Radius of nucleus $R = R _0 A ^{\frac{1}{3}}$
Density of nucleus $=\frac{\text { Mass of nucleus }}{\text { volume of nucleus }}$
$\rho=\frac{ m \times A }{\frac{4}{3} \pi R ^3}$
Where $m$ : mass of proton or neutron
$\rho =\frac{ m \times A }{\frac{4}{3} \pi R _0{ }^3 A }$
$\rho \propto A ^0$
Hence density of nucleus is independent of mass number