Bainbridge's mass spectrometer, shown in Fig. 28.33, separates ions having the same velocity. The ions, after entering through slits, $S_1$ and $S_2$, pass through a velocity selector composed of an electric field produced by the charged plates $\mathrm{P}$ and $\mathrm{P}^{\prime}$, and a magnetic field $\vec{B}$ perpendicular to the electric field and the ion path. The ions that then pass undeviated through the crossed $\vec{E}$ and $\vec{B}$ fields enter into a region where a second mas they are made to follow circular pa a modern detector) registers thei ions, $q / m=E / r B B^{\prime}$, where $r$ is the $r$