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IMPERFECTIONS INIMPERFECTIONS INCRYSTALSCRYSTALS
BY, MAYUR BAGALE AND SUSHANT MODI.
IMPERFECTIONS IN CRYSTALS
ISSUES TO ADDRESS...
• How do defects affect material properties?• What types of defects arise in solids?• Are defects undesirable?
Crystalline Imperfections There is no such thing as a perfect crystal! • Thermodynamically “impossible”
• “defects” lower the energy of a crystal & make it more stable
• always have vacancies and impurities, to some extent
Defect does not necessarily imply a bad thing • addition of C to Fe to make steel
• addition of Cu to Ni to make thermocouple wires
• addition of Ge to Si to make thermoelectric materials
• addition of Cr to Fe for corrosion resistance
• introduction of grain boundaries to strengthen materials
…… and so on
“Defect” (in this context) can be either desirable or undesirable.
In general, a defect simply refers to a disruption in the crystalline
order of an otherwise periodic material.
CRYSTALLINE CRYSTALLINE IMPERFECTIONS IMPERFECTIONS areare frequently frequently classified according to geometry or classified according to geometry or dimensionality of the defect.dimensionality of the defect.
Point defectsPoint defects Line defectsLine defects Interfacial defects Interfacial defects Bulk or volume defects Bulk or volume defects
Point Defects Atoms in solid possess vibrational energy, some
atoms have sufficient energy to break the bonds which hold them in eqbm position. Hence once the atoms are free they give rise to Point Defects.
Classes of point defects:Intrinsic defects.1.Vacancy2.InterstitialExtrinsic defects 1.Substitution2.Interstitial
VacanciesA lattice position that is vacant because the
atom is missingThere are naturally occurring vacancies in
all crystalsThe concentrations of vacancies increase
with:increasing temperaturedecreasing activation energy
Vacancies -vacant atomic sites in a structure.
Vacancy
distortion
of planes
Self-Interstitial
If the matrix atom occupies its own interstitial site, the defect is called Self Interstitial.
Self-interstitials in metals introduce large distortions in the surrounding lattice.
self-interstitial
distortion of planes
For Ionic Solids, Frenkel and Schottky defects are likely to form.
Schottky Defects When cation vacancy is associated with anion
vacancy, the defect is called Schottky Defect.Frenkel Defects When an atom leaves its regular site and
occupy nearby interstitial site it gives rise to two defects i.e. one vacancy and other self interstitial these two defects are called as Frenkel Defects.
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• Frenkel Defect
--a cation is out of place.
• Shottky Defect
--a paired set of cation and anion vacancies.
Shottky Defect:
Frenkel Defect
• Equilibrium concentration of defects ~e QD /kT
Adapted from Fig. 13.20, Callister 5e. (Fig. 13.20 is from W.G. Moffatt, G.W. Pearsall, and J. Wulff, The Structure and Properties of Materials, Vol. 1, Structure, John Wiley and Sons, Inc., p. 78.) See Fig. 12.21, Callister 6e.
DEFECTS IN CERAMICDEFECTS IN CERAMIC STRUCTURESSTRUCTURES
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Boltzmann's constant
(1.38 x 10 -23 J/atom-K)
(8.62 x 10 -5 eV/atom-K)
Nv
Nexp
Qv
kT
No. of defects
No. of potential
defect sites.
Activation energy
Temperature
Each lattice site
is a potential
vacancy site
• Equilibrium concentration varies with temperature!
Equilibrium Concentration:Equilibrium Concentration:Point DefectsPoint Defects
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Measuring Activation EnergyMeasuring Activation Energy• We can get Qv from an experiment.
Nv
N= exp
Q v
kT
• Measure this...
N v
N
T
exponential dependence!
defect concentration
• Replot it...
1/ T
N
N vln
-Q v /k
slope
Line Defects
Line defects are imperfections in a crystal structure for which a row of atoms have a local structure that differs from the surrounding crystal.
1. Edge dislocations
2. Screw dislocations
Linear Defect (Dislocations)
Are one-dimensional defects around which atoms are misaligned
Edge dislocation:◦extra half-plane of atoms inserted in a crystal
structure◦Burger vector to dislocation line
Screw dislocation:◦spiral planar ramp resulting from shear
deformation◦Berger vector to dislocation line
Edge DislocationEdge Dislocation
Screw Dislocation
Interfacial Defects Are boundaries that have two dimensions
and normally separate regions of the materials that have different crystal structures.
1. External surface2. Grain boundary3. Twin boundary
External Surfaces
Surface atoms have unsatisfied atomic bonds, and higher surface energies, γ (J/m2 or, erg/cm2) than the bulk atoms.
To reduce surface free energy, material tends to minimize its surface areas against the surface tension (e.g. liquid drop).
Grain Boundaries
Polycrystalline material comprised of many small crystals or grains having different crystallographic orientations.
Atomic mismatch occurs within the regions where grains meet. These regions are called grain boundaries.
Segregation of impurities occurs at grain boundary.Grains tend to grow in size at the expense of smaller grains
to minimize surface energy. This occurs by diffusion, which is accelerated at high temperatures.
Dislocations can usually not cross the grain boundary.
Twin Boundaries
Special type of grain boundaries with twin directions mirrored atomic positions across the boundary.
May be produced by shear deformation of BCC/HCP materials (mechanical twin), or during annealing following deformation (annealing twin) of FCC materials
Bulk or Volume DefectsPores
affect optical, thermal, and mechanical properties
Cracks
affect mechanical propertiesForeign inclusions
affect electrical, mechanical, optical properties
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• Point, Line, and Area defects exist in solids.
• The number and type of defects can be varied and controlled (e.g., T controls vacancy conc.)
• Defects affect material properties (e.g., grain boundaries control crystal slip).
• Defects may be desirable or undesirable (e.g., dislocations may be good or bad, depending on whether plastic deformation is desirable or not.)
SummarySummary
THE END