An applied electric field \( E \) causes free electrons to accelerate, resulting in an average drift velocity \( v_d \). The equation of motion is:
\[ v_d = \frac{e E \tau}{m} \]
Current density \( J \) is the product of electron number density, electron charge, and drift velocity:
\[ J = n e v_d \]
Substituting \( v_d \):
\[ J = n e \left( \frac{e E \tau}{m} \right) = \frac{n e^2 \tau}{m} E \]
Ohm's Law states the relationship between current density \( J \) and electric field \( E \):
\[ J = \sigma E \]
where \( \sigma \) is conductivity. Equating the coefficients of \( E \) from both expressions for \( J \) yields conductivity \( \sigma \):
\[ \sigma = \frac{n e^2 \tau}{m} \]
Resistivity \( \rho \) is the reciprocal of conductivity. Therefore:
\[ \rho = \frac{1}{\sigma} = \frac{m}{n e^2 \tau} \]
The resistivity \( \rho \) is calculated as:
\[ \rho = \frac{m}{n e^2 \tau} \]