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3.0
2.6
2.2
1.8
1.4
1.0
0.6 0
1000
2000
3000
PDMS M n
4000
5000
6000
Fig. 4 Experimental interfacial tension at 25 C between PDMS and PBD 1000 as a function of
the M n of PDMS. Solid line represents the best fit to a M n 1 dependence and the dotted line is the
fit for a M n 0.5 dependence [ 19 , 20 ]
with four poly(dimethyl siloxanes), PDMS, are shown in Fig. 3 as a function of
temperature. Interfacial tension decreases almost linearly with temperature with
temperature coefficients of 0.75
10 2 dyn/(cm C).
The effect of PDMS molecular weight on the interfacial tension at constant
temperature for a constant molecular weight of PBD ( M n ¼
2 to 1.2
10
1.07)
is illustrated in Fig. 4 . The molecular weight dependence was obtained by perfor-
ming nonlinear least-squares regression of the data to an expression of the form
g ¼ g 1 1
980, M w / M n ¼
. This analysis yielded z
0.54 for the present PDMS/PBD
system of the specific range of low molecular weights.
The interfacial tension data for blends of PS of various molecular weights versus
a poly(ethyl ethylene) (PBDH 4080; M n ¼
k int M z
¼
n
1.04) exhibited a similar
behavior with temperature, with temperature coefficients 0.9
4800, M w / M n ¼
10 2
dyn/(cm C), and, qualitatively, with molecular weight. However, fitting the data to
the expression g ¼ g 1
2 to 1.5
10
yielded z
k int M z
n
1
¼
0.68 for PS molecular weights
between 2200 and 10,200.
The measurements for the blends of PS and poly(methyl methacrylate) (PMMA;
M n ¼
10,000, M w / M n ¼
1.05) cover the broadest range of molecular weights
(Fig. 5 ). For
this
system, nonlinear fit of
the data to the expression
resulted in z
k int M z
g ¼ g 1 1
¼
0.90 for PS molecular weights between 2200
n
and 43,700.
These values for the exponent z should be taken with caution because of
experimental errors. However, it was pointed out [ 20 ] that the smallest value for z
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