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Chapter Polymer Science

Apr 09, 2018

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Jyoti Mishra
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  • 8/8/2019 Chapter Polymer Science

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    Chapter 7

    Fundamentals of Polymer Science

    Paul C. Painter

    Michael M. Coleman

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    1st -Or der Tr ans it ions

    GasGas

    LiquidLiquid

    SolidSolid((Crystalline)Crystalline)

    Sma ll M olecules

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    Many Materials form metastable glasses -

    what about polymers like PET, atactic polystyrene?

    Two Possibilities; Observed Behaviordepends on:

    StructureCooling Rate

    Crystallization Kinetics

    Glass Transition

    Liquid

    Gas

    Glass

    Crystal

    TR Tf Tb

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    No Gaseous StateNo Gaseous State

    Liquid State - - Viscoelastic MeltLiquid State - - Viscoelastic Melt

    Semi- CrystallineSemi- CrystallineSolidSolid

    ElastomerElastomerSemi- SolidSemi- Solid

    (like Silly Putty)(like Silly Putty)

    GlassGlass

    Cool CoolCool +

    X- link

    Cool

    Also:x-link ed r ub ber + solvent (gel)

    liquid cr ysta lline polymer s, etc.

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    ~ 1500 Columbus Stumbles Across Haiti~ 1600 Missionaries Observe Indians Making Crude

    Rubber Shoes (Caoutchouc)

    1700 Joseph Priestly Invents a Name

    1820 1st Rubber Shoes1832 Mackintosh

    1833 Goodyear Starts Work on Rubber

    1844 Vulcanization

    1875 Henry Wickham -- Pirate or Con-Man?1922 Stevenson Plan

    1942 Synthetic Rubber Project

    1988 Penn State Rubber Project

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    Material Derived from Trojan-Enz

    Samples Cut Out With a Dog Bone Cutter

    Test -- Tensile Elongation (1 cm per minute)

    UniaxialDeformation

    ~ 1,000 %

    Biaxial

    Deformation~ 300 %

    Estimated Burst

    Pressure ~ 57 psi

    ~ 4 atm.

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    The Issues

    Bonding & the Forces between Chains

    Conformations

    Ordered

    Disordered

    Stacking or Arrangement of Chains in

    Crystalline Domains

    Morphology of Polymer Crystals (and

    Things like Block Copolymers)

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    Interaction Energy Depends Upon the BalanceBetween Attractive and Repulsive Forces

    Attractive Forces

    Type of

    In ter act ion C ha r acter istics

    Approximate

    Strength

    Dispersion Forces

    Dipole / dipole

    (Freely Rotating)

    Short Range

    Varies

    as 1/r6

    ~0.2 to 2

    kcal./mole

    Strong Polar Forces

    & Hydrogen Bonds

    Complex Form,

    but Short Range

    ~ 1 to 10 kcal. /

    mole

    Coulombic, as Found

    in Ionomers

    Long Range,

    Varies 1/r

    ~ 10 to 20 kcal./

    mole (?)

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    In ter action between fluctua ting dipoles whose

    aver age value is zer o (!)

    eg: simple hydr ocar bons

    Dispersion Forces

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    CH 2CH

    C

    N

    +

    CH 2 CH

    C

    N

    +

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    Schemat ic

    Diagramof Cluster s

    in a n

    Ionomer .

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    Hydrocarbons -- PE, IPP, PS, etc.

    Weak Dispersion Forces

    Polar Polymers -- PVC, PAN, etc.

    Eg: Those Containing Heteroatoms (O, N, Cl, F) --

    Dipole/dipole Interactions Hydrogen Bonding Polymers

    Eg: Nylons, Polyurethanes, etc.

    Ionomers

    Eg: Surlyn

    IncreasingIncreasing

    InteractionInteraction

    StrengthStrength