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Ceramics

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Title: Ceramics


1
Ceramics
Thermal Coatings
2
History 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

3
What 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.

4
Crystalline 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

5
AX Structure - CsCl
  • Cl-

Note This is not a BCC structure.
Cs
Simple Cubic Crystal
6
AX Structure - NaCl
2- FCC interpenetrating lattices.
7
Try 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.
8
AX structure - Si C
9
Summary of most common ceramic crystal structures
10
Silicate Ceramics
  • Silica, SiO2
  • Many polymorphsQuartz CrystobaliteTridymite
  • Low density Quartz 2.65g/cm3

11
Crystalline Crystabolite
12
Carbon
  • 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.

13
Diamond
  • 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.

14
Graphite
  • 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.

15
Fullerenes, 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.

16
Properties 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.

17
Try It!
  • Calcualte the theoretical density of pure C60
    based on a FCC unit cell as shown

a1.41 nm
18
Defects in Crystalline Ceramics
  • Vacancy
  • Interstitial
  • Dislocation
  • Grain Boundary

Cation Interstitial Anion Vacancy Cation
Vacancy Schotky Defect Frenkel Defect
Electro- neutrality
19
Mechanical 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.

20
Flexural Test Configuration
Rectangular Circular
21
Stress-Strain Behaviour
22
Mechanical Properties of Various Ceramics
  • a Sintered with about 5 porosity

23
Hardness of Ceramics
24
Relative Hardness
B4C, SiC WC, Al2O3
Glass
25
Effect of Porosity on Stiffness
Where Eo is the theoretical modulus of elasticity
with no porosity, and P is the volume fraction of
porosity.
26
Effect 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

27
Fracture Toughness
28
Amorphous 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.

29
Specific volume of amorphous and crystalline
ceramics.
30
Viscous 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.

31
Ceramic Phase Diagrams
  • Note They are similar to metal alloy systems -
    except the temperatures are generally higher.

32
Binary Eutectic Ceramic Alloy
Spinel
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