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MENA3100, 3/2-10, OBK. X-ray diffraction. XRD. Røntgendiffraksjon. Single crystal. Powder. Diffraction. Crystal. Atomic arrangement. Lattice. Lattice + base. The 14 Bravais lattices. 1848. Bragg’s law. 2 d sin q = n l. Bragg’s law. 2 d sin q = n l. n = 2. 2nd. order.
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MENA3100, 3/2-10, OBK X-ray diffraction XRD Røntgendiffraksjon Single crystal Powder
Crystal Atomic arrangement Lattice
Lattice + base The 14 Bravais lattices 1848
Bragg’s law 2d sinq = nl
Bragg’s law 2d sinq = nl n = 2 2nd. order But XRD is typically done with monochromatic radiation
Bragg’s law 2d sinq = nl 2nd. order from 001 1th. order from 002
The 14 Bravais lattices Face centered cubic lattice g-iron NaCl g-brass
Extinction Utslukning Example: Face centered cubic Special example: Cubic close packed structure
Extinction Utslukning Example: Face centered cubic Special example: Cubic close packed structure
X-ray diffraction Need X-rays Wavelenght CuKa1 = 1.54056 Å MoKa1 = 0.70930 Å Characteristic X-rays CuKa1 = 1.54056 Å CuKa2 = 1.54433 Å Brehmsstrahlung = white radiation I(CuKa1) = 2·I(CuKa2) CuKa = 1.5418 Å
Need sample Single crystal Powder
Need experimental setup Bragg-Brentano geometry (Primary monochromator) Diffractometer (Secondary monochromator)
Characteristic X-rays Brehmsstrahlung = white radiation Want monochromatic radiation Monochromators: Many possibilities
Euclid, The Elements (300 B.C.) Proposition 21, Book III: The angles in the same segment of a circle are equal to another Johansson monochromator
Bragg-Brentano geometry The source S can be:
Need detector … Need some slits … Fixed slits: Smaler area at high angle Smaller area at high angles Variable slits: Same area at all angles S Sample
The experiment Got some crystals Want a powder Gets lot of small crystals
Want powder Random orientation
The result The diffractogram Quartz (Don’t call it spectrum)
Identification PDF = JCPDS
Strain Particle size
CuKa1 = 1.54056 Å CuKa2 = 1.54433 Å Primary and secondary monochromators