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What is particle shape ?
โ€ข Particle shape is the external appearance of a particle.
โ€ข Various different aspects of particle shape are of interest and a range of
descriptors has been devised to allow particle shape to be described.
โ€ข No single shape descriptor is suitable for all applications.
Particle shape can be described qualitatively using the following descriptors :
โ€ข Width/length ratio
โ€ข Convexity
โ€ข Circularity/roundness
๐‘พ๐’Š๐’…๐’•๐’‰/๐’๐’†๐’๐’ˆ๐’•๐’‰ ๐’“๐’‚๐’•๐’Š๐’ =
๐’”๐’‰๐’๐’“๐’•๐’†๐’”๐’• ๐’…๐’Š๐’‚๐’Ž.
๐’๐’๐’๐’ˆ๐’†๐’”๐’• ๐’…๐’Š๐’‚๐’Ž.
=
โŠฅ ๐’•๐’ ๐’๐’๐’๐’ˆ๐’†๐’”๐’• ๐’…๐’Š๐’‚๐’Ž.
๐’๐’๐’๐’ˆ๐’†๐’”๐’• ๐’…๐’Š๐’‚๐’Ž.
=
๐‘ญ ๐’Ž๐’Š๐’
๐‘ญ ๐’Ž๐’‚๐’™
๐‘ช๐’๐’๐’—๐’†๐’™๐’Š๐’—๐’Š๐’•๐’š =
๐‘จ ๐’“๐’†๐’‚๐’
๐‘จ ๐’„๐’๐’๐’—๐’†๐’™
silhouette
๐‘ฌ๐’’๐’–๐’Š๐’—๐’‚๐’๐’†๐’๐’• ๐‘ซ๐’Š๐’‚๐’Ž๐’†๐’•๐’†๐’“(๐‘ซ ๐’†๐’’) = ๐Ÿ
๐‘จ
๐…
convexivity
Width/length ratio
symmetry
๐‘บ๐’š๐’Ž๐’Ž๐’†๐’•๐’“๐’š =
1
2
1 + ๐‘š๐‘–๐‘›
๐‘Ÿ1
๐‘Ÿ2
Raw Image
Input
Image Analysis
(Object Detection)
True Circularity or degree of circularity (Wadell,1933)
๐‘ซ๐’†๐’ˆ๐’“๐’†๐’† ๐’๐’‡ ๐’„๐’Š๐’“๐’„๐’–๐’๐’‚๐’“๐’Š๐’•๐’š =
๐’„๐’Š๐’“๐’„๐’–๐’Ž๐’‡๐’†๐’“๐’†๐’๐’‚๐’„๐’† ๐’๐’‡ ๐’†๐’’๐’–๐’Š๐’—๐’‚๐’๐’†๐’๐’• ๐’„๐’Š๐’“๐’„๐’๐’†
๐’„๐’Š๐’“๐’„๐’–๐’Ž๐’‡๐’†๐’“๐’†๐’๐’„๐’† ๐’๐’‡ ๐’•๐’‰๐’† ๐’‡๐’Š๐’ˆ๐’–๐’“๐’†
Irregularity(Umbaugh, 2005)
๐‘ฐ๐’“๐’“๐’†๐’ˆ๐’–๐’๐’‚๐’“๐’Š๐’•๐’š =
๐Ÿ
๐‘ช๐’๐’™โ€ฒ๐’” ๐’„๐’Š๐’“๐’„๐’–๐’๐’‚๐’“๐’Š๐’•๐’š
Roundness(Wadell,1932)
๐‘น๐’๐’–๐’๐’…๐’๐’†๐’”๐’” =
ฯƒ๐’Š=๐ŸŽ
๐’ ๐’“๐’Š
๐‘น
๐’
Where,
ri is the radius of curvature of particle corners
R is the radius of the largest inscribed sphere
n is the number of particle corners measured
Coxโ€™s True Sphericity(1927)
๐‘ป๐’“๐’–๐’† ๐’”๐’‘๐’‰๐’†๐’“๐’Š๐’„๐’Š๐’•๐’š =
๐’”๐’–๐’“๐’‡๐’‚๐’„๐’† ๐’‚๐’“๐’†๐’‚ ๐’๐’‡ ๐’†๐’’๐’–๐’Š๐’—๐’‚๐’๐’†๐’๐’• ๐’”๐’‘๐’‰๐’†๐’“๐’†
