Figure shows a semi circular coil of radius z along with long straight wires. When a current I flows through this set up, the magnetic field, at O, the centre of semi circular arc, equals
(1) \(\frac{μ_0i}{4\pi Z}(\frac{\pi}{2}-2)\)outwards
(2) \(\frac{μ_0i}{4\pi Z}(\pi + 2)\) outwards
(3) \(\frac{μ_0i}{4\pi Z}({\pi - 2})\)into the plane of the paper
(4) \(\frac{μ_0i}{4\pi Z}({\pi +2})\) into the plane of the paper