dc.description.abstract |
In the first stage of the
investigation,
the effect of high levels of sugars (mixture of 50%
sucrose with 351/'o
glucose syrup) on agarose (0.7 w-L °'o) was characterized by low amplitude
oscillatory measurements of storage modulus (G'), loss modulus (G") and loss tangent (tan 6"
as well as large deformation techniques. Samples were prepared at 90°:, and measured
immediately, or after Storage
at 5°C. The combined Williams-T andel-Ferry W F; /free
volume theory was used to derive the glass transition temperature, the fractional free volume,
and the thermal expansion coefficierit of the
glass. Solution of high
concentrations of sucrose
Crystallizes,
but
addition of the polymer encourages Bitei- olecular interactions, which
transfoý the mixture into a high v iscosi Ly glass. The mechanical properties of glucose syrup
follow
ýýý. iý behavior in the glass transition region and revert to an Arrhenius type prediction
in the CrIa-SSy State. feasurements on sugar Samples
and aýarose-Sugar ii 1x üres were resolved
into a
bas iiriCuuu Gi temperature alone and a
basic
function
of
equency
(time)
alone.
T ie
former traces the energetic cost of vitrification, which increases sharply with decreasing
tempera ure. The layer, at long time scales, is goes erned by the mtinite
molecular weight of the
äcräiGSZ ne ork. In the region of S1 O1 tImes, tie effect of Ze vole ie
is
active rega
dless
of
In a continuation of, investigating
the significance of polymer-cosolute interactions,
the effect
Gi sucrose, glucose, fructose, sorbitol, hylitol, glycerol and ethan-1,2-dial on gelation of high
methoxy pectin was studied under different experimental conditions. The main changes in
procedure in comparison with the work on agarose were: (i) the polymer concentration was
increased from 0.7 to 1.0 wt °'o, (ii) the mixtures prepared at pH AT and subsequently acidified
to pH 3, rather
than
beinte
prepared at neutral pH, (i11) the cosolute concentration was varying
from 50 to 65 w IL °'o and (vi) the mixtures were studied through rheology, calorimetry and
optical rotation. The samples were prepared at 95°C and changes in storage modulus (G') and
loss modulus
(G") during cooling to 5°C, heating to 900
and re-cooling to 5°C, at 1°C/min,
were measured at 1 rad s"1 and 0.5% strain. In all cases, the onset temperature for gelation
during cooling and
the moduli recorded at
5'C
increased With increasing concentration of
cosolute. However, both
values were substantially lower for the liquid cosolutes than for
mixtures with solid cosolutes at the same concentrations. The difference is attributed to
inhibition of pectin-pectin interactions by pectin-cosolute interactions, which in turn are
inhibited by cosolute-cosolute
interactions. On heating there was an initial reduction in
modulus, with the
same temperature-course as
the
increase on cooling; for the solids, this was
followed by an increase
attributable to hydrophobic association of methyl ester substituents.
No SUCH increase was
seen with
the liquid
cosolutes, but DSC
studies showed
two reversible
I.
thermal
ti ansitions in
all cases,
one over the
temperature-range of
the initial
gelation
process
ý
nfý r
'A
f+
.ýýn
on cooling and t
he
oLlleICoincidenf t with the increase in modulus ulon
hea ing
in the presence o1- ý
solid COSO1UteS.
The
absence
of any detectable
increase in modulus on
heating
with
the liquid
COSOtUteS is a
trlbuted
to accumulation of cosolute around tiie polymer chains promoting
hydrophobic association between
methyl ester groups on the same Chain; Or within Cl sters o
chains, v with, therefore no contribution to network
strucLarz. At
high
concentrations of the solid
cosolutes,
the
increase in
modulus
on heating was
followed
by a decrease at
higher
ýempei atur e; this -was attributed to excessive aggregation, and was reflected in
lower
moduli
on subsequent re-coolIný to 5'C, in
coast to the
enhancement in
gel strength
after heating
aril cooling observed at lower
concentration of
the same COSül teS.
in the presence of fructose as
cosolute, calorimetric studies showed an intense endotherm
follovýied immediately by
an intense exotherm on
hea
ng. These transitions occurred over
approximately the same
teMperat'ure-rande
as initial gelation on cooling and
increased in
mag liLude
with
increasing
concentration of the sugar. The displacement of both transitions to
progressively hid her temperature as the rate of heating was increased was much Greater than
anticipated from a simple thermal lag, indicating that the undelying structural chancres are
slow. The proposed interpretation is that fructose is capable of site-binding to pectin in both
the ordered and disordered state |
en_UK |