Title: Ceramics
1Ceramics
Thermal Coatings
2History and Background
- Applications date into antiquity - earthenware,
pottery, clay product, bricks, etc - More modern uses Transparent glass, structural
glass, refractories - Advanced uses Thermal barrier coatings,
structural ceramics, composite armor,
electronics, glass-ceramics - Ceramics can be Amorphous or Crystalline
- Atomic structure contains strong Ionic Bonds
3What are they?
- A compound of metallic and nonmetallic elements,
for which the inter atomic - bonding is predominantly ionic.
- They tend to be oxides, carbides, etc of metallic
elements. - The mechanical properties are usually good high
strength, especially at elevated temperature. - However, they exhibit low to nil-ductility, and
have low fracture toughness.
4Crystalline Ceramics
- As with plastics, the amorphous ceramics tend to
be transparent - The structural ceramics tend to be crystalline
and show greater strength, as well as stability
at high temperature
5AX Structure - CsCl
Note This is not a BCC structure.
Cs
Simple Cubic Crystal
6AX Structure - NaCl
2- FCC interpenetrating lattices.
7Try it!
Compute the theoretical density of Rock Salt
based on its crystal structure.
For this NaCl structure, the crystal lattice
parameter is a 2 ( r Na r Cl -), where r
is ionic radius.
8AX structure - Si C
9Summary of most common ceramic crystal structures
10Silicate Ceramics
- Silica, SiO2
- Many polymorphsQuartz CrystobaliteTridymite
- Low density Quartz 2.65g/cm3
11Crystalline Crystabolite
12Carbon
- Pure carbon has many polymorphs with vastly
varying properties. It also exists in the
amorphous state. - Diamond Is similar to ZnS in structure
- Graphite is considered to be a crystalline
ceramic - Fullerenes, C60, are a newly discovered polymorph
- with interesting properties.
13Diamond
- AX type crystal structure similar
- to that of ZnS.
- Each carbon atom is covalently bonded to four
other C atoms in a diamond-cubic crystal
structure. - The material is optically transparent and
extremely hard (hardest natural material known)
and durable. - In engineering applications, cruder or industrial
forms of diamond, that are much less expensive
than the gemstone forms, are used as abrasives,
indentors, and coatings (especially thin films)
for a variety of applications.
14Graphite
- Layers of hexagonally arranged and
- covalently bonded C atoms.
- Between layers, weaker Van der Walls
- bonds are active, giving easy slip
- on the 0001 crystallographic planes.
- Excellent as a dry lubricant, relatively high
strength at elevated temperatures, high thermal
and electrical conductivity, low thermal
expansion, resistance to thermal shock, and good
machinability. - Usage electrodes, heating elements, crucibles,
casting molds, rocket nozzles, and other
applications.
15Fullerenes, C60
- Molecular form of carbon with a
- hollow spherical structure resembling
- a geodesic dome (soccer ball.)
- Called buckyballs after R. Buckminister
- Fuller, who pioneered the geodesic dome.
- Discovered in 1985 and have since been found to
occur naturally in several sources. - In the solid crystalline state, C60 molecules
pack together in a FCC unit cell arrangement with
a lattice parameter a1.41 nm. - The pure solid material density is about 1.65
g/cm3 and it is relatively soft and is
non-conducting since it has no free electrons.
16Properties of Buckyballs
- When alkali metal anions, most notably K, are in
the structure (usually 3 per C60 molecule), the
resulting molecular material (K3C60) displays the
characteristics of a metal. In fact, K3C60 is
considered to be the first molecular metal ever
encountered. - K3C60 buckyballs and similar molecular materials
become super conducting (practically no
electrical resistance) at about 18K (relatively
high temperature for this phenomenon) - Applications in low-power consumption,
low-pollution, magnetic-levitation and propulsion
devices for mass transit systems. - Other synthetic ceramic materials have been
developed that display superconductivity at even
higher temperatures (up to 100K) above the
temperature of liquid nitrogen, a relatively
inexpensive and abundant coolant.
17Try It!
- Calcualte the theoretical density of pure C60
based on a FCC unit cell as shown
a1.41 nm
18Defects in Crystalline Ceramics
- Vacancy
- Interstitial
- Dislocation
- Grain Boundary
Cation Interstitial Anion Vacancy Cation
Vacancy Schotky Defect Frenkel Defect
Electro- neutrality
19Mechanical Properties
- Brittle Materials, hard to perform a Tension
Test. - Flexural Test (Bend) is often substituted.
- Obtain Flexural Strength (Modulus of Rupture),
Stiffness (Modulus of Elasticity), and Ductility. - Strength is often good, Stiffness my be high, but
Ductility and affected properties are poor. - In crystalline ceramics, dislocation motion is
difficult because of the need to maintain
electro-neutrality. Consequently plastic
deformation is restricted.
20Flexural Test Configuration
Rectangular Circular
21Stress-Strain Behaviour
22Mechanical Properties of Various Ceramics
- a Sintered with about 5 porosity
23Hardness of Ceramics
24Relative Hardness
B4C, SiC WC, Al2O3
Glass
25Effect of Porosity on Stiffness
Where Eo is the theoretical modulus of elasticity
with no porosity, and P is the volume fraction of
porosity.
26Effect of Porosity on Strength
- Where so is the theoretical modulus of rupture
with no porosity, P is the volume fraction of
porosity, and n is an empirical material constant
27Fracture Toughness
28Amorphous Ceramics - Glasses (Na20, Ca0, K2O, etc)
- The viscosity of the material at ambient
temperature is relatively high, but as the
temperature increases there is a continuous
decrease in viscosity. - When the viscosity has decreased to the point
that the ceramic is a fluid, it is considered to
have melted. - At ambient temperature while it is still solid,
it is said to be in the glassy condition. - There is no distinct melting temperature (Tm) for
these materials as there is with the crystalline
materials. - The glass transition temperature, Tg, is used to
define the temperature below which the material
is a solid and defines a practical upper limit
on service temperature.
29Specific volume of amorphous and crystalline
ceramics.
30Viscous Behaviour in Amorphous Ceramics
t shear stress h viscosity of material
- Plastic deformation does not occur by
dislocation motion in amorphous or
non-crystalline ceramics, such as glass. - Deformation is by viscous flow rate of
deformation proportional to applied stress.
31Ceramic Phase Diagrams
- Note They are similar to metal alloy systems -
except the temperatures are generally higher.
32Binary Eutectic Ceramic Alloy
Spinel