In: Physics
In an XRD pattern using Cu Kα radiation, a certain cubic crystal shows peaks at 2θ values (in degrees) of 44.3, 64.4, 81.6, 98.0. It is known that the size of the cubic crystal is greater than 2.5 Angstroms. Based on this information and the location of the peaks, we conclude that the lattice of the crystal is
1. simple cubic 2. face centered cubic
3. body centered cubic 4. none of the other choices
The Bragg's law of crystal diffraction gives
For an (hkl) plane in a cubic crystal,
Considering only n = 1 mode,
For each structure, the possible h,k,l values for diffraction is different.
To find the crystal structure, we have to make the following table.
2 theta | Theta | sin(theta) | sin^2(theta) | m = sin^2(theta)/sin^2(theta(min) | 2*m | 3*m |
44.3 | 22.15 | 0.3768511 | 0.142016782 | 0.999999999 | 2 | 3 |
64.4 | 32.2 | 0.5326352 | 0.283700221 | 1.997652794 | 3.995306 | 5.992958 |
81.6 | 40.8 | 0.6531473 | 0.426601376 | 3.003880034 | 6.00776 | 9.01164 |
98 | 49 | 0.7544251 | 0.569157188 | 4.007675572 | 8.015351 | 12.02303 |
Once we make this table, if the row containing m appears as continuous counting numbers (approximately), the crystal structure is simple cubic
If the row 2*m is showing this property, the crystal is BCC and FCC for 3*m
Here, the periodic nature is there for m itself. So, the crystal structure is simple cubic.