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