Embed
Email

27

Document Sample

Shared by: huanglianjiang1
Categories
Tags
Stats
views:
1
posted:
11/7/2011
language:
English
pages:
36
27 Current and

Resistance

27-1 Moving Charges and Electric Currents





electric currents——that is,

charges in motion.

a. A loop of copper in

electrostatic equilibrium.







b. This movement of charges

is a current i.

27-2 Electric Current









The current I through the conductor has the

Same value at planes aa`,bb`,cc`.

An electric current I in a conductor is defined by:









We can fine the charge that passes through the

plane in a time interval extending from 0 to t by

Integration:

The SI unit for current is the coulomb per

Second,also called the ampere(A):



1 ampere=1 A=1 coulomb per second=1C/s

The Direction of Currents



A current arrow is drawn in the direction in

which positive charge carriers would move,

Even if the actual charge carriers are

negative and move in the opposite direction.

CHECKPOINT 1









What are the magnitude and direction of the

current I in the lower right-hand wire?

Sample Problem 27-1

Step one:



charge electrons molecules

i= per per per

electron molecule second





or

Step two:



molecules molecules moles mass volume

per = per per unit per unit per

second mole mass volume second



Step three:

Step four:









Step five:

27-3 Current Density

Drift Speed

Sample Problem 27-2

Step one:









Step two:

(b)

Step one:







Step two:

Sample Problem 27-3

Step one:



atoms atoms moles mass

n= per unit = per per unit per unit

volume mole mass volume

Step two:









Step three:

Step four:

27-4 Resistance and Resistivity









1 ohm =1Ω=1 volt per ampere = 1V/A

definition of ρ









definition of σ

Calculating Resistance from

Resistivity





Resistance is a property of an object.

Resistivity is a property of a material.

Variation with Temperature

Sample Problem 27-4



Step one:





Step two:





Step three:

27-5 Ohm’s Law









Ohm’s law is an assertion that the current

through a device is always directly proportional

to the potential different applied to the device.

A conducting device obeys Ohm’s law when

the resistance of the device is independent

of the magnitude and polarity of the applied

difference.





A conducting material obeys Ohm’s law when

the resistivity of the material is independent

of the magnitude and direction of the applied

electric field.

27-6 A Microscopic View of

Ohm’s Law

Sample Problem 27-5

Step one:

Step two:

27-7 Power in Electric Circuits

or

Sample Problem 27-6

Step one:

Step two:

27-8 Semiconductors

27-9 Superconductors





Superconductors are materials that lose all

electrical resistance at low temperatures.



Related docs
Other docs by huanglianjiang...
friendorfoe2
Views: 0  |  Downloads: 0
contoterzi_tabella_c
Views: 0  |  Downloads: 0
Chapter 13
Views: 1  |  Downloads: 0
Dear Bishop Brom_
Views: 0  |  Downloads: 0
2008EarlyHybrids
Views: 0  |  Downloads: 0
Trent Draw 20070917
Views: 0  |  Downloads: 0
yearround
Views: 0  |  Downloads: 0
Brooke_Blazevich_Resume
Views: 0  |  Downloads: 0
FTSE_Shariah_Index_Review
Views: 6  |  Downloads: 0
By registering with docstoc.com you agree to our
privacy policy

You are almost ready to download!

You are almost ready to download!