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Linear viscoelastic properties of sucrose ester-stabilized oil-in-water emulsions

Abstract

This paper deals with the influence of composition [sucrose ester SE and oil O concentrations] and temperature on the linear viscoelasticity properties of highly concentrated oil-in-water emulsions, using a hydrophilic sucrose palmitate as emulsifier. Different oil-in-water emulsions were prepared using a sucrose palmitate (SE=1–5 wt %) with a hydrophilic–lipophilic balance of 15, sunflower oil (O=60–80 wt %) and water. Oscillatory measurements were carried out in the linear viscoelasticity region. The relaxation time spectra of the emulsions were calculated using regularization techniques and were fitted to an empirical model proposed by Reference 1996. The results obtained are explained on the basis of the relationship among linear viscoelasticity properties, droplet size distribution, and characteristics of the continuous phase. Thus, an increase in sucrose palmitate concentration produces higher values of the linear viscoelasticity functions and a broader plateau region in the relaxation time spectrum, which suggests a certain enhancement of the elastic network.

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Linear viscoelastic properties of sucrose ester-stabilized oil-in-water emulsions

Author: Guerrero Conejo, Antonio Francisco; Partal López, Pedro; Gallegos Montes, Críspulo
Publisher: American Institute of Physics
Year: 1998
DOI: 10.1122/1.550965
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RESEARCH ARTICLE | NOVEMBER 01 1998
Linea iscoelas ic p ope ies o suc ose es e -s abilized oil-
in-wa e emulsions
A. Gue e o; P. Pa al; C. Gallegos
Jou nal o Rheology 42, 1375–1388 (1998)
h ps://doi.o g/10.1122/1.550965
Rela ed Con en
S udy o geome ical and elec onic s uc u e o lan hanum doped PbTiO3 and PbZ TiO3: Fi s p inciples
calcula ion
AIP Con e ence P oceedings (No embe 2018)
Linea iscoelas ic beha io o comme cial and model mayonnaise
Jou nal o Rheology (Ap il 1992)
Rema ks on high ene gy muon collide
AIP Con e ence P oceedings (Augus 2000)
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Linea iscoelas ic p ope ies o suc ose es e -s abilized
oil-in-wa e emulsions
A. Gue e o
Depa amen o de Ingenie ı
´a Quı
´mica, Uni e sidad de Se illa, C/P. Ga cı
´a
Gonza
´lez s/n, 41012 Se illa, Spain
P. Pa ala) and C. Gallegos
Depa amen o de Ingenie ı
´a Quı
´mica, Uni e sidad de Huel a, Escuela
Poli e
´cnica Supe io , C a. de Palos de la F on e a s/n, 21819, Huel a, Spain
(Recei ed 22 Decembe 1997; inal e ision ecei ed 3 Augus 1998)
Synopsis
This pape deals wi h he in luence o composi ion @suc ose es e SE and oil O concen a ions#and
empe a u e on he linea iscoelas ici y p ope ies o highly concen a ed oil-in-wa e emulsions,
using a hyd ophilic suc ose palmi a e as emulsi ie . Di e en oil-in-wa e emulsions we e p epa ed
using a suc ose palmi a e (SE 51–5 w %) wi h a hyd ophilic–lipophilic balance o 15, sun lowe
oil (O 560–80 w %) and wa e . Oscilla o y measu emen s we e ca ied ou in he linea
iscoelas ici y egion. The elaxa ion ime spec a o he emulsions we e calcula ed using
egula iza ion echniques and we e i ed o an empi ical model p oposed by Madiedo ~1996!. The
esul s ob ained a e explained on he basis o he ela ionship among linea iscoelas ici y
p ope ies, d ople size dis ibu ion, and cha ac e is ics o he con inuous phase. Thus, an inc ease
in suc ose palmi a e concen a ion p oduces highe alues o he linea iscoelas ici y unc ions and
a b oade pla eau egion in he elaxa ion ime spec um, which sugges s a ce ain enhancemen o
he elas ic ne wo k. © 1998 The Socie y o Rheology. @S0148-6055~98!01206-1#
I. INTRODUCTION
Oil-in-wa e ~o/w!emulsions a e manu ac u ed by dispe sing he oil phase in o he
aqueous con inuous phase in he o m o small d ople s ~mos comme cial emulsions
ha e d ople sizes in he ange o 0.1–10
m
m!@Wals a ~1983!#. In o de o ob ain s able
emulsions wi h sui able d ople size dis ibu ions ~DSD!, he emulsi ica ion p ocess e-
qui es a conside able amoun o mechanical ene gy ~in he o de o 1–100 MJ/m3de-
pending on emulsi ica ion machine!@Wals a ~1993!#. I is wo h poin ing ou ha he
emulsi ica ion p ocess is a highly complex uni ope a ion which depends on many a i-
ables ~ empe a u e, esidence ime, agi a ion speed, e c.!@Gallegos and F anco ~1998!#.I
is in ol ed in many di e en indus ies o p oduce a wide a ie y o emulsions ~ ood-
s u s, cosme ics, pha maceu icals, pe ochemicals, ag ochemicals, e c.!@Walke ~1984!;
Yuki e al. ~1990!; Desai, 1990#, which may be o mula ed o co e a wide ange o
dispe se phase olume ac ions
om dilu e o highly concen a ed emulsions, wi h
app oaching a alue o 1.
