2004
DOI: 10.1039/b316621j
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Structural changes in CTAB/H2O mixtures using a rheological approach

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Cited by 80 publications
(79 citation statements)
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References 32 publications
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“…However, three different theories were needed: the cooperative flow model from Bohlin, 35 the soft glass rheology (SGR) model for soft materials, 36,37 and the slip plane theory for cubic phases. 38 These models have been used previously in several studies regarding the rheology of cubic and hexagonal phases and based gel emulsions 4,17,39 and for gels formed with different surfactants, 40,41 so they seemed appropriate to be used in the present system. 35 to explain the flow character and microstructure of a flowing substance by means of rheological data.…”
Section: Modeling the Viscoelastic Parametersmentioning
confidence: 99%
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“…However, three different theories were needed: the cooperative flow model from Bohlin, 35 the soft glass rheology (SGR) model for soft materials, 36,37 and the slip plane theory for cubic phases. 38 These models have been used previously in several studies regarding the rheology of cubic and hexagonal phases and based gel emulsions 4,17,39 and for gels formed with different surfactants, 40,41 so they seemed appropriate to be used in the present system. 35 to explain the flow character and microstructure of a flowing substance by means of rheological data.…”
Section: Modeling the Viscoelastic Parametersmentioning
confidence: 99%
“…The values for the normal hexagonal phase (H 1 ) vary considerably from ~3, to 9.5, in different systems. 15,17,40 The values for H 2 are reported 17 as ~ 6.7. The main cause of this mismatch could be that in all of the systems studied there was no crossover between G' and G'', since the samples were gel-type.…”
Section: Theory Of Cooperative Flow This Theory Was Presented By Bohlinmentioning
confidence: 99%
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“…Starch when heated in the presence of excess water undergoes gelatinization which involves granule swelling, amylose leaching and amylopectin fusion and upon cooling due to retrogradation, solubilized starch forms a viscous dispersion or paste or gel depending on the temperature of processing and concentration of dispersion, varieties, harvesting age and growth season Asaoka et al , 1992Defloor et al 1998;Lagarigue and Alvarez 2001;Moorthy 2001;Fourmann et al 2003). The viscoelastic behavior of starchy food systems is characterized by dynamic rheological tests and can be evaluated by Maxwell and power law models (Montalvo et al 1996;Steffe 1996;Subramanian and Gunasekharan 1997;Cortes et al 1999;Rao 1999;Ak and Gunesekharan 2001;Acharya et al 2004;Cuppola et al 2004;Ortega-Ojeda et al 2004a, b, 2005Nishinari 2007). Reports on the application of these models to quantify the viscoelastic behavior of gelated cassava starch dispersion are scanty.…”
Section: Introductionmentioning
confidence: 99%
“…The dependence of these quantities on the oscillating frequency gives rise to the socalled mechanical spectrum, allowing the quantitative rheological characterization of studied materials. Weak gel model was applied to some of the oscillatory spectra [34,35]:…”
Section: Methodsmentioning
confidence: 99%