Magnetic force on the charged particle is given as FB=q(v×B)=qvBsinθ Here ,θ=90° ⇒ FB=qvBsin90°=qvB Since, the particle is projected perpendicular to the field, so its trajectory will be circular in nature, where necessary centripetal force =FB ⇒
mv2
r′
=qvB
mv2
(
r
2
)
=qvB(∵r′=
r
2
) ⇒ v=
qBr
2n
...(i) Magnetic field inside the solenoid is given as, B=µ0nI Substituting the value of B in Eq. (i), we get v=