Ch 12-Structures and Properties of Ceramics

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    ISSUES TO ADDRESS...

    Structures of ceramic materials:How do they differ from those of metals?

    Point defects:How are they different from those in metals?

    Impurities:How are they accommodated in the lattice and how

    do they affect properties?

    Mechanical Properties:What special provisions/tests are made for ceramic

    materials?

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    Bonding:

    -- Mostly ionic, some covalent.-- % ionic character increases with difference in

    electronegativity.

    Adapted from Fig. 2.7, Callister 7e. (Fig. 2.7 is adapted from Linus Pauling, The Nature of the Chemical

    Bond, 3rd edition, Copyright 1939 and 1940, 3rd edition. Copyright 1960 by

    Cornell University.

    SiC: smallCaF2: large

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    2. Size of ionic radii- Stable structures:

    --maximize the # of nearest oppositely charged neighbors.

    Adapted from Fig. 12.1,

    Callister 7e.

    - -

    - -+

    unstable

    - -

    - -+

    stable

    - -

    - -+

    stable

    1. Charge Neutrality:--Net charge in the

    structure should

    be zero.

    --General form:

    CaF2:Ca2+

    cation

    F-

    F-anions+

    AmXp

    m, p determined by charge neutrality

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    Coordination # increases with

    Adapted from Table 12.2,

    Callister 7e.

    2

    rcationr

    anion

    Coord

    #

    < 0.155

    0.155 - 0.225

    0.225 - 0.414

    0.414 - 0.732

    0.732 - 1.0

    3

    4

    6

    8

    linear

    triangular

    TD

    OH

    cubic

    Adapted from Fig.12.2, Callister 7e.

    Adapted from Fig.

    12.3, Callister 7e.

    Adapted from Fig.12.4, Callister 7e.

    ZnS(zincblende)

    NaCl(sodiumchloride)

    CsCl(cesiumchloride)

    rcationranion

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    rNa = 0.102 nm

    rNa/rCl = 0.564

    cations preferOHsites

    Adapted from Fig.

    12.2, Callister 7e.

    rCl = 0.181 nm

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    939.0181.0

    170.0

    Cl

    Cs

    r

    r

    Adapted from Fig.

    12.3, Callister 7e.

    cubicsites preferred

    So each Cs+ has 8 neighboring Cl-

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    Why is Zn2+ in TD

    sites?

    bonding hybridization of zincfavors T

    Dsites

    8

    So each Zn2+ has 4 neighboring S2-

    Adapted from Fig.

    12.4, Callister 7e.??529.0

    140.0

    074.0

    2

    2

    O

    ZnHO

    r

    r

    Size arguments predict Zn2+

    in OHsites, In observed structure Zn2+

    in TD sites

    Ex: ZnO, ZnS, SiC

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    On the basis of ionic radii, what is the crystal structure of FeO?

    Answer:

    5500

    1400

    0770

    anion

    cation

    .

    .

    .

    r

    r

    based on this ratio,

    --structure = NaCl

    Data from Table 12.3,

    Callister 7e.

    Ionic radius (nm)

    0.053

    0.077

    0.069

    0.100

    0.140

    0.181

    0.133

    Cation

    Anion

    Al3+

    Fe2+

    Fe3+

    Ca2+

    O2-

    Cl-

    F-

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    Calcium Fluorite (CaF2)

    cations in cubic sites

    ex. UO2, ThO2, ZrO2, CeO2

    Adapted from Fig.

    12.5, Callister 7e.

    antifluorite structure cations and anions

    reversed

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    Ex: complex oxide

    BaTiO3

    13

    Adapted from Fig.

    12.6, Callister 7e.

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    A

    AC

    NV)AA(n

    C

    Number of formula units/unit cell

    Volume of unit cell

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    On the basis of crystal structure, compute thetheoretical density for sodium chloride.

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    n= 4 (FCC)

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    On the basis of crystal structure, compute thetheoretical density for sodium chloride.

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    Most common elements on earth are Si & O

    SiO2 (silica) structures are quartz, crystobalite, & tridymite The strong Si-O bond leads to a strong, high melting material

    (1710C)

    Si4+

    O2-

    Adapted from Figs.

