A charged particle projected in a limited magnetic field according to figure. The charged particle does not strike to the opposite plate provided
$B > \frac{qd}{mv}$
$B < \frac{mv}{qd}$
$B < \frac{qd}{mv}$
$B > \frac{mv}{qd}$
In a mass spectrometer used for measuring the masses of ions, the ions are initially accelerated by an electric potential $V$ and then made to describe semicircular paths of radius $R$ using a magnetic field $B$. If $V$ and $B$ are kept constant, the ratio $\left( {\frac{{{\text{charge on the ion}}}}{{{\text{mass of the ion}}}}} \right)$ will be proportional to
A proton, a deuteron and an $\alpha-$particle with same kinetic energy enter into a uniform magnetic field at right angle to magnetic field. The ratio of the radii of their respective circular paths is
A charged particle moves in a uniform magnetic field. The velocity of the particle at some instant makes an acute angle with the magnetic field. The path of the particle will be
An electron and a proton have equal kinetic energies. They enter in a magnetic field perpendicularly, Then
Under the influence of a uniform magnetic field a charged particle is moving in a circle of radius $R$ with constant speed $v$. The time period of the motion