The radius \( r \) of the circular path in a magnetic field is given by the equation: \[ r = \frac{mv}{qB} \] where: \( m \) = mass of the particle,
\( v \) = velocity of the particle,
\( q \) = charge of the particle,
\( B \) = magnetic field strength. For an \( \alpha \) particle (helium nucleus), which contains two protons and two neutrons: \( m_{\alpha} = 4m_p \) (where \( m_p \) is the mass of a proton),
\( q_{\alpha} = 2e \) (where \( e \) is the elementary charge).
For a proton: \( m_p \) and \( q_p = e \).
Given that the paths have the same radius: \[ \frac{4m_p v_{\alpha}}{2eB} = \frac{m_p v_p}{eB} \]
Simplifying the equation, we find: \[ 2v_{\alpha} = v_p \quad {or} \quad v_{\alpha} = \frac{v_p}{2} \]
Thus, the ratio of their velocities \( v_{\alpha} : v_p \) is: \[ \frac{v_{\alpha}}{v_p} = \frac{1}{2} \] Therefore, the ratio of the velocity of the \( \alpha \) particle to the proton is 1:2.