My electromagnetics textbook has a picture of an $RC$ circuit with a current source.
As you can see, there are three current density vectors, $J_i$, $J_c$, and $J_d$. The book labels them as follows:
$J_i =$ impressed (source) electric current density
$J_c =$ conduction electric current density
$J_d =$ displacement electric current density = $\frac{\partial D}{ \partial t}$, where $D$ is electric flux density
It then uses this figure to explain the following Maxwell equation:
$\text{curl }H = J_i + J_c + J_d$, where $H$ is magnetic field intensity
What I don't understand is... Isn't $J_i$ the same as $J_c$? I'm getting this from the idea that if you do a Kirchhoff Current Law evaluation at the top left node (between the source and resistor), then $J_i$ is going in and $J_c$ is going out, thereby making them equal? ... So wouldn't this mean that $J_i$ and $J_c$ are the same current? And if they're the same current, then doesn't that mean that the Maxwell equation is counting it twice?
I'm looking for a solid explanation of why $J_i$ is different than $J_c$, despite Kirchhoff's Current Law.