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Chapter 19
Electric Potential Energy
and the
Electric Potential
19.1 Potential Energy
BABAAB mghmghW GPEGPE −=−=
19.1 Potential Energy
19.1 Potential Energy
BAABW EPEEPE −=
19.2 The Electric Potential Difference
o
B
o
A
o
AB
qqq
W EPEEPE
−=
The potential energy per unit charge
is called 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:
oq
V
EPE
=
SI Unit of Electric Potential: joule/coulomb = volt (V)
o
AB
o
A
o
B
AB
q
W
qq
VV
−
=−=−
EPEEPE
( )
o
AB
o q
W
q
V
−
=
∆
=∆
EPE
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 (+2.0x10-6
C) moves from A to
B is +5.0x10-5
J.
(a) Find the difference in EPE between these
points.
(b) Determine the electrical potential difference
between these points.
BAABW EPEEPE −=
o
AB
o
A
o
B
AB
q
W
qq
VV
−
=−=−
EPEEPE
19.2 The Electric Potential Difference
BAABW EPEEPE −=(a)
J100.5EPEEPE 5−
×−=−=− ABAB W
(b)
V25
C102.0
J100.5
6-
5
−=
×
×−
=
−
=−
−
o
AB
AB
q
W
VV
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. Upon
reaching B, the test charge continues to accelerate toward C. Assuming that
only motion along the line is possible, what will a negative test charge do when
released from rest at B?
19.2 The Electric Potential Difference
A positive charge accelerates from a region of higher electric potential
toward a region of lower electric potential.
A negative charge accelerates from a region of lower potential toward
a region of higher potential.
Therefore, it will begin moving toward A
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 ++++= 2
2
12
2
12
2
1
ω
One electron volt is the magnitude of the amount by which the potential
energy of an electron changes when the electron moves through a potential
difference of one volt.
V1060.1eV1 19−
×=
19.2 The Electric Potential Difference
Example 4 The Conservation of Energy
A particle has a mass of 1.8x10-5
kg and a charge of +3.0x10-5
C. 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?
19.2 The Electric Potential Difference
AABB EPEmvEPEmv +=+ 2
2
12
2
1
BAAB EPEEPEmvmv −+= 2
2
12
2
1
( )BAoAB VVqmvmv −+= 2
2
12
2
1
19.2 The Electric Potential Difference
( )BAoB VVqmv −=2
2
1
(a)
( )
( )( ) ( ) sm1.9kg108.1V25C100.32
2
55
=××=
−=
−−
mVVqv BAoB
( )
( )( ) ( ) sm1.9kg108.1V25C100.32
2
55
=××−−=
−−=
−−
mVVqv BAoA
(b)
19.3 The Electric Potential Difference Created by Point Charges
B
o
A
o
AB
r
kqq
r
kqq
W −=
BAo
AB
AB
r
kq
r
kq
q
W
VV −=
−
=−
Electric Potential
of a point charge
r
kq
V =
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 charge
of 4.0x10-8
C alters the electric potential at a
spot 1.2m away when the charge is
(a) positive and (b) negative.
19.3 The Electric Potential Difference Created by Point Charges
( )( )
V300
m2.1
C100.4CmN1099.8 8229
+=
×+⋅×
==
−
r
kq
V
(a)
(b)
V300−=V
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.
19.3 The Electric Potential Difference Created by Point Charges
( )( ) ( )( ) V240
m60.0
C100.8CmN1099.8
m20.0
C100.8CmN1099.8 82298229
+=
×−⋅×
+
×+⋅×
=
−−
AV
( )( ) ( )( ) V0
m40.0
C100.8CmN1099.8
m40.0
C100.8CmN1099.8 82298229
=
×−⋅×
+
×+⋅×
=
−−
BV
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
kq
V =
The net electric force does no work on a charge as
it moves on an equipotential surface.
19.4 Equipotential Surfaces and Their Relation to the Electric Field
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.
