(c) For conductor $A,\ R_{A} = \frac{\rho l}{\pi r_{1}^{2}},$
For conductor $B,\ R_{B} = \frac{\rho l}{\pi(r_{2}^{2} - r_{1}^{2})}$
$\Rightarrow \frac{R_{A}}{R_{B}} = \frac{r_{2}^{2} - r_{1}^{2}}{r_{1}^{2}} = \left( \frac{r_{2}}{r_{1}} \right)^{2} - 1 = \left( \frac{d_{2}}{d_{1}} \right)^{2} - 1 = \left( \frac{2}{1} \right)^{2} - 1 = 3$