28
Electric Currents Physics Department, New York City College of Technology

Electric Currents

Embed Size (px)

DESCRIPTION

Electric Currents. Physics Department, New York City College of Technology. Electric battery Electric current Resistance Ohm’s law Resistivity Electric energy Electric power Direct current. Alternating current Average power rms values. Key words. Electric battery. - PowerPoint PPT Presentation

Citation preview

Page 1: Electric Currents

Electric Currents

Physics Department, New York City College of Technology

Page 2: Electric Currents

Key words Electric battery Electric current Resistance Ohm’s law Resistivity Electric energy Electric power Direct current

Alternating current

Average power rms values

Page 3: Electric Currents

Electric battery

A battery produces electricity by transforming chemical energy into electrical energy.

Page 4: Electric Currents

Electric battery

In a diagram of a circuit, it is denoted by the symbol

+

Page 5: Electric Currents

Electric current

Electric current is a flow of charge

Page 6: Electric Currents

Electric current

Current is defined as I is current ∆Q is the amount of charge that

passes through the conductor at any location

Δt is the time interval The unit of I is ampere (A)

t

QI

Page 7: Electric Currents

Direction of electric current

Page 8: Electric Currents

Electrical resistance

Defined as R is the resistance of a wire V is the potential difference applied

across the wire I is the current

The symbol of a resistor is

I

VR

Page 9: Electric Currents

Electron motion model

Disc 17, #22

Page 10: Electric Currents

Ohm’s law Resistance R is a

constant independent of V, i.e.,

Experimentally found by Ohm

Generally holds in metal conductors in room temperature

IRV

Page 11: Electric Currents

Ohm’s law

Disc 17, #19 Disc 17, #20 Disc 17, #21

Page 12: Electric Currents

Resistivity

It is experimentally found that

ρ is resistivity and depends on the material

L is the length of a wire A is the cross-sectional area

A

LR

Page 13: Electric Currents

Resistivity

Page 14: Electric Currents

Example #1 A flashlight bulb draws

300mA from its 1.5-V battery. (a) What is the resistance of the bulb?(b) If the battery becomes weak and voltage drops to 1.2V, how would the current change?

Page 15: Electric Currents

Example #1—continued

AmA 3.0300 (a)

0.53.0

5.1

A

V

I

VR

(b) mAAV

R

VI 24024.0

0.5

2.1

Page 16: Electric Currents

Example #2

Connect stereo to speakers. (a) If each wire must be 20m long, what diameter copper wire should be used to keep the resistance less than 0.10 Ω? (b) If the current is 4.0A, what is the potential difference across each wire?

Page 17: Electric Currents

Example #2—continued

(a)

268

104.310.0

)20)(1068.1(m

mm

R

LA

m 81068.1 iscopper for

.08.22

,04.11004.1, 32

mmrd

mmmA

rrA

(b) VAIRV 4.0)1.0)(0.4(

Page 18: Electric Currents

Electric energy Energy transformation between

electric and other forms are very common

Motors transform electric energy into mechanical energy

In electric heaters and hair dryers, electric energy is transformed into thermal energy

In a lightbulb, electric energy is transformed into light and thermal energy

Page 19: Electric Currents

Electric power The electric power transformed by any

device is P is electric power I is current V is potential difference

The unit of electric power is Watt (W) For a resistance R, we have

IVP

RIIRIIVP 2)(

R

VV

R

VIVP

2

)(

Page 20: Electric Currents

Example #3 Calculate the

resistance of a 40-W automobile headlight designed for 12V.

Page 21: Electric Currents

Example #3—continued

6.3)40(

)12(

12,4022

W

V

P

VR

VVWP

Page 22: Electric Currents

Alternating current The voltage and current produced by an

electric generator are sinusoidal

V0 is the peak voltage I0 is the peak current The frequency f is the number of complete

oscillations per second, and

tR

V

R

VI

tVftVV

sin

sin2sin

0

00

f 2

Page 23: Electric Currents

DC and AC

Page 24: Electric Currents

AC power

The power transformed in a resistance R at any instant is

The average power is calculated as

or

tRIRIP 220

2 sin

RIP 202

1

R

VP

20

2

1

Page 25: Electric Currents

AC power—continued

Page 26: Electric Currents

rms (root-mean-square) values rms values and

peak values

The average power in rms values:

VV

VV

II

II

rms

rms

707.02

707.02

02

002

R

V

R

VP

RIRIP

VIP

rms

rms

rmsrms

220

220

2

1

2

1

Page 27: Electric Currents

Example #4

(a) Calculate the resistance and the peak current in a 1000-W hair dryer connected to a 120-V line. (b) What if it is connected to a 240-V line in Britain?

Page 28: Electric Currents

Example #4

(a) AV

W

V

PI

rmsrms 33.8

120

1000

AII rms 8.1120

4.1433.8

120

A

V

I

VR

rms

rms

(b) WV

R

VP rms 4000

4.14

)240( 22