Step 1: Einstein's Photoelectric Equation.
The photoelectric equation is given by:
\[
E_k = hf - \phi
\]
where:
- \( E_k \) is the kinetic energy of the emitted electrons,
- \( h \) is Planck's constant (\( h = 6.626 \times 10^{-34} \, \text{J s} \)),
- \( f \) is the frequency of the incident light,
- \( \phi \) is the work function of the metal.
The stopping potential is related to the kinetic energy of the emitted electrons by the equation:
\[
E_k = eV_s
\]
where \( e \) is the charge of the electron, and \( V_s \) is the stopping potential.
Step 2: Calculating the stopping potential.
The energy of the incident photons is given by:
\[
E = hf = (6.626 \times 10^{-34}) \times (6.0 \times 10^{14}) = 3.976 \times 10^{-19} \, \text{J}
\]
Now, using the photoelectric equation:
\[
E_k = 3.976 \times 10^{-19} - 2.5 \times 10^{-19} = 1.476 \times 10^{-19} \, \text{J}
\]
Now, using the relation \( E_k = eV_s \):
\[
V_s = \frac{E_k}{e} = \frac{1.476 \times 10^{-19}}{1.6 \times 10^{-19}} = 0.92 \, \text{V}
\]
Step 3: Conclusion.
The stopping potential is \( 0.92 \, \text{V} \).