chapter 19 electric potential energy and the electric potential

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Chapter 19 Electric Potential Energy and the Electric Potential

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Page 1: Chapter 19 Electric Potential Energy and the Electric Potential

Chapter 19

Electric Potential Energy and the

Electric Potential

Page 2: Chapter 19 Electric Potential Energy and the Electric Potential

19.1 Potential Energy

BABAAB mghmghW GPEGPE

Page 3: Chapter 19 Electric Potential Energy and the Electric Potential

19.1 Potential Energy

Page 4: Chapter 19 Electric Potential Energy and the Electric Potential

19.1 Potential Energy

BAABW EPEEPE

Page 5: Chapter 19 Electric Potential Energy and the Electric Potential

19.2 The Electric Potential Difference

o

B

o

A

o

AB

qqq

W EPEEPE

The potential energy per unit chargeis called the electric potential.

Page 6: Chapter 19 Electric Potential Energy and the Electric Potential

19.2 The Electric Potential Difference

DEFINITION OF ELECTRIC POTENTIAL

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

oqV

EPE

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

o

AB

o

A

o

BAB q

W

qqVV

EPEEPE

o

AB

o q

W

qV

EPE

Page 7: Chapter 19 Electric Potential Energy and the Electric Potential

19.2 The Electric Potential Difference

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.

(a) Find the difference in EPE between thesepoints.

(b) Determine the potential difference betweenthese points.

BAABW EPEEPE

o

AB

o

A

o

BAB q

W

qqVV

EPEEPE

Page 8: Chapter 19 Electric Potential Energy and the Electric Potential

19.2 The Electric Potential Difference

BAABW EPEEPE (a)

J100.5EPEEPE 5 ABAB W

(b)

V 25C102.0

J100.56-

5

o

ABAB q

WVV

Page 9: Chapter 19 Electric Potential Energy and the Electric Potential

19.2 The Electric Potential Difference

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?

Page 10: Chapter 19 Electric Potential Energy and the Electric Potential

19.2 The Electric Potential Difference

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.

Page 11: Chapter 19 Electric Potential Energy and the Electric Potential

19.2 The Electric Potential Difference

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

EPEkxmghImvE 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

Page 12: Chapter 19 Electric Potential Energy and the Electric Potential

19.2 The Electric Potential Difference

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 frompoint A and accelerates horizontally until it reaches point B. The only force actingon the particle is the electric force, and the electric potential at A is 25V greater thanat C. (a) What is the speed of the particle at point B? (b) If the same particle had anegative charge and were released from point B, what would be its speed at A?

Page 13: Chapter 19 Electric Potential Energy and the Electric Potential

19.2 The Electric Potential Difference

AABB EPEmvEPEmv 2212

21

BAAB EPEEPEmvmv 2212

21

BAoAB VVqmvmv 2212

21

Page 14: Chapter 19 Electric Potential Energy and the Electric Potential

19.2 The Electric Potential Difference

BAoB VVqmv 221(a)

sm1.9kg108.1V 25C100.32

2

55

mVVqv BAoB

sm1.9kg108.1V 25C100.32

2

55

mVVqv BAoA(a)

Page 15: Chapter 19 Electric Potential Energy and the Electric Potential

19.3 The Electric Potential Difference Created by Point Charges

B

o

A

oAB r

kqq

r

kqqW

BAo

ABAB r

kq

r

kq

q

WVV

Potential of apoint charge r

kqV

Page 16: Chapter 19 Electric Potential Energy and the Electric Potential

19.3 The Electric Potential Difference Created by Point Charges

Example 5 The Potential of a Point Charge

Using 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.

Page 17: Chapter 19 Electric Potential Energy and the Electric Potential

19.3 The Electric Potential Difference Created by Point Charges

V 300m 2.1

C100.4CmN1099.8 8229

r

kqV

(a)

(b)

V 300V

Page 18: Chapter 19 Electric Potential Energy and the Electric Potential

19.3 The Electric Potential Difference Created by Point Charges

Example 6 The Total Electric Potential

At locations A and B, find the total electric potential.

Page 19: Chapter 19 Electric Potential Energy and the Electric Potential

19.3 The Electric Potential Difference Created by Point Charges

V 240

m 60.0

C100.8CmN1099.8

m 20.0

C100.8CmN1099.8 82298229

AV

V 0

m 40.0

C100.8CmN1099.8

m 40.0

C100.8CmN1099.8 82298229

BV

Page 20: Chapter 19 Electric Potential Energy and the Electric Potential

19.3 The Electric Potential Difference Created by Point Charges

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 21: Chapter 19 Electric Potential Energy and the Electric Potential

19.4 Equipotential Surfaces and Their Relation to the Electric Field

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

r

kqV

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

Page 22: Chapter 19 Electric Potential Energy and the Electric Potential

19.4 Equipotential Surfaces and Their Relation to the Electric Field

The electric field created by any chargeor group of charges is everywhere perpendicular to the associatedequipotential surfaces and points inthe direction of decreasing potential.

