Einstein's Photoelectric Equation:
\[
K_{\text{max}} = hu - \phi
\]
where,
\( K_{\text{max}} \) = maximum kinetic energy of emitted photoelectrons
\( h \) = Planck’s constant
\( u \) = frequency of incident light
\( \phi \) = work function of the metal
(a) If \( u<u_0 \), where \( u_0 = \frac{\phi}{h} \) is the threshold frequency, the photon energy \( hu \) is insufficient to overcome the work function. Consequently, no photoelectrons are emitted, irrespective of light intensity.
(b) The kinetic energy, \( K_{\text{max}} = hu - \phi \), is dependent solely on frequency \( u \), not intensity. An increase in intensity raises the photon count and, thus, the photoelectron count, but not their kinetic energy.
(c) The equation, expressed in terms of cut-off voltage, is:
\[
e V_0 = hu - \phi \Rightarrow V_0 = \frac{h}{e} u - \frac{\phi}{e}
\]
This equation aligns with the form \( y = mx + c \), indicating a linear relationship between \( V_0 \) and \( u \), with a slope of \( \frac{h}{e} \).