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Ch2 Solid Surfac

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    Atomic Arrangement of the Solid Surface(to lower the free energy of formation)

    (a) reconstruction, (b) segregation, (c) chemisorption,(d) formation of compounds, (e) physisorption,

    (f) nucleation of atoms on the surface

    Figure by MIT OCW. After Estrup, 1975.

    (a) (b) (c) (d)

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    Why is the state of the surface important intribology?

    1. Light load

    contaminants, reconstruction of the surface, etc.

    2. Heavy load Less important Elastic and plastic deformation dominated

    3. Small contacts Important

    4. Large contacts

    Less important

    Important -- mechanical properties, surface

    Contaminants -- adhesion

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    Much progress due to the availability ofinstrumentation

    1. Scanning electron microscope (SEM)2. Atomic force microscope (AFM)

    3. Auger spectroscope4. Etc.

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    Modification of the surface through the useof coating techniques

    1.2. Chemical vapor deposition (CVD)

    3. Physical vapor deposition (PVD)4. Atomic layer deposition (ALD)

    5. Diamond-Like Carbon or Coating (DLC)

    Molecular beam epitaxy (MBE)

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    General Characteristics of Metals

    1. Metallic bonding2.

    3. Defects control mechanical properties. Dislocations Vacancies

    4.energy

    5. Importance of microstructure

    6.multiphase, dispersion strengthened,

    7.

    Structure -- fcc, bcc, hcp

    Higher energy state at the surface -- Surface

    Alloys -- substitutional, interstitial,

    Reactive -- oxides, carbides, intermetallics

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    General Characteristics of Polymers

    1. Covalently bonded long chain molecules2. Thermoplastics, thermosets, elastomers,

    liquid crystal polymers (LCD)3.4.

    5. Low melting point, glass transitiontemperature

    6. Difference in molecular weight at the surfaceand the bulk = f(nucleation conditions)

    Linear polymers -- HDPE, PTFESemicrystalline vs amorphous polymers

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    General Characteristics of Ceramics

    1. Mostly ionic bonding, some have covalentbonding

    2. Combination of metallic and nonmetallicelements

    3.free energy of formation

    4. Carbides are very hard and have very hightemperature

    5. Brittle

    6. Electrically non-conducting

    7. Abrasives

    Oxides and nitrides are very stable -- Low

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    General Characteristics of Composites

    1. Typically resin + fibers or filler or both2. Fiber orientation important

    3. May be designed to achieve specific properties

    4. Used without lubricants

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    General Characteristics of a Solid Surface

    1. Surface energy2. Surface may be different from the bulk in

    atomic structure, mechanical properties,chemical state

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    Electric double layer

    ++ + + + + + + + +

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    Role of lubricants

    1. Change surface energy(monolayer)

    2. Reduce metal to metal contactthrough wetting

    3. Prevent particle agglomeration

    through wetting

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    Mechanical Properties of the Surface

    1. Is the surface harder or softerthan the bulk?

    2. Does it matter?

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    Mechanical Properties of the Surface(aluminum monocrystal after Kramer and Demer, 1961

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    Mechanical Properties of the Surface

    Graph removed for copyright reasons.

    Tribophysics . Englewood Cliffs NJ:Prentice-Hall, 1986. ISBN: 0139309837.

    (Copper -- Fourie, 1968)

    See Figure 2.3 in [Suh 1986]: Suh, N. P.

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    Image force on dislocations near the surface

    1. Dislocations near the surface experience animage force due to the free surface

    i = Gb

    4 (1 )h

    h = Gb4 (1 ) i

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    Thermodynamic analysis of an Interface

    Me tal

    Oxide

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    Thermodynamic analysis of an Interface

    How thick is the interface?

    f (c , c , 2 = f 0 (c ) + Lii ( c xi ) + K i, j

    (1)

    i, j ( 2

    c xi x j

    ) + 12 K i, j(2)

    i, j ( c xi )( c x j ) + ....,...)

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    Thermodynamic analysis of an InterfaceFree energy of a binary system as a function of composition

    Graph removed for copyright reasons.

    Tribophysics . Englewood Cliffs NJ:Prentice-Hall, 1986. ISBN: 0139309837.See Figure 2.6 in [Suh 1986]: Suh, N. P.

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    Thermodynamic analysis of an InterfaceInterfacial free energy as a function of composition

    =

    N v f 0 (c )+

    K (

    dc

    dx )2

    c B(e)

    (1

    c) A(e)

    dx= N v f 0 (c ) + K (

    dc

    dx)2

    dx

    (from Cahn and Hilliard, 1958)


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