume of a conductor is at the same the entire solid volume of a conductor is at the same potential.potential.