The nuclear density in general is independent of mass number \( A \).
The radius of a nucleus is directly proportional to the mass number \( A \).
The binding energy of a nucleus is inversely proportional to its mass defect.
Energy is absorbed when heavy nuclei undergo transmutation into light nuclei.
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Solution and Explanation
The radius of a nucleus is given by:
\[
R = R_0 A^{1/3}
\Rightarrow \text{Volume} \propto R^3 \propto A
\]
Since mass of the nucleus \( \propto A \), density \( \rho = \frac{\text{mass}}{\text{volume}} \approx \text{constant} \)
Thus, nuclear density is roughly constant and independent of \( A \).