The efficiency of a Carnot engine is given by the formula:
\[
\eta = 1 - \frac{T_2}{T_1}
\]
Where:
- \( \eta \) is the efficiency,
- \( T_1 \) is the temperature of the reservoir (hot body),
- \( T_2 \) is the temperature of the sink (cold body).
Now, if the temperature of the reservoir is increased by 50%, the new temperature \( T_1' \) will be:
\[
T_1' = 1.5 \times T_1
\]
If the temperature of the sink is decreased by 50%, the new temperature \( T_2' \) will be:
\[
T_2' = 0.5 \times T_2
\]
Thus, the new efficiency \( \eta' \) will be:
\[
\eta' = 1 - \frac{T_2'}{T_1'} = 1 - \frac{0.5 \times T_2}{1.5 \times T_1}
\]
Simplifying:
\[
\eta' = 1 - \frac{T_2}{3T_1} = \frac{3T_1 - T_2}{3T_1}
\]
Since \( \eta = 1 - \frac{T_2}{T_1} \), the original efficiency is \( \eta = \frac{T_1 - T_2}{T_1} \).
Thus, the new efficiency \( \eta' \) becomes:
\[
\eta' = \frac{3(T_1 - T_2)}{3T_1} = \frac{200 \eta}{3}
\]
Hence, the new efficiency is \( \frac{200\eta}{3} \).