chapter 23 electric potential. 23.1 electrostatic potential energy r gravitational potential energy...

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Chapter 23 Electric Potential

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Page 1: Chapter 23 Electric Potential. 23.1 Electrostatic Potential Energy r Gravitational Potential Energy U g  0 when r  ∞ U g is due to an attractive force

Chapter 23Electric Potential

Page 2: Chapter 23 Electric Potential. 23.1 Electrostatic Potential Energy r Gravitational Potential Energy U g  0 when r  ∞ U g is due to an attractive force

23.1 Electrostatic Potential Energy

r

•Gravitational Potential Energy

•Ug 0 when r ∞

•Ug is due to an attractive force

•Electric Potential Energy

•UE can result from either an attractive force or a repulsive force

•UE 0 when r ∞

+ +-

r r

Page 3: Chapter 23 Electric Potential. 23.1 Electrostatic Potential Energy r Gravitational Potential Energy U g  0 when r  ∞ U g is due to an attractive force

23.1 Electrostatic Potential Energy

•Gravitational Ug

Attractive force•Electric UE

Attractive force•Electric UE

Repulsive force

U

r

U

r

U

r

+- + + - -or

< 0 > 0

Bigger when farther Bigger when farther Bigger when closer

Page 4: Chapter 23 Electric Potential. 23.1 Electrostatic Potential Energy r Gravitational Potential Energy U g  0 when r  ∞ U g is due to an attractive force

Work and Electrostatic Potential energy

Work done BY conservative

force

U

r

U

r

+

-

+

2

1

2

1

FE

+

FE

Move in the direction of force -->positive work

Move opposite the

direction of force --> negative work

2

1

2

1

∆U < 0 ∆U > 0

Page 5: Chapter 23 Electric Potential. 23.1 Electrostatic Potential Energy r Gravitational Potential Energy U g  0 when r  ∞ U g is due to an attractive force

The electrostatic force is conservative – potential energy can be defined.

Change in electric potential energy is negative of work done by electric force:

23-1 Electrostatic Potential Energy and Potential

Difference

Page 6: Chapter 23 Electric Potential. 23.1 Electrostatic Potential Energy r Gravitational Potential Energy U g  0 when r  ∞ U g is due to an attractive force

Potential Difference and E-fields

• Just as the Force points in the direction of LOWER Potential Energy, UE

• The Electric Field points in the direction of LOWER Potential, V

-

-------

+++++++

-

-------

+++++++

-

E E

+F F

Low V High V

Low UE

High UE

Low UE

High UE

Low V High V

Page 7: Chapter 23 Electric Potential. 23.1 Electrostatic Potential Energy r Gravitational Potential Energy U g  0 when r  ∞ U g is due to an attractive force

23-1 Electrostatic Potential Energy and Potential

DifferenceElectric

Potential

Electric Potential Difference: DV

Since only changes in potential energy are important, typically we are most interested in potential difference

Electric potential energy per unit charge

=

~ Volts

for a point charge moving from A to B

Page 8: Chapter 23 Electric Potential. 23.1 Electrostatic Potential Energy r Gravitational Potential Energy U g  0 when r  ∞ U g is due to an attractive force

Only changes in potential can be measured,

23-1 Electrostatic Potential Energy and Potential

Difference

Page 9: Chapter 23 Electric Potential. 23.1 Electrostatic Potential Energy r Gravitational Potential Energy U g  0 when r  ∞ U g is due to an attractive force

Analogy between gravitational and electrical potential energy:

23-1 Electrostatic Potential Energy and Potential

Difference

Two charges have the same electric potential. The 2Q charge has more potential energy

Page 10: Chapter 23 Electric Potential. 23.1 Electrostatic Potential Energy r Gravitational Potential Energy U g  0 when r  ∞ U g is due to an attractive force

23-1 Electrostatic Potential Energy and Potential

Difference

Electrical sources such as batteries and generators supply a constant potential difference. Here are some typical potential differences, both natural and manufactured:

Page 11: Chapter 23 Electric Potential. 23.1 Electrostatic Potential Energy r Gravitational Potential Energy U g  0 when r  ∞ U g is due to an attractive force

23-1 Electrostatic Potential Energy and Potential

DifferenceExample 23-2: Electron in CRT.

Suppose an electron in a cathode ray tube is accelerated from

rest through a potential difference Vb – Va = Vba = +5000 V. (a) What is the change in electric potential energy of the electron? (b) What is the speed of the electron (m = 9.1 × 10-31 kg) as a result of this acceleration?

Page 12: Chapter 23 Electric Potential. 23.1 Electrostatic Potential Energy r Gravitational Potential Energy U g  0 when r  ∞ U g is due to an attractive force

23-2 Relation between Electric Potential and Electric Field

The general relationship between a conservative force and potential energy:

Substituting the potential difference and the electric field:

Page 13: Chapter 23 Electric Potential. 23.1 Electrostatic Potential Energy r Gravitational Potential Energy U g  0 when r  ∞ U g is due to an attractive force

23-2 Relation between Electric Potential and Electric Field

The simplest case is a uniform field:

Page 14: Chapter 23 Electric Potential. 23.1 Electrostatic Potential Energy r Gravitational Potential Energy U g  0 when r  ∞ U g is due to an attractive force

Points to remember

• Increasing U increases stored energy

•Force always points in the direction of LOWER potential energy

•The potential energy is a scalar—no direction•The signs of the charges give the sign on the electric potential energy

•Only changes in potential energy are important

•Energy is NOT a vector

Page 15: Chapter 23 Electric Potential. 23.1 Electrostatic Potential Energy r Gravitational Potential Energy U g  0 when r  ∞ U g is due to an attractive force

Relationships….

Electric Force Electric Field

Electric PotentialElectric PotentialEnergy

Vectorquantities

Scalarquantities

Per unitCharge=

Per unitCharge=

Is the negativeGradient (change) of

Is the negativeGradient of

Property of a charge q Property of a Point P