a!Au ho o whom all co espondence should be add essed.
© 1998 by The Socie y o Rheology, Inc.
J. Rheol. 42~6!, No embe /Decembe 1998 13750148-6055/98/42~6!/1375/14/$20.00
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S abili y is a p ima y equi emen o he comme cial applica ion o emulsions. How-
e e , emulsions a e he modynamically uns able because o hei la ge in e acial a ea
and d ople s end o agg ega e spon aneously. An emulsion is conside ed s able when he
numbe , size dis ibu ion, and a angemen o d ople s do no unde go any disce nible
change o e he s o age ime scale.
An emulsi ie is ypically added o imp o e bo h he emulsi ica ion p ocess and he
emulsi ica ion s abili y. The emulsi ie molecules adso b a he oil–wa e in e ace and
educe he in e acial ension, he eby a o ing emulsi ica ion and o ming a p o ec i e
ba ie a ound he oil d ople s @Dickinson ~1994!#. This inc eases in e d ople in e ac ions
and p o ides enhanced s abili y agains coalescence. The ole o hese in e ac ions is
undamen al in highly concen a ed emulsions, in which e y close packing o d ople s is
ound and he con inuous phase consis s o a hin ilm sepa a ing adjacen d ople s. This
p oduces highly iscoelas ic esponses @O subo and P ud’homme ~1994!# and may lead o
he de elopmen o an ex ensi e loccula ion o d ople s o o m a weak gel-like pa icu-
la e ne wo k depending on he na u e and concen a ion o he emulsi ie @Dickinson
~1989!#. The ex ensi e loccula ion p ocess p o ides enhanced s abili y o he emulsion
since he c eaming a e is signi ican ly dec eased @F anco e al. ~1995a,b, 1997!#.
The iscoelas ic p ope ies o he emulsions depend on he s a e o loccula ion. Un-
loccula ed o weakly loccula ed emulsions show a c osso e poin be ween G8and G9,
which is ela ed o a cha ac e is ic elaxa ion ime o he onse o he e minal o low
egion. This elaxa ion ime inc eases sha ply wi h
because o he s onge in e ac ions
among d ople s @Tad os ~1993!#. Howe e , emulsions using a mix u e o suc ose es e
~SE!and egg yolk p o eins as emulsi ie s usually show ex ensi e loccula ion, depending
on he ene gy inpu and empe a u e du ing he emulsi ica ion p ocess, which has been
p e iously ela ed o he de elopmen o a pla eau egion in he elaxa ion ime spec um
@F anco e al. ~1995b, 1997!#. O he highly concen a ed emulsions s abilized only by
p o eins also show gel-like esponses (G8is much highe han G9, bo h a e almos
pa allel!wi h a wide pla eau egion @Gue e o and Ball ~1994!; Gallegos e al. ~1992!#.
In a p e ious pape , he abili y o a highly hyd ophilic ~hyd ophilic–lipophilic bal-
ance, HLB 515) suc ose palmi a e, used as he only emulsi ie , o o m highly s able
emulsions was es ablished @Pa al e al. ~1994!#. The low beha io and d ople size o
o/w emulsions s abilized by his suc ose palmi a e has also been s udied @Pa al e al.
