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4.11 Thermodynamics of Equilibrium Polymerization
The effect of solvents on the equilibrium constants in anionic polymerization in solution has been
considered in thermodynamic terms [ 407 ].
Sawada [ 407 ] expressed the change in free energy for converting one mole of liquid monomer in
an anionic polymerization to one base-mole of an amorphous polymer,
DF 1c , as follows:
DF 1c ¼ DF m DF p
where,
DF m is the partial molar free energy of the monomer (per mole) in the equilibrium mixture,
relative to that of the pure liquid monomer, and DF p is the partial molar free energy of the polymer
(per base mole) in the equilibrium mixture, relative to that of the amorphous polymer.
Flory [ 409 ] described
DF m and
DF p in a three component system of polymer, monomer, and
solvent as follow:
DF m =RT ¼
ln
' m Þ' s ðX m =X p Þ' p ðX m =X p Þþðw ms ' s þ w ms ' p Þð' s þ ' p Þ
w sp ðX m =X p Þ' s ' p
' m þð
1
DF p =RT ¼
1
' p Þ' m ðX p =X m Þ' s ðX p =X m Þþðw pm ' m þ w ps ' s Þð' m þ ' s Þ
w ms ðX p =X m Þ' m ' s
=n½
ln
' p þð
1
where,
' i
is the volume fraction of component
i
,
X i
is the number of segments per molecule for
component
is the
free energy parameter between any two components. The subscripts m, s, and p indicate monomer,
solvent and polymer, respectively. Flory puts the ration of molar volume as,
i
,
n
is the degree of polymerization,
R
is the gas constant,
T
is the temperature, and
w
v i =v j ¼ X i =X j
assuming that
v p /
v m ¼ n
and expressing
w pm and
w ps in terms of molecular weight-independent
quantities
w mp and
w sp through the relationship:
w pm ¼ w mp ðV p =V m Þ¼V mp n
w ps ¼ w sp nðV m =V s Þ
The free energy of polymerization can then be written:,
DF 1c =RT ¼
' m þ
þðw ms ' s þ w ms ' p Þð' s þ ' p Þw sp ðV m =V s Þ' s ' p ð
=nÞ
' p
=n
ln
1
1
ln
1
ðw mp ' m þ w sp ' s V m =V s Þð' m þ ' s Þþw m ' m ' s
where,
' m is now the equilibrium volume fraction of monomer and the volume fraction of the
polymer is
' p .
Sawata points out [ 407 ] that by neglecting terms 1/
n
when
n
is large, and by replacing (
' s +
' p )by
(1
' m ) and (
' m +
' s )by(1
' p ) one gets a more general expression:
DF 1c =RT ¼
ln
' m þ
1
þ ' s ðw ms w sp V m =V s Þþw ms ð' p ' m Þ
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