Step 1: Radius of a nucleus.
The radius of a nucleus is given by the empirical relation:
\[
R = R_0 A^{1/3}
\]
where $R_0$ is a constant ($R_0 \approx 1.3 \times 10^{-15}\ \text{m}$) and $A$ is the mass number of the nucleus.
Step 2: Volume of the nucleus.
The volume of a nucleus is given by the formula for the volume of a sphere:
\[
V = \frac{4}{3}\pi R^3
\]
Substituting $R = R_0 A^{1/3}$:
\[
V = \frac{4}{3}\pi (R_0 A^{1/3})^3
\]
\[
V = \frac{4}{3}\pi R_0^3 A
\]
Step 3: Mass of the nucleus.
The mass of the nucleus is approximately proportional to the mass number:
\[
M = A m_n
\]
where $m_n$ is the mass of a nucleon (proton or neutron).
Step 4: Density of nuclear matter.
Density is defined as:
\[
\rho = \frac{M}{V}
\]
Substituting the values:
\[
\rho = \frac{A m_n}{\frac{4}{3}\pi R_0^3 A}
\]
\[
\rho = \frac{m_n}{\frac{4}{3}\pi R_0^3}
\]
Step 5: Conclusion.
Since the mass number $A$ cancels out, the density does not depend on the size of the nucleus. Therefore, the density of nuclear matter is approximately the same for all nuclei.