



The binding energy per nucleon in a nucleus is a measure of how strongly the nucleons (protons and neutrons) are bound together. This energy is dependent on the mass number \( A \) of the nucleus, and its trend as a function of \( A \) shows an interesting pattern.
As a function of mass number \( A \), the binding energy per nucleon increases with \( A \) up to iron (\( A \approx 56 \)) and then decreases as \( A \) increases further. This is because:
The correct graph representing this behavior is one that shows a peak at \( A = 56 \) (for iron) with the binding energy per nucleon increasing initially as \( A \) increases and then decreasing for heavier nuclei.
Assertion (A): We cannot form a p-n junction diode by taking a slab of a p-type semiconductor and physically joining it to another slab of an n-type semiconductor.
Reason (R): In a p-type semiconductor, \( n_e \gg n_h \) while in an n-type semiconductor \( n_h \gg n_e \).