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2008
DOI: 10.1007/s11831-008-9027-9
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Recirculating Flows Involving Short Fiber Suspensions: Numerical Difficulties and Efficient Advanced Micro-Macro Solvers

Abstract: is an open access repository that collects the work of Arts et Métiers ParisTech researchers and makes it freely available over the web where possible. SummaryNumerical modelling of non-Newtonian flows usually involves the coupling between equations of motion characterized by an elliptic character, and the fluid constitutive equation, which defines an advection problem linked to the fluid history. There are different numerical techniques to treat the hyperbolic advection equations. In non-recirculating flows,… Show more

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Cited by 48 publications
(41 citation statements)
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“…Thus, an approximate closure relation is needed in order to express the fourth-order moment A as a function of the lower-order moment a. Different closure relations have been introduced and widely used [2] [10] [19] [25]. In what follows we consider the hybrid closure relation, that constitutes a good compromise between implementation simplicity and solution accuracy.…”
Section: Revisiting Jeffery's Modelmentioning
confidence: 99%
“…Thus, an approximate closure relation is needed in order to express the fourth-order moment A as a function of the lower-order moment a. Different closure relations have been introduced and widely used [2] [10] [19] [25]. In what follows we consider the hybrid closure relation, that constitutes a good compromise between implementation simplicity and solution accuracy.…”
Section: Revisiting Jeffery's Modelmentioning
confidence: 99%
“…To determine F Nþ1 and G Nþ1 a non-linear problem has to be solved. An alternate directions strategy has given excellent results in our precedent studies (for example in [15]). This method is performed in two steps:…”
Section: Enriching the Approximation Basismentioning
confidence: 99%
“…Usually, the fourth order moment, A, is expressed from the second order one by considering any of the numerous closure relations proposed in the literature [31][32][33][34]. We do not address this issue here, and from now on, we consider that A = L(a), with L, an appropriate algebraic operator.…”
Section: Micro-mechanical Description Of the Kinematics Of Deformablementioning
confidence: 99%