The efficiency of the Rankine cycle is given by:
\[
\eta = \frac{\text{Net Work Output}}{\text{Total Heat Input}} = \frac{W_{\text{HP}} + W_{\text{LP}} - W_{\text{pump}}}{Q_{\text{in}}}
\]
Where:
- \( W_{\text{HP}} = 400 \, \text{kJ/kg} \) is the work output in the high-pressure turbine,
- \( W_{\text{LP}} = 850 \, \text{kJ/kg} \) is the work output in the low-pressure turbine,
- \( W_{\text{pump}} = 15 \, \text{kJ/kg} \) is the pump work.
The total work output is:
\[
W_{\text{total}} = W_{\text{HP}} + W_{\text{LP}} - W_{\text{pump}} = 400 + 850 - 15 = 1235 \, \text{kJ/kg}.
\]
Now, using the given cycle efficiency (\( \eta = 32% = 0.32 \)):
\[
0.32 = \frac{1235}{Q_{\text{in}}}
\]
Solving for \( Q_{\text{in}} \):
\[
Q_{\text{in}} = \frac{1235}{0.32} = 3859.375 \, \text{kJ/kg}.
\]
The heat rejected in the condenser \( Q_{\text{out}} \) is:
\[
Q_{\text{out}} = Q_{\text{in}} - W_{\text{total}} = 3859.375 - 1235 = 2624.375 \, \text{kJ/kg}.
\]
Thus, the heat rejected in the condenser is \( \boxed{2620.00} \, \text{kJ/kg} \).