Step 1: Bragg’s law.
Bragg’s law states:
\[
n\lambda = 2 d \sin \theta
\]
where \(d\) is the interplanar spacing, \(\theta\) is the Bragg angle, and \(\lambda\) is the wavelength.
Since the wavelength is constant, \(\sin \theta \propto \frac{1}{d}\).
Step 2: Interplanar spacing for cubic lattice.
For a cubic crystal,
\[
d_{hkl} = \frac{a}{\sqrt{h^2+k^2+l^2}}
\]
Thus,
\[
\sin \theta \propto \sqrt{h^2+k^2+l^2}
\]
Step 3: Allowed reflections in FCC.
FCC reflections are allowed only if \(h,k,l\) are all odd or all even.
So, the first few reflections are:
- (111): \(h^2+k^2+l^2 = 3\)
- (200): \(h^2+k^2+l^2 = 4\)
- (220): \(h^2+k^2+l^2 = 8\)
Hence, the first peak corresponds to (111), the second to (200), and the third to (220).
Step 4: Ratio of \(\sin \theta\).
\[
\frac{\sin y}{\sin x} = \frac{\sqrt{8}}{\sqrt{3}} = \sqrt{\frac{8}{3}}
\]
\[
\sqrt{\frac{8}{3}} = \sqrt{2.6667} \approx 1.633
\]
Final Answer:
\[
\boxed{1.6}
\]