To determine the ratio of the radius of a deuteron's path (\( r_d \)) to the radius of a proton's path (\( r_p \)) in a uniform magnetic field, we proceed as follows:
The radius \( r \) of a charged particle's path, when moving perpendicularly to a magnetic field, is given by \(r = \frac{mv}{qB}\), where:
The kinetic energy \( KE \) for both particles is expressed as \(KE = \frac{1}{2}mv^2\). Given that their kinetic energies are equal, we equate these expressions and solve for velocity:
\(\frac{1}{2}m_pv_p^2 = \frac{1}{2}m_dv_d^2\)
Here:
This equality yields the relationship between their velocities:
\(v_p^2 = \frac{m_d}{m_p} v_d^2\)
Therefore, \(v_p = \sqrt{\frac{m_d}{m_p}} v_d\).
For the proton, \(r_p = \frac{m_pv_p}{q_pB}\).
For the deuteron, \(r_d = \frac{m_dv_d}{q_dB}\).
As the charge \(q = +e\) for both particles, it cancels out during comparison.
The ratio of the radii is computed as:
\(\frac{r_d}{r_p} = \frac{\left(\frac{m_dv_d}{qB}\right)}{\left(\frac{m_pv_p}{qB}\right)} = \frac{m_d v_d}{m_p v_p}\)
Substituting \(v_p = \sqrt{\frac{m_d}{m_p}} v_d\):
\(\frac{r_d}{r_p} = \frac{m_d v_d}{m_p \left(\sqrt{\frac{m_d}{m_p}} v_d\right)} = \sqrt{\frac{m_d}{m_p}}\)
Given that \(m_d = 2m_p\) (as a deuteron consists of a proton and a neutron), we find:
\(\frac{r_d}{r_p} = \sqrt{2}\)
The ratio of the deuteron's path radius to the proton's path radius is \( \sqrt{2} : 1 \). The final answer is \( \sqrt{2} : 1 \).