For a solid with face-centered cubic (fcc) structure, the relation between the side length \( a \) and atomic radius \( r \) is:
\[
a = 2\sqrt{2}r.
\]
For the solid with simple cubic structure, the relation between the side length \( a' \) and atomic radius \( r \) is:
\[
a' = 2r.
\]
Now, let the side length of the simple cubic unit cell be \( a' \). Given the relation for the fcc unit cell side length \( a = 2\text{A} \), we can solve for the side length \( a' \) of the simple cubic unit cell:
\[
2\sqrt{2}r = 4r \quad \Rightarrow \quad a' = \sqrt{2} \, \text{A}.
\]
Thus, the side length of the unit cell for the simple cubic lattice will be \( \sqrt{2} \, \text{A} \).