Lecture Script Polymer Sci II Colloid Stability

download Lecture Script Polymer Sci II Colloid Stability

of 28

Transcript of Lecture Script Polymer Sci II Colloid Stability

  • 7/28/2019 Lecture Script Polymer Sci II Colloid Stability

    1/28

  • 7/28/2019 Lecture Script Polymer Sci II Colloid Stability

    2/28

    A state of subdivision in

    which the particles,

    droplets, or bubbles

    dispersed in another

    phase have at least one

    dimension between 1 and

    1000 nm

    all combinations are

    possible between :

    gas, liquid, and solid

    W. Ostwald

    Colloidal systems

  • 7/28/2019 Lecture Script Polymer Sci II Colloid Stability

    3/28

    Surface area of colloidal systems

    Cube (1cm; 1cm; 1cm)after size reduction to an edge length of 500 nm:

    surface area of 60 m2

    Spinning dope (1 cm3)

    after spinning to a fibre with diameter of 1000 nm:

    fiber length of 1273 km

    1 liter of a 0.1 M surfactant solution:

    interfacial area of 40000 m2

  • 7/28/2019 Lecture Script Polymer Sci II Colloid Stability

    4/28

    Surface atoms [in %]

    in dependence on the particle size [in nm]

    0

    10

    2030

    40

    50

    60

    7080

    90

    100

    20 10 5 2 1

    part of surface

    atoms in %%

    nm

  • 7/28/2019 Lecture Script Polymer Sci II Colloid Stability

    5/28

    Colloidal systems

    have large surface areas

    surface atoms become dominant

  • 7/28/2019 Lecture Script Polymer Sci II Colloid Stability

    6/28

    Colloid stability

    Colloidal gold: stabilized against coagulation !

    Creme: stabilized against coagulation !

    Milk: stabilized against coagulation !

  • 7/28/2019 Lecture Script Polymer Sci II Colloid Stability

    7/28

    ParticleParticle interactions

    Interaction Energy ( Vtot)Distance of

    Separation (d) Relationship

    d

  • 7/28/2019 Lecture Script Polymer Sci II Colloid Stability

    8/28

  • 7/28/2019 Lecture Script Polymer Sci II Colloid Stability

    9/28

    DLVO - Theory

    1940 Derjaguin; Landau; Verwey; Overbeek

    Long range attractive van der Waals forces

    Long range repulsive electrostatic forces

  • 7/28/2019 Lecture Script Polymer Sci II Colloid Stability

    10/28

    DLVO Theory

    Van der Waals attractive energy

    a) between two plates:

    b) between two spheres:

    2

    .

    12 d

    AVattr WaalsderVan

    d

    aAV

    attr

    WaalsderVan12

    .

  • 7/28/2019 Lecture Script Polymer Sci II Colloid Stability

    11/28

    Double layer models

    Helmholtz

    Gouy Chapman

    Stern

  • 7/28/2019 Lecture Script Polymer Sci II Colloid Stability

    12/28

    Gouy Chapman model

    planar double layer

    Ions as point charges

  • 7/28/2019 Lecture Script Polymer Sci II Colloid Stability

    13/28

    Electrolyte theory

    kT

    xez

    iii

    i

    enezxd

    xd

    0

    2

    24

    I distribution of ions in the diffuse double layer

    (Boltzmann equation)

    II equation for the room charge density

    III Poisson relation

    Aus I, II und III folgt:

    Poisson

    Boltzmann - relation

    kT

    xezenxn iii

    xnezx iii

    0

    2

    24 x

    xd

    xd

  • 7/28/2019 Lecture Script Polymer Sci II Colloid Stability

    14/28

    Solution of the P-B equation

    xekx

    xxd

    xd

    k

    k

    0

    2

    2

    2

    For small potentials (< 25 mV) :

    Integrable form

    kT

    xez

    i

    ii

    i

    enezdx

    xd

    0

    2

    24

  • 7/28/2019 Lecture Script Polymer Sci II Colloid Stability

    15/28

    DLVO Theory

    Electrostatic repulsive energy

    Resulting repulsive overlap energy

    a) Between two plates:

    c volume concentration of the

    z valent electrolyte

    b) Between two spheres

    drep

    elektrost ekTc

    V k

    k

    64

    .