๐’”๐’–๐’“๐’‡๐’‚๐’„๐’† ๐’‚๐’“๐’†๐’‚ ๐’๐’‡ ๐’•๐’‰๐’† ๐’ƒ๐’๐’…๐’š
โ€œThe degree to which the ratio of its volume to its
surface approaches the same ratio for a sphereโ€
Lappungโ€™s quotient(๐ต๐‘’๐‘๐‘˜๐‘š๐‘Ž๐‘›๐‘›, 1962)
๐‘ณ๐’‚๐’‘๐’‘๐’–๐’๐’ˆโ€ฒ
๐’” ๐’’๐’–๐’๐’•๐’Š๐’†๐’๐’• =
๐Ÿ
๐‘ป๐’“๐’–๐’† ๐’„๐’Š๐’“๐’„๐’–๐’๐’‚๐’“๐’Š๐’•๐’š
(Range : 1-5)
Sphericity and roundness chart
(Cho et, al.,2006)
Fischerโ€™s method of angularity computation (Hawkins,1993)
Powerโ€™s scale of roundness(1953)
Coxโ€™s Circularity or classic shape factor (1927)
โ€œThe degree to which the ratio of the area to the
circumference approaches the same for circleโ€
๐‘ช๐’Š๐’“๐’„๐’–๐’๐’‚๐’“๐’Š๐’•๐’š =
๐Ÿ’๐…๐‘จ
๐’‘ ๐Ÿ
How to describe it ?
Wadellโ€™s sphericity(1933)
๐‘พ๐’‚๐’…๐’†๐’๐’โ€ฒ
๐’” ๐’”๐’‘๐’‰๐’†๐’“๐’Š๐’„๐’Š๐’•๐’š
=
๐’…๐’Š๐’‚๐’Ž๐’†๐’•๐’†๐’“ ๐’๐’‡ ๐’†๐’’๐’–๐’Š๐’—๐’‚๐’๐’†๐’๐’• ๐’„๐’Š๐’“๐’„๐’๐’†
๐’…๐’Š๐’‚๐’Ž๐’†๐’•๐’†๐’“ ๐’๐’‡ ๐’„๐’Š๐’“๐’„๐’–๐’Ž๐’„๐’Š๐’“๐’„๐’๐’†
=
๐’…๐’Š๐’‚๐’Ž๐’†๐’•๐’†๐’“ ๐’๐’‡ ๐’†๐’’๐’–๐’Š๐’—๐’‚๐’๐’†๐’๐’• ๐’”๐’‘๐’‰๐’†๐’“๐’†
๐’…๐’Š๐’‚๐’Ž๐’†๐’•๐’†๐’“ ๐’๐’‡ ๐’„๐’Š๐’“๐’„๐’–๐’Ž๐’”๐’‘๐’‰๐’†๐’“๐’†
Tickellโ€™s Sphericity(1931)
๐‘ป๐’Š๐’„๐’Œ๐’†๐’๐’โ€ฒ
๐’” ๐’”๐’‘๐’‰๐’†๐’“๐’Š๐’„๐’Š๐’•๐’š =
๐’‚๐’“๐’†๐’‚ ๐’๐’‡ ๐’‡๐’Š๐’ˆ๐’–๐’“๐’†
๐’‚๐’“๐’†๐’‚ ๐’๐’‡ ๐’„๐’Š๐’“๐’„๐’–๐’Ž๐’„๐’Š๐’“๐’„๐’๐’†
=
๐’—๐’๐’๐’–๐’Ž๐’† ๐’๐’‡ ๐’ƒ๐’๐’…๐’š
๐’—๐’๐’๐’–๐’Ž๐’† ๐’๐’‡ ๐’„๐’Š๐’“๐’„๐’–๐’Ž๐’”๐’‘๐’‰๐’†๐’“๐’†
โ€ข Affects the flow properties
โ€ข Powder flow - Spherical particles flow easily
โ€ข Liquid flow - Increase in aspect ratio increases viscosity
โ€ข Liquid flow - More spherical shape particles lead to low viscosity
โ€ข Effects porosity
โ€ข Effects friability
โ€ข Effects sedimentation rate
โ€ข Behavior in sieve analysis
โ€ข Powder mixing โ€“ blend time changes
โ€ข Effects โ€“ wall friction, bulk flow properties, abrasivity, adhesion and
cohesion properties.
