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Lecture 2.1 Crystalline Solids
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Poly-crystalline solids - Grains Mono-crystalline solids- Whiskers, Wafers
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Crystal Lattices
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Crystal Systems =>14 Bravais Lattices
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Bravais lattice (abc) Lattice is constructed of repeated unit cells Lattice Point - 1/3a,1/2b,1/4c Crystallographic Direction (vector from 0,0,0 to xyz) which is defined by –[uvw] smallest set of integers having the same ratio as xyz –bar over number = minus number
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Close Packed Structures Cubic, BCC, FCC, HCC are the focus of this course Determining distances and volume fractions in Cubic Structures
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Miller indices for a plane (hkl) Family of Miller Planes {hkl}
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EXAMPLE- Miller Index intercepts on a,b&c axes=3,1&2, respectively reciprocals = 1/3,1/1&1/2, respectively smallest set of integers with same common ratio = 2,6&3 Miller indexes of Plane, (hkl)=(263) also called “reciprocal space plane”
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Family of Planes {110}
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Measuring Structure with X-rays Generate X-ray radiation X-ray Diffraction ( =90) –a o = cubic lattice parameter
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X-Ray Generation Electron Scattering –Broad Band X-rays Electron Kickout –K,L,M shell electron –Replace with higher electron –Transition gives X- rays one wave length K ,K , L , L KK KK
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X-ray Generation Energy Level Diagrams 1 K 2 3 4 -13.6 eV -3.40 eV -1.51 eV L -0.85 eV KK KK LL LL
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X-ray Camera-1 Single Crystal Camera –Broad Band X-rays –all in source –only Bragg (diffracting) wavelengths reflect
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SiGe Crystal
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X-ray Camera-2 (film strip) X-rays of Single All (hkl) planes are exposed at all angles at all times Diffraction of Bragg planes
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Electron Diffraction Electrons of different energy Transmission through sample CCD detector Focused Electrons Thinned Sample CCD Detector
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Seeing Crystal Structure with and Atomic Force Microscope Electron Microscope Atomic Force Microscope Scanning Tunneling Microscope
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Diffracting Planes
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Changing Crystal Structure – Allotropic Phase Change HCP->FCC->BCC->SC Ca(fcc) --(447ºC)-> Ca(bcc) Co(hcp) --(427ºC)--> Co(fcc) Fe(bcc) --(912ºC)-->Fe(fcc) --(1394ºC)-->Fe(hcp) Na(bcc) --(-233ºC)--> Na(hcp) Ti(hcp) --(883ºC)-->Ti(bcc) Zr(hcp) --(872ºC)--> Zr(bcc) Decreasing density with increasing temperature!
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Defects in Crystal Structure Vacancy, Interstitial, Impurity Schottky Defect Frenkel Defect Dislocations – edge dislocation, line, screw Grain Boundary
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Effect of Structure on Mechanical Properties Elasticity Plastic Deformation
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