The induced emf (\( \mathcal{E} \)) in the circuit is given by Faraday's law:
\[
\mathcal{E} = -N \frac{\Delta \Phi_B}{\Delta t},
\]
where \( N = 100 \) is the number of turns, and \( \Delta \Phi_B \) is the change in magnetic flux.
The total change in magnetic flux (\( \Delta \Phi_B \)) is:
\[
\Delta \Phi_B = A \Delta B,
\]
where \( A = 24 \, \text{cm}^2 = 24 \times 10^{-4} \, \text{m}^2 \) is the cross-sectional area, and \( \Delta B = 2 \times 1.5 = 3 \, \text{T} \) is the change in magnetic field (from \( 1.5 \, \text{T} \) in one direction to \( 1.5 \, \text{T} \) in the opposite direction).
Substitute values:
\[
\Delta \Phi_B = 24 \times 10^{-4} \times 3 = 7.2 \times 10^{-3} \, \text{Wb}.
\]
The total emf induced is:
\[
\mathcal{E} = \frac{N \Delta \Phi_B}{R},
\]
where \( R = 12 \, \Omega \).
Substitute \( N = 100 \):
\[
\mathcal{E} = \frac{100 \cdot 7.2 \times 10^{-3}}{12} = 6 \times 10^{-3} \, \text{C}.
\]
Thus, the charge flowing through the circuit is \( \boxed{60 \, \text{mC}} \).