28
Phys102 Lecture 12 Electric Currents and Resistance Key Points Ohm’s Law Resistivity Electric Power Alternating Current References SFU Ed: 25-1,2,3,4,5,6,7. 6 th Ed: 18-1,2,3,4,5,6,7

Phys102 Lecture 12 Electric Currents and Resistance

  • Upload
    others

  • View
    5

  • Download
    0

Embed Size (px)

Citation preview

Page 1: Phys102 Lecture 12 Electric Currents and Resistance

Phys102 Lecture 12

Electric Currents and Resistance

Key Points

• Ohm’s Law

• Resistivity

• Electric Power

• Alternating Current

References

SFU Ed: 25-1,2,3,4,5,6,7.

6th Ed: 18-1,2,3,4,5,6,7

Page 2: Phys102 Lecture 12 Electric Currents and Resistance

Volta discovered that

electricity could be

created if dissimilar

metals were

connected by a

conductive solution

called an electrolyte.

This is a simple

electric cell.

25-1 The Electric Battery

Page 3: Phys102 Lecture 12 Electric Currents and Resistance

A battery transforms chemical energy into

electrical energy.

Chemical reactions within the cell create a

potential difference between the terminals by

slowly dissolving them. This potential

difference can be maintained even if a current is

kept flowing, until one or the other terminal is

completely dissolved.

25-1 The Electric Battery

Page 4: Phys102 Lecture 12 Electric Currents and Resistance

Electric current is the rate of flow of charge

through a conductor:

Unit of electric current: the ampere, A:

1 A = 1 C/s.

25-2 Electric Current

The instantaneous current is given by:

Page 5: Phys102 Lecture 12 Electric Currents and Resistance

A complete circuit is one where current can

flow all the way around. Note that the

schematic drawing doesn’t look much like the

physical circuit!

25-2 Electric Current

Page 6: Phys102 Lecture 12 Electric Currents and Resistance

By convention, current is defined as flowing

from + to -. Electrons actually flow in the

opposite direction, but not all currents consist

of electrons.

25-2 Electric Current

Page 7: Phys102 Lecture 12 Electric Currents and Resistance

Experimentally, it is found that the

current in a wire is proportional to

the potential difference between its

ends:

25-3 Ohm’s Law: Resistance

and Resistors

Page 8: Phys102 Lecture 12 Electric Currents and Resistance

The ratio of voltage to current is called the

resistance:

25-3 Ohm’s Law: Resistance

and Resistors

Page 9: Phys102 Lecture 12 Electric Currents and Resistance

25-3 Ohm’s Law: Resistance

and Resistors

Example 25-4: Flashlight bulb

resistance.

A small flashlight bulb draws 300

mA from its 1.5-V battery. (a) What

is the resistance of the bulb? (b) If

the battery becomes weak and the

voltage drops to 1.2 V, how would

the current change?

Page 10: Phys102 Lecture 12 Electric Currents and Resistance

The resistance of a wire is directly

proportional to its length and inversely

proportional to its cross-sectional area:

The constant ρ, the resistivity, is

characteristic of the material.

25-4 Resistivity

Page 11: Phys102 Lecture 12 Electric Currents and Resistance

25-4 ResistivityThis table gives the resistivity and temperature

coefficients of typical conductors, semiconductors,

and insulators.

Page 12: Phys102 Lecture 12 Electric Currents and Resistance

25-4 ResistivityConceptual Example 25-6: Stretching

changes resistance.

Suppose a wire of resistance R could be

stretched uniformly until it was twice its

original length. What would happen to

its resistance?

Page 13: Phys102 Lecture 12 Electric Currents and Resistance

Power, as in kinematics, is the energy

transformed by a device per unit time:

25-5 Electric Power

or

Page 14: Phys102 Lecture 12 Electric Currents and Resistance

The unit of power is the watt, W.

For ohmic devices, we can make the

substitutions:

25-5 Electric Power

Page 15: Phys102 Lecture 12 Electric Currents and Resistance

25-5 Electric PowerExample 25-8: Headlights.

Calculate the resistance of a 40-W

automobile headlight designed for 12 V.

Page 16: Phys102 Lecture 12 Electric Currents and Resistance

What you pay for on your electric bill is

not power, but energy – the power

consumption multiplied by the time.

We have been measuring energy in

joules, but the electric company

measures it in kilowatt-hours, kWh:

1 kWh = (1000 W)(3600 s) = 3.60 x 106 J.

25-5 Electric Power

Page 17: Phys102 Lecture 12 Electric Currents and Resistance

25-5 Electric PowerExample 25-9: Electric heater.

An electric heater draws a steady 15.0

A on a 120-V line. How much power

does it require and how much does it

cost per month (30 days) if it operates

3.0 h per day and the electric company

charges 9.2 cents per kWh?

Page 18: Phys102 Lecture 12 Electric Currents and Resistance

25-6 Power in Household Circuits

Conceptual Example 25-12: A dangerous

extension cord.

Your 1800-W portable electric heater is too

far from your desk to warm your feet. Its

cord is too short, so you plug it into an

extension cord rated at 11 A. Why is this

dangerous?

Page 19: Phys102 Lecture 12 Electric Currents and Resistance

Current from a battery

flows steadily in one

direction (direct current,

DC). Current from a

power plant varies

sinusoidally (alternating

current, AC).

25-7 Alternating Current

Page 20: Phys102 Lecture 12 Electric Currents and Resistance

The voltage varies sinusoidally with time:

as does the current:

25-7 Alternating Current

,,

Page 21: Phys102 Lecture 12 Electric Currents and Resistance

Multiplying the current and the voltage gives

the power:

25-7 Alternating Current

Page 22: Phys102 Lecture 12 Electric Currents and Resistance

Usually we are interested in the average power:

25-7 Alternating Current

.

Page 23: Phys102 Lecture 12 Electric Currents and Resistance

The current and voltage both have average

values of zero, so we square them, take the

average, then take the square root, yielding the

root-mean-square (rms) value:

25-7 Alternating Current

Page 24: Phys102 Lecture 12 Electric Currents and Resistance

25-7 Alternating CurrentExample 25-13: Hair dryer.

(a) Calculate the resistance and the peak current

in a 1000-W hair dryer connected to a 120-V line.

(b) What happens if it is connected to a 240-V line

in Britain?

Page 25: Phys102 Lecture 12 Electric Currents and Resistance

• A battery is a source of constant potential

difference.

• Electric current is the rate of flow of electric

charge.

• Conventional current is in the direction that

positive charge would flow.

• Resistance is the ratio of voltage to current:

Summary of Chapter 25

Page 26: Phys102 Lecture 12 Electric Currents and Resistance

• Ohmic materials have constant resistance,

independent of voltage.

• Resistance is determined by shape and

material:

• ρ is the resistivity.

Summary of Chapter 25

Page 27: Phys102 Lecture 12 Electric Currents and Resistance

• Power in an electric circuit:

• Direct current is constant.

• Alternating current varies sinusoidally:

Summary of Chapter 25

Page 28: Phys102 Lecture 12 Electric Currents and Resistance

• The average (rms) current and voltage:

Summary of Chapter 25