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A seminar talk
on
X-Ray Diffraction(XRD)
Presented by
GITA KRUSHNA SATAPATHY
Regd. no-160705120038
Plan of Talk
• What is XRD?
• Why XRD?
• Diffraction Methods.
• Applications of XRD.
• Advantages & Disadvantages.
Definition
The atomic planes of a crystal cause an incident beam of
X-rays to interfere with one another as they leave the crystal.
The phenomenon is called X-ray diffraction.
What is X-ray Diffraction ?
Why XRD?
 Measure the interplanar spacing between layers of
atoms.
 Determine the orientation of a single crystal or grain.
 Determine crystal structure of an unknown material.
 Measure the size, shape and internal stress of small
crystalline regions.
Diffraction Methods
Method Wavelength Angle Specimen
Bragg’s
Laue
Variable
Variable
Variable
Fixed
Single
Crystal
Single
Crystal
Rotating
Crystal
Fixed Variable (in
part)
Single
Crystal
Powder Fixed Variable Powder
Bragg’s Method
n=2dsin
n: Order of reflection
d: Plane spacing
=
: Bragg Angle
λ < 2d
 Path difference must be integral multiples of the wavelength
& in=out
in out
2
2 2 2
a
h k l 
Laue Method
 The diffraction spots generally
lying on an ellipse
Back-reflection method
 The diffraction spots generally
lying on an hyperbola.
Zone axis
crystal
Incident beam
Film
Reflection Zone axis
crystal
Incident beam Film
 Used to assess crystal perfection from the size and shape .
 It is the only method for the study of large and thick
specimens.
 Crystal orientation is determined from the position of the
spots.
Transmission Laue method
Rotating Crystal Method
 Determine the shape & size of unit cell as well as
the arrangement of atoms inside the cell.
 The Lattice constant of the crystal.
film
 Determine the crystal structure of un known material.
Powder Method
 Useful for determining the complex structures of metals
and alloys.
 Determine the unit cell dimensions.
 Measure the sample purity.
Incident Beam Sample
Film
Determination of Structure Factor
2 ( )
1
n n n
N
i hu kv lw
hkl nF f e   
 
Bravais Lattice Reflections possibly present Reflections necessarily absent
Simple All None
Body Centered (h+k+l): Even (h+k+l): Odd
Face Centered h, k, and l unmixed i.e. all
odd or all even
h, k, and l: mixed
 h,k,l : miller indices
 u,v,w : co-ordinates of the atoms in the lattice
 N : number of atoms
 fn : scattering factor
Applications of XRD
BCC
FCC
Significance of Peak Shape in XRD
 Peak position
 Peak width
 Peak intensity
 Important for
 Particle or
grain size
 Residual
strain
 Plane spacing
Bragg’s Law
n = 2d sin
For 1st order reflection n=1
So  = 2d sin
For cubic crystals
hkl 2 2 2
2 2
2 2 2 2
a
d
h k l
which gives rise to
sin θ
h k l 4a
which is a constant


 

 
INTERPLANAR SPACING & LATTICE
CONSTANT DETERMINATION
Crystallite size can be calculated using Scherer Formula
T=
Kλ
𝑩𝒄𝒐𝒔θ
 T = crystallite thickness
 λ (X-ray wavelength, Å)
 K (Scherer’s constant) ~ 0.9
 B=Full width with half maximum
 =Diffraction angle at peak position
PARTICLE SIZE DETERMINATION
STRAIN EFFECTS
Also applicable for
Phase analysis
Lattice parameter determination
Strain determination
Texture and orientation analysis
Order-disorder transformation & Thin film
characterization
Advantages & Disadvantages of XRD
Compared to Other Methods
Advantages
 Least expensive, the most convenient.
 Widely used method to determine crystal structures.
 The best method for phase analysis.
 X-Rays are not absorbed very much by air, so the sample
need not be in an evacuated chamber.
Disadvantages
 X-Rays do not interact very strongly with lighter
elements.
 The intensity is 𝟏𝟎 𝟖 times less than that of electron
diffraction.
Xrd

