To find the ratio of the density of iron at room temperature to that at $900^{\circ}C$, we need to consider the change in crystal structure from body-centered cubic (bcc) to face-centered cubic (fcc) and how this affects the volume and, consequently, the density.
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$bcc$ structure has:
- 2 atoms per unit cell.
- The relationship between atomic radius $r$ and the edge length $a$ of the cube is $a = \frac{4r}{\sqrt{3}}$.
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$fcc$ structure has:
- 4 atoms per unit cell.
- The relationship between atomic radius $r$ and the edge length $a$ of the cube is $a = \frac{4r}{\sqrt{2}}$.
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Calculate the density for each structure:
- Density, $\rho = \frac{\text{Mass of atoms in unit cell}}{\text{Volume of unit cell}}$.
- For $bcc$:
- Mass of atoms = 2 atoms × Atomic mass, assuming molar mass $M$.
- Volume = $a^3 = \left(\frac{4r}{\sqrt{3}}\right)^3$.
- For $fcc$:
- Mass of atoms = 4 atoms × Atomic mass.
- Volume = $a^3 = \left(\frac{4r}{\sqrt{2}}\right)^3$.
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Determine the density ratio:
- The density ratio is given by:
- $\frac{\rho_{\text{bcc}}}{\rho_{\text{fcc}}} = \frac{2 \times \left(\frac{4r}{\sqrt{3}}\right)^3}{4 \times \left(\frac{4r}{\sqrt{2}}\right)^3}$.
- Simplifying yields, $\frac{3\sqrt{3}}{4\sqrt{2}}$.
This calculation shows that the ratio of the density of iron at room temperature (bcc structure) to that at $900^{\circ}C$ (fcc structure) is $\frac{3\sqrt{3}}{4\sqrt{2}}$, aligned with the correct option.