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 \( A \).