When a charged particle enters a uniform magnetic field perpendicular to its velocity, it experiences a centripetal force due to the Lorentz force, and follows a circular path. The radius of the circular motion is given by the formula:
\[
r = \frac{mv}{qB}
\]
where:
- \( m \) is the mass of the particle
- \( v \) is the velocity
- \( q \) is the charge
- \( B \) is the magnetic field strength
Let’s compute the radius for both particles:
For the proton:
- mass \( m_p = m \)
- charge \( q_p = e \)
\[
r_p = \frac{mv}{eB}
\]
For the \( \alpha \)-particle (which is a helium nucleus):
- mass \( m_\alpha = 4m \) (2 protons + 2 neutrons)
- charge \( q_\alpha = 2e \) (due to 2 protons)
\[
r_\alpha = \frac{4m \cdot v}{2eB} = \frac{2mv}{eB}
\]
Now, take the ratio of the radii:
\[
\frac{r_p}{r_\alpha} = \frac{\frac{mv}{eB}}{\frac{2mv}{eB}} = \frac{1}{2}
\]
Hence,
\[
\text{Ratio of radii } = \frac{r_p}{r_\alpha} = \frac{1}{2}
\]