โ€ข Adds more importance to particle size
โ€ข Some products work well when :
โžข More spherical โ€“ glass beads for highway paint, proppants
โžข Less spherical - abrasives
Unconfined yield
strength of various
shaped particles as
vs consolidation
pressure
Convexity vs
particle size for
various
pharmaceutical
samples
viscosity vs volume fraction
for various shape of
particles
What is itโ€™s significance ?
How is it measured ?
FESEM (Field Emission Scanning Electron Microscope)
coated stub stub holder
schematic diagram
coal fly ash
SEM-(Energy Dispersive X-ray Spectroscopy)EDAX
results for fly ash
Principle : High energy field emitted e- are incident in vacuum
on a sample to eject secondary e- , backscattered e- , auger e-
and X-rays. These signals contain information about the
surface morphology and the composition of the sample.
FE-SEMQuanta200
FEG
secondary emission in SEM
Standard : ASTM E3 - 11(2017)
Make/Model : Hitachi - SU3500, SU1510, SU8000; FEI โ€“ Quanta
250 FEG; Carl Zeiss - ZEISS Sigma 300, GeminiSEM 500
Recent Activities !!!
SEM and EDS/EDAX of Gypsum sample
TEM (Transmission Electron Microscope)
TEM
holder
grid
schematic diagram
coal fly ash
Principle : High energy field emitted e- in vacuum
are made to transmit pass through a sample
containing grid to fall on a florescent screen or a
image capturing screen
TECNAI G2 20 S-TWIN
Standard : ASTM F1877 - 16
Make/Model :
Hitachi - HF5000, HF3500,
HF9500, HF9500, HF7800,
HF7700; Carl Zeiss โ€“ LIBRA 120
FEI โ€“ TECNAI G2 20 S-TWIN;
image system of
TEM
bright vs dark field
imaging
single crystalamorphous polycrystalline crystal
SelectedArea
ElectronDiffraction
(SAED)โ†ด
How is it measured ? Contd โ€ฆ
XRD (X-ray diffraction)
PANalytical โ€“ Empyrean
Standard : ASTM C1365 - 18
Make/Model : Malvern โ€“ Aeris Research Edition,
PANalytical โ€“ Empyrean, Empyrean Nano,
Empyrean Alpha 1; Bruker - D2 PHASER, D8
ENDEAVOR, D8 ADVANCE
system schematic
Braggโ€™s Law : ๐’๐€ = ๐Ÿ๐’… ๐’‰๐’Œ๐’ ๐ฌ๐ข๐ง ๐œฝ
Where,
n is order
๐œ† is wavelength
๐‘‘โ„Ž๐‘˜๐‘™ is the interplaner distance
๐œƒ is the angle of maximum diffraction
sample holder powder XRD sample preparation
diffraction peak associated with planes of atoms
Principle : X-ray diffraction is based on constructive interference of
monochromatic X-rays and a crystalline sample. These X-rays are generated by
a cathode ray tube, filtered to produce monochromatic radiation, collimated to
concentrate, and directed toward the sample.
