3
Most read
6
Most read
11
Most read
CRYSTAL
IMPERFECTIONS
WHY SHOULD WE STUDY CRYSTAL IMPERFECTIONS?
Technically important properties such as
mechanical strength.
Ductility’ Crystal growth, magnetic hysteresis, dielectric
strength, conduction in Semiconductors are greatly
affected by relatively minor changes in crystal Structure
caused by DEFECTS/ IMPERFECTIONS.
Crystal Imperfections are the defects in the regular
geometrical arrangement of the atoms in a Crystalline
solid.
A Perfect Crystal is an idealization; there is no such thing in
nature.
The defects may be the results of the crystal deformation or
rapid cooling from high temperature or high energy radiation
striking the solid.
The defects influence the mechanical, electrical, and optical
behavior of the crystal.
The imperfections may be classified widely as:
 Point Defects
 Line Defects
 Surface Defects
 Volume Defects
1. POINT DEFECTS
These are the lattice errors at isolated points , takes place due to
the imperfect packing of atoms during crystallization or due to the
vibrations of atoms at high temperatures.
number of defects at equilibrium concentration , at a
certain temperature is given by
Where
n —number of imperfections
N—number of atomic sites per mole
Ed—free energy required to form defects
kb—Boltzmann’s constant (kb= 8.62*10-5 eV/K)
T —Absolute temperature
(a)VACANCIES
A simplest point defects in a crystal.
Refers to missing atom or vacant atomic site.
Arise either from imperfect packing during original crystallisation or
from thermal vibrations at high temperatures.
(b)FRENKEL DEFECT
It is formed by a cat ion leaving its normal position and moving into
an interstial site.
(c)SCHOTTKY DEFECT
It is formed by removing one cat ion and one anion from the interior
of the crystal and then placing them both at an external surface.
Crystal imperfections
Crystal imperfections
(d)COMPOSITIONAL DEFECTS
• These arise from impurity atoms during crystallisation.
• They occur on lattice point as a Substitutional impurity or as an
interstitial impurity.
• Substitutional impurity is created when a foreign atom substitutes
for a parent atom in the crystal lattice.
• Interstitial impurity is a small sized foreign atom occupying an
interstitial position between the regularly positioned atoms.
(e)ELECTRONIC DEFECTS
• These are the errors in charge distribution in solids.
• These are primarily necessary in electrical conductivity & related
phenomenon
• Prominent example is pn junction formation and transistor junction
formations.
2. LINE IMPERFECTIONS/ DISLOCATIONS
• 1-D defects around which some of the atoms are misaligned.
• These are responsible for the useful property of ductility in metals,
ceramics and crystalline polymers.
• Types :- Edge Dislocations and Screw Dislocations.
(a)EDGE DISLOCATIONS
• The perfect crystal is considered to be made up of vertical planes
parallel to one another and to the side faces. If one of these vertical
planes doesn’t extend from top to bottom of the crystal but ends
partway within the crystal then there exists a Dislocation.
• The bond lengths above the slip plane are compressed to smaller
than that of the equilibrium value. And below the slip plane bond
lengths are found to be pulled apart and are in a state of tension.
(b) SCREW DISLOCATIONS
• It is formed by a shear stress that is applied to produce the
distortion. The upper region of the crystal is shifted one atomic
distance to the right relative to bottom portion.
*BURGERS VECTOR.
• The magnitude & direction of the lattice distortion associated with
a dislocation is expressed in terms of a BURGERS VECTOR.
• If The BURGERS Vector and the orientation of the dislocation line
are known , then the dislocation is completely described.
• This vector indicates how much and at what direction the lattice
above the slip plane appears to have been shifted with respect to
the lattice below the plane.
• The burgers vector is perpendicular to the dislocation line in Edge
Dislocations and it is parallel to the dislocation line in Screw
Dislocations.
Edge dislocation
Edge dislocation
Taken by Callister’s MATERIALS SCIENCE AND ENGINEERING Adopted by R Balasubrmaniam page no.350
3. SURFACE IMPERFECTIONS
• Two Dimensional defects.
• These arise from a change in the stacking of atomic planes on or
across a boundary.
(a) External surface imperfections
• Imperfections represented by a boundary.
• The external surface of a material is an imperfection itself because
the bonds do not extend beyond it since surface atoms are not
entirely surrounded by other atoms on other side, they posses
higher energy than that of internal atoms.
(b) Internal surface imperfections
These are manifested by such defects as Grain boundaries, Tilt
boundaries, Twin boundaries, Stacking faults.
Grain boundaries: These separate crystals/ grains of different
orientation in a polycrystalline material during crystallisation.
The shape of a grain is usually influenced by the presence of
surrounding grains. Hence a region of transition exists in which
the atomic packing is Imperfect.
• In the boundary where the crystal or grains change abruptly,
the orientation of difference between neighboring grains is
more than 10˚-15˚ ,& the boundaries are known as high
angle grain boundaries.
• The boundary between 2 crystals which have different
crystalline arrangements or different compositions is called
an interface.
Grain boundaries
Taken by Callister’s MATERIALS SCIENCE AND ENGINEERING Adopted by R Balasubrmaniam page no.360
Tilt Boundaries
• This is a low angle boundary as the orientation difference is
between 2 neighboring crystals is less than 10˚
• this is composed of edge dislocation lying one above the other.
• The tilt angle,
• Where, b—magnitude of Burgers vector,
Twin Boundaries
• The atomic arrangement on one side of a twin boundary is a mirror
reflection of arrangement on the other side.
• These occur always in pairs such that the orientation change
introduced by one is restored by another.
Stacking Defects
• This type of fault arises from the stacking of one atomic place out of
sequence on another while the lattice on either side of the fault is
perfect.
Tilt boundaries Twin boundaries
4. VOLUME IMPERFECTIONS
• 3 Dimensional Imperfections
• These may arise when there is only a small electrostatic
dissimilarities b/w the stacking sequences of close packed planes in
metals. For example cracks.
• When clusters of atoms are missing, a large vacancies or voids are
created which are also the volume imperfections.
Reference
• SOLID STATE PHYSICS by S O PILLAI.
• MATERIAL SCIENCE by S L KAKANI and AMIT
KAKANI.
• Callister’s MATERIALS SCIENCE AND
ENGINEERING Adopted by R Balasubrmaniam

