Step 1: The magnetic force on a charged particle moving in a circular path is given by:
\[
F = \frac{mv^2}{r}
\]
where:
- \( m \) is the mass of the particle,
- \( v \) is its velocity,
- \( r \) is the radius of the circular path.
The force experienced by the particle is also equal to the magnetic force:
\[
F = qvB
\]
where:
- \( q \) is the charge,
- \( B \) is the magnetic field strength.
Equating the two expressions for force gives:
\[
\frac{mv^2}{r} = qvB
\]
Step 2: Solving for the linear momentum \( p = mv \), we get:
\[
p = \frac{qrB}{v}
\]
Since the velocity is proportional to the radius and the charge, the ratio of linear momenta of the two particles is proportional to the product of the charge and mass ratio.
Step 3: Let the charge and mass ratio of the two particles be \( \frac{q_1}{q_2} = \frac{1}{2} \) and \( \frac{m_1}{m_2} = \frac{2}{3} \).
The ratio of the linear momenta is given by:
\[
\frac{p_1}{p_2} = \frac{q_1 m_1 r_1}{q_2 m_2 r_2}
\]
\[
\frac{p_1}{p_2} = \frac{1/2 \times 2/3 \times 3}{4} = \frac{3}{8}
\]