Chemistry Reference
In-Depth Information
The Gibbs function of suprasegmental (cluster) structure self-assembly
at temperature
T
=
T
g
- D
T
was calculated as follows [45]:
,
(4.20)
i
G
D =D D
ST
where D
S
is entropy change in this process course, which can be estimated
as follows [47]:
D
S
= (3 ÷ 5)×
k
×
f
g
×ln
f
g.
(4.21)
In the Eq. (4.21), the coefficient (3 ÷ 5) takes into account conforma-
tional molecular changes contribution to D
S
,
k
is Boltzmann constant,
f
g
is a
polymer relative fluctuation free volume.
Let us consider now the results of the concept [44, 45] application to
polymers yielding process description. The yielding can be considered as
polymer structure loss of its stability in the mechanical stresses field and
the yield strain e
Y
is measure of this process resistance. In Ref. [44], it is
indicated that specific lifetime of suprasegmental structures
t
im
is connected
with
D
as follows:
im
(
)
-D
t
im
~ exp
G
im
RT
(4.22)
where
R
is the universal gas constant.
Assuming, that
t
im
~
t
Y
(
t
Y
is time, necessary for yield stress is
Y
achieve-
ment) and taking into account, that e
Y
~
t
Y
, it can be written [43]:
(
)
-D
im
e
~ exp
G
RT
(4.23)
Y
Let us note, that the Eq. (4.23) correctness in reference to polymers
means, that yielding process in them is controlled by supra segmental struc-
tures thermodynamical stability.
(
)
-D
, corresponding to
the Eq. (4.23), for all groups of the considered in Ref. [43] polymers. De-
spite definite (and expected) data scattering it is obvious, that all data break
down into two branches, the one of which is approximated by a straight line.
Such division reasons are quite obvious: the data with negative value of
im
im
exp
G
RT
D
cover one (right) branch and with positive ones − the other (left) one.
The last group consists of semicrystalline polymers with devitrificated at
testing temperature loosely packed matrix (polytetrafluoroethylene, polyeth-
ylenes, polypropylene). The cluster model [18, 24] postulates thermofluctua-
tion character of clusters formation and their decay at
T
>
T
g
. Therefore, such