Biomedical Engineering Reference
In-Depth Information
M
w
=
3
.0 × 10
4
M
w
/
M
n
< 1.05
0
One-phase solution
(i)
One-phase
gel
Two-phase solution
(iii)
(ii)
−
10
Two-phase gel
(iv)
−
20
0
10 0
Concentration (g L
−
1
)
200
300
Phase diagram of a narrowM
w
distribution aPS in nitropropane. Adapted with permission from Tan
et al.(
1983
) © 1983 American Chemical Society.
Figure 8.10
High-sensitivity calorimetric measurements were carried out to evaluate the heat
associated with the sol
gel transition. A transition was detected with DSC cooling
scans, corresponding to the same temperature as T
gel
measured by the tilted test tube
method. From the exotherm associated with this transition, a
-
'
heat of gelation
'
of the
2Jg
−
1
was calculated, which is a very low value, probably undetectable by
earlier authors. The phase diagrams (
Figures 8.9
and
8.10
) for aPS indicate that gelation
occurs as a distinct transition and that the phenomenon is not caused by phase separation.
In this case, gelation behaviour is determined by polymer
order of 1
-
solvent interactions, but does
not correlate in a simple way with the binodal curve. Gel formation does not appear to
correlate with the glass transition of the highly plasticized polymer either, as was the case
for aPS-TD. The critical gelation concentration (in our notation, c
0
) is strongly dependent
on M
w
. The authors also conclude that chain overlap is a necessary condition for gel
formation; since the
-
is so small, this may be reasonable.
The gelation behaviour of the polydisperse aPS-CS
2
system was compared with two
narrow M
w
distribution samples, one of a similar M
w
and the other of a similar M
n
.The
narrow fraction with similar M
w
exhibits a sol
'
heat of gelation
'
gel transition at higher temperature and
has a lower c
0
than the polydisperse system. On the other hand, the polymer with
similar M
n
shows very comparable gelation behaviour, i.e. almost identical sol
-
gel
transition temperature and c
0
.Presumablythelow-M
w
tail of the polydisperse poly-
mers remained in solution at the sol
-
-
gel transition and hence did not in
uence the
gelation behaviour.
In order to further clarify the mechanisms of gelation of aPS in CS
2
, Yanxiang and
Deyan (
1997
) investigated solutions by IR spectroscopy. They examined the possibility
of a conformational change in the polymer inducing gelation, and made some interesting
observations. In the IR spectra of aPS, the spectral region 500
600 cm
−
1
has been found
-
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