
Magnetic field due to $2.5 A \rightarrow \frac{2.5 \mu_0}{2 \pi \times 2.5}=\frac{\mu_0}{2 \pi} \odot$
Resultant Magnetic field $B_{net}=\frac{2 \mu_0}{2 \pi}-\frac{\mu_0}{2 \pi}=\frac{\mu_0}{2 \pi} \otimes$
$(A)$ If $\vec{B}$ is along $\hat{z}, F \propto(L+R)$
$(B)$ If $\overrightarrow{ B }$ is along $\hat{ x }, F =0$
$(C)$ If $\vec{B}$ is along $\hat{y}, F \propto(L+R)$
$(D)$ If $\overrightarrow{ B }$ is along $\hat{ z }, F =0$




