Introductory Physics Volume Two
Introductory Physics Volume Two
Introductory Physics Volume Two
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3.3 Ohm’s Law 59<br />
Some materials, such a copper, allow charge to pass through it<br />
with very little resistance, and therefore it takes very little electric field<br />
to sustain a large current. Other materials, such a carbon, resist the<br />
flow of charge, and it requires more electric field to sustain the same<br />
current. Carbon is more resistive. This property is quantified in the<br />
following law.<br />
Fact: Ohm’s Law: Resistivity<br />
For many materials the current density and the electric field are<br />
proportional.<br />
⃗J = σ ⃗ E<br />
The constant σ is called the conductivity and depends on the material.<br />
The inverse of the conductivity is called the resistivity:<br />
ρ = 1/σ.<br />
Not all materials follow this relationship: those that do are called<br />
ohmic materials, those that do not are called non-ohmic.<br />
Here is a table with the resistivity of a few materials.<br />
Material Resistivity(×10 −8 Ω · m)<br />
Silver 1.6<br />
Copper 1.7<br />
Aluminum 2.8<br />
Tungsten 5.5<br />
Iron 10<br />
Nichrome 100<br />
Carbon 3500<br />
Silcon 64000000000<br />
Wood 1000000000000000<br />
Amber 50000000000000000000000<br />
Imagine a piece of conductive material, with two terminals connected<br />
to it, and with a current I passing into the material through<br />
terminal a and draining out through terminal b. Such a circuit element<br />
is called a Resistor.<br />
In order to sustain this current there will need to be an electric field<br />
in the conductor going from terminal a to terminal b. Thus there will