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Metals
Strong, ductile
Ceramics
brittle, glassy, elastic, non-conducting
Polymers
soft, ductile, plastics
Hydrogen bonds
O-N-F
Lattice parameter equation for BCC
sqrt(3)*a=4R
Lattice parameter equation for FCC
a = 2R*sqrt(2)
Coordination number
Number of touching atoms
Isotropic
materials with properties independent of direction
First three planes of BCC
110 200 211
First three planes of FCC
111 200 220
First three planes of Diamond Cubic
111 220 311
BCC reflection rule
when h+k+l = even number
FCC reflection rule
occurs when h,k,l are all even or all odd numbers
HCP reflection rule
doesn’t occur (h+2k) = 3n, 1 odd
Interstitial Defect
extra atom
Substitution alloy
Atoms are subbed in, atomic radius is within 15%
Interstitial Alloy
solute is much smaller than solvent, within 40%
Schottky defect
cation and anion vacancy
Freckel defect
vacancy and interstitial
Burger Vector
the displacement vector that closes the loop of line defect
Interfacial defects
boundaries that separate regions have different crystal structures
Hexagonal crystal system
a=b=|c, 90 90 120
Tetragonal crystal system
a=b=|c, 90 90 90
Scanning electron microscopy
Small electron beam is scanned repeatedly over the surface area. Variations change strength of beam. Magnification is limited by beam size.
Diffusion flux
How fast diffusion occurs
Elastic stress/strain
reversible
Plastic stress/strain
non-reversible
Tensile strength
max stress on stress-strain curve
Brittle material
Has very little elastic deformation before cracking
Ductile
deforms more before fracture
Toughness
Equal to area under stress-strain curve up to the point of fracture. Same measurement as modulus of resilience
Slip direction and burgers vector
In the same direction
Isotropic-Anisotropic
Anisotropy can be caused by stretching an isotropic material
n-type semiconductor
Doped with elements having more valance electrons then the base material
p-type semiconductor
Doped with elements having less valance electrons then the base material