(a) Maximum kinetic energy and intensity:
The maximum kinetic energy of emitted photoelectrons depends only on the frequency of the incident light, not on its intensity. This is because a single photon interacts with a single electron, and the energy of the photon is given by \( E = h\nu \). Intensity affects the number of photons (and hence number of electrons ejected), not the energy per photon.
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(b) Photoelectric current and intensity:
The photoelectric current is proportional to the number of photoelectrons emitted per second. Higher intensity means more photons per unit area per second, resulting in more electrons being ejected (provided the frequency is above the threshold), thus increasing the current.
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(c) Stopping potential and frequency:
According to Einstein’s photoelectric equation:
\[
K_{\text{max}} = h\nu - \phi
\]
Since \( K_{\text{max}} = eV_0 \), we get:
\[
eV_0 = h\nu - \phi \Rightarrow V_0 = \dfrac{h}{e} \nu - \dfrac{\phi}{e}
\]
This is a linear equation in \( \nu \), which shows that the stopping potential \( V_0 \) varies linearly with frequency for a given surface.