๐‘ซ๐’†๐’ƒ๐’š๐’† โˆ’ ๐‘บ๐’‰๐’†๐’‚๐’“๐’†๐’“ ๐’†๐’’๐’–๐’‚๐’•๐’Š๐’๐’ โˆถ ๐‰ =
๐‘ฒ๐€
๐œท ๐œ๐จ๐ฌ ๐œฝ
๐‘Šโ„Ž๐‘’๐‘Ÿ๐‘’,
๐œ = ๐‘š๐‘’๐‘Ž๐‘› ๐‘ ๐‘–๐‘ง๐‘’ ๐‘œ๐‘“ ๐‘๐‘Ÿ๐‘ฆ๐‘ ๐‘ก๐‘Ž๐‘™๐‘™๐‘–๐‘›๐‘’ ๐‘‘๐‘œ๐‘š๐‘Ž๐‘–๐‘›, ๐‘คโ„Ž๐‘–๐‘โ„Ž ๐‘š๐‘Ž๐‘ฆ๐‘๐‘’
๐‘ ๐‘š๐‘Ž๐‘™๐‘™๐‘’๐‘Ÿ ๐‘œ๐‘Ÿ ๐‘’๐‘ž๐‘ข๐‘Ž๐‘™ ๐‘ก๐‘œ ๐‘”๐‘Ÿ๐‘Ž๐‘–๐‘› ๐‘ ๐‘–๐‘ง๐‘’
๐พ = ๐‘‘๐‘–๐‘š๐‘’๐‘›๐‘ ๐‘–๐‘œ๐‘›๐‘™๐‘’๐‘ ๐‘  ๐‘ โ„Ž๐‘Ž๐‘๐‘’ ๐‘“๐‘Ž๐‘๐‘ก๐‘œ๐‘Ÿ ~0.9
๐œ† = ๐‘‹ โˆ’ ๐‘Ÿ๐‘Ž๐‘ฆ ๐‘ค๐‘Ž๐‘ฃ๐‘’๐‘™๐‘’๐‘›๐‘”๐‘กโ„Ž
๐›ฝ = ๐‘™๐‘–๐‘›๐‘’ ๐‘‘๐‘Ÿ๐‘œ๐‘Ž๐‘‘๐‘›๐‘–๐‘›๐‘” ๐‘Ž๐‘ก โ„Ž๐‘Ž๐‘™๐‘“ ๐‘กโ„Ž๐‘’
๐‘š๐‘Ž๐‘ฅ๐‘–๐‘š๐‘ข๐‘š ๐‘–๐‘›๐‘ก๐‘’๐‘›๐‘ ๐‘–๐‘ก๐‘ฆ ๐น๐‘Š๐ป๐‘€
๐œƒ = ๐ต๐‘Ÿ๐‘Ž๐‘”๐‘” ๐‘Ž๐‘›๐‘”๐‘™๐‘’
How is it measured ? Contd โ€ฆ

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Particle Shape

  • 1. What is particle shape ? โ€ข Particle shape is the external appearance of a particle. โ€ข Various different aspects of particle shape are of interest and a range of descriptors has been devised to allow particle shape to be described. โ€ข No single shape descriptor is suitable for all applications. Particle shape can be described qualitatively using the following descriptors : โ€ข Width/length ratio โ€ข Convexity โ€ข Circularity/roundness ๐‘พ๐’Š๐’…๐’•๐’‰/๐’๐’†๐’๐’ˆ๐’•๐’‰ ๐’“๐’‚๐’•๐’Š๐’ = ๐’”๐’‰๐’๐’“๐’•๐’†๐’”๐’• ๐’…๐’Š๐’‚๐’Ž. ๐’๐’๐’๐’ˆ๐’†๐’”๐’• ๐’…๐’Š๐’‚๐’Ž. = โŠฅ ๐’•๐’ ๐’๐’๐’๐’ˆ๐’†๐’”๐’• ๐’…๐’Š๐’‚๐’Ž. ๐’๐’๐’๐’ˆ๐’†๐’”๐’• ๐’…๐’Š๐’‚๐’Ž. = ๐‘ญ ๐’Ž๐’Š๐’ ๐‘ญ ๐’Ž๐’‚๐’™ ๐‘ช๐’๐’๐’—๐’†๐’™๐’Š๐’—๐’Š๐’•๐’š = ๐‘จ ๐’“๐’†๐’‚๐’ ๐‘จ ๐’„๐’๐’๐’—๐’†๐’™ silhouette ๐‘ฌ๐’’๐’–๐’Š๐’—๐’‚๐’๐’†๐’๐’• ๐‘ซ๐’Š๐’‚๐’Ž๐’†๐’•๐’†๐’“(๐‘ซ ๐’†๐’’) = ๐Ÿ ๐‘จ ๐… convexivity Width/length ratio symmetry ๐‘บ๐’š๐’Ž๐’Ž๐’†๐’•๐’“๐’š = 1 2 1 + ๐‘š๐‘–๐‘› ๐‘Ÿ1 ๐‘Ÿ2 Raw Image Input Image Analysis (Object Detection)