19.4 Equipotential Surfaces and Their Relation to the Electric Field
s
V
E
∆
∆
−=
19.4 Equipotential Surfaces and Their Relation to the Electric Field
Example 9 The Electric Field and Potential
Are Related
The plates of the capacitor are separated by
a distance of 0.032 m, and the potential difference
between them is VB-VA=-64V. Between the
two equipotential surfaces shown in color, there
is a potential difference of -3.0V. Find the spacing
between the two colored surfaces.
19.4 Equipotential Surfaces and Their Relation to the Electric Field
mV100.2
m0.032
V64 3
×=
−
=
∆
∆
−=
s
V
E
m105.1
mV100.2
V0.3 3
3
−
×=
×
−
−=
∆
−=∆
E
V
s
19.5 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.
19.5 Capacitors and Dielectrics
THE RELATION BETWEEN CHARGE AND POTENTIAL
DIFFERENCE FOR A CAPACITOR
The magnitude of the charge in each place of the
capacitor is directly proportional to the magnitude
of the potential difference between the plates.
CVq =
The capacitance C is the proportionality constant.
SI Unit of Capacitance: coulomb/volt = farad (F)
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 constant
E
Eo
=κ
19.5 Capacitors and Dielectrics
19.5 Capacitors and Dielectrics
THE CAPACITANCE OF A PARALLEL PLATE CAPACITOR
d
VE
E o
==
κ
( )AqE oo ε=
V
d
A
q o






=
κε
d
A
C oκε
=Parallel plate capacitor
filled with a dielectric
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 plate
form a capacitor. When the key is pressed, the
capacitance increases. The change in capacitance is
detected, 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. The
plate area is 9.50x10-5
m2
and the capacitor is filled with
a material whose dielectric constant is 3.50.
Determine the change in capacitance detected by the
computer.
19.5 Capacitors and Dielectrics
( ) ( )( )( ) F106.19
m100.150
m1050.9mNC1085.850.3 12
3-
252212
−
−−
×=
×
×⋅×
==
d
A
C oκε
( ) ( )( )( ) F10589.0
m105.00
m1050.9mNC1085.850.3 12
3-
252212
−
−−
×=
×
×⋅×
==
d
A
C oκε
F100.19 12−
×=∆C

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Chapter 19-powerpoint-1234856218860660-2

  • 1. Chapter 19 Electric Potential Energy and the Electric Potential
  • 2. 19.1 Potential Energy BABAAB mghmghW GPEGPE −=−=
  • 5. 19.2 The Electric Potential Difference o B o A o AB qqq W EPEEPE −= The potential energy per unit charge is called the electric potential.
  • 6. 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: oq V EPE = SI Unit of Electric Potential: joule/coulomb = volt (V) o AB o A o B AB q W qq VV − =−=− EPEEPE ( ) o AB o q W q V − = ∆ =∆ EPE
  • 7. 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 (+2.0x10-6 C) moves from A to B is +5.0x10-5 J. (a) Find the difference in EPE between these points. (b) Determine the electrical potential difference between these points. BAABW EPEEPE −= o AB o A o B AB q W qq VV − =−=− EPEEPE
  • 8. 19.2 The Electric Potential Difference BAABW EPEEPE −=(a) J100.5EPEEPE 5− ×−=−=− ABAB W (b) V25 C102.0 J100.5 6- 5 −= × ×− = − =− − o AB AB q W VV
  • 9. 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. Upon reaching B, the test charge continues to accelerate toward C. Assuming that only motion along the line is possible, what will a negative test charge do when released from rest at B?
  • 10. 19.2 The Electric Potential Difference A positive charge accelerates from a region of higher electric potential toward a region of lower electric potential. A negative charge accelerates from a region of lower potential toward a region of higher potential. Therefore, it will begin moving toward A
  • 11. 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 ++++= 2 2 12 2 12 2 1 ω One electron volt is the magnitude of the amount by which the potential energy of an electron changes when the electron moves through a potential difference of one volt. V1060.1eV1 19− ×=
  • 12. 19.2 The Electric Potential Difference Example 4 The Conservation of Energy A particle has a mass of 1.8x10-5 kg and a charge of +3.0x10-5 C. 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?
