(c) Magnetic induction at the centre of a circular coil
$\ \ \ \ \ \ \ \ \ \ \ \ \ \ \ B = \frac{\mu_{0}}{2}\ .\frac{ni}{R}$
$\Rightarrow \ \ \ \ \ \ \ \ \ \ B \propto \frac{n}{R}\ $
Here, $\ \ \ n_{1} = 1,\ n_{2} = 2,$
$\ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ l = 2\pi R_{1} = 2 \times 2\pi R_{2}$
$\Rightarrow \ \ \ \ \ \ \ \ R_{2} = \frac{R_{1}}{2}$
$\therefore\ \ \ \ \ \ \ \ \ \frac{B_{1}}{B_{2}} = \frac{n_{1}}{n_{2}} \times \frac{R_{2}}{R_{1}}$
$\ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ = \frac{1}{2} \times \frac{R_{1}/2}{r} = \frac{1}{4}$
$\ \ \ \ \ \ B_{1}:B_{2} = 1\ :4$