Biomedical Engineering Reference
In-Depth Information
Glassy region
G
'
Cross-over
Plateau region
G
”
Terminal zone
slope = 2
log
ω
Figure 2.16
Mechanical spectrum of a polymer solution
-
viscoelastic liquid.
2.5.1.3
Frequency and strain dependence
Polymer solutions
The mechanical spectrum of a polymer solution (a viscoelastic liquid) has the general
form illustrated in
Figure 2.16
(Ross-Murphy,
1994
; Kavanagh and Ross-Murphy,
1998
).
At low frequencies (note the double log scale) G
00
is greater than G
0
, but as the oscillatory
frequency increase, G
0
increases more rapidly than G
00
log
representation, compared to a slope of 1 for G
00
), and at some frequency there is a cross-
over. After this, both G
0
and G
00
become much less frequency-dependent
(with a slope ~2 in the log
-
-
the so-called
'
region.
Whether the cross-over region is reached in the frequency window of conventional
oscillatory measurements depends upon polymer concentration, relative molecular mass
(M) and chain
rubbery plateau
'
flexibility. At the same time, the mechanical spectrum measured will be
essentially independent of the amount of shear strain, out to, say, 100% in
'
(i.e. a strain, in terms of the geometry of deformation, of unity). Rheologists may express
this by saying that the linear viscoelastic (LV) strain extends out to c.100%.
'
strain units
Polymer gels
The mechanical spectrum of a viscoelastic solid will have a
nite G
0
, with a value usually
50 times) that of G
00
at all frequencies, as in
Figure 2.17
(Clark and
Ross-Murphy,
1987
; te Nijenhuis,
1997
). In this respect it shows some similarities with
the plateau region of the solution mentioned above; such a plateau is often referred to,
somewhat imprecisely, as gel-like, for exactly this reason.
The strain-dependent behaviour, for polymer gels is more dif
well above (say 5
-
cult to generalize,
although the LV strain is rarely as great as 100% (some gelatin gels may be the exception
here), and may be extremely low
-
say 0.1% or less. At values just greater than the LV
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