Step 1: Conceptual Foundation:
This problem integrates two core principles: the work-energy theorem for charged particles in electric fields and the dynamics of charged particles in uniform circular motion within magnetic fields. The objective is to establish a relationship between the radius of the circular trajectory and the initial accelerating voltage along with the final velocity.
Step 2: Essential Formulas and Methodology:
1. Acceleration of a charged particle (\(q\)) by a potential difference (\(V\)) results in kinetic energy gain equivalent to the work done: \(KE = qV\). Since \(KE = \frac{1}{2}mu^2\), it follows that \(qV = \frac{1}{2}mu^2\).2. Upon entering a magnetic field (\(B\)) perpendicularly, the magnetic force acts as the centripetal force for circular motion: \(quB = \frac{mu^2}{r}\).3. Rearranging the second equation yields the radius of the circular path: \(r = \frac{mu}{qB}\).
Step 3: Detailed Derivation:
We have established two primary equations:(i) \(V = \frac{mu^2}{2q}\)(ii) \(r = \frac{mu}{qB}\)The problem requires determining the proportionality of \(r\) with respect to \(V\) and \(u\). Combining the equations is necessary to derive this relationship. Consider the expression \(V/u\), as presented in option (A).From equation (i), we can derive:\[ \frac{V}{u} = \frac{mu^2/2q}{u} = \frac{mu}{2q} \]Comparing this with the expression for radius \(r\) from equation (ii):\[ r = \frac{mu}{qB} \]Both \(r\) and \(V/u\) are directly proportional to the term \(mu/q\). We can express \(r\) in terms of \(V/u\) as follows:\[ r = \frac{mu}{qB} = \frac{2}{B} \left( \frac{mu}{2q} \right) = \frac{2}{B} \left( \frac{V}{u} \right) \]Given that the magnetic field \(B\) is uniform and constant, the proportionality is established as:\[ r \propto \frac{V}{u} \]
Step 4: Conclusion:
The radius of the circular trajectory is directly proportional to the ratio \(V/u\).