~1997!#. An e olu ion owa ds smalle sizes and na owe dis ibu ions was obse ed as
suc ose palmi a e and oil concen a ions we e aised, which led o an inc ease in he
emulsion iscosi y.
The objec i e o he p esen pape is o s udy he in luence o composi ion ~suc ose
palmi a e and oil concen a ions!and empe a u e on he linea iscoelas ici y p ope ies
o highly concen a ed o/w emulsions using a hyd ophilic suc ose palmi a e as an emul-
si ie . The ela ionship among he linea iscoelas ici y unc ions, d ople size dis ibu-
ion, and s abili y is also analyzed.
II. EXPERIMENT
Di e en oil-in-wa e emulsions we e p epa ed using a Ryo o suc ose palmi a e ~P-
1570, HLB 515) om he Mi subishi–Kasei Food Co po a ion ~Tokyo, Japan!. This
emulsi ie was used as ecei ed. Sun lowe oil was pu chased in a local s o e. Oil-in-
wa e emulsions we e p epa ed using an Ul a-Tu ax T-50 homogeneize . Sun lowe oil
was added o a solu ion o he emulsi ie in dis illed wa e a 55 °C, and mixed a a speed
o 5000 pm o 3.5 min. The suc ose palmi a e concen a ion ~SE! anged om 1% o
1376 GUERRERO, PARTAL, AND GALLEGOS
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5% ~w !and he oil con en ~O! om 60% o 80% ~w !(
50.59–0.77). Emulsions
we e s o ed a 5 °C.
Oscilla o y shea measu emen s we e pe o med in a Haake RS100 RheoS ess he-
ome e , using a cone-and-pla e senso sys em C35/4 ~4°, 35 mm!. The s ess ange o
linea iscoelas ici y was de e mined h ough a dynamic s ess sweep a a ixed equency
~6.28 ad/s!. All samples had he same ecen pas he mal and heological his o y. Rheo-
logical es s we e ca ied ou in he ange o 5–35 °C.
The elaxa ion ime spec um o each emulsion a each empe a u e was calcula ed by
using a comme cial so wa e p og am ~RHEOSPEC!, which is based on egula iza ion
echniques.
III. RESULTS AND DISCUSSION
A. In luence o suc ose palmi a e concen a ion
The e olu ion o he s o age and loss moduli wi h equency as a unc ion o he
suc ose palmi a e concen a ion is shown in Figs. 1~a!and 1~b!. Bo h moduli show a
con inuous inc ease wi h emulsi ie concen a ion. The s o age modulus G8is always
highe han he loss modulus G9wi hin he expe imen al equency ange. Hence, he
emulsions p esen a p edominan ly elas ic esponse, al hough a c osso e poin ends o
appea in he low- equency egime. Mo eo e , he e is a endency o G8 o exhibi a
pla eau egion @Fig. 1~a!#. This zone, a in e media e equencies, is known as he pla eau
egion and may be ela ed o he o ma ion o an elas ic s uc u al ne wo k due o in e -
ac ions among he emulsi ie molecules loca ed a he oil–wa e in e ace o adjacen
d ople s @Dickinson ~1989!; F anco e al. ~1995b!#. This beha io is ypical o highly
concen a ed emulsions such as comme cial o model mayonnaises @Gallegos e al.
~1992!; Gue e o and Ball ~1994!# and salad d essings @Mun
˜oz and She man ~1992!;
F anco e al. ~1995b!#. The pla eau egion has been ex ensi ely desc ibed in polyme
heology in e ms o an en anglemen ne wo k among polyme chains in which he
FIG. 1. In luence o suc ose palmi a e @~a!,~b!# on he s o age and loss moduli; and no malized linea iscoelas-
ici y unc ions o suc ose palmi a e-s abilized emulsions ~c!(T525°C).
1377OIL-IN-WATER EMULSIONS
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mo ion o molecules is cons ained by he neighbo ing molecules @Fe y ~1980!;Wu
~1989!#. When he emulsion is s abilized by p o eins @Gallegos e al. ~1992!; Gue e o
and Ball ~1994!#, he h ee-dimensional ne wo k is a o ed by en anglemen s among
p o ein segmen s adso bed a he oil–wa e in e ace. The same beha io was epo ed
when a suc ose s ea a e was used in combina ion wi h egg yolk @F anco e al. ~1995b!#.
