(a) We know that thermoelectric power
$S = \frac{dE}{dT}$
Given, $E = K\left( T - T_{r} \right)\left\lbrack T_{0} - \frac{1}{2}\left( T + T_{r} \right) \right\rbrack$
By differentiating the above equation w.r.t. $T$ and putting $T = \frac{1}{2}\ T_{0},\ $we get $S = \frac{1}{2}kT_{0}$