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 X-Rays are electromagnetic radiations with
wave lengths of the order of 0.1nm.
 X-rays are produced when electrons from a
heated filament strike the metal target.
 In 1912 physicist Max Von Laue discovered
that a crystalline solid , consisting as it does of
regular array of atoms ,might form a natural
three - dimensional diffraction grating for x-
rays.
 Question:
So if all electromagnetic radiation can diffract,
why are X-rays used in crystallography?
Ans….
 X-rays have wavelengths on the order of a few
angstroms (1 Angstrom = 0.1nm). This is the
typical inter-atomic distance in crystalline
solids, making X-rays the correct order of
magnitude for diffraction of atoms of
crystalline materials.
 A grating with d= wavelength is desirable for x-
ray diffraction.
 diffraction occurs when a wave encounters a
series of regularly spaced obstacles that are;
 Capable of scattering the wave.
 Have spacing that are comparable in magnitude
to the wavelength
 If a collimated beam of x-rays, is allowed to
fall on a crystal ,intense beams appear in certain
sharply defined directions.
 if these beams fall on a photographic film, they
form an assembly of Laue spots.
 fundamentally, the x-rays are diffracted by
electrons ,diffraction by nuclei being negligible
in most cases.
 thus the diffracting characteristics of a unit cell
depend on how the electron are distributed
throughout the volume of the unit cell.
 by studying the directions of diffracted x-ray
beams, we can learn the basic symmetry of the
crystal.
 and by studying intensities we can learn how
the electron are distributed in a unit cell.
 In 1914 W.H Bragg and W.L Bragg study the
atomic structure of crystal by using X-rays
 Consider the two parallel planes of atoms A-A´
And B-B‛ which are separated by interplanar
spacing d.
 Now assume that a parallel , monochromatic
beam of x-rays of wavelength ⋏ is incident on
these two planes at an angle ⏀.
 two rays in this beam , labeled 1 and 2 are
scattered by atoms P and Q.
 ray 2 covered some extra path as compared to
ray 1
 this extra path is called path difference .
 Constructive interference of scattered rays 1‘
and 2‘ at an angle ⏀ to the plane, if the path
difference between 1- P-1’ and 2-Q-2‘ ,is equal to
whole number , n , of wavelength;
 so
 n⋏=SQ+QT
 n⋏=d sin⏀+ d sin⏀
 n⋏=2d sin⏀
 this is known as Bragg’s law.
X-ray  diffraction

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X-ray diffraction

  • 1.
  • 2.  X-Rays are electromagnetic radiations with wave lengths of the order of 0.1nm.  X-rays are produced when electrons from a heated filament strike the metal target.  In 1912 physicist Max Von Laue discovered that a crystalline solid , consisting as it does of regular array of atoms ,might form a natural three - dimensional diffraction grating for x- rays.
  • 3.  Question: So if all electromagnetic radiation can diffract, why are X-rays used in crystallography? Ans….  X-rays have wavelengths on the order of a few angstroms (1 Angstrom = 0.1nm). This is the typical inter-atomic distance in crystalline solids, making X-rays the correct order of magnitude for diffraction of atoms of crystalline materials.
  • 4.  A grating with d= wavelength is desirable for x- ray diffraction.  diffraction occurs when a wave encounters a series of regularly spaced obstacles that are;  Capable of scattering the wave.  Have spacing that are comparable in magnitude to the wavelength
  • 5.  If a collimated beam of x-rays, is allowed to fall on a crystal ,intense beams appear in certain sharply defined directions.  if these beams fall on a photographic film, they form an assembly of Laue spots.  fundamentally, the x-rays are diffracted by electrons ,diffraction by nuclei being negligible in most cases.
  • 6.  thus the diffracting characteristics of a unit cell depend on how the electron are distributed throughout the volume of the unit cell.  by studying the directions of diffracted x-ray beams, we can learn the basic symmetry of the crystal.  and by studying intensities we can learn how the electron are distributed in a unit cell.
  • 7.  In 1914 W.H Bragg and W.L Bragg study the atomic structure of crystal by using X-rays  Consider the two parallel planes of atoms A-A´ And B-B‛ which are separated by interplanar spacing d.  Now assume that a parallel , monochromatic beam of x-rays of wavelength ⋏ is incident on these two planes at an angle ⏀.  two rays in this beam , labeled 1 and 2 are scattered by atoms P and Q.
  • 8.  ray 2 covered some extra path as compared to ray 1  this extra path is called path difference .  Constructive interference of scattered rays 1‘ and 2‘ at an angle ⏀ to the plane, if the path difference between 1- P-1’ and 2-Q-2‘ ,is equal to whole number , n , of wavelength;  so
  • 9.  n⋏=SQ+QT  n⋏=d sin⏀+ d sin⏀  n⋏=2d sin⏀  this is known as Bragg’s law.