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Vacancies and Intersticials
Two Ions:
# Cation vacancies = # Anion vacancies (electroneutrality)
More cation than anion interstitials (size)
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cation vacancy - cation interstial pair
any time an atom/anion moves from latice site to its interstitial site |
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Paired anion and cation vacancies |
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Substitutional Impurities/ Charge Neutrality (Ceramics) |
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Definition
If the replacing atom has a different charge than the replaced, then vacancies must occur.
EX. NaCl, with a Ca taking place of a Na.
Na +1, Ca +2, so there must be a cation vacancy as well to keep it balanced.
NaCl, Cl -, O 2- |
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More complicated in Ceramics b.c. electroneutrality.
Diffusion occurs through vacancy mechanism.
Diffusion of an anion must be accompanied by diffusions of cation(s) with equal charge.
Diffusion rate is limited by the slower moving ion
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Ceramics vs Metal
Brittleness |
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Definition
Ceramics are more brittle
Crystalline - dislocation motion
Highly ionic solids - dislocation motion is difficult.
Few slip systems
Moving same charged ions close together - repel |
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Definition
Flaws/cracks within the structure.
Propagated stress is much lower than you would expect:
(Initiation sites)Stress concentration/riser (from small flaws)
No mechanisms for plastic deformation = unimpeded propogation fo cracks
K=Yo(pi*a)^1/2
Cracks can propogate slowly at lower stresses, but only in moist environments where corrosion processes are occuring at the crack tips |
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Definition
One point is different from the normal repeating structure
Vacanies = much mroe likely than self interstitials
Vacancy Atoms
Interstitial Atoms
Substitutional Atoms |
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Definition
Defect in the structure with one dimension
Dislocations |
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2 or more dimensions in the defect
Grain Boundaries |
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All crystalline solids have vacancies. Increases entropy (degree of disorder) |
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Equilibrium Concentration |
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Equilibrium vacancy concentration varies with temperature. Increasing Temp causes surface island of atoms to grow. So higher temperature = more vancancies = more atoms moved to "surface island" (Nv/N = exp(-Qv/kT)) Nv= Number of defects N= Number of possible defect sites (lattice sites) Qv= Activation energy k= Boltzmann's constant |
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k Used in Equilibrium Concentration equation (Nv/N = exp(-Qv/kT)) |
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extra atoms positioned between atomic sites |
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Substitutional Impurities |
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Definition
Always 10^22-!0^23 impurity atoms/m^3 Alloys = Deliberately added for metals Sterling silver = 7.5% Cu = stronger, but still corrosion resistant. Adding impurity atoms results in solid solution/second phase formation Solute = minority Solvent = majority |
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Definition
Liquid Solutions: Immiscible = won't mix (oil& water) Miscible = will happily mix Same with Solid: Immiscible = Fe+Mg, will form two separate phases Miscible: Complete Solid Solution: They can exist on each others lattice sites. Same crystal structures Partial: Only a certain amount will be miscible. After too much is added, it will no longer sit. Substitutional Sold Solution: They will sit on the atomic sites Interstitial Sold Solution: They will sit in the interstitial sites |
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Definition
When enough B is put into A, there will be a second phase particle, where there will be a different composition. Often different structure. So the ratio will be different, and for example, have a spot that is BCC in a mainly FCC structure. |
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Substituional Solid Solution |
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Definition
Conditions: 1) Difference between atomic r < 15% 2) Similar electronegativities 3) Same crystal structure for pure metals 4) Valency: If all else is fine, then a metal of higher valency will dissolve a metal of lower valency |
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Impurities in Solids (Composition) |
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Definition
Weight %: C1 = m1/(m1+m2) Atomic %: C1 = nm1/(nm1+nm2) n= number of atoms |
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Line defects Slips between crystal planes Permanent (plastic) deformation Atoms become misaligned 1) Edge Dislocation 2) Screw Dislocation |
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Extra half-plane of atoms inserted into a crystal structure Allows plastic deformation at much lower stress than if they weren't present b is perpendicular to dislocation line Edge dislocation line (|), going into the screen | : : : : : : : : : : : : : |
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b, measure of lattice distortation When you go around in a nxn square, b is the vector that gets you back to your starting point. |
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requires the successive bumping of a half plane of atoms Bonds across the slipping planes are broken and remade in succession Shifts it one at a time, meaning much less energy needed, meaning much less stress. |
