To solve this problem, we need to understand how charged particles behave in a magnetic field. The path of a charged ion in a magnetic field is circular, and the radius of this path is determined by the magnetic force acting on the ion. The formula for the radius of the path is given by:
\(r = \frac{mv}{qB}\)
where \(r\) is the radius of the circular path, \(m\) is the mass of the ion, \(v\) is the velocity of the ion, \(q\) is the charge of the ion, and \(B\) is the magnetic field strength.
Since the kinetic energy (\(KE\)) of both ions is the same, we know that:
\(\text{KE} = \frac{1}{2}mv^2\)
This implies:
\(v = \sqrt{\frac{2 \times \text{KE}}{m}}\)
Substituting the velocity (\(v\)) in the formula for radius (\(r\)):
\(r = \frac{m\sqrt{\frac{2 \times \text{KE}}{m}}}{qB} = \frac{\sqrt{2m \times \text{KE}}}{qB}\)
Now, compute the radius for both ions:
Now we compare the radii to determine which ion is deflected more. In doing so, we look at the expression \(\frac{\sqrt{2m \times \text{KE}}}{q}\). The ion with the smaller radius is deflected more:
Thus, the correct choice is that the lighter ion will be deflected more than the heavier ion. Therefore, the statement "lighter ion will be deflected more than heavier ion" is correct.
Two identical circular loops \(P\) and \(Q\) each of radius \(r\) are lying in parallel planes such that they have common axis. The current through \(P\) and \(Q\) are \(I\) and \(4I\) respectively in clockwise direction as seen from \(O\). The net magnetic field at \(O\) is: 
Find magnetic field at midpoint O. Rings have radius $R$ and direction of current is in opposite sense. 