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Handbook of Solvents - George Wypych - ChemTech - Ventech!

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

tribution to χ 1 stipulated by the difference in free volumes <strong>of</strong> polymer and solvent. Both<br />

terms <strong>of</strong> the equation are larger than zero, and as temperature increases the first term decreases<br />

and the second term increases. The expression can be given in a reduced form (with<br />

some additional substitutions): 12<br />

χ1 *<br />

V1<br />

~ 13<br />

13<br />

*<br />

P1<br />

V 1 X 12 V 1<br />

* 13<br />

RT1<br />

P1<br />

V 1 1 24<br />

/<br />

~ / *<br />

~ /<br />

⎛ ⎞<br />

=<br />

⎜ ⎟<br />

⎜ ⎟<br />

− ⎝ ⎠<br />

+<br />

⎡<br />

⎢<br />

⎢<br />

⎢<br />

⎛<br />

⎢<br />

⎜<br />

/ −V<br />

⎣⎢<br />

⎝<br />

~ / 13<br />

3 1<br />

⎞<br />

⎟<br />

⎠<br />

⎤<br />

⎥<br />

⎥<br />

⎥<br />

⎥<br />

⎦⎥<br />

2<br />

τ [4.2.6]<br />

where: ~<br />

* *<br />

V1, P1, T1reduced<br />

molar volume <strong>of</strong> solvent, pressure and temperature consequently<br />

X12 contact interaction parameter.<br />

These parameters can be calculated if factors <strong>of</strong> the volumetric expansion, isothermal<br />

compressibility, thermal capacity <strong>of</strong> a solvent and enthalpy <strong>of</strong> mixing <strong>of</strong> solution components<br />

are known.<br />

With temperature decreasing, the first term <strong>of</strong> the right side <strong>of</strong> the expression [4.2.6]<br />

increases and the second term decreases. Such behavior implies the presence <strong>of</strong> the upper<br />

and lower critical temperatures <strong>of</strong> mixing. Later Flory developed another expression for χ1 that includes the parameter <strong>of</strong> contact interactions, X12: 13,14<br />

χ<br />

1<br />

⎡<br />

=<br />

V RT ⎣<br />

* *<br />

2<br />

PV ⎛ 1 1 s ⎞ 2 X<br />

⎢<br />

12 ⎜<br />

⎟<br />

~ ⎟ *<br />

⎢<br />

1 ⎝s1<br />

⎠ P1<br />

*<br />

α1T<br />

⎛P<br />

⎞ 2<br />

+ ⎜<br />

2 ⎜ *<br />

⎝P1<br />

⎠<br />

⎟ −<br />

⎧⎪<br />

⎨ τ<br />

⎩⎪<br />

s<br />

s<br />

2<br />

1<br />

X<br />

P<br />

12<br />

*<br />

1<br />

⎫⎪<br />

⎬<br />

⎭⎪<br />

2<br />

⎤<br />

⎥<br />

⎥<br />

⎦<br />

[4.2.7]<br />

where:<br />

s1,s2 ratios <strong>of</strong> surfaces <strong>of</strong> molecules to their volumes obtained from structural data.<br />

The large amount <strong>of</strong> experimental data is then an essential advantage <strong>of</strong> the Flory’s<br />

theory. 9 Simple expressions exist for parameter X12 in the terms <strong>of</strong> Xij characteristic parameters<br />

for chemically different segments <strong>of</strong> molecules <strong>of</strong> components 1 and 2. Each segment<br />

or chemical group has an assigned value <strong>of</strong> characteristic length (αi, αj) or surface area as a<br />

fraction <strong>of</strong> the total surface <strong>of</strong> molecule: 15<br />

Χ12 = ∑ αi 1 −αi 2 α j 1 −α<br />

j 2 Χij<br />

[4.2.8]<br />

i, j<br />

Bondi’s approach may be used to obtain surface areas <strong>of</strong> different segments or chemical<br />

groups. 16 To some extent Huggins’ new theory 17-21 is similar to Flory’s theory.<br />

4.2.2 CHEMICAL STRUCTURE<br />

Chemical structure and the polarity determine dissolution <strong>of</strong> polymers. If the bonds in polymer<br />

and solvent are similar, then the energy <strong>of</strong> interaction between homogeneous and heterogeneous<br />

molecules is nearly identical which facilitates solubility <strong>of</strong> polymer. If the<br />

chemical structure <strong>of</strong> polymer and solvent molecule differ greatly in polarity, then swelling<br />

and dissolution does not happen. It is reflected in an empirical rule that “like dissolves like”.<br />

( , , )( , , )

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