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Spiral planar ramp resulting from shear deformation b is parallel to the dislocation line |
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Dislocation Close-Packed Directions # |
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Definition
FCC: Many close-packed planes/directions HCP: Only one plane, 3 directions BCC: None |
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Also a planar defect Because surface atoms don't have all the bonds, there are a higher energy state due to surface energy Driving force to reduce this (easily done in liquids, water -drop-) |
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Regions between crystales less atomic bonding along the grain Impurity atoms tend to segregate here 1) Tilt Boundaries 2) Phase Boundaries 3) Twin Boundaries |
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When edge dislocations line up |
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between two different phases in an alloy |
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A reflection of atom positions across the twin plane |
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ABCABC packing sequence is disturbed ABCABABC |
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Catalysts and surface defects |
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Increases the rate of reactions Active sites on catalysts are normally surface defects |
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Mass transport by atomic motion. 1)Vacancy Diffusion 2)Interstitial Diffusion |
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In alloys, from regions of high to low concentration. Time to reach equilibrium dependent on how easily atoms can move through vacancies and interstitial diffusion |
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not easily visible, but still, even without concentration gradient, atoms still move |
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Diffuse carbon atoms into host iron atoms at surface Carbon is much smaller than iron, making interstitial diffusion. Presence of carbon makes surface harder |
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atoms exchanging position with vacancies also applies to substitutional impurity atoms rate depends on: -Number of vacancies -Temperature -Activation energy to exchange |
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Smaller solute atoms can diffuse between atoms Moves around in interstitial sites More rapid than vacancy diffusion |
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J=Flux=moles diffusion/(SA*t) mol/cm^2s or kg/m^2s Measured empirically (by experiment) make thin film, impose gradient, measure how fast moving through membrane |
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Concentration profile is not a function of time. AKA rate of diffusion is independent of time. Rate stays constant over time. J=-D*(dC/dx) D=Diffusion coefficient dC/dx~=C2-C1/x2-x1 Units: mol/m^2s, then C=mol/m^3, then D=m^2/s |
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Fick's First Law of Diffusion |
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Definition
D=Do*exp(-Qd/RT) Do=pre-exponential Qd=activation energy R=gas constant 8.314J/mol*K T=temp in K |
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Non-Steady State Diffusion |
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Definition
Most practical cases Flux & concentration gradient change with time Implies net accumulation or depletion of diffusing species Both function of time and Position C=C(x,t) Fick's Second Law |
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Definition
pd = partial deriv pd^2= second pd, or pd of pd pdC/pdt = D*(pd^2C/pdx^2) Given that surface concentration is constant (Cs), and there is a point far away that stays at initial concentration(Co), C(x,t)-Co/Cs-Co= 1-erf(x/(2*root(D*t)) erf(z) If there is specific concentration desired (C1), then left hand side becomes constant, and so must the right: x/(2*root(Dt)) or x^2/(4)Dt x~= root(Dt) |
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Definition
Elastic means reversible. Bonds are being stretched. Linear-elastic: Relationship between force and change in length is linear. |
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Plastic Deformation (Metals) |
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Permanent. Generally, elastic to a point, but after a certain point, a slip occurs. After slip, it will still recover the amount of the elastic deformation |
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Definition
Up and down. Tensile stress(o-) = Ft/A = N/m^2 |
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t=Fs/A Stress in the Plane of the area Area is always ORIGINAL area |
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equal stress in one direction as another direction. So F on L = F on Right |
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emf=d/L (change in length over original Length) Tensile strain= same direction as pulling (up/down) Lateral strain(emfL)= other direction., d/W Shear strain(y)=x/y=tan() |
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Modulus of Elasticity (E) |
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Definition
Hooke's Law: stress(o-)=E*emf Units: (GPa or psi) |
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Pull on sample in one direction, what is strain in opposite? v=-(emfL/emf) if v> than .5, the density will increase. |
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How much deformation is possible before it breaks. %EL = Lf-Lo/Lo |
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Ernergy needed to break a unit volume of material Area under stress-strain curve |
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Resistance to permanent indenting Large hardness: resistance to plastic deformation or cracking in compression better wear proppoerties |
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