If an $emf$ leaves from point A, the concepts at play in the following diagram are straightforward:
at any time, the $I_{R}$ = $I_{c}$
as time increases, $\Delta V$ across $R$ decreases and it increases across $C$.
If I added another resistor, $R_{2}$, after capacitor $C$, what would the new resistor's current be?
My logic was that resistor two's current initially = 0, because charge first accumulates on the capacitor before it can travel onwards. $I_{R2}$ increases afterwards
My textbook claims, however, that $I_{R}$ = $I_{2R}$ = $I_{C}$. I disagree. How can $I_{2R}$ = $I_{C}$. If that were true, and the coulombs of charge passing through $C$ all continued to $R_{2}$, $C$ wouldn't accumulate any charge.