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Electric Electric Potential Potential AP Physics: M. Blachly AP Physics: M. Blachly Textbook: 17:1-3 Textbook: 17:1-3
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Page 1: Electric Potential AP Physics: M. Blachly Textbook: 17:1-3.

Electric Electric PotentialPotential

AP Physics: M. BlachlyAP Physics: M. Blachly

Textbook: 17:1-3Textbook: 17:1-3

Page 2: Electric Potential AP Physics: M. Blachly Textbook: 17:1-3.

Review of Work

Work done by the force given by:

• W = F d cos()

• Positive: Force is in direction moved

• Negative: Force is opposite direction moved

• Zero: Force is perpendicular to direction moved

Page 3: Electric Potential AP Physics: M. Blachly Textbook: 17:1-3.

TnR

If a positive charge were moved from very far away on the right to one of the positions shown, at what position would it have the greatest amount of stored energy?

+ ABCD

Page 4: Electric Potential AP Physics: M. Blachly Textbook: 17:1-3.

Work on Charges

Work, force, electric field and Electrical Energy are always considered from the point of view of a positive charge.

Page 5: Electric Potential AP Physics: M. Blachly Textbook: 17:1-3.

Electrostatic Potential Energy and Potential Difference

The electrostatic force is conservative – potential energy can be defined

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

(17-1)

Page 6: Electric Potential AP Physics: M. Blachly Textbook: 17:1-3.

Electrostatic PE and Potential Difference

Electric potential (Voltage) is defined as potential energy per unit charge:

(17-2a)

Page 7: Electric Potential AP Physics: M. Blachly Textbook: 17:1-3.

TnR

Given the definition of the voltage, what would be the proper units for Voltage?

A.Joules

B.Joules/Volt

C.Joules/Coulomb

D.Volts/Coulomb

Page 8: Electric Potential AP Physics: M. Blachly Textbook: 17:1-3.

Electrostatic PE and Potential Difference

Electric potential is defined as potential energy per unit charge:

(17-2a)

Unit of electric potential: the volt (V).

1 V = I J/C.

Page 9: Electric Potential AP Physics: M. Blachly Textbook: 17:1-3.

17.1 Electrostatic Potential Energy

Only changes in potential can be measured, allowing free assignment of V = 0. (like solving gravitational PE problems)

(17-2b)

Page 10: Electric Potential AP Physics: M. Blachly Textbook: 17:1-3.

17.1 Electrostatic PE

Analogy between gravitational and electrical potential energy:

Page 11: Electric Potential AP Physics: M. Blachly Textbook: 17:1-3.

Electric Potential and Electric Field

Work is charge multiplied by potential:

Work is also force multiplied by distance:

Page 12: Electric Potential AP Physics: M. Blachly Textbook: 17:1-3.

Equi-potential Lines

Page 13: Electric Potential AP Physics: M. Blachly Textbook: 17:1-3.

17.3 Equipotential Lines

An equipotential is a line or surface over which the potential is constant.

Electric field lines are perpendicular to equipotentials.

The surface of a conductor is an equipotential.

Page 14: Electric Potential AP Physics: M. Blachly Textbook: 17:1-3.

17.3 Equipotential Lines

Page 15: Electric Potential AP Physics: M. Blachly Textbook: 17:1-3.

The electron

How much potential energy does a single electron have if it is moved across a potential of 1.0 volts?

19

19

so

1.6 10 C 1 V

1.6 10 J

UV

q

U qV

Page 16: Electric Potential AP Physics: M. Blachly Textbook: 17:1-3.

The Electron Volt, a Unit of Energy

One electron volt (eV) is the energy gained by an electron moving through a potential difference of one volt.

Page 17: Electric Potential AP Physics: M. Blachly Textbook: 17:1-3.

Potential Due to Point Charges

The electric potential due to a point charge can be derived using calculus.

(17-5)

212

2

C8.85 10

N×mo

Page 18: Electric Potential AP Physics: M. Blachly Textbook: 17:1-3.

Concept Check

A charge of 3.0 nC is placed at the origin. What is the voltage at a point that is 30. cm away?

V = 90 V

What about at a point that is a mile away?

V = 0.017 V

What about a point that is infinitely far away?

