Physics 213 General Physics Lecture 5. 2 Last Meeting: Capacitance Today: Current and Resistance.

25
Physics 213 General Physics Lecture 5

Transcript of Physics 213 General Physics Lecture 5. 2 Last Meeting: Capacitance Today: Current and Resistance.

Page 1: Physics 213 General Physics Lecture 5. 2 Last Meeting: Capacitance Today: Current and Resistance.

Physics 213General Physics

Lecture 5

Page 2: Physics 213 General Physics Lecture 5. 2 Last Meeting: Capacitance Today: Current and Resistance.

2

Last Meeting: Capacitance

Today: Current and Resistance

Page 3: Physics 213 General Physics Lecture 5. 2 Last Meeting: Capacitance Today: Current and Resistance.

Energy Stored in a Capacitor

Energy stored = ½ Q ΔV

From the definition of capacitance, this can be rewritten in different forms

C2

QVC

2

1VQ

2

1Energy

22

Page 4: Physics 213 General Physics Lecture 5. 2 Last Meeting: Capacitance Today: Current and Resistance.

4

NC

C

CCC

eq

eq

...111

2

21

VCEnergy

NCC

CCC

eq

eq

...

C CC

C

Page 5: Physics 213 General Physics Lecture 5. 2 Last Meeting: Capacitance Today: Current and Resistance.

Quiz: The plates of a connected parallel-plate capacitor of capacitance C are brought together to one-third their original separation. The energy stored is now

(a) W/9(b) W/3(c) 3W(d) 9W

Answer: c

221 1,

2 2

QW CV W

C

Page 6: Physics 213 General Physics Lecture 5. 2 Last Meeting: Capacitance Today: Current and Resistance.

QUIZ

A fully charged parallel-plate capacitor remains connected to a battery while you slide a dielectric between the plates. Do the following quantities increase, decrease, or stay the same? (a) C; (b) Q; (c) E between the plates; (d) V.

Page 7: Physics 213 General Physics Lecture 5. 2 Last Meeting: Capacitance Today: Current and Resistance.

QUIZ

(a) C increases

(b) Q increases

(c) E stays the same

(d) V remains the same

Page 8: Physics 213 General Physics Lecture 5. 2 Last Meeting: Capacitance Today: Current and Resistance.

8

Page 9: Physics 213 General Physics Lecture 5. 2 Last Meeting: Capacitance Today: Current and Resistance.

9

Page 10: Physics 213 General Physics Lecture 5. 2 Last Meeting: Capacitance Today: Current and Resistance.

10

Page 11: Physics 213 General Physics Lecture 5. 2 Last Meeting: Capacitance Today: Current and Resistance.

Charge Carrier Motion in a Conductor

The zig-zag black line represents the motion of a charge carrier in a conductorThe net drift speed is small

The sharp changes in direction are due to collisions

The net motion of electrons is opposite the direction of the electric field

Page 12: Physics 213 General Physics Lecture 5. 2 Last Meeting: Capacitance Today: Current and Resistance.

Charge Carrier Motion in a Conductor

The drift speed Vd is small (~1meter/hour)

The fermi speed Vf is very fast! Due to quantum mechanics of electrons. (~106 meters/second)

Charge rearrangements and signals travel near speed of light (~108 meters/second)

fv

Page 13: Physics 213 General Physics Lecture 5. 2 Last Meeting: Capacitance Today: Current and Resistance.

13

Page 14: Physics 213 General Physics Lecture 5. 2 Last Meeting: Capacitance Today: Current and Resistance.

14

Page 15: Physics 213 General Physics Lecture 5. 2 Last Meeting: Capacitance Today: Current and Resistance.

15

Page 16: Physics 213 General Physics Lecture 5. 2 Last Meeting: Capacitance Today: Current and Resistance.

16

Page 17: Physics 213 General Physics Lecture 5. 2 Last Meeting: Capacitance Today: Current and Resistance.

17

Page 18: Physics 213 General Physics Lecture 5. 2 Last Meeting: Capacitance Today: Current and Resistance.

18

Page 19: Physics 213 General Physics Lecture 5. 2 Last Meeting: Capacitance Today: Current and Resistance.

19

Variety of Resistors

Page 20: Physics 213 General Physics Lecture 5. 2 Last Meeting: Capacitance Today: Current and Resistance.

Temperature Variation of Resistivity

For most metals, resistivity increases with increasing temperature

With a higher temperature, the metal’s constituent atoms vibrate with increasing amplitude

The electrons find it more difficult to pass through the atoms

fv

Page 21: Physics 213 General Physics Lecture 5. 2 Last Meeting: Capacitance Today: Current and Resistance.

Temperature Variation of Resistivity, contFor most metals, resistivity increases

approximately linearly with temperature over a limited temperature range

ρ is the resistivity at some temperature T

ρo is the resistivity at some reference temperature To To is usually taken to be 20° C

is the temperature coefficient of resistivity

)]TT(1[ oo

Page 22: Physics 213 General Physics Lecture 5. 2 Last Meeting: Capacitance Today: Current and Resistance.

22

Energy is turned to heat (random motion)

Page 23: Physics 213 General Physics Lecture 5. 2 Last Meeting: Capacitance Today: Current and Resistance.

Electrical Energy and Power

The rate at which the energy is lost is the power

From Ohm’s Law, alternate forms of power are

QV I V

t

22 V

I RR

Page 24: Physics 213 General Physics Lecture 5. 2 Last Meeting: Capacitance Today: Current and Resistance.

Electrical Energy and Power, cont2

2 VI R

R

Page 25: Physics 213 General Physics Lecture 5. 2 Last Meeting: Capacitance Today: Current and Resistance.

Electrical Energy and Power, final

The SI unit of power is Watt (W)I must be in Amperes, R in ohms and V in

Volts

The unit of energy used by electric companies is the kilowatt-hourThis is defined in terms of the unit of power and

the amount of time it is supplied1 kWh = 3.60 x 106 J