(b) Current in coil of tangent galvanometer
$\ \ \ \ \ \ \ \ i = \frac{2rB_{H}}{\mu_{0}n}\tan\theta$
$\Longrightarrow \ n = \frac{2rB_{H}}{\mu_{0}i}\tan\theta$
$\therefore\ \ \ \ n = \frac{2 \times 16 \times 10^{- 2} \times 0.36 \times 10^{- 4}}{4\pi \times 10^{- 7} \times 20 \times 10^{- 3}}\tan{45{^\circ}}$
$\ \ \ \ \ \ \ \ \ \ \ \ = 458$