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Question: A proton, a deuteron and an \(\alpha - \)particle having the same kinetic energy are moving in circu...

A proton, a deuteron and an α\alpha - particle having the same kinetic energy are moving in circular trajectories in a constant magnetic field. If rp,rd{r_p},{r_d} and rα{r_\alpha } denote, respectively, the radii of the trajectories of these particles, then
A. rα=rp<rd{r_\alpha } = {r_p} < {r_d}
B. rα>rd>rp{r_\alpha } > {r_d} > {r_p}
C. rα=rd>rp{r_\alpha } = {r_d} > {r_p}
D. rp=rd=rα{r_p} = {r_d} = {r_\alpha }

Explanation

Solution

When charged particles are moving in a magnetic field, they experience a force which acts at right angle to the velocity of the particles. The right hand rule can be used to determine the direction of the force. When the expression for the magnetic force is combined with the electric force, the combined force is called Lorentz force. Since the magnetic force is perpendicular to the velocity, a charged particle follows a curved path in a magnetic field. The particle continues to follow the path to form a circular path.

Complete step-by-step answer:
Radius of the circular path is, r=mvqBr = \dfrac{{mv}}{{qB}}, where mm is the mass of charged particle, qq is charge and vv is the velocity of charged particle.
The kinetic energy of a charged particle in the magnetic field is given by,
K=12mv2K = \dfrac{1}{2}m{v^2} or v=2Kmv = \sqrt {\dfrac{{2K}}{m}}
Therefore r=mqB2Km=2KmqBr = \dfrac{m}{{qB}}\sqrt {\dfrac{{2K}}{m}} = \dfrac{{\sqrt {2Km} }}{{qB}} , where KK is the kinetic energy and BB is the strength of magnetic field. As KK and BB are constants. So rr is proportional to the mq\dfrac{{\sqrt m }}{q}. rp:rd:rα=mpqp:mdqd:mαqα{r_p}:{r_d}:{r_\alpha } = \dfrac{{\sqrt {{m_p}} }}{{{q_p}}}:\dfrac{{\sqrt {{m_d}} }}{{{q_d}}}:\dfrac{{\sqrt {{m_\alpha }} }}{{{q_\alpha }}} , where rp,rd,rα{r_p},{r_d},{r_\alpha } is the radius of proton, deuteron and α\alpha - particle respectively , mp,md,mα{m_{p,}}{m_d},{m_\alpha }is the mass of the particles and qp,qd,qα{q_p},{q_d},{q_\alpha } is the charge of particles. So
me:2me:4m2e=1:2:1\Rightarrow \dfrac{{\sqrt m }}{e}:\dfrac{{\sqrt {2m} }}{e}:\dfrac{{\sqrt {4m} }}{{2e}} = 1:\sqrt 2 :1
rα=rp<rd\Rightarrow {r_\alpha } = {r_p} < {r_d} , the radii of the trajectories of these particles.

So, the correct answer is “Option A”.

Note: We know that magnetic force is always perpendicular to the velocity so that it does not work on the charge particles. Kinetic energy of particles and speed thus remains constant. The direction of motion is only affected not the speed. The particle continues to follow the curved path and forms a complete circle.