
- A$\frac{{2{\mu _0}i}}{{3\pi a}}\sqrt {4 - {\pi ^2}} $
- ✓$\frac{{{\mu _0}i}}{{3\pi a}}\sqrt {4 + {\pi ^2}} $
- C$\frac{{2{\mu _0}i}}{{3\pi {a^2}}}\sqrt {4 + {\pi ^2}} $
- D$\frac{{2{\mu _0}i}}{{3\pi a}}\sqrt {(4 - {\pi ^2})} $

Part $(2)$: ${B_2} = \frac{{{\mu _0}}}{{4\pi }}.\frac{{\pi \,i}}{{(a/2)}} \otimes $(along $-Z-$axis)
Part $(3)$: ${B_3} = \frac{{{\mu _0}}}{{4\pi }}.\frac{i}{{(a/2)}}\left( \downarrow \right)$(along $-Y-$axis)
Part $(4)$: ${B_4} = \frac{{{\mu _0}}}{{4\pi }}.\frac{{\pi i}}{{(3a/2)}}\odot$(along $+Z-$axis)
Part $(5)$: ${B_5} = \frac{{{\mu _0}}}{{4\pi }}.\frac{i}{{(3a/2)}}\left( \downarrow \right)$(along -$Y$ $-$ axis) ${B_2} - {B_4} = \frac{{{\mu _0}}}{{4\pi }}.\frac{{\pi i}}{a}\left( {2 - \frac{2}{3}} \right) = \frac{{{\mu _0}i}}{{3a}} \otimes $(along -$Z$ $-$ axis) ${B_3} + {B_5} = \frac{{{\mu _0}}}{{4\pi }}.\frac{1}{a}\left( {2 + \frac{2}{3}} \right) = \frac{{8{\mu _0}i}}{{12\pi a}}\left( \downarrow \right)$ (along -$Y$$ -$ axis)
Hence net magnetic field ${B_{net}} = \sqrt {{{({B_2} - {B_4})}^2} + {{({B_3} + {B_5})}^2}} $$ = \frac{{{\mu _0}i}}{{3\pi a}}\sqrt {{\pi ^2} + 4} $
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$(A)$ The current through the circuit, $I$ is $0.3 \ A$
$(B)$ The current through the circuit, I is $0.3 \sqrt{2} \ A$.
$(C)$ The voltage across $100 \Omega$ resistor $=10 \sqrt{2} \ V$
$(D)$ The voltage across $50 \Omega$ resistor $=10 \ V$