    2

    2

    2

    22

    0

    22

    .

    1

    18

    kT

    ze

    kT

    ze

    drep

    elektrost

    e

    ee

    ze

    TkV

    k

  • 7/28/2019 Lecture Script Polymer Sci II Colloid Stability

    16/28

    Vtot(d)= Vattr(d) + Vrep(d)

    Vvan der Waals

    = - A a / 12 d Velectrost.

    = k e-kd

    AHamaker constant

    aparticle radius

    d

    distance between the particles

    1/k - thickness of the double-layer

  • 7/28/2019 Lecture Script Polymer Sci II Colloid Stability

    17/28

    Electrostatic stabilization

    stabilized against coagulation

    Kinetically stable state

    energetic metastable state in the

    secondary minimum

    with an energy barrier

  • 7/28/2019 Lecture Script Polymer Sci II Colloid Stability

    18/28

    Critical coagulation concentration (CCC)

    The energy barrier disappears by adding a

    critical amount of low molecular salts

  • 7/28/2019 Lecture Script Polymer Sci II Colloid Stability

    19/28

    DLVO Theory

    (CCC)

    Vtot / dd = 0 Vtot = 0

    for two spheres:

    2

    266

    3

    0

    3553

    2

    2

    2

    2

    122

    0

    22

    1

    1

    4

    1039,3

    121

    18

    kT

    ze

    kT

    ze

    kT

    ze

    kT

    ze

    e

    e

    Aze

    Tkccc

    daA

    e

    eeze

    Tk

  • 7/28/2019 Lecture Script Polymer Sci II Colloid Stability

    20/28

    DLVOTheory

    (CCC)

    For two spheres the ccc should be related to

    the valency (1 : 2 : 3) of the counterions as:

    1000 : 16 : 1,3

  • 7/28/2019 Lecture Script Polymer Sci II Colloid Stability

    21/28

    CCC of a colloidal dispersion as a function of

    the salt concentration

    AlCl3

    CaCl2

    MgCl2

    KCl

    NaCl

    electrolyte

    1,79,3 10-5

    136,5 10-4

    137,2 10-4

    10005,0 10-2

    10005,1 10-2

    Schulze-Hardy-ratioCCC of a

    Arsensulfid -Dispersion

  • 7/28/2019 Lecture Script Polymer Sci II Colloid Stability

    22/28

    Steric stabilization

    What will be happen when we add polymers

    to a colloidal dispersion ?

  • 7/28/2019 Lecture Script Polymer Sci II Colloid Stability

    23/28

    ParticleParticle interactions

    Polymer adsorption layer

  • 7/28/2019 Lecture Script Polymer Sci II Colloid Stability

    24/28

    ParticleParticle interactions

    Overlap of the

    polymer adsorption layer

  • 7/28/2019 Lecture Script Polymer Sci II Colloid Stability

    25/28

    Overlap of the adsorption layer

    Osmotic repulsion

    Entropic repulsion

    Enthalpic repulsion

  • 7/28/2019 Lecture Script Polymer Sci II Colloid Stability

    26/28

    Sterically stabilized systems can

    be controlled by

    The thickness of the adsorption layer

    The density of the adsorption layer

    The temperature

  • 7/28/2019 Lecture Script Polymer Sci II Colloid Stability

    27/28

    Stabilization and destabilization in

    dependence on the molecular

    weight of the added polymer

  • 7/28/2019 Lecture Script Polymer Sci II Colloid Stability

    28/28

    Stabilization and destabilization in

    dependence on the

    polymer-concentration