Step 1: Use the density relation for a crystal lattice.
The density of a crystal is given by
\[
\rho=\frac{ZM}{N_Aa^3}
\]
where
\[
\rho=11.21\ g\,cm^{-3}
\]
\[
Z=4 \quad \text{(for fcc lattice)}
\]
\[
M=\text{atomic mass}
\]
\[
N_A=6.023\times10^{23}\ mol^{-1}
\]
\[
a=4\ \text{\AA}
\]
Step 2: Convert edge length into centimeters.
Since
\[
1\ \text{\AA}=10^{-8}\ cm
\]
\[
a=4\times10^{-8}\ cm
\]
Therefore,
\[
a^3=(4\times10^{-8})^3
\]
\[
=64\times10^{-24}
\]
\[
=6.4\times10^{-23}\ cm^3
\]
Step 3: Substitute the values into the density formula.
\[
11.21
=
\frac{4M}
{(6.023\times10^{23})(6.4\times10^{-23})}
\]
First calculate the denominator:
\[
(6.023\times10^{23})(6.4\times10^{-23})
=
38.5472
\]
Hence,
\[
11.21=\frac{4M}{38.5472}
\]
Step 4: Solve for \(M\).
\[
4M
=
11.21\times38.5472
\]
\[
4M
\approx432
\]
\[
M
=
\frac{432}{4}
\]
\[
M
=
108
\]
Step 5: Final conclusion.
Therefore, the atomic weight of the element is
\[
\boxed{108.0\ g\ mol^{-1}}
\]
Hence, option (3) is correct.