More Related Content

PPTX
Crystal defects
PPTX
Crystal Defects
PPTX
Mine Waste Management
PDF
PPTX
Microprocessor controlled injection molding machine
PDF
05 dislocation theory
PPTX
Glass ppt
PPTX
Physics
Crystal defects
Crystal Defects
Mine Waste Management
Microprocessor controlled injection molding machine
05 dislocation theory
Glass ppt
Physics

What's hot (20)

PPTX
Crystal imperfections
PPTX
Surface defects in crystals
PPT
Imperfections in(new)2
PPTX
Crystal structures in material science
PPTX
Induction furnace
PPTX
Strengthening Mechanisms of Metals and alloys
PPTX
Crystal Structure, BCC ,FCC,HCP
PPTX
Dendratic growth
PPTX
High Temperature Materials
PDF
Eutectic, eutectoid, peritectoid, peritectic
PPTX
CERAMICS
PPTX
Solid solution strengthening
PPT
Phase Diagram
PPT
Phase transformation edited.ppt1
PPTX
Crystal systems
PPTX
Powder metallurgy
PPTX
Defects in crystal
Crystal imperfections
Surface defects in crystals
Imperfections in(new)2
Crystal structures in material science
Induction furnace
Strengthening Mechanisms of Metals and alloys
Crystal Structure, BCC ,FCC,HCP
Dendratic growth
High Temperature Materials
Eutectic, eutectoid, peritectoid, peritectic
CERAMICS
Solid solution strengthening
Phase Diagram
Phase transformation edited.ppt1
Crystal systems
Powder metallurgy
Defects in crystal
Ad

Viewers also liked (20)

