Drift velocity and mobility are key concepts in understanding the flow of electric current through a conductor. This article explains these concepts starting from the basic idea of charge flow, leading to drift velocity, and then to mobility.
When a potential difference V is applied across a conductor of length l, it produces an electric field E inside the conductor:
E = V / l
Consider a conductor with cross-sectional area A and length l. Let n be the number of free electrons per unit volume, and e the charge of an electron.
The total charge q contributed by electrons in the volume Al can be expressed as:
q = n × e × A × l
If this charge q flows in time t, then current I is:
I = q / t = (n × e × A × l) / t
Since velocity is distance over time, and here electrons drift a length l in time t:
vd = l / t
Substitute into the equation:
I = n × e × A × vd
⇒ vd = I / (n × e × A)
This shows that:
Mobility μ is defined as the drift velocity per unit electric field:
μ = vd / E
Substituting E = V / l and vd = l / t gives:
μ = (l / t) / (V / l) = l² / (V × t)
Alternatively, using microscopic theory, mobility is given by:
μ = e × τ / m
Mobility depends on the following factors:
Understanding drift velocity and mobility is crucial for analyzing current flow in conductors, semiconductors, and nanomaterials—making these concepts highly important for exams.