Given:
\[
h_1 = 3344 \, \text{kJ/kg}, \quad s_1 = 6.5 \, \text{kJ/kg$\cdot$K}, \quad \eta_{\text{turbine}} = 0.9, \quad \dot{m} = 102 \, \text{kg/s}
\]
From steam tables (assuming isentropic expansion), let:
\[
h_{2s} = 2230 \, \text{kJ/kg}
\]
Using the isentropic efficiency formula:
\[
\eta_{\text{turbine}} = \frac{h_1 - h_2}{h_1 - h_{2s}}
\Rightarrow h_2 = h_1 - \eta_{\text{turbine}} \cdot (h_1 - h_{2s})
\]
\[
h_2 = 3344 - 0.9 \cdot (3344 - 2230) = 3344 - 0.9 \cdot 1114 = 3344 - 1002.6 = 2341.4 \, \text{kJ/kg}
\]
Power output:
\[
\dot{W}_{\text{turbine}} = \dot{m} \cdot (h_1 - h_2) = 102 \cdot (3344 - 2341.4) = 102 \cdot 1002.6 = 102265.2 \, \text{kW}
\]
\[
\dot{W}_{\text{turbine}} = \frac{102265.2}{1000} = \boxed{102.3 \, \text{MW}}
\]