We know that the kinetic energy of the emitted photoelectrons is given by the photoelectric equation:
\[
K.E. = h f - \phi
\]
where:
- \( K.E. \) is the kinetic energy of the emitted photoelectrons,
- \( h \) is Planck's constant,
- \( f \) is the frequency of the incident light,
- \( \phi \) is the work function of the metal.
Let the initial frequency be \( f_1 \) and the corresponding kinetic energy be \( K.E_1 = 0.5 \, {eV} \):
\[
K.E_1 = h f_1 - \phi \tag{1}
\]
Let the final frequency be \( f_2 = 1.1 f_1 \) (since the frequency is increased by 10%), and the corresponding kinetic energy be \( K.E_2 = 0.7 \, {eV} \):
\[
K.E_2 = h f_2 - \phi = h (1.1 f_1) - \phi \tag{2}
\]
Now, subtract equation (1) from equation (2):
\[
K.E_2 - K.E_1 = h (1.1 f_1) - \phi - (h f_1 - \phi)
\]
\[
0.7 - 0.5 = h (1.1 f_1 - f_1)
\]
\[
0.2 = h \times 0.1 f_1
\]
\[
h f_1 = 2 \, {eV}
\]
Substitute this value into equation (1):
\[
0.5 = 2 - \phi
\]
\[
\phi = 1.5 \, {eV}
\]
Thus, the work function of the metal is 1.5 eV, which corresponds to option (C).