Step 1: Identify the given parameters.
Heat supplied to the engine, \( Q_H = 250 \, \text{kJ/s} \).
Temperature at which heat is supplied, \( T_H = 227^\circ\text{C} = 227 + 273 = 500 \, \text{K} \).
Temperature at which heat is rejected, \( T_C = 27^\circ\text{C} = 27 + 273 = 300 \, \text{K} \).
The cycle is reversible, which implies it is a Carnot cycle operating between these two temperatures.
Step 2: Recall the efficiency of a reversible (Carnot) heat engine.
The efficiency \( \eta \) of a Carnot heat engine is given by:
\[
\eta = 1 - \frac{T_C}{T_H} = \frac{W_{net}}{Q_H},
\]
where \( W_{net} \) is the net work done by the engine.
Step 3: Calculate the efficiency of the Carnot cycle.
Using the given temperatures:
\[
\eta = 1 - \frac{300 \, \text{K}}{500 \, \text{K}} = 1 - 0.6 = 0.4.
\]
So, the efficiency of the reversible heat engine is 40%.
Step 4: Relate the heat rejected \( Q_C \) to the heat supplied \( Q_H \) and the net work done \( W_{net} \).
From the first law of thermodynamics for a cycle:
\[
Q_H - Q_C = W_{net}.
\]
Also, we know that \( \eta = \frac{W_{net}}{Q_H} \), so \( W_{net} = \eta Q_H \).
Step 5: Calculate the net work done by the engine.
\[
W_{net} = \eta Q_H = 0.4 \times 250 \, \text{kJ/s} = 100 \, \text{kJ/s}.
\]
Step 6: Calculate the amount of heat rejected \( Q_C \).
Using the first law of thermodynamics:
\[
Q_C = Q_H - W_{net} = 250 \, \text{kJ/s} - 100 \, \text{kJ/s} = 150 \, \text{kJ/s}.
\]
Alternatively, for a reversible heat engine, the ratio of heat transferred is proportional to the ratio of absolute temperatures:
\[
\frac{Q_C}{Q_H} = \frac{T_C}{T_H}.
\]
\[
Q_C = Q_H \times \frac{T_C}{T_H} = 250 \, \text{kJ/s} \times \frac{300 \, \text{K}}{500 \, \text{K}} = 250 \times 0.6 = 150 \, \text{kJ/s}.
\]
Step 7: Select the correct answer.
The amount of heat rejected is 150 kJ/s, which corresponds to option 2.