Download presentation
Presentation is loading. Please wait.
Published byShavonne Haynes Modified over 9 years ago
2
27 Current and Resistance 27-1 Moving Charges and Electric Currents electric currents——that is, charges in motion.
3
a.A loop of copper in electrostatic equilibrium. b. This movement of charges is a current i.
4
27-2 Electric Current The current I through the conductor has the Same value at planes aa`,bb`,cc`.
5
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:
6
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
7
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.
8
CHECKPOINT 1 What are the magnitude and direction of the current I in the lower right-hand wire? What are the magnitude and direction of the current I in the lower right-hand wire?
9
Sample Problem 27-1 charge electrons molecules i= per per per electron molecule second Step one: or
10
Step two: molecules molecules moles mass volume per = per per unit per unit per second mole mass volume second Step three:
11
Step four: Step five:
12
27-3 Current Density
13
Drift Speed
14
Sample Problem 27-2 Step one: Step two:
15
(b) Step one: Step two:
16
Sample Problem 27-3 atoms atoms moles mass n= per unit = per per unit per unit volume mole mass volume Step one:
17
Step two: Step three:
18
Step four:
19
27-4 Resistance and Resistivity 1 ohm =1Ω = 1 volt per ampere = 1V/A
20
definition of ρ definition of σ
21
Calculating Resistance from Resistivity Resistance is a property of an object. Resistivity is a property of a material.
23
Variation with Temperature
24
Sample Problem 27-4 Step one: Step two: Step three:
25
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.
26
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
27-6 A Microscopic View of Ohm ’ s Law
29
Sample Problem 27-5 Step one:
31
Step two:
32
27-7 Power in Electric Circuits
33
or
34
Sample Problem 27-6 Step one:
35
Step two:
36
27-8 Semiconductors
37
27-9 Superconductors Superconductors are materials that lose all electrical resistance at low temperatures.
Similar presentations
© 2025 SlidePlayer.com. Inc.
All rights reserved.