PPTX
Imperfections in solids
PPT
Imperfections in
PPT
Defects in crystalline materials
PPT
Crystalline defects
PPTX
Crystal defects
DOC
Defects
PDF
Crystal imperfections
PPT
Crystal imperfections dislocations
PPTX
Crystal Defects
PPT
Mechanical Properties of Metals
PPTX
Imperfections in
PPTX
PPTX
Line defects & planes
PPTX
Gas nitriding #
PPSX
Nitriding and carbonitriding copy
PPTX
Mme 323 materials science week 5 - imperfection in solids
PPTX
Crystal Structures & their imperfection
PPTX
Em321 lesson 08b solutions ch6 - mechanical properties of metals
PPTX
Point defects
Imperfections in solids
Imperfections in
Defects in crystalline materials
Crystalline defects
Crystal defects
Defects
Crystal imperfections
Crystal imperfections dislocations
Crystal Defects
Mechanical Properties of Metals
Imperfections in
Line defects & planes
Gas nitriding #
Nitriding and carbonitriding copy
Mme 323 materials science week 5 - imperfection in solids
Crystal Structures & their imperfection
Em321 lesson 08b solutions ch6 - mechanical properties of metals
Point defects
Ad

Similar to Crystal imperfections (20)

PPTX
CRYSTAL IMPERFECTIONS _ metallurgy .pptx
PPTX
Lattice imperfection
PPTX
Chapter 2 Crystal defects.pptx
PPTX
Chapter 2 Crystal defects complete.pptx
PDF
K.Srinivasulureddy-SNIST-Metallurgy & Material Science-MMS-UNIT-1
PDF
Unit 1-k.srinivasulureddy-Metallurgy & Material science
PPTX
Material science and Metallurgy Lecture 10.pptx
PPTX
Crystal defects
PPTX
Str metal and material.pptx
PPTX
Basics Of Crystal Structure (Miller Indices, Defects In crystal)
PPTX
IMPERFECTIONS IN SOLIDS.pptx
PDF
IMPERFECTIONS IN SOLIDS.pdf
PPTX
Material Science and Metallurgy
PDF
CH 6 CVIL 223 Structural Imperfections and Atom Movements.pdf
PDF
IMPERFECTIONS IN SOLIDS - II.pdf
PDF
Crystal defects
PPTX
Crystaldefect 150719104034-lva1-app6891-converted
PPT
types of crystal defects, dislocations and descriptions
PPT
SURFACE IMPERFECTIONS In crystal structure
PPTX
U1 structureofmaterials matrlsci&metallrgy3rdsmdbatu
CRYSTAL IMPERFECTIONS _ metallurgy .pptx
Lattice imperfection
Chapter 2 Crystal defects.pptx
Chapter 2 Crystal defects complete.pptx
K.Srinivasulureddy-SNIST-Metallurgy & Material Science-MMS-UNIT-1
Unit 1-k.srinivasulureddy-Metallurgy & Material science
Material science and Metallurgy Lecture 10.pptx
Crystal defects
Str metal and material.pptx
Basics Of Crystal Structure (Miller Indices, Defects In crystal)
IMPERFECTIONS IN SOLIDS.pptx
IMPERFECTIONS IN SOLIDS.pdf
Material Science and Metallurgy
CH 6 CVIL 223 Structural Imperfections and Atom Movements.pdf
IMPERFECTIONS IN SOLIDS - II.pdf
Crystal defects
Crystaldefect 150719104034-lva1-app6891-converted
types of crystal defects, dislocations and descriptions
SURFACE IMPERFECTIONS In crystal structure
U1 structureofmaterials matrlsci&metallrgy3rdsmdbatu

Recently uploaded (20)

