x-rays physics

Upload: bbkanil

Post on 04-Jun-2018

232 views

Category:

Documents


0 download

TRANSCRIPT

  • 8/13/2019 X-rays physics

    1/14

    X-ray Diffraction

  • 8/13/2019 X-rays physics

    2/14

    X-ray Generation

    X-ray tube (sealed) Pure metal target (Cu)

    Electrons removerinner-shell electronsfrom target.

    Other electrons fallinto hole.

  • 8/13/2019 X-rays physics

    3/14

    X-ray Generation

    The incoming electronmust have enough energy

    to remove inner 1selectrons from the copperatoms.

    This energy correspondsto the Cu absorption edge

    The 2sand 2pelectronsfall back into the 1s shelland emit the K1K2

    lines.

  • 8/13/2019 X-rays physics

    4/14

    X-ray Spectrum from Tube

  • 8/13/2019 X-rays physics

    5/14

    Energy Calculations

    Plancks constant (h) = 6.6 * 10-34

    joule-sec 1 electron-volt = 1.6016 * 10-19joule

    Speed of light (c) = 3.0 * 108

    m/s Photon frequency= c/ Photon Energy E = h= hc/

  • 8/13/2019 X-rays physics

    6/14

    Energy Calculations

    What is the minimum potential in KV that isrequired to excite Cu K-series radiation from a Cu-

    target X-ray tube? Absorption edge of Cu = 1.380

    E = hc/= (6.60 10-34)(3*108)/(1.380*10-10) E = 1.435*10-15joule

    E = 1.435*10-15/1.6016*10-19 = 8958 ev The potential on the tube must exceed 8.958 KV

  • 8/13/2019 X-rays physics

    7/14

    Diffraction

    Diffraction is the coherent scattering of waves

    from a periodic array of scatterers. The wavelength of light is about half a micron

    Light is diffracted by the tracks in a CD. The wavelengths of X-rays is about the same

    as the interatomic distances in crystals. Crystals diffract X-rays.

  • 8/13/2019 X-rays physics

    8/14

    X-Ray Diffraction

    Atoms separated bydistancedwill scatter inphase when the path length

    difference is an integralnumber of wavelengths.

    Path length difference B-C-

    D = n n= 2dsin

  • 8/13/2019 X-rays physics

    9/14

    X-ray Diffraction Experiment

    We use the monochromatic K1-2lines forour diffraction experiment.

    The wavelength is 1.5405

    We use a diffracted beam monochromatorto clean up the X-rays entering the detector.

    We use a powdered sample so that allorientations are present in the sample.

    We move the detector through angle 2.

  • 8/13/2019 X-rays physics

    10/14

  • 8/13/2019 X-rays physics

    11/14

    Miller Indices

    The real use of Miller indicesis to describe diffractionplanes.

    For a lattice plane with Millerindicesh klin anorthorhombic latticea b c,

    d = 1 / [(h/a)2+(k/b)2+(l/c)2]1/2

    For cubic:

    d = a/[h2+k2+l2]1/2

  • 8/13/2019 X-rays physics

    12/14

    Diffraction Calculations

    For forsteritea= 4.75;b= 10.20; c = 5.98

    Calculate 2for the (201) lattice spacing for Cuk(=1.5405) d = 1 / [(h/a)2+(k/b)2+(l/c)2]1/2

    d = 1/ [(2/4.75)2+(1/5.98)2]1/2

    d= 1/0.4530 = 2.207

    2= 2 sin-1/2d =2* sin-1(1.5405/4.414)

    2= 2 * 20.43 = 40.86

  • 8/13/2019 X-rays physics

    13/14

    XPOW

    XPOW uses the unit cell and atom position data tocalculate the diffraction pattern.

    Intensities can be calculated knowing the positionand scattering characteristics of each atom.

    Fhkl= square root of integrated intensity. fj= scattering of atomjat angle 2

    Atomjlocated at fractional coordinatesxj, yj, zj.

    =

    ++=

    n

    j

    lzkyhxi

    jhkl

    jjjefF1

    )(2

  • 8/13/2019 X-rays physics

    14/14

    Uses of X-ray Powder Diffraction

    Mineral identification Determination of Unit Cell Parameters

    Modal (phase percentage) Analysis Crystal Structure Determination