When the frequency of incident light on a photosensitive material is increased, what happens to the stopping potential, assuming intensity is kept constant?
Figure 11.4 and its description state: 'The stopping potential is more negative for higher frequencies of incident radiation.' This implies that as frequency increases, the stopping potential increases in magnitude (becomes more negative). This is also consistent with $V_0 = (h/e)(\nu - \nu_0)$, where $h/e$ is positive.