Q139 / 150 · MHT CET 2011 · Physics
A long straight conductor is bent into shape as shown. If it carries $1 \mathrm{~A}$ and its radius is $R$, then magnetic ficld $B$ at the centre of circular coil


- A$\infty$
- BZero
- C$\frac{\mu_{0} i(\pi+1)}{2 \pi R}$
- Correct answerD$\frac{\mu_{0} i(\pi-1)}{2 \pi R}$
Solution
Magnetic field at centre $O=$ magnetic field due to reaction $A B+$ magnetic field due to section $P Q R$
$$
B_{0}=B_{A B}+B_{P Q R}
$$

but $B_{A B}=\frac{\mu_{0} i}{2 \pi R}$ (upside the plane of paper) and $B_{P Q R}=\frac{\mu_{0} i}{2 R}$ (inside the plane of paper) Hence $B_{0}=\frac{\mu_{0} i}{2 R}-\frac{\mu_{0} i}{2 \pi R}$ $$ B_{0}=\frac{\mu_{0} i(\pi-1)}{2 \pi R} $$

but $B_{A B}=\frac{\mu_{0} i}{2 \pi R}$ (upside the plane of paper) and $B_{P Q R}=\frac{\mu_{0} i}{2 R}$ (inside the plane of paper) Hence $B_{0}=\frac{\mu_{0} i}{2 R}-\frac{\mu_{0} i}{2 \pi R}$ $$ B_{0}=\frac{\mu_{0} i(\pi-1)}{2 \pi R} $$
Hence, the correct answer is option: 'D'.