Concept:
The density of atomic nuclei is approximately constant for all elements irrespective of their mass numbers. This happens because the radius of a nucleus depends on the mass number according to the relation:
\[
R = R_0 A^{1/3}
\]
where:
- \(R\) = radius of nucleus
- \(R_0\) = nuclear constant
- \(A\) = mass number
Since volume of a nucleus is proportional to \(R^3\),
\[
V \propto (A^{1/3})^3
\]
\[
V \propto A
\]
Also, mass of nucleus is directly proportional to mass number \(A\).
Thus,
\[
\text{Density} = \frac{\text{Mass}}{\text{Volume}}
\]
\[
\rho \propto \frac{A}{A}
\]
\[
\rho = \text{constant}
\]
Therefore, all nuclei have nearly the same density.
Step 1: Write the relation for nuclear density.
Density is given by:
\[
\rho = \frac{\text{Mass of nucleus}}{\text{Volume of nucleus}}
\]
Mass of nucleus:
\[
m \propto A
\]
Radius of nucleus:
\[
R = R_0 A^{1/3}
\]
Volume of nucleus:
\[
V = \frac{4}{3}\pi R^3
\]
Substituting the radius relation:
\[
V \propto (A^{1/3})^3
\]
\[
V \propto A
\]
Step 2: Find the density dependence.
Since,
\[
\rho \propto \frac{A}{A}
\]
\[
\rho = \text{constant}
\]
Thus nuclear density does not depend on mass number.
Step 3: Compare the two nuclei.
Given mass numbers:
\[
A_1 = 64
\]
\[
A_2 = 27
\]
Since nuclear density is constant for all nuclei:
\[
\rho_1 = \rho_2
\]
Therefore,
\[
\rho_1 : \rho_2 = 1:1
\]
Hence, the correct answer is:
\[
\boxed{1:1}
\]