The magnetic induction at the centre O in the figure shown is
μ0i4 1R1−1R2
μ0i4 1R1+1R2
μ0i4 R1−R2
μ0i4 R1+R2
In the following figure, magnetic fields at O due to sections 1, 2, 3 and 4 are considered as B1 , B2, B3 and B4, respectively.
B1 = B3 = 0
B2 = μ04π. πR1 ⊗B4 = μ04π. πiR2 ⊙As B2 > B4 So Bnet = B2 −B4 ⇒ Bnet = μ0i4 1R1 −1R2 ⊗