V = 0 V

Page 19: Electric Potential AP Physics: M. Blachly Textbook: 17:1-3.

Potential Due to Point Charges

These plots show the potential due to (a) positive and (b) negative charge.

Page 20: Electric Potential AP Physics: M. Blachly Textbook: 17:1-3.

Potential Due to Point Charges

Using potentials instead of fields can make solving problems much easier – potential is a scalar quantity, whereas the field is a vector.

Page 21: Electric Potential AP Physics: M. Blachly Textbook: 17:1-3.

Example: Old fashioned TV

An electron is accelerated across a potential of 5000 V. What is the velocity of the electron after passing through this potential difference?

Page 22: Electric Potential AP Physics: M. Blachly Textbook: 17:1-3.

Example: Old fashioned TV

An electron (m = 9.11E-31 kg) is accelerated across 5000 V. Find the velocity in terms of c.

21

2

PE KE

qV mv

19

31

7

2

2 1.6 10 C 5000 J

9.11 10 kg

4.19 10 m/s 0.140

qVv

m

v

v c

Page 23: Electric Potential AP Physics: M. Blachly Textbook: 17:1-3.

17.7 Capacitance

A capacitor consists of two conductors that are close but not touching. A capacitor has the ability to store electric charge.

Page 24: Electric Potential AP Physics: M. Blachly Textbook: 17:1-3.

17.7 Capacitance

Parallel-plate capacitor connected to battery. (b) is a circuit diagram.

Page 25: Electric Potential AP Physics: M. Blachly Textbook: 17:1-3.

Capacitance

Charge vs. Voltage for a Capacitor

Q = 0.5 V

0

1

2

3

4

5

6

0 2 4 6 8 10

Voltage (V)

Sto

red

Cha

rge

(C)

Page 26: Electric Potential AP Physics: M. Blachly Textbook: 17:1-3.

17.7 Capacitance

When a capacitor is connected to a battery, the charge on its plates is proportional to the voltage:

(17-7)

The quantity C is called the capacitance.

Unit of capacitance: the farad (F)

Page 27: Electric Potential AP Physics: M. Blachly Textbook: 17:1-3.

TnR

What is a Farad?

A.Coulomb/Joule

B.Coulomb/Volt

C.Joule/Coulomb

D.Volt/Coulomb

Answer: B

Page 28: Electric Potential AP Physics: M. Blachly Textbook: 17:1-3.

17.7 Capacitance

The capacitance does not depend on the voltage; it is a function of the geometry and materials of the capacitor.

For a parallel-plate capacitor:

212

2

C8.85 10

N×m

o

o

AC

d

Page 29: Electric Potential AP Physics: M. Blachly Textbook: 17:1-3.

17.8 Dielectrics

A dielectric is an insulator, and is characterized by a dielectric constant K.

Capacitance of a parallel-plate capacitor filled with dielectric:

(17-9)

Page 30: Electric Potential AP Physics: M. Blachly Textbook: 17:1-3.

17.8 Dielectrics

Dielectric strength is the maximum field a dielectric can experience without breaking down.

Page 31: Electric Potential AP Physics: M. Blachly Textbook: 17:1-3.

17.8 Dielectrics

The molecules in a dielectric tend to become oriented in a way that reduces the external field.

Page 32: Electric Potential AP Physics: M. Blachly Textbook: 17:1-3.

17.8 Dielectrics

This means that the electric field within the dielectric is less than it would be in air, allowing more charge to be stored for the same potential.

Page 33: Electric Potential AP Physics: M. Blachly Textbook: 17:1-3.

TnR

For a capacitor connected to a battery of fixed voltage, what will adding a dielectric material do?A.Decrease the charge

storedB. Increase the charge storedC.It will not affect the amount

of charge stored.

Answer: B

Page 34: Electric Potential AP Physics: M. Blachly Textbook: 17:1-3.

17.9 Storage of Electric Energy

A charged capacitor stores electric energy; the energy stored is equal to the work done to charge the capacitor.

221 1 1

2 2 2

QU QV CV

C

Page 35: Electric Potential AP Physics: M. Blachly Textbook: 17:1-3.

17.9 Storage of Electric Energy

The energy density, defined as the energy per unit volume, is the same no matter the origin of the electric field:

(17-11)

The sudden discharge of electric energy can be harmful or fatal. Capacitors can retain their charge indefinitely even when disconnected from a voltage source – be careful!

