To solve this problem, we need to understand the behavior of capacitors in circuits over time, specifically when they are discharging.
Given that capacitors \( A \) and \( B \) are initially charged to a potential \( V = 5 \, \text{V} \) and connected in two different circuits at time \( t = 0 \), we need to calculate the charge on each capacitor at time \( t = CR \).
Thus, at time \( t = CR \), we have:
Therefore, the correct answer is:
A circuit consisting of a capacitor C, a resistor of resistance R and an ideal battery of emf V, as shown in figure is known as RC series circuit. 
As soon as the circuit is completed by closing key S₁ (keeping S₂ open) charges begin to flow between the capacitor plates and the battery terminals. The charge on the capacitor increases and consequently the potential difference Vc (= q/C) across the capacitor also increases with time. When this potential difference equals the potential difference across the battery, the capacitor is fully charged (Q = VC). During this process of charging, the charge q on the capacitor changes with time t as
\(q = Q[1 - e^{-t/RC}]\)
The charging current can be obtained by differentiating it and using
\(\frac{d}{dx} (e^{mx}) = me^{mx}\)
Consider the case when R = 20 kΩ, C = 500 μF and V = 10 V.