  • 13. 19.2 The Electric Potential Difference AABB EPEmvEPEmv +=+ 2 2 12 2 1 BAAB EPEEPEmvmv −+= 2 2 12 2 1 ( )BAoAB VVqmvmv −+= 2 2 12 2 1
  • 14. 19.2 The Electric Potential Difference ( )BAoB VVqmv −=2 2 1 (a) ( ) ( )( ) ( ) sm1.9kg108.1V25C100.32 2 55 =××= −= −− mVVqv BAoB ( ) ( )( ) ( ) sm1.9kg108.1V25C100.32 2 55 =××−−= −−= −− mVVqv BAoA (b)
  • 15. 19.3 The Electric Potential Difference Created by Point Charges B o A o AB r kqq r kqq W −= BAo AB AB r kq r kq q W VV −= − =− Electric Potential of a point charge r kq V =
  • 16. 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 charge of 4.0x10-8 C alters the electric potential at a spot 1.2m away when the charge is (a) positive and (b) negative.
  • 17. 19.3 The Electric Potential Difference Created by Point Charges ( )( ) V300 m2.1 C100.4CmN1099.8 8229 += ×+⋅× == − r kq V (a) (b) V300−=V
  • 18. 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.
  • 19. 19.3 The Electric Potential Difference Created by Point Charges ( )( ) ( )( ) V240 m60.0 C100.8CmN1099.8 m20.0 C100.8CmN1099.8 82298229 += ×−⋅× + ×+⋅× = −− AV ( )( ) ( )( ) V0 m40.0 C100.8CmN1099.8 m40.0 C100.8CmN1099.8 82298229 = ×−⋅× + ×+⋅× = −− BV
  • 20. 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 kq V = The net electric force does no work on a charge as it moves on an equipotential surface.
  • 21. 19.4 Equipotential Surfaces and Their Relation to the Electric Field 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.
  • 22. 19.4 Equipotential Surfaces and Their Relation to the Electric Field s V E ∆ ∆ −=
  • 23. 19.4 Equipotential Surfaces and Their Relation to the Electric Field Example 9 The Electric Field and Potential Are Related The plates of the capacitor are separated by a distance of 0.032 m, and the potential difference between them is VB-VA=-64V. Between the two equipotential surfaces shown in color, there is a potential difference of -3.0V. Find the spacing between the two colored surfaces.
  • 24. 19.4 Equipotential Surfaces and Their Relation to the Electric Field mV100.2 m0.032 V64 3 ×= − = ∆ ∆ −= s V E m105.1 mV100.2 V0.3 3 3 − ×= × − −= ∆ −=∆ E V s
  • 25. 19.5 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.
  • 26. 19.5 Capacitors and Dielectrics THE RELATION BETWEEN CHARGE AND POTENTIAL DIFFERENCE FOR A CAPACITOR The magnitude of the charge in each place of the capacitor is directly proportional to the magnitude of the potential difference between the plates. CVq = The capacitance C is the proportionality constant. SI Unit of Capacitance: coulomb/volt = farad (F)
  • 27. 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 constant E Eo =κ
  • 28. 19.5 Capacitors and Dielectrics
  • 29. 19.5 Capacitors and Dielectrics THE CAPACITANCE OF A PARALLEL PLATE CAPACITOR d VE E o == κ ( )AqE oo ε= V d A q o       = κε d A C oκε =Parallel plate capacitor filled with a dielectric
  • 30. 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 plate form a capacitor. When the key is pressed, the capacitance increases. The change in capacitance is detected, 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. The plate area is 9.50x10-5 m2 and the capacitor is filled with a material whose dielectric constant is 3.50. Determine the change in capacitance detected by the computer.
  • 31. 19.5 Capacitors and Dielectrics ( ) ( )( )( ) F106.19 m100.150 m1050.9mNC1085.850.3 12 3- 252212 − −− ×= × ×⋅× == d A C oκε ( ) ( )( )( ) F10589.0 m105.00 m1050.9mNC1085.850.3 12 3- 252212 − −− ×= × ×⋅× == d A C oκε F100.19 12− ×=∆C