
$\therefore \quad F_{B C}=F_{A B}=\frac{\mu_{0} I^{2} l}{2 \pi d}$
As, $\vec{F}_{A B} \perp \vec{F}_{B C}$ net force on wire $B$
$F_{\text {net }}=\sqrt{2} F_{B C}=\frac{\sqrt{2} \mu_{o} I^{2} l}{2 \pi d}$
$F_{\text {net }}=\frac{\mu_{o} I^{2} l}{\sqrt{2} \pi d}$ or $\frac{F_{\text {net }}}{l}=\frac{\mu_{o} I^{2}}{\sqrt{2} \pi d}$
$[1]$ The magnetic field strength may have been increased while the particle was travelling in air
$[2]$ The particle lost energy by ionising the air
$[3]$ The particle lost charge by ionising the air
