Concept:
The density of a crystal lattice is given by
\[
\rho = \frac{Z M}{a^3 N_A}
\]
where
- \(Z\) = Number of atoms per unit cell
- \(M\) = Molar mass
- \(a\) = Edge length of the unit cell
- \(N_A\) = Avogadro's number
For a Body-Centered Cubic (BCC) structure:
\[
Z = 2
\]
Also, the relation between atomic radius \(r\) and edge length \(a\) in BCC is
\[
a = \frac{4r}{\sqrt{3}}
\]
Step 1: {Calculate the edge length of the unit cell.}
\[
a = \frac{4r}{\sqrt{3}}
\]
Given \(r = 173\,\text{pm}\)
\[
a = \frac{4 \times 173}{\sqrt{3}} \approx 400\,\text{pm}
\]
Convert to cm:
\[
400\,\text{pm} = 4 \times 10^{-8}\,\text{cm}
\]
Step 2: {Substitute values into density formula.}
\[
\rho = \frac{Z M}{a^3 N_A}
\]
\[
\rho = \frac{2 \times 56}{(4 \times 10^{-8})^3 \times 6.022 \times 10^{23}}
\]
Step 3: {Simplify the expression.}
\[
a^3 = 64 \times 10^{-24}
\]
\[
\rho \approx \frac{112}{6.022 \times 64 \times 10^{-1}}
\]
\[
\rho \approx 7.2\,\text{g cm}^{-3}
\]
Thus, the density of the metal is approximately \(7.2\,\text{g cm}^{-3}\).
Hence, the correct option is (A).