Question
The Picture — before & after
Joining by a wire forces both to one potential, but the total charge is unchanged. That single conservation law pins down the unknown capacity.
Concept
Charge before = charge after: \(C_1V_1+C_2V_2=(C_1+C_2)V_c.\) The common potential is the charge-weighted average of the two starting potentials.
Method & Steps
Easy Trick
The common potential lands closer to whichever conductor holds more charge. 4.6 is \(0.6\) above 4 and \(0.4\) below 5, a \(3:2\) split — so the unknown carries \(3/2\) the charge-influence of the 2-unit one ⇒ \(C_2 = 3\). (Lever rule: \(C_1(V_c-V_1)=C_2(V_2-V_c)\).)
Question
The Circuit
The 2 µF and 4 µF share the same two nodes → parallel (= 6 µF). That block is in series with the single 6 µF, all driven by 12 V.
Concept
Series chain carries one common charge \(Q\). Find \(Q\) from \(C_{eq}\), then the parallel block’s voltage is \(Q/C_{block}\) — and the 2 µF, being inside that block, shares exactly that voltage.
Method & Steps
Easy Trick
Two equal blocks in series (6 µF and \(2\!\parallel\!4=6\,\mu F\)) split the 12 V evenly → 6 V each. Every capacitor inside the parallel block sees that same 6 V, so the 2 µF reads 6 V directly.