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Solution Thermodynamics

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Statistical thermodynamics of a polymer chain. How much space ... Enthalpy of mixing. DHMix = kT cf2N1 ...where c is the dimensionless Flory Huggins parameter. ... – PowerPoint PPT presentation

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Title: Solution Thermodynamics


1
Solution Thermodynamics
  • Richard Thompson
  • Department of Chemistry
  • University of Durham
  • r.l.thompson_at_dur.ac.uk

2
Overview
  • Part 1
  • Statistical thermodynamics of a polymer chain
  • How much space does a polymer chain occupy?
  • Part 2
  • Chemical thermodynamics of polymer solutions
  • What determines solubility of a polymer?
  • Examine
  • (i) Models of polymer chain structure in solution
  • (ii) Interactions between polymers and solvents

3
The freely jointed chain
  • Simplest measure of a chain is the length along
    the backbone
  • For n monomers each of length l, the contour
    length is nl

4
A more useful measure is the end-to-end distance
r
  • For an isolated polymer in a solvent the
    end-to-end distance will change continuously due
    to molecular motion
  • But many conformation give rise to the same value
    of r, and some values of r are more likely than
    others e.g.,
  • Only one conformation with r nl - a fully
    extended chain
  • Many conformation have r 0, (cyclic polymers)
  • Define the root mean square end-to-end distance

5
A freely jointed chain in 1D
  • Each link (monomer) can step to either left or
    right with equal probability
  • End-to-end distance

l
vector of each monomer ? l
6
End-to-End Distance
  • If i j then ri . rj l2
  • If i ? j then ri . rj l. l l2
  • or - l.- l l2
  • or - l. l -l2
  • or l.- l -l2
  • all with equal probability
  • Hence lt ri . rj gt i ? j 0

7
See handout notes for derivation Key result for
a freely jointed chain
8
Bond angles and steric effects
  • Real chains are not freely jointed
  • Links between monomers subject to bond angle
    restrictions
  • Rotation hindered by steric effects
  • E.g., n-butane
  • Each bond angle q 109.5
  • Different conformations arise from rotation of 1
    and 2 about 3-4 bond
  • Steric interactions between methyl groups ? not
    all angles of rotation have the same energy

9
Valence angle model
  • Simplest modification to the freely jointed chain
    model
  • Introduce bond angle restrictions
  • Allow free rotation about bonds
  • Neglecting steric effects (for now)
  • If all bond angles are equal to q,
  • indicates that the result is for the valence
    angle model
  • E.g. for polyethylene q 109.5 and cos q
    -1/3, hence,

10
Rotational isomeric state theory
  • Steric effects lead to
  • f is defined by f 0 as the planar trans
    orientation
  • ltcosf gt is the average of cosf , based on the
    probability of each angle f , determined by its
    associated energy and the Boltzmann relation
  • Generally f lt 90ยบ are the most energetically
    favourable angles
  • Steric effects cause chains to be more stretched
  • What about temperature effects????

11
Steric parameter and the characteristic ratio
  • In general
  • where s is the steric parameter, which is usually
    determined for each polymer experimentally
  • A measure of the stiffness of a chain is given by
    the characteristic ratio
  • C? typically ranges from 5 - 12

12
An equivalent freely jointed chain
  • A real polymer chain may be represented by an
    equivalent freely-jointed chain
  • Comprised of N monomers of length b such that the
    chains have the same contour length, i.e., Nb
    nl
  • Normally has fewer, longer joints

13
Excluded volume
  • Freely jointed chain, valence angle and
    rotational isomeric states models all ignore
  • long range intramolecular interactions (e.g.
    ionic polymers)
  • polymer-solvent interactions
  • Such interactions will affect
  • Define
  • where is the expansion parameter

14
The expansion parameter
  • ar depends on balance between i) polymer-solvent
    and ii) polymer-polymer interactions
  • If (ii) are more favourable than (i)
  • ar lt 1
  • Chains contract
  • Solvent is poor
  • If (ii) are less favourable than (i)
  • ar gt 1
  • Chains expand
  • Solvent is good
  • If these interactions are equivalent, we have
    theta condition
  • ar 1
  • Same as in amorphous melt

15
The theta temperature
  • For most polymer solutions ar depends on
    temperature, and increases with increasing
    temperature
  • At temperatures above some theta temperature, the
    solvent is good, whereas below the solvent is
    poor, i.e.,
  • What determines whether or not a polymer is
    soluble?

T gt q ar gt 1
T q ar 1
T lt q ar lt 1
Often polymers will precipitate out of solution,
rather than contracting
16
R.M.S. Radius of Gyration lts2gt1/2
  • Another way of characterising size
  • Defined as the average distance of chain segments
    from the centre of the chain
  • For linear polymers,
  • Particularly useful for branched/cyclic polymers
  • Cannot meaningfully define an end-to-end distance
  • R.M.S. radius of gyration is uniquely defined and
    a useful measure of size (or volume occupied)

17
Flory Huggins Theory
  • Dissolution of polymer increases conformational
    entropy of system
  • Molar entropy of mixing normally written as
  • where fi is the volume and volume fraction of
    each component (solvent 1 and polymer 2), ri
    is approximately the degree of polymerisation of
    each component (r1 1, r2 N)
  • Note that increasing the r2 decreases the
    magnitude of DSmix

18
Flory Huggins Theory 2
  • Enthalpy of mixing
  • DHMix kT cf2N1
  • where c is the dimensionless Flory Huggins
    parameter.
  • For dilute solution of high molecular weight
    polymers, NN1
  • DHMix RT cf2
  • Remember condition for thermodynamically stable
    solution
  • DGMix DHMix - TDSMix lt 0

19
Practical Use of Polymer TDsFractionation
  • Consider solution in poor solvent of two
    polymers, p1 and p2.
  • Flory-Huggins tells us that if p2 has higher
    molecular weight it should precipitate more
    readily than p1
  • add non-solvent until solution becomes turbid
  • heat, cool slowly and separate precipitate
  • finite drop in temperature always renders finite
    range of molecular weight insoluble
  • some p2 will also remain soluble!

1 phase clear solution
T
p2
2 phase cloudy
p1
f2 volume fraction polymer
20
Summary
  • A little knowledge goes a long way!
  • Simple models enable us to predict the size of
    polymer chains in solution
  • Critical to dynamic properties of solutions (next
    lecture)
  • Solubility of polymers generally decreases with
    increasing molecular weight.
  • Can exploit this in fractionation procedures to
    purify polymers
  • There are practical limits to how well
    fractionation can work
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