The incident photon energy, calculated as \[\frac{hc}{\lambda} = eV_s + \phi\], is substituted with the given values: \[\frac{1240}{300} \, \text{eV} - 2.13 \, \text{eV} = eV_s\]. This simplifies to \[4.13 \, \text{eV} - 2.13 \, \text{eV} = eV_s\], yielding a stopping potential of \[V_s = 2 \, \text{V}\].