Page 23: Chapter 19 Electric Potential Energy and the Electric Potential

19.4 Equipotential Surfaces and Their Relation to the Electric Field

Page 24: Chapter 19 Electric Potential Energy and the Electric Potential

19.4 Equipotential Surfaces and Their Relation to the Electric Field

s

VE

Page 25: Chapter 19 Electric Potential Energy and the Electric Potential

19.4 Equipotential Surfaces and Their Relation to the Electric Field

Example 9 The Electric Field and PotentialAre Related

The 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.

Page 26: Chapter 19 Electric Potential Energy and the Electric Potential

19.4 Equipotential Surfaces and Their Relation to the Electric Field

mV100.2m 0.032

V 64 3

s

VE

m105.1mV100.2

V 0.3 33

E

Vs

Page 27: Chapter 19 Electric Potential Energy and the Electric Potential

19.5 Capacitors and Dielectrics

A parallel plate capacitor consists of two metal plates, one carrying charge +q andthe other carrying charge –q.

It is common to fill the region betweenthe plates with an electrically insulatingsubstance called a dielectric.

Page 28: Chapter 19 Electric Potential Energy and the Electric Potential

19.5 Capacitors and Dielectrics

THE RELATION BETWEEN CHARGE AND POTENTIALDIFFERENCE FOR A CAPACITOR

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

CVq The capacitance C is the proportionality constant.

SI Unit of Capacitance: coulomb/volt = farad (F)

Page 29: Chapter 19 Electric Potential Energy and the Electric Potential

19.5 Capacitors and Dielectrics

THE DIELECTRIC CONSTANT

If a dielectric is inserted between the plates of a capacitor, the capacitance can increase markedly.

Dielectric constantE

Eo

Page 30: Chapter 19 Electric Potential Energy and the Electric Potential

19.5 Capacitors and Dielectrics

Page 31: Chapter 19 Electric Potential Energy and the Electric Potential

19.5 Capacitors and Dielectrics

THE CAPACITANCE OF A PARALLEL PLATE CAPACITOR

d

VEE o

AqE oo

Vd

Aq o

d

AC o

Parallel plate capacitorfilled with a dielectric

Page 32: Chapter 19 Electric Potential Energy and the Electric Potential

19.5 Capacitors and Dielectrics

Conceptual Example 11 The Effect of a Dielectric When a Capacitor Has a Constant Charge

An empty capacitor is connected to a battery and charged up.The capacitor is then disconnected from the battery, and a slabof dielectric material is inserted between the plates. Does the voltage across the plates increase, remain the same, or decrease?

q=CV the voltage V across the plates must decrease in order to remain unchanged

Page 33: Chapter 19 Electric Potential Energy and the Electric Potential

19.5 Capacitors and Dielectrics

Example 12 A Computer Keyboard

One common kind of computer keyboard is based on the idea of capacitance. Each key is mounted on one end of a plunger, the other end being attached to a movable metal plate. The movable plate and the fixed plateform a capacitor. When the key is pressed, the capacitance increases. The change in capacitance isdetected, thereby recognizing the key which has been pressed.

The separation between the plates is 5.00 mm, but is reduced to 0.150 mm when a key is pressed. Theplate area is 9.50x10-5m2 and the capacitor is filled witha material whose dielectric constant is 3.50.

Determine the change in capacitance detected by the computer.

Page 34: Chapter 19 Electric Potential Energy and the Electric Potential

19.5 Capacitors and Dielectrics

F106.19

m100.150

m1050.9mNC1085.850.3 123-

252212

d

AC o

F10589.0

m105.00

m1050.9mNC1085.850.3 123-

252212

d

AC o

F100.19 12C

Page 35: Chapter 19 Electric Potential Energy and the Electric Potential

19.5 Capacitors and Dielectrics

ENERGY STORAGE IN A CAPACITOR

221Energy CV

2

21Energy Ed

d

Ao

221

VolumeEnergydensity Energy Eo

Ad Volume

Page 36: Chapter 19 Electric Potential Energy and the Electric Potential

19.6 Biomedical Applications of Electrical Potential Differences

Page 37: Chapter 19 Electric Potential Energy and the Electric Potential

19.6 Biomedical Applications of Electrical Potential Differences

Page 38: Chapter 19 Electric Potential Energy and the Electric Potential

19.6 Biomedical Applications of Electrical Potential Differences

Page 39: Chapter 19 Electric Potential Energy and the Electric Potential

19.6 Biomedical Applications of Electrical Potential Differences

Page 40: Chapter 19 Electric Potential Energy and the Electric Potential

19.6 Biomedical Applications of Electrical Potential Differences

Page 41: Chapter 19 Electric Potential Energy and the Electric Potential

19.6 Biomedical Applications of Electrical Potential Differences