Relaxation time of free electrons drifting in a conductor is the average time elapsed between two successive collisions.
Deduction of Ohm’s Law: Consider a conductor of length l and cross-sectional area A. When a potential difference V is applied across its ends, the current produced is I. If n is the number of electrons per unit volume in the conductor and vd the drift velocity of electrons, then the relation between current and drift velocity is
I = – neAvd …(i)
Where – e is the charge on electron (e = 1.6 × 10–19 C)
Electric field produced at each point of wire, \(E=\frac{V}{l}\) (ii)
If τ is relaxation time and E is electric field strength, then drift velocity


Current density \(J(=\frac{I}{A})=\frac{ne^2\,r}{mI}V.\)
This is relation between current density J and applied potential difference V.
Under given physical conditions (temperature, pressure) for a given conductor

∴ This constant is called the resistance of the conductor (i.e. R).

This is Ohm’s law. From equation (vi) it is clear that the resistance of a wire depends on its length (l), cross-sectional area (A), number of electrons per m3 (n) and the relaxation time (τ)
Expression for resistivity:

Clearly, resistivity of a conductor is inversely proportional to number density of electrons and relaxation time.
Resistivity of the material of a conductor depends upon the relaxation time, i.e., temperature and the number density of electrons.
This is because constantan and manganin show very weak dependence of resistivity on temperature.