
(a) On passing current through the coil, it acts as a magnetic dipole. Torque acting on magnetic dipole is counter balanced by the moment of additional weight about position $O$. Torque acting on a magnetic dipole
$\tau = MB\sin\theta = (NiA)B\sin{90{^\circ}} = NiAB$
Again $\tau = Force \times Lever\ arm = \mathrm{\Delta}mg \times l$
$\Rightarrow NiAB = \mathrm{\Delta}mgl;\ \mathrm{\Delta}m = 60 \times 10^{- 3}g = 60 \times 10^{- 6}\ kg$
$\Rightarrow B = \frac{\mathrm{\Delta}mgl}{NiA} = \frac{60 \times 10^{- 6} \times 9.8 \times 30 \times 10^{- 2}}{200 \times 22 \times 10^{- 3} \times 1 \times 10^{- 4}} = 0.4\ T$