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The dependence tgd ( D ch ), obtained for the considered copolymers at two
measurement frequencies (1 and 10 kHz) is adduced i n Fig. 2.1 . This depen-
dence exists within the clearly determined limits. At D ch = 1.0 it tries to attain
tgd = 0, that was to be expected from the made above assumptions. At D ch =
2.0 the value tgd is approximately equal to its maximum value. Therefore,
the linear dependence tgd( D ch ) can be used for this parameter prediction in
different D ch ranges.
Similar linear dependences for SP - OPD with various C form were ob-
tained in Ref. [7] and they testify to molecular mobility level reduction at
d f decrease and extrapolate to various (nonintegral) d f values at D ch = 1.0.
The comparison of these data with the Eq. (1.5) appreciation shows, that
D ch reduction is due to local order level enhancement and the condition D ch
= 1.0 is realized at d f values, differing from 2.0 (as it was supposed earlier
in Ref. [23]). This is defined by polymers structure quasiequilibrium state
achievement, which can be described as follows [24]. Actually, tendency of
thermodynamically nonequilibrium solid body, which is a glassy polymer, to
equilibrium state is classified within the frameworks of cluster model as lo-
cal order level enhancement or j cl increase [24-26]. However, this tendency
is balanced by entropic essence straightening and tauting effect of polymeric
medium macromolecules, that makes impossible the condition j cl = 1.0 at-
tainment. At fully tauted macromolecular chains ( D ch = 1.0) j cl increase is
ceased and polymer structure achieves its quasiequilibrium state at d f vari-
ous values depending on copolymer type, that is defined by their macromol-
ecules different flexibility, characterized by parameter C .
Let us consider within the frameworks of irreversible aggregation mod-
el one more possible interpretation of polymers structure features - the so
called diffusion-limited aggregation (DLA) [27, 28].
According to the Ref. [29] for DLA the value d f ≈ 2.5. The spatial distri-
bution of DLA elements (in our case - statistical segments) can be character-
ized with the aid of two dimensions: d f and chemical dimension d l , which are
defined as follows:
,
(2.6)
d
N
~
r
f
,
(2.7)
d
N ~
l
l
where N is particles number in cluster between two arbitrary points of clus-
ter, r and l are distances between these points [30]. The value r is the piece
length, connecting these points and l is defined as the shortest way over
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