According to Gauss's law, the electric flux through a surface is proportional to the net charge enclosed by the surface:
\[
\Phi_E = \frac{Q_{\text{enc}}}{\varepsilon_0}
\]
The total charge enclosed by the surface \( S_2 \) is the sum of the charges inside \( S_1 \) and the charge \( Q \) placed between \( S_1 \) and \( S_2 \). Therefore, the total charge enclosed by \( S_2 \) is:
\[
Q_{\text{enc}} = q_1 + q_2 + q_3 + Q
\]
The flux through surface \( S_1 \) is proportional to the charge inside it:
\[
\Phi_{S_1} = \frac{q_1 + q_2 + q_3}{\varepsilon_0}
\]
The flux through surface \( S_2 \) is four times the flux through \( S_1 \):
\[
\Phi_{S_2} = 4 \cdot \Phi_{S_1} = \frac{4 \cdot (q_1 + q_2 + q_3)}{\varepsilon_0}
\]
Using Gauss's law for \( S_2 \):
\[
\Phi_{S_2} = \frac{q_1 + q_2 + q_3 + Q}{\varepsilon_0}
\]
Equating the two expressions for \( \Phi_{S_2} \):
\[
\frac{4 \cdot (q_1 + q_2 + q_3)}{\varepsilon_0} = \frac{q_1 + q_2 + q_3 + Q}{\varepsilon_0}
\]
Solving for \( Q \):
\[
4 \cdot (q_1 + q_2 + q_3) = q_1 + q_2 + q_3 + Q
\]
\[
Q = 3 \cdot (q_1 + q_2 + q_3)
\]
Substituting the values of \( q_1 \), \( q_2 \), and \( q_3 \):
\[
Q = 3 \cdot (-3 \, \mu C - 2 \, \mu C + 9 \, \mu C) = 3 \cdot 4 \, \mu C = 12 \, \mu C
\]
Thus, the charge \( Q \) is \( 12 \, \mu C \).