1 / 23

X-ray crystallography

X-ray crystallography. What tools do we have to ID minerals so far?. How do we know atomic structure of minerals?. Atoms are 1-5Å apart so how do we see this?. X-rays. Between 0.1 and 10Å (1Å = 0.1 nm). X-rays. Amplitude Wavelength. X-ray interference. Constructive is in phase.

michon
Télécharger la présentation

X-ray crystallography

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. X-ray crystallography

  2. What tools do we have to ID minerals so far?

  3. How do we know atomic structure of minerals? • Atoms are 1-5Å apart so how do we see this?

  4. X-rays • Between 0.1 and 10Å (1Å = 0.1 nm)

  5. X-rays • Amplitude • Wavelength

  6. X-ray interference Constructive is in phase Destructive if out of phase

  7. Wave behavior Interference and diffraction If a wave encounters a barrier with several holes, the propagating wave will have sharper peaks of intensity at certain angles.

  8. X-rays interact with atoms • Atoms cause scattering • Diffraction: coherent scattering of waves off a periodic arrangement of matter

  9. Generation of X-rays • Need • Vacuum environment • Source of electrons • Large accelerating voltage • Target metal

  10. Generation of X-rays • Tungsten filament as source of e- • E- sent to target metal (usually Cu) • X-rays generated off Cu • Higher voltage, faster e-, more energy

  11. X-ray Crystallography X-ray generation W C a t h o d e C u A n o d e ( - ) ( + ) electrons X - r a y s

  12. Two types of X-rays generated • Continuous spectra (white radiation) • Electrons hit target surface, loose energy, stop • NO change of target electron configuration • Removed by filtering

  13. Two types of X-rays generated • Characteristic radiation • Electrons interact with target electron configuration • Fingerprint of target metal

  14. Two types of X-rays generated • Bombarding electrons dislodge electron from target • K-shell or L-shell • If vacancy in K-shell filled from L-shell, Kradiation • If vacancy if K-shell filled from M-shell, K radiation

  15. Two types of X-rays generated • K radiation has more energy than K radiation

  16. Two types of X-rays generated • K radiation has more energy than K radiation • Quantized energy and characteristic of metal target

  17. Table 2-1: Wavelengths in Nanometer Units of Characteristic Emission Lines for Selected Elements. Element K[alpha] K[alpha]1 K[alpha]2 K[beta]1 L[alpha]1 Cr 0.229092 0.228962 0.229351 0.228480 **** Cu 0.154178 0.154051 0.1544330 0.139217 1.3357 Mo 0.071069 0.070926 0.071354 0.063225 0.54062 W 0.021060 0.020899 0.021381 0.018436 0.14763

  18. Characteristic radiation more intense than continuous • Want Ka radiation to go to sample so need to filter everything else

  19. Sample sees monochromatic radiation

  20. X-ray detection • Photographically • Electronic detectors • Result: see planes of atoms and what orientation planes are in • Don’t get image of individual atoms

  21. X-ray diffraction • Works thanks to Bragg Equation • X-rays diffract at specific angles based on spacing of atomic planes

  22. X-ray Crystallography Destructive and constructive interference of waves Bragg Equation: in phase in phase Y x q q q d

  23. X-ray Crystallography nl=2dsinq n is the “order” As soon as the crystal is rotated, the beam ceases (This is diffraction, not reflection) Only get diffraction at certain angles! Relation between l and d and q Y x q q d

More Related