2012
DOI: 10.1021/ie300351j
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Gelation and Breakage Behavior of Model Wax–Oil Systems: Rheological Properties and Model Development

Abstract: Gelation and breakage of model wax−oil systems is investigated using microscopy, densitometry, rheometry, and XRD. Various model waxy oils are prepared, including 1 to 20 wt % (w/w) macrocrystalline wax in dodecane, 1 to 20 wt % microcrystalline wax in dodecane, and 5 wt % macrocrystalline wax in Primol 352. The influence of shear history, thermal history, and fluid composition is ascertained. A novel gel breakage model is introduced which spans the entire mechanical response of wax gels from initial Hookean b… Show more

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Cited by 58 publications
(69 citation statements)
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References 15 publications
(34 reference statements)
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“…To examine various values of the compressibility number, d ¼ 4310 23 and d ¼ 4310 25 are considered while the other parameters are fixed. The pressure profiles corresponding to these parameters are shown in Figure 12a and b.…”
Section: Effect Of Compressibilitymentioning
confidence: 99%
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“…To examine various values of the compressibility number, d ¼ 4310 23 and d ¼ 4310 25 are considered while the other parameters are fixed. The pressure profiles corresponding to these parameters are shown in Figure 12a and b.…”
Section: Effect Of Compressibilitymentioning
confidence: 99%
“…The gel state is assumed to follow a point function of absolute strain instead of time. [21][22][23] Hence, a strain-dependent apparent viscosity is established without a true yield stress. Gelled waxy crude oil may be classified as an irreversible thixotropic material with a known degradation and breakdown behavior.…”
Section: Introductionmentioning
confidence: 99%
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“…Creeping flow is defined by a corresponding high viscosity [6,[21][22][23][24]. In alternate approach, initial creep can be associated with elastic deformation [25]. However, in this study, initial creeping flow is accounted for by a high viscosity of the gel.…”
Section: Introductionmentioning
confidence: 97%
“…A viscosidade dos fluidos Newtonianos varia inversamente com a temperatura absoluta, apresentando um comportamento exponencial conforme a lei de Arrhenius (28).…”
Section: Figura 36: Geometria Couette Double Gapunclassified