A particle of mass $m$ and charge $q$, accelerated by a potential difference $V$ enters a region of a uniform transverse magnetic field $B$. If $d$ is the thickness of the region of $B$, the angle $\theta$ through which the particle deviates from the initial direction on leaving the region is given by
$\sin \theta = Bd{\left( {\frac{q}{{2mV}}} \right)^{\frac{1}{2}}}$
$\cos \theta = Bd{\left( {\frac{q}{{2mV}}} \right)^{\frac{1}{2}}}$
$\tan \theta = Bd{\left( {\frac{q}{{2mV}}} \right)^{\frac{1}{2}}}$
$\cot \theta = Bd{\left( {\frac{q}{{2mV}}} \right)^{\frac{1}{2}}}$
An electron having kinetic energy $T$ is moving in a circular orbit of radius $R$ perpendicular to a uniform magnetic induction $\vec B$ . If kinetic energy is doubled and magnetic induction tripled, the radius will become
A charged particle moves with velocity $v$ in a uniform magnetic field $\overrightarrow B $. The magnetic force experienced by the particle is
A uniform beam of positively charged particles is moving with a constant velocity parallel to another beam of negatively charged particles moving with the same velocity in opposite direction separated by a distance $d.$ The variation of magnetic field $B$ along a perpendicular line draw between the two beams is best represented by
A positively charged particle enters in a region of uniform. Transverse magnetic field as shown in figure find net deviation in path of the particle.
At $t = 0$ a charge $q$ is at the origin and moving in the $y-$ direction with velocity $\overrightarrow v = v\,\hat j .$ The charge moves in a magnetic field that is for $y > 0$ out of page and given by $B_1 \hat z$ and for $y < 0$ into the page and given $-B_2 \hat z .$ The charge's subsequent trajectory is shown in the sketch. From this information, we can deduce that