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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

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