Taking in o accoun ha he emulsions s udied a e s abilized exclusi ely by a low
molecula weigh su ac an ~suc ose palmi a e!and ha e high alues o dispe se phase
olume ac ion ~oil d ople s!, he pla eau egion was a ibu ed o an ex ensi e loc-
cula ion p ocess ha a o s emulsion s abili y by o ming a gel-like pa icula e ne -
wo k @Dickinson ~1989!# due o in e d ople in e ac ions. Simila e ec s we e epo ed
by Ebe e al. ~1988! o highly concen a ed emulsions s abilized by a
ce yl ime hylamonium-b omide su ac an .
In he pla eau egion, he loss angen passes h ough a minimum, which has been used
o calcula e an app oxima e alue o he pla eau modulus, GN
0@Wu ~1989!; A end e al.
~1994!; F anco e al. ~1995b!#. The pla eau modulus is a iscoelas ic pa ame e , de ined
as an ex apola ion o he en anglemen con ibu ion o G8o G9a high equency
@Baumgae el e al. ~1992!#. This pa ame e may be app oxima ed om he minimum in
an
d
as ollows @Wu ~1989!#:
GN
05@G8# an
d
→minimum.~1!
As a esul , he pla eau modulus GN
0unde goes an exponen ial inc ease when suc ose
palmi a e concen a ion is aised @Fig. 2~a!#, as co esponds o a mo e s uc u ed sys em.
The e olu ion o G8and G9, and also o he o he iscoelas ic unc ions wi h e-
quency ~i.e., loss angen !, is a he simila up o 3% suc ose palmi a e. This simila i y
allows one o supe pose all he iscoelas ic unc ions ~be ween 1% and 3% suc ose
palmi a e!by using he pla eau modulus as a no maliza ion ac o @Fig. 1~c!#. Howe e ,
he no maliza ion p ocedu e ails a he highes concen a ions o he emulsi ie ~4% and
5%!, because an inc ease in loss angen was obse ed om 3% o 5%.
As has been p e iously epo ed @Pa al e al. ~1997!#, an inc ease in SE concen a ion
p oduces a dec ease in d ople size and polydispe si y, which leads o an inc ease in he
speci ic in e acial a ea a@Fig. 2~b!#. Assuming sphe ical d ople s, ‘‘a’’ is ela ed o he
Sau e mean diame e as ollows:
a56/ds ,ds 5
(nidi
3
(nidi
2,~2!
whe e niis he numbe o d ople s ha ing diame e di.
Howe e , he e is a c i ical concen a ion ~3% SE!abo e which he slope o his
inc ease is lowe . To unde s and his change, he p ope ies o he con inuous phase used
o he p epa a ion o he emulsions should also be aken in o conside a ion. Thus, he
emulsions con aining 70% oil and 1%–3% SE we e p epa ed om a con inuous phase
con aining 3%–10% SE, which we e iso opic micella solu ions (L1) a he empe a u e
o emulsi ica ion ~50 °C!, as may be seen in he phase diag am shown in a p e ious pape
@Calaho o e al. ~1992!#. A concen a ions highe han 10% ~as co esponds o emul-
sions con aining 4% and 5% SE! he ini ial con inuous phase was always a dilu e dispe -
sion o lamella liquid-c ys alline (L
a
) po ions in an iso opic micella ma ix, a he
emulsi ica ion empe a u e ~50 °C!. The e o e, he abo e-men ioned c i ical concen a ion
co esponds o he ansi ion om L1micella solu ion o he L11L
a
dispe sion. As a
esul , a ema kable inc ease in he low-shea limi ing iscosi y
h
oc is obse ed o he
su ac an –wa e sys em @Fig. 2~c!#. This inc ease seems o impai he emulsi ica ion
p ocess, leading o a lowe inc ease in he in e acial a ea @Fig. 2~b!#.
1378 GUERRERO, PARTAL, AND GALLEGOS
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On he o he hand, he excess o su ac an o e he amoun necessa y o sa u a e he
in e ace as a monolaye (
e
SE) con inuously inc eases wi h SE concen a ion @Fig. 2~b!#.
The excess o su ac an has been calcula ed as ollows:
e
SE 5
~C
/a
!
