This problem requires calculating the lattice parameter ('a') of a face-centered cubic (fcc) metal using information from an X-ray diffraction (XRD) experiment. We can use Bragg's Law and the formula for interplanar spacing in cubic crystals.
$\theta = \frac{2\theta}{2} = \frac{78^\circ}{2} = 39^\circ$
For {311} planes in an fcc lattice, the indices are $h=3, k=1, l=1$. The sum of squares is:
$h^2 + k^2 + l^2 = 3^2 + 1^2 + 1^2 = 9 + 1 + 1 = 11$
Bragg's Law is $n\lambda = 2d \sin\theta$. Assuming the first-order peak ($n=1$):
$\lambda = 2d \sin\theta$
Rearranging for $d$:
$d = \frac{\lambda}{2 \sin\theta}$
Substitute the values:
$d = \frac{0.154 \text{ nm}}{2 \times \sin(39^\circ)}$
Using $\sin(39^\circ) \approx 0.6293$:
$d \approx \frac{0.154 \text{ nm}}{2 \times 0.6293} \approx \frac{0.154}{1.2586} \approx 0.12236$ nm
The formula for interplanar spacing ($d_{hkl}$) in a cubic system is:
$d_{hkl} = \frac{a}{\sqrt{h^2 + k^2 + l^2}}$
Rearranging to solve for the lattice parameter 'a':
$a = d_{hkl} \times \sqrt{h^2 + k^2 + l^2}$
Substitute the calculated $d$ and the sum of squares:
$a \approx 0.12236 \text{ nm} \times \sqrt{11}$
Using $\sqrt{11} \approx 3.3166$:
$a \approx 0.12236 \text{ nm} \times 3.3166 \approx 0.4058$ nm
The calculated lattice parameter is approximately 0.4058 nm, which is closest to the option 0.4 nm.
| 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 _______________