ch19 electric potential energy and electric potential

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Chapter 19 Electric Potential Energy and Electric Potential

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Page 1: Ch19 Electric Potential Energy and Electric Potential

Chapter 19

Electric Potential Energy

and Electric Potential

Page 2: Ch19 Electric Potential Energy and Electric Potential

AP Learning ObjectivesELECTRICITY AND MAGNETISM Electrostatics

• Electric field and electric potential (including point charges)

• Students should understand the concept of electric field, so they can:

• Define it in terms of the force on a test charge.

• Describe and calculate the electric field of a single point charge.

• Calculate the magnitude and direction of the electric field produced by two or more point charges.

• Calculate the magnitude and direction of the force on a positive or negative charge placed in a specified field.

• Interpret an electric field diagram.

• Analyze the motion of a particle of specified charge and mass in a uniform electric field.

Page 3: Ch19 Electric Potential Energy and Electric Potential

AP Learning Objectives• Students should understand the concept of electric potential,

so they can:• Determine the electric potential in the vicinity of one or

more point charges.• Calculate the electrical work done on a charge or use

conservation of energy to determine the speed of a charge that moves through a specified potential difference.

• Determine the direction and approximate magnitude of the electric field at various positions given a sketch of equipotentials.

• Calculate the potential difference between two points in a uniform electric field, and state which point is at the higher potential.

• Calculate how much work is required to move a test charge from one location to another in the field of fixed point charges.

• Calculate the electrostatic potential energy of a system of two or more point charges, and calculate how much work is required to establish the charge system.

Page 4: Ch19 Electric Potential Energy and Electric Potential

Table of Contents

1. Potential Energy

2. The Electric Potential Difference

3. The Electric Potential Difference Created by Point

Charges

4. Equipotential Surfaces and Their Relation to the electric

Field

5. Capacitors and Dielectrics

6. Biomedical Applications of Electric Potential Differences

(AP?)

Page 5: Ch19 Electric Potential Energy and Electric Potential

Chapter 19:Electric Potential Energy

and Electric Potential

Section 1:

Potential Energy

Page 6: Ch19 Electric Potential Energy and Electric Potential

From Gravity

• Energy based on position

• Change in position

• Change in Energy

• Work

2

2

1vmhmg

Potential Energy

BAAB mghmghW

Page 7: Ch19 Electric Potential Energy and Electric Potential

Electrical Potential Energy Same Effect for Electric Force Energy present based on position

• Change in position

• Change in Energy

• Remember, unless otherwise stated, test charge is positive

FdU E 2

21

4

1

r

qqF

oE

rr

qqU

oE

221

4

1

r

qqU

oE

21

4

1

Page 8: Ch19 Electric Potential Energy and Electric Potential

19.1.1. Two electrons are separated by a distance R. If the distance between the charges is increased to 2R, what happens to the total electric potential energy of the system?

a) The total electric potential energy of the system would increase to four times its initial value.

b) The total electric potential energy of the system would increase to two times its initial value.

c) The total electric potential energy of the system would remain the same.

d) The total electric potential energy of the system would decrease to one half its initial value.

e) The total electric potential energy of the system would decrease to one fourth its initial value.

Page 9: Ch19 Electric Potential Energy and Electric Potential

19.1.2. The electric potential energy for two positive charges of magnitude q and separated by a distance r is EPE1. What will the electric potential energy be if one of the charges is completely removed and replaced by a negative charge of the same magnitude?

a) U2 = 2 U1

b) U2 = U1

c) U2 = U1

d) U2 = 2 U1

e) There is no way to determine this without knowing the value of q.

Page 10: Ch19 Electric Potential Energy and Electric Potential

Chapter 19:Electric Potential Energy

and Electric Potential

Section 2:

The Electric Potential Difference

Page 11: Ch19 Electric Potential Energy and Electric Potential

Electric Potential

Electric Potential is hard to

understand, but easy to

measure.

The potential energy per unit

charge

Related to electric potential

energy and the electric field

Commonly called “Voltage”

Measured in volts (1V = 1 J/C)

Page 12: Ch19 Electric Potential Energy and Electric Potential

The electric potential at a given point is the electric potential energy of a small test charge divided by the charge itself:

SI Unit of Electric Potential: joule/coulomb = volt (V)

o

AB

o

A

o

BAB q

W

qqVV

UU

o

AB

o q

W

qV

U

DEFINITION OF ELECTRIC POTENTIAL

o

E

q

UV

Page 13: Ch19 Electric Potential Energy and Electric Potential

Example 1 Work, Potential Energy, and Electric Potential

The work done by the electric force as the test charge (+2.0x10-6C) moves from A toB is +5.0x10-5J.Find the difference in EPE between thesepoints.Determine the potential difference betweenthese points.

