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Handbook of Solvents - George Wypych - ChemTech - Ventech!

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112 Valery Yu. Senichev, Vasiliy V. Tereshatov<br />

2<br />

2<br />

[ ( dS . d. P) ( pS . pP . ) ]<br />

VS<br />

χH = δ − δ + δ −δ<br />

RT<br />

[4.1.19]<br />

where δd. S , δd.P , δp. S , δp.P<br />

are Hansen’s parameters <strong>of</strong> solvent and polymer (see the next section).<br />

Chen implied that χH was the enthalpy contribution to the Flory-Huggins parameter χ1 and plotted the solubility data in a δh −χH diagram where δh was the H-bond parameter in<br />

the Hansen approach. In these diagrams sphere-like volumes <strong>of</strong> Hansen’s solubility have<br />

degenerated to circles.<br />

The disadvantage <strong>of</strong> this method lies in the beforehand estimating characteristics <strong>of</strong><br />

the polymer. Among other two-dimensional methods used for the representation <strong>of</strong> solubility<br />

data was the δp-δh diagram proposed by Henry 19 and the δ-δh diagram proposed by<br />

Hoernschemeyer, 20 but their representations <strong>of</strong> the solubility region were less correct. All<br />

these approaches involving hydrogen bond parameter ignored the fact that hydrogen bond<br />

interaction was the product <strong>of</strong> hydrogen bonding donating and accepting capability. 21-23<br />

On the basis <strong>of</strong> chemical approach to hydrogen bonding, Rider proposed a model <strong>of</strong><br />

solubility for liquids in which the enthalpy limited the miscibility <strong>of</strong> polymers and solvents.<br />

24,25 For substances capable to form hydrogen bonds, Rider proposed a new factor relating<br />

miscibility with an enthalpy <strong>of</strong> mixing which depends on an enthalpy <strong>of</strong> the hydrogen<br />

bond formation. He has introduced the quantity <strong>of</strong> a hydrogen bond potential (HBP). If the<br />

quantity <strong>of</strong> HBP is positive it promotes miscibility and if it is negative it decreases miscibility.<br />

( )( )<br />

HBP = b −bC −C<br />

1 2 1 2 [4.1.20]<br />

where:<br />

b1,b2 donor parameters <strong>of</strong> solvent and solute, respectively<br />

C1,C2 acceptor parameters <strong>of</strong> solvent and solute, respectively<br />

For certain polymers Rider has drawn solubility maps. Thus the area <strong>of</strong> solubility was<br />

represented by a pair <strong>of</strong> symmetric quarters <strong>of</strong> a plane lying in coordinates b,C. 24 Values <strong>of</strong><br />

parameters were defined from data for enthalpies <strong>of</strong> hydrogen bonds available from the earlier<br />

works. The model is a logical development <strong>of</strong> the Hansen method. A shortcoming <strong>of</strong><br />

this model is in neglecting all other factors influencing solubility, namely dispersion and<br />

polar interactions, change <strong>of</strong> entropy, molecular mass <strong>of</strong> polymer and its phase condition.<br />

The model was developed as a three-dimensional dualistic model (see Section 4.1.5).<br />

4.1.4 HANSEN’S SOLUBILITY<br />

The Hansen approach 26-30 assumed that the cohesive energy can be divided into contributions<br />

<strong>of</strong> dispersion interactions, polar interactions, and hydrogen bonding.<br />

E = Ed + Ep + Eh<br />

[4.1.21]<br />

where:<br />

E total cohesive energy<br />

Ed,Ep,Eh contributions <strong>of</strong> dispersion forces, permanent dipole-permanent dipole forces, and<br />

hydrogen bonds.<br />

Dividing this equation by the molar volume <strong>of</strong> solvent, V1, gives:

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