From the relation,
η = 1 − \(\frac{T_2}{T_1}\)
or, \(\frac{T_2}{T_1}\) = 1 - \(\frac{30}{100}\) = \(\frac{7}{10}\)
or, T1 = \(\frac{10T_2}{7}\) = \(\frac{10\times200}{7}\)= 285.71 K
New efficiency is now 50%,
η' = 1 − \(\frac{T_2}{T_1}\)
\(\frac{T_2}{T_1}\) = 1 - η'
\(\frac{T_2}{T_1}\) = 1 - \(\frac{50}{100}\) or \(\frac{1}{2}\)
2T2 = T1
or, T1 = 2 × 200 K
T1 = 400 K
Now increase in temperature of source,
= 400 K – 285.71 K
= 114.3 K