  • 2. True Circularity or degree of circularity (Wadell,1933) ๐‘ซ๐’†๐’ˆ๐’“๐’†๐’† ๐’๐’‡ ๐’„๐’Š๐’“๐’„๐’–๐’๐’‚๐’“๐’Š๐’•๐’š = ๐’„๐’Š๐’“๐’„๐’–๐’Ž๐’‡๐’†๐’“๐’†๐’๐’‚๐’„๐’† ๐’๐’‡ ๐’†๐’’๐’–๐’Š๐’—๐’‚๐’๐’†๐’๐’• ๐’„๐’Š๐’“๐’„๐’๐’† ๐’„๐’Š๐’“๐’„๐’–๐’Ž๐’‡๐’†๐’“๐’†๐’๐’„๐’† ๐’๐’‡ ๐’•๐’‰๐’† ๐’‡๐’Š๐’ˆ๐’–๐’“๐’† Irregularity(Umbaugh, 2005) ๐‘ฐ๐’“๐’“๐’†๐’ˆ๐’–๐’๐’‚๐’“๐’Š๐’•๐’š = ๐Ÿ ๐‘ช๐’๐’™โ€ฒ๐’” ๐’„๐’Š๐’“๐’„๐’–๐’๐’‚๐’“๐’Š๐’•๐’š Roundness(Wadell,1932) ๐‘น๐’๐’–๐’๐’…๐’๐’†๐’”๐’” = ฯƒ๐’Š=๐ŸŽ ๐’ ๐’“๐’Š ๐‘น ๐’ Where, ri is the radius of curvature of particle corners R is the radius of the largest inscribed sphere n is the number of particle corners measured Coxโ€™s True Sphericity(1927) ๐‘ป๐’“๐’–๐’† ๐’”๐’‘๐’‰๐’†๐’“๐’Š๐’„๐’Š๐’•๐’š = ๐’”๐’–๐’“๐’‡๐’‚๐’„๐’† ๐’‚๐’“๐’†๐’‚ ๐’๐’‡ ๐’†๐’’๐’–๐’Š๐’—๐’‚๐’๐’†๐’๐’• ๐’”๐’‘๐’‰๐’†๐’“๐’† ๐’”๐’–๐’“๐’‡๐’‚๐’„๐’† ๐’‚๐’“๐’†๐’‚ ๐’๐’‡ ๐’•๐’‰๐’† ๐’ƒ๐’๐’…๐’š โ€œThe degree to which the ratio of its volume to its surface approaches the same ratio for a sphereโ€ Lappungโ€™s quotient(๐ต๐‘’๐‘๐‘˜๐‘š๐‘Ž๐‘›๐‘›, 1962) ๐‘ณ๐’‚๐’‘๐’‘๐’–๐’๐’ˆโ€ฒ ๐’” ๐’’๐’–๐’๐’•๐’Š๐’†๐’๐’• = ๐Ÿ ๐‘ป๐’“๐’–๐’† ๐’„๐’Š๐’“๐’„๐’–๐’๐’‚๐’“๐’Š๐’•๐’š (Range : 1-5) Sphericity and roundness chart (Cho et, al.,2006) Fischerโ€™s method of angularity computation (Hawkins,1993) Powerโ€™s scale of roundness(1953) Coxโ€™s Circularity or classic shape factor (1927) โ€œThe degree to which the ratio of the area to the circumference approaches the same for circleโ€ ๐‘ช๐’Š๐’“๐’„๐’–๐’๐’‚๐’“๐’Š๐’•๐’š = ๐Ÿ’๐…๐‘จ ๐’‘ ๐Ÿ How to describe it ? Wadellโ€™s sphericity(1933) ๐‘พ๐’‚๐’…๐’†๐’๐’โ€ฒ ๐’” ๐’”๐’‘๐’‰๐’†๐’“๐’Š๐’„๐’Š๐’•๐’š = ๐’…๐’Š๐’‚๐’Ž๐’†๐’•๐’†๐’“ ๐’๐’‡ ๐’†๐’’๐’–๐’Š๐’—๐’‚๐’๐’†๐’๐’• ๐’„๐’Š๐’“๐’„๐’๐’† ๐’…๐’Š๐’‚๐’Ž๐’†๐’•๐’†๐’“ ๐’๐’‡ ๐’„๐’Š๐’“๐’„๐’–๐’Ž๐’„๐’Š๐’“๐’„๐’๐’† = ๐’…๐’Š๐’‚๐’Ž๐’†๐’•๐’†๐’“ ๐’๐’‡ ๐’†๐’’๐’–๐’Š๐’—๐’‚๐’๐’†๐’๐’• ๐’”๐’‘๐’‰๐’†๐’“๐’† ๐’…๐’Š๐’‚๐’Ž๐’†๐’•๐’†๐’“ ๐’๐’‡ ๐’„๐’Š๐’“๐’„๐’–๐’Ž๐’”๐’‘๐’‰๐’†๐’“๐’† Tickellโ€™s Sphericity(1931) ๐‘ป๐’Š๐’„๐’Œ๐’†๐’๐’โ€ฒ ๐’” ๐’”๐’‘๐’‰๐’†๐’“๐’Š๐’„๐’Š๐’•๐’š = ๐’‚๐’“๐’†๐’‚ ๐’๐’‡ ๐’‡๐’Š๐’ˆ๐’–๐’“๐’† ๐’‚๐’“๐’†๐’‚ ๐’๐’‡ ๐’„๐’Š๐’“๐’„๐’–๐’Ž๐’„๐’Š๐’“๐’„๐’๐’† = ๐’—๐’๐’๐’–๐’Ž๐’† ๐’๐’‡ ๐’ƒ๐’๐’…๐’š ๐’—๐’๐’๐’–๐’Ž๐’† ๐’๐’‡ ๐’„๐’Š๐’“๐’„๐’–๐’Ž๐’”๐’‘๐’‰๐’†๐’“๐’†
