Step 1: Understanding the Concept:
When the charged capacitor, already disconnected from its battery, is connected in parallel with an uncharged one, charge flows until both have the same potential. The total charge does not change.
Step 2: Initial charge.
\(Q = C_1V_1\).
Step 3: Final state.
The capacitors in parallel have capacitance \(C_1 + C_2\) and common potential \(V_2\), so
\[ V_2 = \frac{Q}{C_1 + C_2} = \frac{C_1V_1}{C_1 + C_2} \]
Step 4: Check the options.
Options (A), (C) and (D) divide by the wrong capacitance or use the wrong charge.
Final Answer:
The common potential is \(\dfrac{C_1V_1}{C_1 + C_2}\), option (B).
\[ \boxed{\frac{C_1V_1}{C_1+C_2}} \]