A long insulated copper wire is closely wound as a spiral of ‘N’ turns. The spiral has inner radius ‘a’ and outer radius ‘b’. The spiral lies in the XY plane and a steady current ‘I’ flows through the wire. The Z-component of the magnetic field at the centre of the spiral is :
μ0IN2(b−a)lnba
B=∫dB=∫baμ0(dN)I2x=μ0I2∫baN dx(b−a)x
=μ0IN2(b−a)lnba