  • 3. โ€ข Affects the flow properties โ€ข Powder flow - Spherical particles flow easily โ€ข Liquid flow - Increase in aspect ratio increases viscosity โ€ข Liquid flow - More spherical shape particles lead to low viscosity โ€ข Effects porosity โ€ข Effects friability โ€ข Effects sedimentation rate โ€ข Behavior in sieve analysis โ€ข Powder mixing โ€“ blend time changes โ€ข Effects โ€“ wall friction, bulk flow properties, abrasivity, adhesion and cohesion properties. โ€ข Adds more importance to particle size โ€ข Some products work well when : โžข More spherical โ€“ glass beads for highway paint, proppants โžข Less spherical - abrasives Unconfined yield strength of various shaped particles as vs consolidation pressure Convexity vs particle size for various pharmaceutical samples viscosity vs volume fraction for various shape of particles What is itโ€™s significance ?
  • 4. How is it measured ? FESEM (Field Emission Scanning Electron Microscope) coated stub stub holder schematic diagram coal fly ash SEM-(Energy Dispersive X-ray Spectroscopy)EDAX results for fly ash Principle : High energy field emitted e- are incident in vacuum on a sample to eject secondary e- , backscattered e- , auger e- and X-rays. These signals contain information about the surface morphology and the composition of the sample. FE-SEMQuanta200 FEG secondary emission in SEM Standard : ASTM E3 - 11(2017) Make/Model : Hitachi - SU3500, SU1510, SU8000; FEI โ€“ Quanta 250 FEG; Carl Zeiss - ZEISS Sigma 300, GeminiSEM 500
  • 5. Recent Activities !!! SEM and EDS/EDAX of Gypsum sample
