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Lorentz force (per unit 3-volume) f on a continuous charge distribution (charge density ρ) in motion. The 3-current density J corresponds to the motion of the charge element dq in volume element dV and varies throughout the continuum.
$$I=\iint_{\partial\lambda}{\textbf{J}\cdot d \textbf{S}}=\frac{dq}{dt}$$
I hope is help. In fact, Maxwell there was no tensor knowledge, was ONLY calculus of numbers and vector! He work each number out for each vector! Amazing!
Divergence theorem is mathematical identity which says in calculus:
$$\frac{\partial{\rho}}{\partial{t}}+\nabla \cdot \textbf{J}$$
Yes? Is worked backwards:
$$I=\iint_{\partial\lambda}{\textbf{J}\cdot d \textbf{S}}=\frac{dq}{dt}$$
I hope is help. In fact, Maxwell there was no tensor knowledge, was ONLY calculus of numbers and vector! He work each number out for each vector! Amazing!