Polymer Physics: Finding Molecular Stats

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    weights Oli omers Telomers

    Pleistomers Telechelic polymers Macromers

    Measurement of MW are usually ondissolved polymers

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    Wetting of surface Then diffusion of solvent into polymer (case I Fickian

    diffusion, or case II swelling)

    Finally, polymer diffuses and dissolves

    Solubility parameter determines which solventwill dissolve which polymer, from:

    21/ 2 1/ 2

    M M MG H T S

    E E

    1 2

    1 2

    anM M

    V V

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    Solubility parameter is the cohesive energy

    density, EV

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    experiments: For cross-linked polymers, from swelling coefficient,

    0 1m m

    Q m

    For non-cross-linked polymers, from intrinsic

    viscosity of the polymer in different solutions

    Or theoretically, from group molar attraction constant

    G

    M

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    . , . ,104g/mol3 1/21.05 .

    104

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    ,

    Ideal solutions is when the heat of mixing is zero, andRaoults law is obeyed

    For incompressible mixtures,

    1 1 2 2 1 1 2 2( ln ln )MG N G N G kT N n N n

    1 1 2 2( ln ln )MS k N n N n

    ,relationlnMS k

    0 1 2where !/ ! !N N N

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    For ol mer ofx-mers then

    1 1 2 2( ln ln )MS k N v N v

    ori iiM

    i

    i

    kV V

    1

    1

    1 2

    where vN xN

    2

    1 2

    and v N xN

    solutions also exist

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    For dilute solutions we use Flor -Hu ins theor with

    1 to represent heat of mixingMH

    1 2

    1 1 2 2 1 1 2

    so ( ln ln )M

    v

    G kT N v N v N v

    2

    1 2 2 1 2

    1ln(1 ) 1G RT v v v

    and the osmotic pressure is:

    2 2 1 2

    1 1

    n(1 ) 1v v vv V x

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    By separating out the second virial coefficient, we can

    n e ory - empera ure:2

    22 1

    1vA

    1

    1 2

    1

    At T when , 02

    A

    A To relate 1 to solubility parameter,

    21V 1 1 2

    and is related to the -temperature by

    RT

    5 3 1/ 2

    12 1mC M

    T

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    Example:

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    -

    divided by total number of molecules

    End-group analysis Specific functionalities at the ends ofmolecules measured from titration etc,

    Usually for low MW because of poorsensitivity at high MW.

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    2 1T RT

    Properties thatdepends on number of

    0

    2

    mc v nc H M

    molecules and nottheir chemistry

    0lim

    f

    c

    f n

    c H M

    ,

    depression, vaporpressure lowering,

    1 12

    1

    o

    o

    P PX

    P

    osmo c pressure0

    limc

    n

    RT

    c M

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    Osmotic ressure exists because of the difference

    between chemical potentials of the pure solvent andthe solvent in a solutionc

    2

    rom ,

    1

    nM

    At Flor -tem erature, = 0, so osmotic ressure is

    2 3 ...n

    c M

    independent of concentration, one concentration cangiveMn

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    -

    light-scattering (or X-ray and small-angle neutronscattering) Scattering occurs when radiation hits a particle with

    size close to the radiation wavelength ue o uc ua ons n re rac ve n ex, g sscattered, and measurements of the intensities atdifferent angles give the size

    2 2 2 2

    1 0

    4

    2 ( / )1where ( ) and

    I w n dn dcHcR H

    R RT c I V N

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    The basic equation is

    For very small particles, P() = 1, is the scattering form2

    2( ) ( ) ( )w

    A cR R solvent M P

    factor

    0

    3

    ( ) where turbidity fromx

    R I I e

    For particles > 0.05 times wavelength, P() 1, is thesingle chain form factor. At very small angles,

    2 2 2 24 42( ) 1 exp( ) 1 ...3g

    g g

    g

    R KP R K R K R K

    14where sin2

    K

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    Limiting to zero angle and zero concentration

    2

    0

    1

    2 ...( ) w

    c

    H A cR M

    2 21

    0

    41 11 sin ...

    ( ) 3 ' 2g

    wc

    cH R

    R M

    Summing both equations gives the Zimm plot

    PlottingH[c/R()] vs sin2 (/2), we get

    22

    2

    1

    3( ') (initial slope)

    16 (intercept)g

    R

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    The radius of gyration must be determined when

    So the range of angles are limited

    1gK R

    g ,usually between 45 to 135

    The radius of gyration is related to the end-to-enddistance, r, by

    22

    g

    rR

    For random coils, rdepends on MW, r2 = CM, and

    r n l

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    D namic li ht scatterin measures fluctuation of

    scattering intensity with time at very small volumes forvery short times

    g ves mo ecu ar mo on an us on coe c en

    Used to study aggregation, adsorption, structural

    chan es chain d namics

    2 2

    0( , ) (1 )(1 )app z g DcD K c D CR K k

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    expensive Fast and chea methods measures relative MW

    such as by intrinsic viscosity, and using Gel

    Permeation Chromatography Intrinsic viscosity

    Calculates the viscosity-average MW

    1/1

    , where a between 0.5 and 0.8aa

    i iiv

    i i

    N MM

    N M

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    Dissolvin ol mers in solution increases solution

    viscosity Define:

    0solvent viscosity =

    relative viscosity,

    0

    specific viscosity, 1sp rel

    0 0

    nintrinsic viscosity, sp rel

    c cc c

    ninherent viscosity =

    rel

    c

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    For a dilute dis ersion of uniform ri id non-interactin

    spheres, 0 2(1 2.5 )v

    Assuming the polymer molecule is an equivalentsphere of radiusRe, then

    0 2

    0

    2.5sp en

    VV

    2 1/ 2 301

    0

    42.53

    sp eA

    c

    RN Mc M

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    An em irical correlation for MW and intrinsic viscosit

    the Mark-Houwink-Sakurada equation:K a

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    Theoreticall the constant a can be used to determine

    the shape of the molecule (Table 3.11) The MHS equation can also be expressed as

    3/ 2

    21/ 2 3 1/ 2 30K

    rM M

    In a Flory -solvent or a good solvent,

    3/

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    Ex erimentall a series of dilute ol mer solutions is

    prepared and their viscosity measured (usingUbbelhode viscometer usually),

    en ca cu a e rom nown an a

    2

    'sp

    k cc

    2ln''rel k c

    c

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    Chromatography(GPC) Separation based on

    size-exclusion

    so ca e zeExclusionChromatography

    (SEC) Related to HPLC

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    Stationary phase usually made of cross-linkedpolymers with pores

    Mobile phase usually solvent that can dissolve thepolymers of interest

    ,time is the length of time a particular fraction remainsin the column

    Distribution of analyte between mobile and stationaryphase

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    The distribution coefficient is related to Gibbs freeenergy:R i

    d

    V VK

    V

    exp

    d

    d

    S HK

    GPC HPLCbut usually dK K K

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    Smaller particles pass through the column slower Larger particles pass through the column faster

    Detection usually by concentration (refractive index or

    UV absorption) or by molar mass (light-scattering,

    Calibration is required, usually with polymer standardsof PS, PMMA, PEO etc

    But there is error when using non-similar polymers(Rg2/Mnot similar)

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    So use a universal calibration From MHS equation, a polymer hydrodynamic volume

    is proportional to MW:

    3/ 22 3

    0M r o ns ea o p o ng vs e u on vo ume, we p oVHvs elution volume

    ,

    but what will it not work for?

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