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 $ $\frac{{{R_A}}}{{{R_B}}} = \frac{{r_2^2 - r_1^2}}{{r_1^2}} = {\left( {\frac{{{r_2}}}{{{r_1}}}} \right)^2} - 1 = {\left( {\frac{{{d_2}}}{{{d_1}}}} \right)^2} - 1 = {\left( {\frac{2}{1}} \right)^2} - 1 = 3$