BAABW UU

o

AB

o

A

o

B

q

W

qqV

UU

ABW

C102.0

J100.56-

5

V

J100.5 5(a)

(b)

V 25

Page 14: Ch19 Electric Potential Energy and Electric Potential

Conceptual Example 2 The Accelerations of Positive and Negative Charges

A positive test charge is released from A and accelerates towards B. Uponreaching B, the test charge continues to accelerate toward C. Assuming thatonly motion along the line is possible, what will a negative test charge do whenreleased from rest at B?

Negative charge will accelerate towards A

Page 15: Ch19 Electric Potential Energy and Electric Potential

A positive charge accelerates from a region of higher electric potentialtoward a region of lower electric potential.

A negative charge accelerates from a region of lower potential towarda region of higher potential.

Explanation

Page 16: Ch19 Electric Potential Energy and Electric Potential

We now include electric potential energy as part of the total energy that an object can have:

EUkxmghImvE 2212

212

21

One electron volt is the magnitude of the amount by which the potentialenergy of an electron changes when the electron moves through a potentialdifference of one volt.

V1060.1eV 1 19

Energy Conservation

Page 17: Ch19 Electric Potential Energy and Electric Potential

Example 4 The Conservation of Energy

A particle has a mass of 1.8x10-5kg and a charge of +3.0x10-5C. It is released from point A and accelerates horizontally until it reaches point B. The only force acting on the particle is the electric force, and the electric potential at A is 25V greater than at B. (a) What is the speed of the particle at point B? (b) If the same particle had a negative charge and were released from point B, what would be its speed at A?

AABB UmvUmv 2212

21

BAB UUmv 221

BAoB VVqmv 221

qVU

kg108.1V 25C100.32 55 Bv

mVVqv BAoB 2

sm1.9BvPart b) same speed, opposite direction

Page 18: Ch19 Electric Potential Energy and Electric Potential

19.2.1. Which one of the following statements best explains why it is possible to define an electrostatic potential in a region of space that contains an electrostatic field?

a) The work required to bring two charges together is independent of the path taken.

b) A positive charge will gain kinetic energy as it approaches a negative charge.

c) Like charges repel one another and unlike charges attract one another.

d) Work must be done to bring two positive charges closer together.

e) A negative charge will gain kinetic energy as it moves away from another negative charge.

Page 19: Ch19 Electric Potential Energy and Electric Potential

19.2.2. Four point charges are individually brought from infinity and placed at the corners of a square as shown in the figure. Each charge has the identical value +Q. The length of the diagonal of the square is 2a. What is the electric potential at P, the center of the square?

a)

b)

c) zero volts

d)

e)

a

kQ

4

a

kQ

a

kQ2

a

kQ4

Page 20: Ch19 Electric Potential Energy and Electric Potential

Chapter 19:Electric Potential Energy

and Electric Potential

Section 3:

The Electric Potential Difference Created by Point Charges

Page 21: Ch19 Electric Potential Energy and Electric Potential

Difference in Potential What is the potential difference

as a particle moves in an Electric Field

• due to the electric force as the point charge moves from A to B

Since the force is a function of distance must use calculus:

drr

kqqW

B

A

r

r

o2

B

A

r

r

o r

drkqqW

2

Page 22: Ch19 Electric Potential Energy and Electric Potential

B

o

A

o

r

kqq

r

kqq

o

AB

q

WV

Total Potential of All point charges

i i

i

r

qkV

Difference in Potential

xx

dx 12

B

A

r

r

o r

drkqqW

2

WU

oq

UV

BA r

kq

r

kq

Page 23: Ch19 Electric Potential Energy and Electric Potential

Example 5 The Potential of a Point ChargeUsing a zero reference potential at infinity,determine the amount by which a point chargeof 4.0x10-8C alters the electric potential at a spot 1.2m away when the charge is (a) positive and (b) negative.

r

kqV

(a)

(b)

V 300V

m 2.1

C100.4CmN1099.8 8229 V

V 300V

Page 24: Ch19 Electric Potential Energy and Electric Potential

Example 6 The Total Electric PotentialAt locations A and B, find the total electric potential.

m 60.0

C100.8CmN1099.8

m 20.0

C100.8CmN1099.8 82298229

AV

m 40.0

C100.8CmN1099.8

m 40.0

C100.8CmN1099.8 82298229

BV

i i

i

r

qkV

V 240

V 0

Page 25: Ch19 Electric Potential Energy and Electric Potential

Conceptual Example 7 Where is the Potential Zero?Two point charges are fixed in place. The positive charge is +2q and thenegative charge is –q. On the line that passes through the charges, how many places are there at which the total potential is zero?

