Electric Potential
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Transcript of Electric Potential
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Electric Potential
Electric forces are conservative.Work done by an electric force is W=-qoEdDU=-W
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Figure 20-1Change in Electric Potential Energy
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Electric Potential
,
o o
U WVq qJ jouleSIunit volt VC coulomb
D D
Definition of Electric Potential V
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Electric Potential
When working with electric potential we measure only changes in electric potential.The zero point can be set arbitrarily.
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Figure 20-2Electric Field and Electric Potential
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Electric Potential
Electric field and the rate of change of electric potential.
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q E sWV E sq qVEs
DD D
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Electric Potential
Electric potential of point charges.
electric potential energy for a point charge
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kqVr
kqqU q Vr
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Solve problems 1-7, 16-19, and 21-24 on pages 672 and 673.
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Electric fields around conductorsExcess electric charges move to the surface of a conductor because that is where they are least affected by the internal charges of the material.
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Figure 19-18Charge Distribution
on a Conducting Sphere
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Electric fields around conductorsWhen electric charges are at rest, the electric field within a conductor is zero. This works even if the conductor has an internal cavity.
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Figure 19-19Electric Field Near a Conducting Surface
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Electric fields around conductors
Electric field lines enter conductor surfaces at right angles.
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Figure 19-21Shielding Works in Only One Direction
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Figure 19-20Intense Electric Field Near a Sharp Point
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Electric fields around conductors
Electric field lines are more intense near a sharp point.
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Charging by induction
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Figure 19-22abCharging by Induction
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Figure 19-22cdCharging by Induction
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Capacitors
A capacitor is a device that has the ability “capacity” to store electric charge and energy.
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Capacitors
Capacitance
charge
: :
is defined asQC Q the on the platesV
V electric potential across the platescoulombUnit farad Fvolt
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Figure 20-13A Parallel-Plate Capacitor
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Capacitors
2
122
1 C =8.85 10 Coulomb's constant 4
o
o
Permitivity of free space
kk N m
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Capacitors
Capacitance of a parallel plate capacitor
d= distance between platesA= area of the plates
oACd
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Capacitors
A dielectric material is an insulator that increases the capacitance of a capacitor when placed between the plates.Each material has a dielectric constant k not to be confused with k.(p 665)
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Figure 20-15The Effect of a Dielectric on the Electric Field of a Capacitor
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Capacitors
Capacitance of a parallel plate capacitor filled witha dielectric
d= distance between platesA= area of the plates
dielectric constant
oACd
k
k
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Capacitors
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Energy stored in a capacitor
1 12 2 2
QU QV CVC