For FCC crystals, the Bragg angle \( x \) corresponds to the first diffraction peak and \( y \) corresponds to the third diffraction peak. The diffraction pattern for FCC crystals follows the relationship between the Miller indices and the diffraction angle. For the first and third peaks, the Miller indices are (111) and (333), respectively.
The general equation for Bragg’s law is:
\[
n\lambda = 2d \sin \theta
\]
Where:
- \( n \) is the order of the diffraction,
- \( \lambda \) is the wavelength of the incident radiation,
- \( d \) is the interplanar spacing, and
- \( \theta \) is the Bragg angle.
Now, the relationship between the Bragg angle \( x \) and \( y \) for the FCC crystal is as follows:
- For the first peak, \( n = 1 \) and \( d_1 = \frac{a}{\sqrt{3}} \),
- For the third peak, \( n = 3 \) and \( d_3 = \frac{a}{\sqrt{9}} \).
From this, we know that the ratio of the sine of the angles is:
\[
\frac{\sin y}{\sin x} = \frac{\sqrt{3}}{1} = 1.73
\]
Thus, the ratio lies between 1.4 and 1.8.