The correct option is A 4πR2i
Using, →τ=→μ×→B,
τ=μBsinθ
=NiABsinθ
Here, the magnetic field and the coil are on the same plane. So, the angle θ will be 90∘ as the magnetic moment vector in this case is always perpendicular to the magnetic field.
Note: The angle 30∘ is given to confuse you.
⇒τ=1×i×πR2×4×sin90∘=4πR2i