
And we know, $\frac{m v^{2}}{R}=q v B$
$\Rightarrow \quad R=\frac{m v}{q B}$
$\because \sin \alpha=\frac{d q B}{m v}$
$\sin \alpha=B d \sqrt{\frac{q}{2 m V}}\left[\because q V=\frac{1}{2} m v^{2}\right]$

Statement $1$: A charged particle is moving at right angle to a static magnetic field . During the motion the kinetic energy of the charge remains unchanged.
Statement $2$: Static magnetic field exert force on a moving charge in the direction perpendicular to the magnetic field.
