Chemistry Reference
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A hc
A disp, PC-SAFT
A assoc
+
+
Fig. 2 Helmholtz energy contributions of PC SAFT
system (Fig. 2 ). The hard-chain system is obtained as in SAFT as the sum of the
hard-sphere and chain-formation contributions A hs and A chain . Since the dispersion
term A disp,PC-SAFT now describes the attraction of chain molecules rather than that
of nonbonded segments, it appears to be a function of chain length m :
A res
A hc
A disp ; PC SAFT
A assoc
¼
þ
ð
m
Þþ
(6)
Modeling with PC-SAFT (as well as with original SAFT and related models)
requires three pure-component parameters for a nonassociating molecule. As for the
above-mentioned van der Waals equation, these parameters have a physical mean-
ing. The first parameter of PC-SAFT is the segment diameter s (SAFT uses the
segment volume v 00 ), which corresponds to the van der Waals parameter b .
Parameter e is the energy related to the interaction of two segments, corresponding
to the van der Waals parameter a . The third parameter considers the deviation from
the spherical shape of the molecules: the segment number m . In the case of a
polymer molecule, the latter is proportional to the molecular weight. To describe a
binary system, again an additional binary parameter ( k ij ) is used to correct for
deviations of the geometric mean of the energy parameter.
According to ( 6 ), different expressions are used to describe the various con-
tributions within the PC-SAFT model. The hard-chain contribution reads as:
X
ln g ii d ii
A hc
NkT ¼
m A hs
NkT
x i m i
ð
1
Þ
(7)
i
"
#
3
2
3
2
A hs
NkT ¼
1
z 0
3 z 1 z 2
1
z
z
Þ þ
2 þ
3 z 0
ln 1
ð
z 3
Þ
(8)
ð
z 3
2
z
z 3 1
ð
z 3
Þ
X
m
¼
x i m i
(9)
i
6 r X
i
x i m i d i ;
z n ¼
z 3 ¼
(10)
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