
Magnetic field due to the current carrying long wire is \(\text {B} = \frac{\mu _0 I}{2 \pi r}\)
Where r is perpendicular distance from wire
Now from Lorentz force
\(\vec F_m = q (\vec v \times \vec B ) = q \left[v \cdot \hat j \times \frac{\mu _0 I}{2 \pi y} (\hat k)\right]\)
\(\vec {F}_ m = \frac{\mu _0 I (qv)}{2 \pi y} \hat i\)