    12.9-10, Callister 7e.

    crystobalite

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    Silica gels - amorphous SiO2

    Si4+ and O2- not in well-orderedlattice

    Charge balanced by H+ (to formOH-) at dangling bonds

    very high surface area > 200 m2/g

    SiO2 is quite stable, thereforeunreactive

    makes good catalyst support

    Adapted from Fig.

    12.11, Callister 7e.

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    Combine SiO44- tetrahedra by having them share corners,

    edges, or faces

    Cations such as Ca2+, Mg2+, & Al3+ act to neutralize & provideionic bonding

    Mg2SiO4 Ca2MgSi2O7

    Adapted from Fig.

    12.12, Callister 7e.

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    Layered silicates (clay silicates)

    SiO4 tetrahedra connectedtogether to form 2-D plane

    (Si2O5)2-

    So need cations to balance charge= Adapted from Fig.

    12.13, Callister 7e.

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    Kaolinite clay alternates (Si2O5)2- layer with Al2(OH)4

    2+ layer

    Note: these sheets loosely bound by van der Waals forces

    Adapted from Fig.

    12.14, Callister 7e.

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    tetrahedral carbon

    hard no good slip planes

    brittle can cut it

    large diamonds jewelry

    small diamonds

    often man made - used for

    cutting tools and polishing diamond films

    hard surface coat tools,medical devices, etc.

    Adapted from Fig.

    12.15, Callister 7e.

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    layer structure aromatic layers

    weak van der Waals forces between layers

    planes slide easily, good lubricant

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    Adapted from Fig.

    12.17, Callister 7e.

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    Fullerenes or carbon nanotubes

    wrap the graphite sheet by curving into ball or tube

    Buckminister fullerenes

    Like a soccer ball C60 - also C70 + others

    Adapted from Figs.

    12.18 & 12.19,

    Callister 7e.

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    Frenkel Defect--a cation is out of place.

    Shottky Defect--a paired set of cation and anion vacancies.

    Equilibrium concentration of defectskT/QDe~

    Adapted from Fig. 12.21, Callister

    7e. (Fig. 12.21 is from W.G.

    Moffatt, G.W. Pearsall, and J.

    Wulff, The Structure and

    Properties of Materials, Vol. 1,

    Structure, John Wiley and Sons,

    Inc., p. 78.)

    Shottky

    Defect:

    Frenkel

    Defect

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    Ex: NaCl

    Substitutional cation impurity

    Na+ Cl-

    initial geometry Ca2+ impurity resulting geometry

    Ca2+

    Na+

    Na+

    Ca2+

    cationvacancy

    Substitutional anion impurity

    initial geometry O2- impurity

    O2-

    Cl-

    an ion vacancy

    Cl-

    resulting geometry

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    Adapted from Fig. 12.32,Callister 7e.F

    L/2 L/2

    d= midpoint

    deflection

    cross section

    R

    b

    d

    rect. circ.

    Determine elastic modulus according to:

    F x

    linear-elastic behaviord

    F

    dslope =

    E= Fd

    L3

    4bd3= Fd

    L3

    12pR4

    rect.crosssection

    circ.crosssection

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    Adapted from Fig. 12.32,

    Callister 7e.F

    L/2 L/2

    d= midpoint

    deflection

    cross section

    R

    b

    d

    rect. circ.

    location of max tension

    Flexural strength:

    Typ. values:

    Data from Table 12.5, Callister 7e.

    sfs

    1.5FfL

    bd2

    FfL

    pR3 Si nitrideSi carbide

    Al oxide

    glass (soda)

    250-1000

    100-820

    275-700

    69

    304

    345

    393

    69

    Material sfs (MPa) E(GPa)

    xF

    Ff

    dfsd

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    Ceramic materials have covalent & ionic bonding.

    Structures are based on:-- charge neutrality

    -- maximizing # of nearest oppositely charged neighbors.

    Structures may be predicted based on:-- ratio of the cation and anion radii.

    Defects

    -- must preserve charge neutrality

    -- have a concentration that varies exponentially w/T.

    Room Tmechanical response is elastic, but fracture

    is brittle, with negligible deformation.

    Elevated Tcreep properties are generally superior to

    those of metals (and polymers).