lec-2d.pdf
TRANSCRIPT
-
X-Ray Diffraction Allows information about the crystal structure of material
to be obtained.
(a) Destructive and (b) constructive interactions between x-rays and the crystal structure of a material. Diffraction occurs at angles that satisfy the Bragg equation.
-
X-rays that strike certain crystallographic planes at specific angles are reinforced and diffracted according to the Braggs law:
where = half the angle between the diffracted beam and the original beam direction, = wavelength of the x-raysdhkl = interplanar spacing between the planes that cause Bragg diffraction
hkld2sin =
222 lkhadhkl ++
=
-
(a) Schematic of an x-ray powder diffractometer showing the incident and diffracted beam, the sample in powdered form, and the movable x-ray detector. (b) The diffraction pattern of gold powder.
-
Analysis of the diffraction pattern allows the identification of the unknown material and the indexation of the diffracted peaks and their Bragg planes (hkl).
BCC: FCC:
)(4
sin 22222 lkh
a++=
)(4
sin 22222
2
lkha
++=
,......12,10,8,6,4,2222 =++ lkh
,......16,12,11,8,4,3222 =++ lkh
-
Example Problem
The results of an X-ray diffraction experiment using x-rays with = 0.07107 nm show that diffracted peaks occur at the following 2angles:
Peak 2 Peak 2
1 20.20 5 46.19
2 28.72 6 50.90
3 35.36 7 55.28
4 41.07 8 59.42
-
Determine the crystal structure, the indices of the plane producing each peak, and the lattice parameter (a) of the material.
2sin 222 lkh ++Peak 2 (hkl)1 20.20 0.0308 1 2 110
2 28.72 0.0615 2 4 200
3 35.36 0.0922 3 6 211
4 41.07 0.1230 4 8 220
5 46.19 0.1539 5 10 310
6 50.90 0.1847 6 12 222
7 55.28 0.2152 7 14 321
8 59.42 0.2456 8 16 400
0308.0sin2
-
So, the crystal structure of the material is BCC.
Use any diffracted peak to determine dhkl and , say peak 8 or (400)
So the material is BCC iron.
222400 lkhda ++=
nmd 071699.0)71.29sin(2
07107.0sin2400
===
= (0.071699)(4) = 0.2868 nm
nmaR 1242.04
3 ==
-
X-Ray DiffractionExample Problem