PPTX
A powerpoint on colorectal cancer with brief background
PPTX
2currentelectricity1-201006102815 (1).pptx
PPTX
Toxicity Studies in Drug Development Ensuring Safety, Efficacy, and Global Co...
PPTX
AP CHEM 1.2 Mass spectroscopy of elements
PDF
Communicating Health Policies to Diverse Populations (www.kiu.ac.ug)
PPT
Cell Structure Description and Functions
PDF
Unit 5 Preparations, Reactions, Properties and Isomersim of Organic Compounds...
PPT
1. INTRODUCTION TO EPIDEMIOLOGY.pptx for community medicine
PDF
5.Physics 8-WBS_Light.pdfFHDGJDJHFGHJHFTY
PDF
From Molecular Interactions to Solubility in Deep Eutectic Solvents: Explorin...
PPTX
LIPID & AMINO ACID METABOLISM UNIT-III, B PHARM II SEMESTER
PDF
Sustainable Biology- Scopes, Principles of sustainiability, Sustainable Resou...
PDF
Worlds Next Door: A Candidate Giant Planet Imaged in the Habitable Zone of ↵ ...
PPTX
TORCH INFECTIONS in pregnancy with toxoplasma
PPT
Biochemestry- PPT ON Protein,Nitrogenous constituents of Urine, Blood, their ...
PPT
LEC Synthetic Biology and its application.ppt
PPTX
Platelet disorders - thrombocytopenia.pptx
PPT
Enhancing Laboratory Quality Through ISO 15189 Compliance
PPTX
diabetes and its complications nephropathy neuropathy
PPTX
PMR- PPT.pptx for students and doctors tt
A powerpoint on colorectal cancer with brief background
2currentelectricity1-201006102815 (1).pptx
Toxicity Studies in Drug Development Ensuring Safety, Efficacy, and Global Co...
AP CHEM 1.2 Mass spectroscopy of elements
Communicating Health Policies to Diverse Populations (www.kiu.ac.ug)
Cell Structure Description and Functions
Unit 5 Preparations, Reactions, Properties and Isomersim of Organic Compounds...
1. INTRODUCTION TO EPIDEMIOLOGY.pptx for community medicine
5.Physics 8-WBS_Light.pdfFHDGJDJHFGHJHFTY
From Molecular Interactions to Solubility in Deep Eutectic Solvents: Explorin...
LIPID & AMINO ACID METABOLISM UNIT-III, B PHARM II SEMESTER
Sustainable Biology- Scopes, Principles of sustainiability, Sustainable Resou...
Worlds Next Door: A Candidate Giant Planet Imaged in the Habitable Zone of ↵ ...
TORCH INFECTIONS in pregnancy with toxoplasma
Biochemestry- PPT ON Protein,Nitrogenous constituents of Urine, Blood, their ...
LEC Synthetic Biology and its application.ppt
Platelet disorders - thrombocytopenia.pptx
Enhancing Laboratory Quality Through ISO 15189 Compliance
diabetes and its complications nephropathy neuropathy
PMR- PPT.pptx for students and doctors tt

