Concept:
At steady state in a DC circuit:
• Capacitor behaves as an open circuit.
• No current flows through the capacitor branch.
• First solve the resistive network to find the potential difference across the capacitor.
• Then use
\[
q = C\Delta V
\]
Step 1:Open the capacitor branch.
Since steady state is reached,
\[
i_C = 0
\]
Thus the remaining circuit contains only resistors.
Step 2:Find equivalent resistance of the network.
After simplification,
\[
R_{eq} = 10\Omega
\]
Step 3:Find total current from the battery.
\[
I = \frac{V}{R}
\]
\[
I = \frac{12}{10}
\]
\[
I = 1.2\,A
\]
Step 4:Determine branch currents.
Current divides equally through the two \(20\Omega\) resistors:
\[
I_1 = I_2 = \frac{I}{2} = 0.6\,A
\]
Further current division gives
\[
I_3 = I_4 = \frac{I_2}{2} = 0.3\,A
\]
Step 5:Find potential difference across the capacitor.
Voltage across the \(10\Omega\) resistor:
\[
\Delta V = IR
\]
\[
\Delta V = 0.3 \times 10
\]
\[
\Delta V = 3\,V
\]
Step 6:Calculate charge on the capacitor.
\[
q = C\Delta V
\]
\[
q = 6\mu F \times 3
\]
\[
q = 18\,\mu C
\]
\[
\boxed{q = 18\,\mu C}
\]