Consider that a wire of length l and area of cross-section A be subjected to an electric field of strength E.
If V = Potential difference applied across the end of the wire,
∴ E = \(\frac{V}{l}\) or V = EI

Let n = number of free electrons per unit volume of the conductor,
vd = Drift velocity of electrons
∴ Charge flowing through the conductor wire,
q = n Ale
Time taken by the electrons to cross the conductor,
t = \(\frac{\text { Distance }}{\text { Velocity }} = \frac{l}{v_d}\)
Current I = \(\frac{\text {Charge} }{\text {time}} = \frac{nAle}{\frac{l}{v_d}}\)
I = n vd Ae ........................(1)
This is the required relation between current and drift velocity.
Since n, A and e are constants,
∴ I ∝ vd
Hence, the current flowing through a conductor is directly proportional to the drift velocity. The small value of drift velocity (is 10-3 ms-1) produces a large amount of electric current, due to the presence of extremely large number of free electrons in a conductor.
I = nvd eA
∴ Current density,
J = \(\frac{I}{A}\) = nevd
or J ∝ vd