(d) Resistance of a conductor varies linearly with temperature as
$R_{t} = R_{0}(1 + \alpha t)$
For the first conductor
$T_{t_{1}} = R_{0}\left( 1 + \alpha_{1}t_{1} \right)$
$or\ \ \ \ \alpha_{1} = \frac{Rt_{1} - R_{0}}{t}\ \ \ \ \ldots.(i)$
Similarly, for second conductor
$\alpha_{2} = \frac{Rt_{2} - R_{0}}{t_{2}}\ \ \ldots\ldots..(ii)$
From Eq. (i) and Eq. (ii), we get
$\frac{\alpha_{1}}{\alpha_{2}} = \frac{t_{2}}{t_{1}}$