The nuclear radius \( R \) of a nucleus is related to its mass number \( A \) by the formula:
\[
R = R_0 \cdot A^{1/3}
\]
Where:
- \( R_0 \) is a constant that can be determined experimentally (approximately \( 1.2 \, \text{fm} \) or \( 1.2 \times 10^{-15} \, \text{m} \)),
- \( A \) is the mass number of the nucleus.
First, we are given the radius of \(^{27}Al\), which is 3.6 fermi, and we can use the relation to find the nuclear radius of \(^{125}Fe\). We know:
\[
R_{Al} = R_0 \cdot A_{Al}^{1/3}
\]
So, for \(^{125}Fe\):
\[
R_{Fe} = R_0 \cdot A_{Fe}^{1/3}
\]
Substituting the given values:
\[
R_{Al} = 3.6 \, \text{fm} = R_0 \cdot (27)^{1/3}
\]
Thus,
\[
R_0 = \frac{3.6}{(27)^{1/3}} = 1.2 \, \text{fm}
\]
Now, calculating the radius for \(^{125}Fe\):
\[
R_{Fe} = 1.2 \cdot (125)^{1/3} \approx 6 \, \text{fm} = 6 \times 10^{-15} \, \text{m}
\]
Thus, the nuclear radius of \(^{125}Fe\) is approximately \( 6 \times 10^{-15} \, \text{m} \).