The problem is based on the photoelectric effect, which relates to the energy of electrons emitted from a surface when light of a certain wavelength falls on it. The stopping potential (\(V_0\)) is the potential required to stop the most energetic photoelectrons emitted due to the light incident on the surface.
According to Einstein's photoelectric equation, the energy of the incident light is related to the stopping potential and the work function of the material:
\(E = \text{hf} = \text{h}\frac{c}{\lambda}\), where:
Energy for the photoelectric effect can also be expressed as:
\(\text{E} = \text{eV}_0 + \phi\)
Where:
Now, let's solve the problem using this step-by-step approach:
\(\text{E}_2 = \text{h}\frac{c}{\lambda_2} = \text{eV}_{02} + \phi\)
Where:
This can be rearranged to solve for \frac{1}{\lambda_2} = \frac{1}{\lambda_1} + \frac{\text{e(V}_{02} - \text{V}_{01})}{\text{hc}}
Substitute the values:
\lambda_2 \approx 382 \ \text{nm}.
Thus, the new wavelength is 382 nm.