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Xrd

  • 1. A seminar talk on X-Ray Diffraction(XRD) Presented by GITA KRUSHNA SATAPATHY Regd. no-160705120038
  • 2. Plan of Talk • What is XRD? • Why XRD? • Diffraction Methods. • Applications of XRD. • Advantages & Disadvantages.
  • 3. Definition The atomic planes of a crystal cause an incident beam of X-rays to interfere with one another as they leave the crystal. The phenomenon is called X-ray diffraction. What is X-ray Diffraction ?
  • 4. Why XRD?  Measure the interplanar spacing between layers of atoms.  Determine the orientation of a single crystal or grain.  Determine crystal structure of an unknown material.  Measure the size, shape and internal stress of small crystalline regions.
  • 5. Diffraction Methods Method Wavelength Angle Specimen Bragg’s Laue Variable Variable Variable Fixed Single Crystal Single Crystal Rotating Crystal Fixed Variable (in part) Single Crystal Powder Fixed Variable Powder
  • 6. Bragg’s Method n=2dsin n: Order of reflection d: Plane spacing = : Bragg Angle λ < 2d  Path difference must be integral multiples of the wavelength & in=out in out 2 2 2 2 a h k l 
  • 7. Laue Method  The diffraction spots generally lying on an ellipse Back-reflection method  The diffraction spots generally lying on an hyperbola. Zone axis crystal Incident beam Film Reflection Zone axis crystal Incident beam Film  Used to assess crystal perfection from the size and shape .  It is the only method for the study of large and thick specimens.  Crystal orientation is determined from the position of the spots. Transmission Laue method
  • 8. Rotating Crystal Method  Determine the shape & size of unit cell as well as the arrangement of atoms inside the cell.  The Lattice constant of the crystal. film  Determine the crystal structure of un known material.
  • 9. Powder Method  Useful for determining the complex structures of metals and alloys.  Determine the unit cell dimensions.  Measure the sample purity. Incident Beam Sample Film
  • 10. Determination of Structure Factor 2 ( ) 1 n n n N i hu kv lw hkl nF f e      Bravais Lattice Reflections possibly present Reflections necessarily absent Simple All None Body Centered (h+k+l): Even (h+k+l): Odd Face Centered h, k, and l unmixed i.e. all odd or all even h, k, and l: mixed  h,k,l : miller indices  u,v,w : co-ordinates of the atoms in the lattice  N : number of atoms  fn : scattering factor Applications of XRD
  • 12. Significance of Peak Shape in XRD  Peak position  Peak width  Peak intensity  Important for  Particle or grain size  Residual strain  Plane spacing
  • 13. Bragg’s Law n = 2d sin For 1st order reflection n=1 So  = 2d sin For cubic crystals hkl 2 2 2 2 2 2 2 2 2 a d h k l which gives rise to sin θ h k l 4a which is a constant        INTERPLANAR SPACING & LATTICE CONSTANT DETERMINATION
  • 14. Crystallite size can be calculated using Scherer Formula T= Kλ 𝑩𝒄𝒐𝒔θ  T = crystallite thickness  λ (X-ray wavelength, Å)  K (Scherer’s constant) ~ 0.9  B=Full width with half maximum  =Diffraction angle at peak position PARTICLE SIZE DETERMINATION
  • 16. Also applicable for Phase analysis Lattice parameter determination Strain determination Texture and orientation analysis Order-disorder transformation & Thin film characterization
  • 17. Advantages & Disadvantages of XRD Compared to Other Methods Advantages  Least expensive, the most convenient.  Widely used method to determine crystal structures.  The best method for phase analysis.  X-Rays are not absorbed very much by air, so the sample need not be in an evacuated chamber. Disadvantages  X-Rays do not interact very strongly with lighter elements.  The intensity is 𝟏𝟎 𝟖 times less than that of electron diffraction.