Csa
21, ~3!
whe e Cis he suc ose palmi a e concen a ion,
is he emulsion densi y, ‘‘a’’ is he
speci ic in e acial a ea,
is he dispe se phase olume ac ion ~oil d ople s!, and Csa is
he concen a ion necessa y o sa u a e he in e ace as a monolaye . Taking in o accoun
he su ace p essu e-a ea iso he m ob ained by Ab an e al. ~1988! o he suc ose palmi-
a e, he Csa alue was es ima ed as 0.36531026g/cm2@Pa al e al. ~1997!#.
Once he emulsi ica ion p ocess is o e , he con inuous phase o hese highly concen-
a ed emulsions consis s o a e y hin ilm sepa a ing adjacen d ople s. The consis ency
o his ilm, a o ed by he inc ease in
e
SE, as well as he inc ease in he speci ic su ace
a ea, explain he la ge alues o he iscoelas ic unc ions and he exponen ial ise in he
pla eau modulus shown in Fig. 2~a!.
Figu e 3 shows he elaxa ion ime spec um o selec ed emulsions ob ained by means
o he Tikhono egula iza ion p ocedu e using he RHEOSPEC so wa e. As may be ob-
se ed in Fig. 1, he ecalcula ion o he iscoelas ic unc ions om he elaxa ion ime
spec um ob ained by he egula iza ion echnique ~RHEOSPEC so wa e!is e y accu a e.
FIG. 2. ~a!In luence o suc ose palmi a e concen a ion on he pla eau modulus; ~b!excess o su ac an o e
he amoun necessa y o sa u a e he in e ace as a monolaye and speci ic in e acial a ea as a unc ion o
suc ose palmi a e concen a ion; ~c! iscosi y o he ini ial su ac an -con aining solu ion ~SCS!a which oil is
added ~please no e ha he concen a ion o his solu ion is SCS 5SE33.3) a 50 °C.
1379OIL-IN-WATER EMULSIONS
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To exp ess quali a i ely he elaxa ion da a, De Rosa and Win e ~1994!p oposed an
empi ical model, de i ed om he Baumgae el–Schausbe ge –Win e ~BSW!spec um
@Baumgae el e al. ~1992!#, and he Chambon–Win e ~CW!spec um @Chambon and
Win e ~1985!#. Al hough his model was p oposed o desc ibe he elaxa ion p ocess o
polyme mel s, i has been also used o emulsions as salad d essings @F anco e al.
~1995b!#. This model equi es wo unc ions o desc ibe he ansi ion, pla eau, and e -
minal egions o he elaxa ion ime spec um. A simple empi ical equa ion, which com-
p ises he h ee egions o he spec um, has ecen ly been p oposed by Madiedo ~1996!
and Madiedo and Gallegos ~1997!:
H~l!5
a
lm1
b
ln
11~l/l !p,~4!
whe e m,nand (n–p) a e he slopes o he ansi ion, pla eau, and pseudo e minal zones,
espec i ely; and l is a cha ac e is ic elaxa ion ime ela ed o he bounda y o he
pla eau egion. Since he c osso e equency was no eached o he emulsions s udied,
l will be conside ed a i ing pa ame e in his pape . As may be no ed, hese pa ame e s
a e ela i ely simila o he pa ame e s o he BSW–CW model @Madiedo and Gallegos
~1997!#. Pa ame e s
a
and
b
ha e he ollowing exp essions:
a
5mH0
~m2n!l0
m,~5!
b
5nH0
l0
n~n2m!,~6!
whe e l0is a cha ac e is ic elaxa ion ime ela ed o he onse o he pla eau egion and
H0is he alue o he spec um co esponding o his elaxa ion ime. I he slope o he
pla eau egion is posi i e, n.0, Eq. ~4!p edic s a maximum alue o H(l) o a
elaxa ion ime lmax 5l @n/(n2p)#1/p, which was ela ed by De Rosa and Win e ~1994!
FIG. 3. In luence o suc ose palmi a e concen a ion on he elaxa ion ime spec a o suc ose palmi a e-
s abilized emulsions (T525°C).
