To understand the deflection of the ions in a magnetic field, let's discuss the relevant physics principles.
The deflection of a charged particle in a magnetic field is determined by the radius of the circular path it follows, given by the formula:
\(r = \frac{mv}{qB}\)
where:
Given that the kinetic energy (\(KE\)) of the ions is the same, we know:
\(\frac{1}{2} mv^2 = KE\)
From which we can solve for \(v\):
\(v = \sqrt{\frac{2 \cdot KE}{m}}\)
Substitute this expression of \(v\) into the formula for \(r\):
\(r = \frac{m \cdot \sqrt{\frac{2 \cdot KE}{m}}}{qB} = \frac{\sqrt{2m \cdot KE}}{qB}\)
Thus, the radius of the path mainly depends on the ratio \(\frac{m}{q}\), as \(B\) and \(KE\) are constants:
Let's calculate the \(\frac{m}{q}\) ratio for the ions:
Since the formula predictions depend on this ratio, you would expect He\(^+\) ions to have a smaller radius than O\(^{2+}\) at first glance. However, because the kinetic energy is equal and the charge to mass ratio is inherently accounted for in the equal energy condition, under equal kinetic energies and not simply velocities, all ions experience an equal distribution of kinetic energy into equal trajectory deflection regardless of polarization effect on mass ratio/charge.
Conclusion: Given equal energy and a graduated potential translating common ke into common shared effects on the \(\frac{m}{q}\) effect, \(r\) for both would ultimately balance.
Correct Answer: All the ions will be deflected equally.