Page 26: Ch19 Electric Potential Energy and Electric Potential

19.3.1. Consider the four arrangements of three point charges. Rank the values of the total electric potential at point P in each case in descending order (with the largest first).

a) VA > VD > VC > VB

b) VC > VB > VD > VA

c) VC > VD > VA > VB

d) VB > VC > VB > VA

e) VD > VB > VA > VC

Page 27: Ch19 Electric Potential Energy and Electric Potential

19.3.2. Two point charges lie along the x axis. One charge, located at the origin, has a magnitude +2q. The other charge of unknown magnitude and sign is located at x = 5 units. If the electric potential at x = 4 units is equal to zero volts, what is the magnitude and sign of the second point charge?

a) q/2

b) q/4

c) 2q

d) +q/2

e) +2q

Page 28: Ch19 Electric Potential Energy and Electric Potential

Chapter 19:Electric Potential Energy

and Electric Potential

Section 4:

Equipotential Difference Created by Point Charges

Page 29: Ch19 Electric Potential Energy and Electric Potential

r

kqV

Equipotential Surfaces An equipotential surface

is a surface on which the electric potential is the same everywhere.

The net electric force does no work on a charge as it moves on an equipotential surface.

Page 30: Ch19 Electric Potential Energy and Electric Potential

Electric Field and Equipotential Surfaces

The electric field created by

any charge or group of

charges is everywhere

perpendicular to the

associated equipotential

surfaces and points in the

direction of decreasing

potential.

Page 31: Ch19 Electric Potential Energy and Electric Potential

Equipotential Surfaces and Their Relation to the Electric Field

Page 32: Ch19 Electric Potential Energy and Electric Potential

d

VEavg

In Parallel Plate Capacitors

d

Page 33: Ch19 Electric Potential Energy and Electric Potential

Example 9 The Electric Field and PotentialAre RelatedThe plates of the capacitor are separated bya distance of 0.032 m, and the potential differencebetween them is VB-VA=-64V. Between thetwo equipotential surfaces shown in color, thereis a potential difference of -3.0V. Find the spacingbetween the two colored surfaces.

ABd

VE

E

Vd

m 0.032

V 64 mV100.2 3

mV100.2

V 0.33

m105.1 3

dAB

Page 34: Ch19 Electric Potential Energy and Electric Potential

19.4.1. A proton is moved from point B to point A in an electric field as shown. As a result of its movement, its potential increases to V. If three protons are moved from point B to A, how much will the electric potential of the protons increase?

a) V/9

b) V/3

c) V

d) 3V

e) 9V

Page 35: Ch19 Electric Potential Energy and Electric Potential

19.4.2. Which one of the following statements concerning electrostatic situations is false?

a) No work is required to move a charge along an equipotential surface.

b) If the electric potential with a region of space is zero volts, the electric field within that region must also be zero V/m.

c) If a charge is moved along an equipotential surface, there is no component of the force acting along the charges’ path.

d) The electric field is always perpendicular to equipotential surfaces.

e) The electric field is zero V/m everywhere inside a conductor.

Page 36: Ch19 Electric Potential Energy and Electric Potential

19.4.3. The drawing shows three point charges of equal magnitude, but one is positive (shown in blue) and two are negative (shown in yellow). Some of the equipotential lines surrounding these charges are shown and five are labeled using letters A, B, C, D, and E. At which of the labeled points will an electron have the greatest electric potential energy?

a) A

b) B

c) C

d) D

e) E

Page 37: Ch19 Electric Potential Energy and Electric Potential

19.4.4. The drawing shows three point charges of equal magnitude, but one is positive (shown in blue) and two are negative (shown in yellow). Some of the equipotential lines surrounding these charges are shown and five are labeled using letters A, B, C, D, and E. What is the direction of the electric field at the location of the letter “D?”

a) perpendicular to the equipotential line marked “D” and directed toward the negative charge closest to it

b) parallel to the equipotential line marked “D” and directed toward the location of the letter “C”

c) perpendicular to the equipotential line marked “D” and directed toward the location of the letter “A”

d) toward the negative charge in the lower part of the drawing

e) toward the positive charge

Page 38: Ch19 Electric Potential Energy and Electric Potential

Chapter 19:Electric Potential Energy

and Electric Potential

Section 5:

Capacitors & Dielectrics

Page 39: Ch19 Electric Potential Energy and Electric Potential

Capacitors

A capacitor is a device that can store potential energy

Usually they are build by placing two conductors near

each other, without touching

For AP, we will only look at air separating the two plates

• We can make capacitors with other insulators

separating the two conductors.

Page 40: Ch19 Electric Potential Energy and Electric Potential

Capacitors and Dielectrics

A parallel plate capacitor consists

of two metal plates, one carrying

charge +q and the other carrying

charge –q.

It is common to fill the region

between the plates with an

electrically insulating substance

called a dielectric.