1380 GUERRERO, PARTAL, AND GALLEGOS
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wi h he elaxa ion ime a which H(l) equals GN
0 imes n. Howe e , his maximum does
no always appea . Consequen ly, he elaxa ion ime spec um calcula ed om he egu-
la iza ion me hod o each emulsion was analyzed acco ding o he Madiedo and Gal-
legos ~1997!model @Eq. ~4!#.
The elaxa ion ime spec a calcula ed om he Tikhono egula iza ion me hod, o
each suc ose palmi a e concen a ion, a e shown in Fig. 3. As may be seen, he abo e-
men ioned model sa is ac o ily desc ibes he elaxa ion ime spec a ob ained o hese
emulsions. The shape o he spec um is always simila . A pla eau egion is always
clea ly obse ed. Likewise, a egion cha ac e ized by a end o each he e minal zone
o low egion may be no ed. The inc ease in emulsi ie concen a ion p oduces an in-
c ease in he elaxa ion ime spec um highe han one o de o magni ude, which is
app oxima ely he same inc ease unde gone by GN
0and indica es ha an enhancemen o
he elas ic ne wo k is p oduced.
Howe e , Table I shows a maximum alue in l ollowed by a dec ease, which
co esponds o a displacemen o he pla eau egion owa ds a sho e elaxa ion ime o
highe equency. This displacemen has also been ound o salad d essing emulsions
s abilized by p o eins and suc ose es e @F anco e al. ~1997!#. The slope o he pla eau
egion does no change wi h SE concen a ion showing alues close o ze o. The only
excep ion was he emulsion con aining 5% SE, which shows a posi i e alue o n,
indica i e o a highe deg ee o s uc u e. A signi ican inc ease in he s abili y o hese
emulsions was also ound as SE became highe @Pa al e al. ~1994!#.
B. In luence o oil concen a ion
The e olu ion o he s o age and loss moduli wi h equency is simila o all he oil
concen a ions s udied, G8always being highe han G9@Figs. 4~a!and 4~b!#. Thus, he
loss angen is oughly independen o he oil concen a ion. As a esul , he pla eau
modulus @which is shown in Fig. 5~a!# was success ully used o no malize bo h s o age
and loss moduli as a unc ion o equency (a
8
), leading o a mas e cu e o each o
hem @Fig. 4~c!#. Howe e , some sca e may be obse ed in G9a high equencies @Fig.
4~c!#. An empi ical ho izon al shi ac o , (a
850.4) was necessa y o he smalles oil
concen a ion because o a equency displacemen o he pla eau egion as was p e i-
ously ound o salad d essing emulsions @F anco e al. ~1997!#.
Figu e 5~a!shows he alues o pa ame e GN
0as a unc ion o he dispe se phase
olume ac ion. An inc ease in his pa ame e , wi h a end o each an almos cons an
TABLE I. In luence o concen a ion on bo h he pseudo e minal elax-
a ion ime (l ) and slope o he pla eau egion ~n!, o suc ose palmi a e-
s abilized emulsions.
%SE %O nl
~s!
1% 70% 0.017 59
2% 70% 20.006 80
3% 70% 20.013 84
4% 70% 20.025 66
5% 70% 0.045 18
3% 60% 0.003 28
3% 65% 20.035 93
3% 75% 0.004 62
3% 80% 20.002 144
1381OIL-IN-WATER EMULSIONS
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alue abo e 70% (
50.68), was obse ed. Simila ly, he iscoelas ic moduli inc ease
wi h oil concen a ion bu only up o a ce ain alue which depends on equency. Thus,
a low equencies, he emulsion con aining 80% oil has he highes alues o G8and G9
@Figs. 4~a!and 4~b!#, while a in e media e and high equencies he e a e no di e ences
in G8 om 70% o 80% and he highes alues o G9co espond o 70% oil. This
FIG. 4. In luence o oil concen a ion @~a!,~b!# on he s o age and loss moduli; and no malized linea iscoelas-
ici y unc ions o suc ose palmi a e-s abilized emulsions ~c!(T525°C).
FIG. 5. ~a!In luence o dispe se phase olume ac ion ~oil!on he pla eau modulus; ~b!excess o su ac an
o e he amoun necessa y o sa u a e he in e ace as a monolaye and speci ic in e acial a ea as a unc ion o
dispe se phase olume ac ion.
1382 GUERRERO, PARTAL, AND GALLEGOS
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