  • 6. TEM (Transmission Electron Microscope) TEM holder grid schematic diagram coal fly ash Principle : High energy field emitted e- in vacuum are made to transmit pass through a sample containing grid to fall on a florescent screen or a image capturing screen TECNAI G2 20 S-TWIN Standard : ASTM F1877 - 16 Make/Model : Hitachi - HF5000, HF3500, HF9500, HF9500, HF7800, HF7700; Carl Zeiss โ€“ LIBRA 120 FEI โ€“ TECNAI G2 20 S-TWIN; image system of TEM bright vs dark field imaging single crystalamorphous polycrystalline crystal SelectedArea ElectronDiffraction (SAED)โ†ด How is it measured ? Contd โ€ฆ
  • 7. XRD (X-ray diffraction) PANalytical โ€“ Empyrean Standard : ASTM C1365 - 18 Make/Model : Malvern โ€“ Aeris Research Edition, PANalytical โ€“ Empyrean, Empyrean Nano, Empyrean Alpha 1; Bruker - D2 PHASER, D8 ENDEAVOR, D8 ADVANCE system schematic Braggโ€™s Law : ๐’๐€ = ๐Ÿ๐’… ๐’‰๐’Œ๐’ ๐ฌ๐ข๐ง ๐œฝ Where, n is order ๐œ† is wavelength ๐‘‘โ„Ž๐‘˜๐‘™ is the interplaner distance ๐œƒ is the angle of maximum diffraction sample holder powder XRD sample preparation diffraction peak associated with planes of atoms Principle : X-ray diffraction is based on constructive interference of monochromatic X-rays and a crystalline sample. These X-rays are generated by a cathode ray tube, filtered to produce monochromatic radiation, collimated to concentrate, and directed toward the sample. ๐‘ซ๐’†๐’ƒ๐’š๐’† โˆ’ ๐‘บ๐’‰๐’†๐’‚๐’“๐’†๐’“ ๐’†๐’’๐’–๐’‚๐’•๐’Š๐’๐’ โˆถ ๐‰ = ๐‘ฒ๐€ ๐œท ๐œ๐จ๐ฌ ๐œฝ ๐‘Šโ„Ž๐‘’๐‘Ÿ๐‘’, ๐œ = ๐‘š๐‘’๐‘Ž๐‘› ๐‘ ๐‘–๐‘ง๐‘’ ๐‘œ๐‘“ ๐‘๐‘Ÿ๐‘ฆ๐‘ ๐‘ก๐‘Ž๐‘™๐‘™๐‘–๐‘›๐‘’ ๐‘‘๐‘œ๐‘š๐‘Ž๐‘–๐‘›, ๐‘คโ„Ž๐‘–๐‘โ„Ž ๐‘š๐‘Ž๐‘ฆ๐‘๐‘’ ๐‘ ๐‘š๐‘Ž๐‘™๐‘™๐‘’๐‘Ÿ ๐‘œ๐‘Ÿ ๐‘’๐‘ž๐‘ข๐‘Ž๐‘™ ๐‘ก๐‘œ ๐‘”๐‘Ÿ๐‘Ž๐‘–๐‘› ๐‘ ๐‘–๐‘ง๐‘’ ๐พ = ๐‘‘๐‘–๐‘š๐‘’๐‘›๐‘ ๐‘–๐‘œ๐‘›๐‘™๐‘’๐‘ ๐‘  ๐‘ โ„Ž๐‘Ž๐‘๐‘’ ๐‘“๐‘Ž๐‘๐‘ก๐‘œ๐‘Ÿ ~0.9 ๐œ† = ๐‘‹ โˆ’ ๐‘Ÿ๐‘Ž๐‘ฆ ๐‘ค๐‘Ž๐‘ฃ๐‘’๐‘™๐‘’๐‘›๐‘”๐‘กโ„Ž ๐›ฝ = ๐‘™๐‘–๐‘›๐‘’ ๐‘‘๐‘Ÿ๐‘œ๐‘Ž๐‘‘๐‘›๐‘–๐‘›๐‘” ๐‘Ž๐‘ก โ„Ž๐‘Ž๐‘™๐‘“ ๐‘กโ„Ž๐‘’ ๐‘š๐‘Ž๐‘ฅ๐‘–๐‘š๐‘ข๐‘š ๐‘–๐‘›๐‘ก๐‘’๐‘›๐‘ ๐‘–๐‘ก๐‘ฆ ๐น๐‘Š๐ป๐‘€ ๐œƒ = ๐ต๐‘Ÿ๐‘Ž๐‘”๐‘” ๐‘Ž๐‘›๐‘”๐‘™๐‘’ How is it measured ? Contd โ€ฆ