Analyzing the Circuit Structure
When tackling mixed capacitor circuits, the first and most crucial step is to clearly identify which components are in series and which are in parallel. Looking at our circuit diagram, we can see that the total charge Q supplied by the battery flows entirely through capacitor C1.
After passing through C1, the circuit splits into two branches at a junction. One branch contains C2 and the other contains C3. Because these two capacitors are connected across the same two nodes, they are in a parallel combination. This entire parallel block is, in turn, connected in series with C1.
The Power of Parallel Connections
A fundamental property of parallel circuits is that the potential difference (voltage) across all parallel branches is identical. The problem states that the voltage across C2 is 20 V.
Because C3 is in parallel with C2, it must share the exact same voltage. Therefore, we immediately know that V3=20 V. This is a massive stepping stone because we now have both the capacitance (C3=8μF) and the voltage (V3=20 V) for the third capacitor.
Using the core electrostatic formula Q=CV, we can calculate the charge stored on C3:
Q3=C3×V3
Q3=8μF×20 V=160μC
Applying Charge Conservation
Now, let's trace the flow of charge. The total charge Q=750μC arrives at the junction and must split between the two parallel branches. According to the principle of conservation of charge, the total incoming charge must equal the sum of the outgoing charges in the branches.
Mathematically, this is expressed as:
The Final Calculation
We know the total charge is 750μC and we just found that 160μC goes to C3. Substituting these values into our conservation equation gives us a simple linear equation to solve for Q2:
Subtracting 160μC from both sides, we find the charge on C2:
And there we have it! The charge on capacitor C2 is 590μC.