The photoelectric effect can be explained using the equation:
\[
E_{\text{photon}} = h \cdot f = \text{Work Function} + K_{\text{max}}
\]
Where \( E_{\text{photon}} \) is the energy of the incident light, \( h \) is Planck's constant, \( f \) is the frequency of the light, and \( K_{\text{max}} \) is the maximum kinetic energy of the emitted photoelectrons.
For the emission of photoelectrons, the energy of the incoming photon should be equal to or greater than the work function of the metal.
We are given that the work function of the metal is 3eV.
To cause the emission of photoelectrons, the energy of the photon should be at least 3eV.
We know the energy of a photon is related to its frequency by:
\[
E = h \cdot f
\]
Where \( E = 3 \, \text{eV} \).
For visible light, the color that corresponds to a frequency that can cause electron emission at 3eV is blue light.
Therefore, the color of the light is blue.