Ohm's law in its microscopic form relates the electric field $\vec{E}$ in a conductor to the current density $\vec{j}$ by: \[ \vec{j} = \sigma \vec{E} \] Here, $\sigma$ is the conductivity of the material. To find the electric field in terms of current density, rearrange the equation: \[ \vec{E} = \frac{1}{\sigma} \vec{j} \] Since resistivity $\rho = \frac{1}{\sigma}$, we substitute: \[ \vec{E} = \rho \vec{j} \] Thus, the correct form of Ohm's law in terms of resistivity is $\vec{E} = \rho \vec{j}$.
Ohm’s law in terms of conductivity and resistivity is: \[ E = ρj \] where:
E is the electric field,
j is the current density,
ρ is the resistivity.
Alternatively, using the relationship \( \sigma = 1 / \rho \), you can express current density as: \[ j = \sigma E \] This is consistent with the definition of resistivity and conductivity. Thus, the correct answer is \( E = ρj \).