This solution calculates the percentage volume change when pure iron transforms from a Body Centered Cubic (BCC) structure to a Face Centered Cubic (FCC) structure, using the provided lattice parameters. The calculation focuses on the change in volume per atom.
First, calculate the volume of the BCC unit cell.
Given the BCC lattice parameter $ a_{BCC} = 0.293 \text{ nm} $. The volume is:
$ V_{BCC} = a_{BCC}^3 = (0.293 \text{ nm})^3 \approx 0.02515 \text{ nm}^3 $
Since a BCC unit cell contains 2 atoms, the volume per atom is:
$ V_{atom, BCC} = \frac{V_{BCC}}{2} = \frac{0.02515 \text{ nm}^3}{2} \approx 0.01258 \text{ nm}^3 $
Next, calculate the volume of the FCC unit cell.
Given the FCC lattice parameter $ a_{FCC} = 0.363 \text{ nm} $. The volume is:
$ V_{FCC} = a_{FCC}^3 = (0.363 \text{ nm})^3 \approx 0.04783 \text{ nm}^3 $
Since an FCC unit cell contains 4 atoms, the volume per atom is:
$ V_{atom, FCC} = \frac{V_{FCC}}{4} = \frac{0.04783 \text{ nm}^3}{4} \approx 0.01196 \text{ nm}^3 $
Calculate the percentage change in volume per atom relative to the BCC phase.
The formula for percentage volume change is:
$ \% \Delta V = \frac{V_{atom, FCC} - V_{atom, BCC}}{V_{atom, BCC}} \times 100 $
Substitute the calculated volumes per atom:
$ \% \Delta V = \frac{0.01196 \text{ nm}^3 - 0.01258 \text{ nm}^3}{0.01258 \text{ nm}^3} \times 100 $
$ \% \Delta V = \frac{-0.00062}{0.01258} \times 100 \approx -4.92\% $
Rounding the result to one decimal place gives -4.9%.
| Column I | Column II |
|---|---|
| (P) Tetragonal | (1) $a \neq b \neq c$, $\alpha = \beta = \gamma = 90^\circ$ |
| (Q) Rhombohedral | (2) $a = b \neq c$, $\alpha = \beta = \gamma = 90^\circ$ |
| (R) Orthorhombic | (3) $a \neq b \neq c$, $\alpha = \gamma = 90^\circ \neq \beta$ |
| (S) Monoclinic | (4) $a = b = c$, $\alpha = \beta = \gamma \neq 90^\circ$ |
The lattice parameter of face-centered cubic iron ($\gamma$-Fe) is 0.3571 nm. The radius (in nm) of the octahedral void in $\gamma$-Fe is _______________