When the switch is closed at t = 0, the left capacitor, which was fully charged, begins to discharge while the right capacitor starts to charge. The charge on the right capacitor can be expressed as q = cV/2 (1 - 1/2 e^(-t/RC)), indicating that it reaches a maximum charge of CV/2 over time. Initially, the left capacitor's charge distributes equally between both capacitors, leading to each having a charge of CV/4 immediately after the switch closes. The battery's role becomes negligible at the moment of switch closure, as the charge rearranges instantaneously between the capacitors. Understanding the initial conditions and the behavior of the capacitors is crucial for solving the problem accurately.