The resistance of a conductor is given by:
R = ῤ L / A
Where R is resistance, ῤ is resistivity of the material, L is the length of the conductor, and A is its cross-sectional area.
Resistance is directly proportional to the length of the conductor. A longer conductor has more collisions of electrons with ions, hence greater opposition to current. Doubling the length doubles the resistance.
Thicker wires have larger cross-sectional area. Since resistance is inversely proportional to area, a thicker wire allows more electrons to flow simultaneously, reducing resistance.
* In metals, resistance increases with rise in temperature because atomic vibrations increase collisions.
* In semiconductors, resistance decreases with rise in temperature since more electrons gain energy to conduct.
Alloys have resistances that remain nearly constant with temperature (low temperature coefficient). This makes them stable and reliable for use in standard resistors and measuring instruments.
Impurities disturb the regular lattice structure of the conductor, increasing electron scattering and collisions. This raises the resistance. Controlled impurities are used in alloys to achieve desired resistance.
When a wire is stretched:
* Its length increases.
* Its cross-sectional area decreases.
Since R α L / A, the resistance increases significantly. This principle is used in strain gauges.