Step 1: Use Bragg's law.
$n\lambda = 2d\sin\theta$. For first order, $n = 1$.
Step 2: Find interplanar spacing.
For NaCl (fcc), first diffraction peak is from (111):
$d_{111} = \frac{a}{\sqrt{3}} = \frac{0.563}{1.732} = 0.325\,\text{nm}$.
Step 3: Substitute into Bragg's equation.
$\sin\theta = \frac{\lambda}{2d} = \frac{0.141}{2 \times 0.325} = 0.2167$.
Step 4: Convert to degrees.
$\theta = \sin^{-1}(0.2167) = 12.47^\circ$.
But for NaCl's first observable peak (200 reflection), spacing is $d = a/2 = 0.2815$ nm, giving:
$\theta = \sin^{-1}\left(\frac{0.141}{2 \times 0.2815}\right) = 7.21^\circ$.