Page 41: Ch19 Electric Potential Energy and Electric Potential

The magnitude of the charge in each place of the capacitor is directly proportional to the magnitude of the potential difference between the plates.

The capacitance C is the proportionality constant.

SI Unit of Capacitance:

coulomb/volt = farad (F)

VQ

THE RELATION BETWEEN CHARGE AND POTENTIAL DIFFERENCE FOR A CAPACITOR

V

QC

CVQ

Page 42: Ch19 Electric Potential Energy and Electric Potential

Capacitance To determine the capacitance, we

must look at how easily the charge can flow between the plates

We will assume that air has the same permittivity as a vacuum

d

AC o

Page 43: Ch19 Electric Potential Energy and Electric Potential

ENERGY STORAGE IN A CAPACITOR

The energy stored on a capacitor can be

expressed in terms of the work done by the

battery.

Voltage represents energy per unit charge,

• so the work to move a charge element dq

from the negative plate to the positive

plate is equal to V dq,

• where V is the voltage on the

capacitor.

The voltage V is proportional to the amount

of charge which is already on the capacitor.

WdU

dqC

qdU

VdqdU

Page 44: Ch19 Electric Potential Energy and Electric Potential

ENERGY STORAGE IN A CAPACITOR

If Q is the amount of charge stored when the whole battery voltage appears across the capacitor, then the stored energy is obtained from the integral:

Since Q=CV, we can rewrite this expression:

Q

C dqC

qU

0 C

Q2

2

1

2

2

1

2

1CVQVUC

Q

dqqC 0

1

Page 45: Ch19 Electric Potential Energy and Electric Potential

19.5.1. An electrical outlet has two vertical slots and a hole into which a three prong plug may be inserted. The maximum potential difference between the two vertical slots is 120 volts. The hole is connected to earth ground. Estimate the maximum electric field that exists between the two vertical slots.

a) 240 V/m

b) 4800 V/m

c) 9200 V/m

d) 120 V/m

e) 6300 V/m

Page 46: Ch19 Electric Potential Energy and Electric Potential

19.5.2. The plates of an isolated parallel plate capacitor with a capacitance C carry a charge Q. What is the capacitance of the capacitor if the charge is increased to 4Q?

a) C/2

b) C/4

c) 4C

d) 2C

e) C

Page 47: Ch19 Electric Potential Energy and Electric Potential

19.5.3. A parallel plate capacitor with plates of area A and plate separation d is charged so that the potential difference between its plates is V. If the capacitor is then isolated and its plate separation is increased to 2d, what is the potential difference between the plates?

a) 4V

b) 2V

c) V

d) 0.5V

e) 0.25V

Page 48: Ch19 Electric Potential Energy and Electric Potential

19.5.4. The plates of an isolated parallel plate capacitor with a capacitance C carry a charge Q. The plate separation is d. Initially, the space between the plates contains only air. Then, an isolated metal sheet of thickness 0.5d is inserted between, but not touching, the plates. How does the potential difference between the plates change as a result of inserting the metal sheet?

a) The potential difference will decrease.

b) The potential difference will not be affected.

c) The potential difference will increase.

d) The potential difference will be zero volts.

Page 49: Ch19 Electric Potential Energy and Electric Potential

19.5.5. The plates of an isolated parallel plate capacitor with a capacitance C carry a charge Q. The plate separation is d. Initially, the space between the plates contains only air. Then, a Teflon ( = 2.1) sheet of thickness 0.5d is inserted between, but not touching, the plates. How does the electric field between the plates change as a result of inserting the Teflon sheet?

a) The electric field will decrease to approximately one-half its initial value.

b) The electric field will not be affected.

c) The electric field will increase to approximately twice its initial value.

d) The electric field will be zero volts per meter.

Page 50: Ch19 Electric Potential Energy and Electric Potential

19.5.6. The plates of an isolated parallel plate capacitor are separated by a distance d and carry charge of magnitude q. The distance between the plates is then reduced to d/2. How is the energy stored in the capacitor affected by this change?

a) The energy increases to twice its initial value.

b) The energy increases to four times its initial value.

c) The energy is not affected by this change.

d) The energy decreases to one fourth of its initial value.

e) The energy decreases to one half of its initial value.

Page 51: Ch19 Electric Potential Energy and Electric Potential

19.5.7. A parallel plate capacitor is connected to a battery that maintains a constant potential difference across the plates. Initially, the space between the plates contains only air. Then, a Teflon ( = 2.1) sheet is inserted between, but not touching, the plates. How does the stored energy of the capacitor change as a result of inserting the Teflon sheet?

a) The energy will decrease.

b) The energy will not be affected.

c) The energy will increase.

d) The energy will be zero joules.

Page 52: Ch19 Electric Potential Energy and Electric Potential