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a
b
0.6
0.6
0.4
0.4
0.2
0.2
0.0
0.0
0
1
2
3
4
0
1
2
3
4
G / G
C
G / G
C
Fig. 16 Smeared criticality in LCEs from the point of view of the distribution function
w
G
(
G
)of
the internal mechanical field
G
. The depicted distributions are calculated for
hGi¼
0.8
G
C
and
s
G
¼
0.8
G
C
corresponding to an effectively supercritical LCE (b). The extent of the below-critical
component (
G < G
C
) of each LCE is given by the surface of the
shaded area
0.8
G
C
corresponding to an effectively subcritical LCE (a) and for
hGi¼
2.0
G
C
and
s
G
¼
5 Tailoring the Thermomechanical Response of LCEs
by Influencing the Critical Behaviour
In the previous sections, the basic principles of the PN-N transition in LCEs and the
experimental techniques were introduced to the reader. The issue of a “smeared
mental results providing an insight for the understanding of the PN-N transition are
presented. These data were obtained by deuteron NMR and ac calorimetry on side-
chain and main-chain LCEs. The distinct role of each parameter that affects the
critical behaviour of the PN-N phase transition of LCEs will be demonstrated in
different subsections. These parameters influence the relative strength of the
locked-in mechanical field
G
and, as demonstrated in the previous sections, they
may alter the order of the PN-N transition.
5.1
Impact of Chemical Composition: Crosslinking Density
The idea that the critical behaviour of LCEs may be influenced by varying the
geometry and density of the crosslinkers was introduced in an early theoretical
gradual (more supercritical-like) thermoelastic response and birefringence temper-
systematic and dedicated experimental investigation, by means of
2
H-NMR and
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