ceramics
means “burnt stuff,” indicating that desirable properties of these materials are normally achieved through a high-temperature heat treatment process called firing
cation
- positively charged because they have given up their valence electrons to the nonmetallic ions
anion
negatively charged
rock salt crystal structure
cesium chloride crystal structure
- anions are located at each of the corners of a cube, whereas the cube center is a single cation
zinc blende or sphalerite structure
- all ions are tetrahedrally coordinated
tetrahedral position
four atoms (three in one plane, and a single one in the adjacent plane) surround one type
octahedral position
six ion spheres, three in each of the two planes
silicates
silicon dioxide or silica (SiO2)
- material is electrically neutral and all atoms have stable electronic structures
fused silica or vitreous silica
silica made to exist as a noncrystalline solid or glass having a high degree of atomic randomness, which is characteristic of the liquid
network formers
other oxides that form glassy structures
network modifiers
oxides that do not form polyhedral networks, their cations are incorporated within and modify the SiO4-4 network
intermediates
other oxides, such as TiO2 and Al2O3 although not network formers, substitute for silicon and become part of and stabilize the network
carbon
exists in two allotropic forms—diamond and graphite—as well as in the amorphous state
diamond
metastable carbon polymorph at room temperature and atmospheric pressure
graphite
- furthermore, it is a stable polymorph at ambient temperature and pressure
delocalized
does not belong to a specific atom or bond
defect structure
designate the types and concentrations of atomic defects in ceramics
electroneutrality
state that exists when there are equal numbers of positive and negative charges from the ions
Frenkel defect
Schottky defect
stoichiometry
state for ionic compounds wherein there is the exact
ratio of cations to anions as predicted by the chemical formula
stress raisers
points at which the magnitude of an applied tensile stress is amplified and no mechanism such as plastic deformation exists to slow down or divert such cracks