The radius of the circular path of a charged particle in a magnetic field is given by $r = \frac{mv}{qB}$, where $m$ is the mass, $v$ is the velocity, $q$ is the charge, and $B$ is the magnetic field strength. Specific charge is the ratio $\frac{q}{m}$. Let the specific charges be $s_1 = \frac{q_1}{m_1}$ and $s_2 = \frac{q_2}{m_2}$, with $s_1:s_2 = 2:1$. Let the masses be $m_1$ and $m_2$, with $m_1:m_2 = 1:4$. Since the kinetic energies are equal, $\frac{1}{2}m_1v_1^2 = \frac{1}{2}m_2v_2^2$, so $\frac{v_1^2}{v_2^2} = \frac{m_2}{m_1} = \frac{4}{1}$. Thus, $v_1 = 2v_2$. $r_1 = \frac{m_1v_1}{q_1B}$ and $r_2 = \frac{m_2v_2}{q_2B}$. $\frac{r_1}{r_2} = \frac{m_1v_1/q_1}{m_2v_2/q_2} = \frac{v_1/s_1}{v_2/s_2} = \frac{v_1}{v_2} \times \frac{s_2}{s_1} = \frac{2v_2}{v_2} \times \frac{1}{2} = 1$. Therefore, $r_1:r_2 = 1:1$.