The efficiency \( \eta \) of a heat engine is given by the Carnot efficiency formula:
\[
\eta = 1 - \frac{T_{\text{sink}}}{T_{\text{source}}}
\]
Where:
- \( T_{\text{sink}} \) is the temperature of the sink (in Kelvin),
- \( T_{\text{source}} \) is the temperature of the source (in Kelvin).
Given:
- \( T_{\text{source}} = 127^\circ C = 400 \, \text{K} \),
- \( T_{\text{sink}} = 27^\circ C = 300 \, \text{K} \).
### Step 1: Initial Efficiency
The initial efficiency is:
\[
\eta_{\text{initial}} = 1 - \frac{300}{400} = 1 - 0.75 = 0.25
\]
### Step 2: Final Efficiency
We want to double the efficiency, so the new efficiency \( \eta_{\text{final}} \) should be:
\[
\eta_{\text{final}} = 2 \times \eta_{\text{initial}} = 2 \times 0.25 = 0.50
\]
### Step 3: Solve for New Temperature of Source
Using the Carnot efficiency formula for the final efficiency:
\[
0.50 = 1 - \frac{300}{T_{\text{source, final}}}
\]
Solving for \( T_{\text{source, final}} \):
\[
\frac{300}{T_{\text{source, final}}} = 0.50
\]
\[
T_{\text{source, final}} = \frac{300}{0.50} = 600 \, \text{K}
\]
### Step 4: Increase in Temperature
The increase in the temperature of the source is:
\[
\Delta T = 600 - 400 = 200 \, \text{K} = 200^\circ C
\]
Thus, the temperature of the source needs to be increased by:
\[
\boxed{(B) \, 200^\circ C}
\]