



Step 1: Understanding the Photoelectric Effect
The photoelectric effect refers to the phenomenon where electrons are emitted from a metal surface when light of a certain minimum frequency (or maximum wavelength) shines on it. This effect led to the quantum understanding of light as being made up of discrete packets called photons.
The key observations from the photoelectric effect are:
The photoelectric equation is given by: \[ K_{\text{max}} = h\nu - \phi \] Where:
To measure \( K_{\text{max}} \), we apply a reverse (retarding) voltage called the stopping potential \( V_0 \), such that: \[ eV_0 = K_{\text{max}} = h\nu - \phi \] This stopping potential is the minimum voltage needed to stop the most energetic photoelectrons from reaching the anode. Importantly, it depends only on the frequency of the light and is independent of its intensity.
On the other hand, the saturation current is the maximum current achieved when all emitted photoelectrons are collected. Since more light intensity means more photons hitting the surface (assuming frequency is constant), it leads to the emission of more electrons, thereby increasing the saturation current. Hence:
Step 2: Interpreting the Graphs
In typical photoelectric effect experiments:
If two different light intensities \( I_1 \) and \( I_2 \) (with \( I_2 > I_1 \)) are used but with the same wavelength:
Conclusion: The correct graph is the one where the stopping potential remains unchanged between \( I_1 \) and \( I_2 \), but the saturation current for \( I_2 \) is greater than for \( I_1 \). Thus, the correct option is (C).
The stopping potential (\(V_0\)) versus frequency (\(\nu\)) of a graph for the photoelectric effect in a metal is given. From the graph, the Planck's constant (\(h\)) is:

In the diagram shown below, both the strings AB and CD are made of the same material and have the same cross-section. The pulleys are light and frictionless. If the speed of the wave in string AB is \( v_1 \) and in CD is \( v_2 \), then the ratio \( \frac{v_1}{v_2} \) is:
