(d) The residence of conductor
$R = \frac{\rho l}{A} = \frac{1}{\pi r^{2}}$
$or\ \ \ R \propto \frac{l}{r^{2}}$
$\therefore\ \frac{R_{1}}{R_{2}} = \frac{l_{1}}{l_{2}} \times \frac{r_{2}^{2}}{r_{1}^{2}} = \frac{2}{1} \times \left( \frac{2}{1} \right)^{2} = \frac{8}{1}$
Thermal potential between the ends of the roads are same. So, heat conducted per second
$H = \frac{\mathcal{Q}}{t} \propto \frac{1}{R}$
$\therefore\frac{H_{1}}{H_{2}} = \frac{R_{2}}{R_{1}} = \frac{1}{8} = 1:8$