Electric Potential

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Electric Potential Electric forces are conservative. Work done by an electric force is W=-q o Ed DU=-W

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Electric Potential. Electric forces are conservative. Work done by an electric force is W=- q o Ed D U=-W. Figure 20-1 Change in Electric Potential Energy. Electric Potential. Definition of Electric Potential V. Electric Potential. - PowerPoint PPT Presentation

Transcript of Electric Potential

Page 1: Electric Potential

Electric Potential

Electric forces are conservative.Work done by an electric force is W=-qoEdDU=-W

Page 2: Electric Potential

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.

o

o o

q E sWV E sq qVEs

DD D

D

D

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Electric Potential

Electric potential of point charges.

electric potential energy for a point charge

oo

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