(b) $E = K\left( T - T_{r} \right)T_{0} + \frac{1}{2}K(T^{2} - T_{r}^{2})$
$\frac{dE}{dT} = KT_{0} + \frac{1}{2}K \times 2T = KT_{0} + KT$
At temperature $T = T_{0}$/2,
Thermo-electric power is $\frac{dE}{dT} = KT_{0} + K\frac{T_{0}}{2} = \frac{3}{2}K{\ T}_{0}$.