The integral form: $\frac{d q}{d t}+\oint_{S} \vec{j} \cdot d \vec{S}=0$
The differential form: ${\frac {\partial \rho }{\partial t}}+\nabla \cdot \vec{j} =0$
How to intuitively understand the change from total derivative to partial?
The integral form: $\frac{d q}{d t}+\oint_{S} \vec{j} \cdot d \vec{S}=0$
The differential form: ${\frac {\partial \rho }{\partial t}}+\nabla \cdot \vec{j} =0$
How to intuitively understand the change from total derivative to partial?
In answer to first question:
The quantity $q$ is the total charge of the system, so it’s not going to vary across space (because it’s the sum charge), so it can only vary across time.
However, the quantity $\rho$ is a charge density. The distribution of charge can vary across space (some areas have more charge/volume than others). It can also vary across time. Because it has multiple parameters, we have to take a partial derivative.