Let the given circular ABC part of wire subtends an angle θ at its centre. Then, magnetic field due to this circular part is B′=Bc×2πθ=4πμ0×e2πi×2πθ ⇒B′=4πμ0⋅riθ
Given, i=40A,r=3.14cm=3.14×10−2m θ=360∘−90∘=270∘=23πrad ∴B′=3.14×10−210−7×40×23π=60×10−5 B′=6×10−4T