Crystal imperfections

  • 2. WHY SHOULD WE STUDY CRYSTAL IMPERFECTIONS? Technically important properties such as mechanical strength. Ductility’ Crystal growth, magnetic hysteresis, dielectric strength, conduction in Semiconductors are greatly affected by relatively minor changes in crystal Structure caused by DEFECTS/ IMPERFECTIONS.
  • 3. Crystal Imperfections are the defects in the regular geometrical arrangement of the atoms in a Crystalline solid. A Perfect Crystal is an idealization; there is no such thing in nature. The defects may be the results of the crystal deformation or rapid cooling from high temperature or high energy radiation striking the solid. The defects influence the mechanical, electrical, and optical behavior of the crystal.
  • 4. The imperfections may be classified widely as:  Point Defects  Line Defects  Surface Defects  Volume Defects
  • 5. 1. POINT DEFECTS These are the lattice errors at isolated points , takes place due to the imperfect packing of atoms during crystallization or due to the vibrations of atoms at high temperatures. number of defects at equilibrium concentration , at a certain temperature is given by Where n —number of imperfections N—number of atomic sites per mole Ed—free energy required to form defects kb—Boltzmann’s constant (kb= 8.62*10-5 eV/K) T —Absolute temperature
  • 6. (a)VACANCIES A simplest point defects in a crystal. Refers to missing atom or vacant atomic site. Arise either from imperfect packing during original crystallisation or from thermal vibrations at high temperatures. (b)FRENKEL DEFECT It is formed by a cat ion leaving its normal position and moving into an interstial site. (c)SCHOTTKY DEFECT It is formed by removing one cat ion and one anion from the interior of the crystal and then placing them both at an external surface.
  • 9. (d)COMPOSITIONAL DEFECTS • These arise from impurity atoms during crystallisation. • They occur on lattice point as a Substitutional impurity or as an interstitial impurity. • Substitutional impurity is created when a foreign atom substitutes for a parent atom in the crystal lattice. • Interstitial impurity is a small sized foreign atom occupying an interstitial position between the regularly positioned atoms. (e)ELECTRONIC DEFECTS • These are the errors in charge distribution in solids. • These are primarily necessary in electrical conductivity & related phenomenon • Prominent example is pn junction formation and transistor junction formations.
  • 10. 2. LINE IMPERFECTIONS/ DISLOCATIONS • 1-D defects around which some of the atoms are misaligned. • These are responsible for the useful property of ductility in metals, ceramics and crystalline polymers. • Types :- Edge Dislocations and Screw Dislocations. (a)EDGE DISLOCATIONS • The perfect crystal is considered to be made up of vertical planes parallel to one another and to the side faces. If one of these vertical planes doesn’t extend from top to bottom of the crystal but ends partway within the crystal then there exists a Dislocation. • The bond lengths above the slip plane are compressed to smaller than that of the equilibrium value. And below the slip plane bond lengths are found to be pulled apart and are in a state of tension.
  • 11. (b) SCREW DISLOCATIONS • It is formed by a shear stress that is applied to produce the distortion. The upper region of the crystal is shifted one atomic distance to the right relative to bottom portion. *BURGERS VECTOR. • The magnitude & direction of the lattice distortion associated with a dislocation is expressed in terms of a BURGERS VECTOR. • If The BURGERS Vector and the orientation of the dislocation line are known , then the dislocation is completely described. • This vector indicates how much and at what direction the lattice above the slip plane appears to have been shifted with respect to the lattice below the plane. • The burgers vector is perpendicular to the dislocation line in Edge Dislocations and it is parallel to the dislocation line in Screw Dislocations.
  • 13. Edge dislocation Taken by Callister’s MATERIALS SCIENCE AND ENGINEERING Adopted by R Balasubrmaniam page no.350
  • 14. 3. SURFACE IMPERFECTIONS • Two Dimensional defects. • These arise from a change in the stacking of atomic planes on or across a boundary. (a) External surface imperfections • Imperfections represented by a boundary. • The external surface of a material is an imperfection itself because the bonds do not extend beyond it since surface atoms are not entirely surrounded by other atoms on other side, they posses higher energy than that of internal atoms. (b) Internal surface imperfections These are manifested by such defects as Grain boundaries, Tilt boundaries, Twin boundaries, Stacking faults.
  • 15. Grain boundaries: These separate crystals/ grains of different orientation in a polycrystalline material during crystallisation. The shape of a grain is usually influenced by the presence of surrounding grains. Hence a region of transition exists in which the atomic packing is Imperfect. • In the boundary where the crystal or grains change abruptly, the orientation of difference between neighboring grains is more than 10˚-15˚ ,& the boundaries are known as high angle grain boundaries. • The boundary between 2 crystals which have different crystalline arrangements or different compositions is called an interface.
  • 16. Grain boundaries Taken by Callister’s MATERIALS SCIENCE AND ENGINEERING Adopted by R Balasubrmaniam page no.360
  • 17. Tilt Boundaries • This is a low angle boundary as the orientation difference is between 2 neighboring crystals is less than 10˚ • this is composed of edge dislocation lying one above the other. • The tilt angle, • Where, b—magnitude of Burgers vector, Twin Boundaries • The atomic arrangement on one side of a twin boundary is a mirror reflection of arrangement on the other side. • These occur always in pairs such that the orientation change introduced by one is restored by another. Stacking Defects • This type of fault arises from the stacking of one atomic place out of sequence on another while the lattice on either side of the fault is perfect.
  • 18. Tilt boundaries Twin boundaries
  • 19. 4. VOLUME IMPERFECTIONS • 3 Dimensional Imperfections • These may arise when there is only a small electrostatic dissimilarities b/w the stacking sequences of close packed planes in metals. For example cracks. • When clusters of atoms are missing, a large vacancies or voids are created which are also the volume imperfections.
  • 20. Reference • SOLID STATE PHYSICS by S O PILLAI. • MATERIAL SCIENCE by S L KAKANI and AMIT KAKANI. • Callister’s MATERIALS SCIENCE AND ENGINEERING Adopted by R Balasubrmaniam