The mass density \( \rho \) of a nucleus is defined as the mass per unit volume.
For a nucleus with mass number \( A \) and radius \( R \), we can express the mass and volume as follows:
- The mass of the nucleus is proportional to the mass number \( A \), i.e., the mass \( M \) is proportional to \( A \),
- The volume \( V \) of the nucleus is proportional to \( R^3 \), where \( R \) is the radius of the nucleus.
The volume is given by the formula for the volume of a sphere:
\[
V = \frac{4}{3} \pi R^3
\]
Since the mass number \( A \) is proportional to the volume, the mass density is given by:
\[
\rho = \frac{\text{mass}}{\text{volume}} = \frac{A}{\frac{4}{3} \pi R^3}
\]
We know from the liquid drop model of the nucleus that the radius \( R \) is proportional to \( A^{1/3} \).
Thus, we have:
\[
R \propto A^{1/3}
\]
Substituting this into the equation for density:
\[
\rho \propto \frac{A}{R^3} = \frac{A}{A} = 1
\]
Therefore, the mass density \( \rho \) is independent of \( A \).
Thus, the correct answer is Option (4), which states that the mass density is independent of \( A \).