Step 1: Understanding the Concept:
The density of a crystal is determined by the mass of the atoms in its unit cell and the volume of the unit cell. Different crystal structures (like face-centered cubic, fcc, and body-centered cubic, bcc) have different numbers of atoms per unit cell and can have different unit cell volumes.
Step 2: Key Formula or Approach:
The formula for the density (\(\rho\)) of a crystal is:
\[ \rho = \frac{Z \times M}{N_A \times a^3} \]
where:
- \(Z\) = number of atoms per unit cell
- \(M\) = molar mass of the element
- \(N_A\) = Avogadro's number
- \(a\) = edge length of the unit cell
To find the ratio of densities \(\frac{\rho_{fcc}}{\rho_{bcc}}\), we can set up the ratio of their formulas. The terms \(M\) and \(N_A\) will cancel out as we are dealing with the same metal.
\[ \frac{\rho_{fcc}}{\rho_{bcc}} = \frac{Z_{fcc} / a_{fcc}^3}{Z_{bcc} / a_{bcc}^3} = \left(\frac{Z_{fcc}}{Z_{bcc}}\right) \times \left(\frac{a_{bcc}}{a_{fcc}}\right)^3 \]
Step 3: Detailed Explanation:
First, identify the values for each structure:
- For fcc structure:
- Number of atoms per unit cell, \(Z_{fcc} = 4\).
- Edge length, \(a_{fcc} = 3.5\) Å.
- For bcc structure:
- Number of atoms per unit cell, \(Z_{bcc} = 2\).
- Edge length, \(a_{bcc} = 3.0\) Å.
Now, substitute these values into the ratio formula:
\[ \frac{\rho_{fcc}}{\rho_{bcc}} = \left(\frac{4}{2}\right) \times \left(\frac{3.0 \text{ Å}}{3.5 \text{ Å}}\right)^3 \]
\[ \frac{\rho_{fcc}}{\rho_{bcc}} = 2 \times \left(\frac{3.0}{3.5}\right)^3 = 2 \times \left(\frac{6}{7}\right)^3 \]
\[ \frac{\rho_{fcc}}{\rho_{bcc}} = 2 \times \frac{6^3}{7^3} = 2 \times \frac{216}{343} = \frac{432}{343} \]
Now, perform the division:
\[ \frac{432}{343} \approx 1.2594... \]
This value is approximately 1.26.
Step 4: Final Answer:
The ratio of the densities of fcc and bcc is approximately 1.26. Therefore, option (B) is correct.