The efficiency \(\eta\) of a Carnot engine is given by:
\[
\eta = 1 - \frac{T_c}{T_h}
\]
where \(T_c\) is the temperature of the cold reservoir (sink) and \(T_h\) is the temperature of the hot reservoir (source). Initially, the efficiency is 25%, with \(T_c = 300 \, {K}\), so:
\[
0.25 = 1 - \frac{300}{T_h} \Rightarrow T_h = \frac{300}{0.75} = 400 \, {K}
\]
To achieve 50% efficiency:
\[
0.50 = 1 - \frac{300}{T_h'} \Rightarrow T_h' = \frac{300}{0.50} = 600 \, {K}
\]
The increase in the temperature of the source is:
\[
\Delta T = T_h' - T_h = 600 \, {K} - 400 \, {K} = 200 \, {K}
\]