Download Resistivity

Survey
yes no Was this document useful for you?
   Thank you for your participation!

* Your assessment is very important for improving the workof artificial intelligence, which forms the content of this project

Document related concepts

Maxwell's equations wikipedia , lookup

Electromagnet wikipedia , lookup

Lorentz force wikipedia , lookup

Superconductivity wikipedia , lookup

History of electromagnetic theory wikipedia , lookup

Electrostatics wikipedia , lookup

Electric charge wikipedia , lookup

Metadyne wikipedia , lookup

Electrical resistivity and conductivity wikipedia , lookup

Electrical resistance and conductance wikipedia , lookup

Transcript
Chapter 27
Current and Resistance
Dr. Jie Zou
PHY 1361
1
Outline

Electric current (27.1)



Definition for current
Microscopic model of current
Resistance (27.2)




Current density
Ohm’s law
Resistance
Conductivity and resistivity
Dr. Jie Zou
PHY 1361
2
Electric current


Whenever there is a net flow
of charge through some
region, an electric current
is said to exist.
Definition of electric current:
The current is the time rate
at which charge flows
through this surface.


Charges in motion
through an area A.
Dr. Jie Zou

Average current: Iav = Q/t.
Instantaneous current: I =
dQ/dt
SI unit of current: ampere (A),
1 A = 1C/s
PHY 1361
3
Electric current (cont.)

Direction of the current:



It is conventional to assign to the current the
same direction as the flow of positive charge.
The direction of the current is opposite the
direction of flow of electrons.
It is common to refer to a moving charge
(positive or negative) as a mobile charge
carrier.

For example, the mobile charge carriers in a metal
are electrons.
Dr. Jie Zou
PHY 1361
4
Quick Quiz 27.1

Consider positive and negative charges moving
horizontally through the four regions shown in the
figure below. Rank the current in these four regions,
from lowest to highest.
Dr. Jie Zou
PHY 1361
5
Microscopic model of current

We can relate current to the motion
of the charge carriers by describing
a microscopic model of conduction
in a metal.





Dr. Jie Zou
n: charge carrier density or the number
of mobile charge carriers per unit
volume.
vd: drift speed.
q: the charge on each carrier.
Q = the total charge in the gray
section = (nA x)q = (nAvd t)q
Current in a conductor in terms of
microscopic quantities:
Iav = Q/t = nqvdA.
PHY 1361
6
More about the drift speed vd



Dr. Jie Zou
When a potential difference is
applied across the conductor,
an electric field is set up in the
conductor; this field exerts an
electric force on the electrons,
producing a current.
The resultant motion of
electrons is zigzag due to
repeated collisions with the
metal atoms.
The electrons move slowly
along the conductor at the
drift velocity vd.
PHY 1361
7
Example 27.1 Drift speed in a
copper wire

A copper wire has a cross-sectional area
of 3.31 x 10-6 m2. If it carries a current
of 10.0 A, what is the drift speed of the
electrons? Assume that each copper
atom contributes one free electron tot
eh current. The density of copper is
8.95 g/cm3.

Answer = 2.22 x 10-4 m/s – Typical drift
speeds are Very low!
Dr. Jie Zou
PHY 1361
8
Resistance

Current density J: current per unit area.




Georg Simon
Ohm (17891854)
A current density J and an electric field E are
established in a conductor whenever a
potential difference is maintained across the
conductor.
Ohm’s law: For many materials (most
metals), the ratio of the current density to
the electric field is a constant  that is
independent of the electric field producing
the current.


Dr. Jie Zou
J  I/A = nqvd. (SI unit: A/m2)
Current density is a vector quantity: J = nqvd.
J = E; : conductivity of the conductor.
Materials that obey Ohm’s law are said to be
ohmic; otherwise, nonohmic.
PHY 1361
9
Resistance of a uniform
material along the length l

 l 
V    I  RI
 A 
It can be shown that
 R = l/A = the resistance of the
conductor.
Definition of resistance: R  V/I.
 SI unit of R: ohm (); 1   1V/1A
Resistivity :  = 1/




SI unit of : m
Resistance of a uniform block of
l
material along the length l: R  
A

Dr. Jie Zou
R depends on the geometry as well as on
resistivity of the substance (see Table 27.1).
PHY 1361
10
Examples


Example 27.2: The resistance of a conductor
Calculate the resistance of an Al cylinder that
has a length of 10.0 cm and a cross-sectional
area of 2.00 x 10-4 m2.
Example 27.3: (A) Calculate the resistance
per unit length of a Nichrome wire, which has
a radius of 0.321 mm. (B) If a potential
difference of 10 V is maintained across a 1.0m length of the Nichrome wire, what is the
current in the wire?
Dr. Jie Zou
PHY 1361
11