In steady state, no current passes through the capacitor. Hence, the capacitor acts as an open circuit.
The circuit can be analyzed as follows:
1. Current \( i_2 = 0 \) through the capacitor.
2. The current \( i_1 \) in the resistors is determined by the total resistance of the branch excluding the capacitor.
The total resistance of the \( 6 \, \Omega \) and \( 4 \, \Omega \) resistors in series is:
\[
R_{\text{total}} = 6 + 4 = 10 \, \Omega.
\]
The current in the circuit is:
\[
i_1 = \frac{3}{R_{\text{total}}} = \frac{3}{10} = 0.3 \, \text{A}.
\]
The potential difference across the \( 6 \, \Omega \) resistor is:
\[
V = i_1 \cdot R = 0.3 \cdot 6 = 1.8 \, \text{V}.
\]
Since the capacitor is in parallel with the \( 6 \, \Omega \) resistor, the potential difference across the capacitor is also \( 1.8 \, \text{V} \).
The charge accumulated in the capacitor is:
\[
Q = C \cdot V,
\]
where \( C = 4 \, \mu\text{F} \) and \( V = 1.8 \, \text{V} \).
Substitute the values:
\[
Q = 4 \cdot 1.8 = 7.2 \, \mu\text{C}.
\]
Thus, the charge accumulated in the capacitor is \( \boxed{7.2 \, \mu\text{C}} \).