The maximum kinetic energy of the photoelectrons emitted is related to the wavelength of light by Einstein's photoelectric equation:
\[
K = h\nu - \phi
\]
where:
- \( K \) is the maximum kinetic energy of the photoelectrons,
- \( h \) is Planck's constant,
- \( \nu \) is the frequency of the incident light,
- \( \phi \) is the work function of the material.
Since the frequency \( \nu \) is related to the wavelength \( \lambda \) by the equation \( \nu = \frac{c}{\lambda} \), where \( c \) is the speed of light, we can write the kinetic energy as:
\[
K = h \left( \frac{c}{\lambda} \right) - \phi
\]
Now, let’s compare the kinetic energies for the two wavelengths:
- For \( \lambda_1 \), the maximum kinetic energy is \( K_1 = h \left( \frac{c}{\lambda_1} \right) - \phi \),
- For \( \lambda_2 \), the maximum kinetic energy is \( K_2 = h \left( \frac{c}{\lambda_2} \right) - \phi \).
Given that \( \lambda_1 = 2\lambda_2 \), we have:
\[
K_1 = h \left( \frac{c}{2\lambda_2} \right) - \phi
\]
\[
K_2 = h \left( \frac{c}{\lambda_2} \right) - \phi
\]
From the equations above, we can see that \( K_1 \) is less than \( K_2 / 2 \). This is because the frequency of the light corresponding to \( \lambda_1 \) is half of the frequency corresponding to \( \lambda_2 \), leading to a smaller kinetic energy for \( \lambda_1 \).
Thus, the correct answer is:
\[
\text{(C) } K_1<K_2 / 2
\]