Page 36: Electric Potential AP Physics: M. Blachly Textbook: 17:1-3.

17.9 Storage of Electric Energy

Heart defibrillators use electric discharge to “jump-start” the heart, and can save lives.

Camera’s use a capacitor discharge to fire the flash

Page 37: Electric Potential AP Physics: M. Blachly Textbook: 17:1-3.

17.10 Cathode Ray Tube

A cathode ray tube contains a wire cathode that, when heated, emits electrons. A voltage source causes the electrons to travel to the anode.

Page 38: Electric Potential AP Physics: M. Blachly Textbook: 17:1-3.

17.10 Cathode Ray Tube

The electrons can be steered using electric fields.

Page 39: Electric Potential AP Physics: M. Blachly Textbook: 17:1-3.

17.10 Cathode Ray Tube

Televisions and computer monitors (except for LCD and plasma models) have a largecathode ray tube as their display. Variations in the field steer the electrons on their way to the screen.

Page 40: Electric Potential AP Physics: M. Blachly Textbook: 17:1-3.

17.11 The Electrocardiogram (ECG or EKG)

The electrocardiogram detects heart defects by measuring changes in potential on the surface of the heart.

Page 41: Electric Potential AP Physics: M. Blachly Textbook: 17:1-3.

Summary of Chapter 17

• Electric potential energy:

• Electric potential difference: work done to move charge from one point to another

• Relationship between potential difference and field:

Page 42: Electric Potential AP Physics: M. Blachly Textbook: 17:1-3.

Summary of Chapter 17

• Equipotential: line or surface along which potential is the same

• Electric potential of a point charge:

Page 43: Electric Potential AP Physics: M. Blachly Textbook: 17:1-3.

Summary of Chapter 17

• Capacitor: nontouching conductors carrying equal and opposite charge

•Capacitance:

• Capacitance of a parallel-plate capacitor:

Page 44: Electric Potential AP Physics: M. Blachly Textbook: 17:1-3.

Summary of Chapter 17

• A dielectric is an insulator

• Dielectric constant gives ratio of total field to external field

• Energy density in electric field:

Page 45: Electric Potential AP Physics: M. Blachly Textbook: 17:1-3.

Capacitor Networks

When there are multiple capacitors in series, the capacitors will all have the same charge.

1 2 1 2

1 2

1 2

1 2

[1] and [2]

Since , we can rewrite [2] as

and since Q is all the same,

1 1 1 capacitor network in series

n n

n

n

n

Q Q Q V V V

Q CV

Q Q Q

C C C

C C C

Page 46: Electric Potential AP Physics: M. Blachly Textbook: 17:1-3.

Example Problem: Series

What is the equivalent capacitance of a network consisting of a 9.0 µF capacitor and a 18 µF capacitor in series? (Answer in µF).

What will be the charge on the smaller capacitor if this network is connected to a 12 volt battery? (Answer in µC )

What will be the voltage on the bigger capacitor?

Page 47: Electric Potential AP Physics: M. Blachly Textbook: 17:1-3.

Capacitor Networks

When there are multiple capacitors in parallel, the capacitors will all have the same voltage.

1 2 1 2

1 1 2 2

1 2

[1] and [2]

Since , we can rewrite [2] as

and since V is all the same,

capacitor network in parallel

n n

n n

n

V V V Q Q Q

Q CV

V C VC V C

C C C

Page 48: Electric Potential AP Physics: M. Blachly Textbook: 17:1-3.

Example Problem: Parallel

What is the equivalent capacitance of a network consisting of a 9.0 µF capacitor and a 18 µF capacitor in parallel? (Answer in µF).

What will be the voltage on the smaller capacitor if this network is connected to a 12 volt battery? (Answer in V )

What will be the charge on the smaller capacitor? (Answer in µC )

Page 49: Electric Potential AP Physics: M. Blachly Textbook: 17:1-3.

Example: Capacitors

Page 50: Electric Potential AP Physics: M. Blachly Textbook: 17:1-3.

Example: Capacitors

Page 51: Electric Potential AP Physics: M. Blachly Textbook: 17:1-3.

Example: Capacitors