If the charged particle is moving in a magnetic field B, with a velocity v it experiances a force given by, F=q(v×B)= qvB sinθ
where, θ is the angle between v and B
If θ=π/2 therefore, sin π/2=1
Hence, F= qvB
The magnetic force acting on it is maximum when the angle between the direction of motion and
magnetic field is π/2