Progress and Trends in Rheology V 1998
DOI: 10.1007/978-3-642-51062-5_41
|View full text |Cite
|
Sign up to set email alerts
|

The FENE-L and FENE-LS Closure Approximations for the Kinetic Theory of Finitely Extensible Dumbbells

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

1
45
0

Year Published

1999
1999
2018
2018

Publication Types

Select...
8

Relationship

1
7

Authors

Journals

citations
Cited by 18 publications
(46 citation statements)
references
References 2 publications
1
45
0
Order By: Relevance
“…For constitutive equations inspired by molecular models, one option is to describe the polymer population by the conformation tensor, A, defined as the ensemble average of the tensorial product of the individual end-to-end vectors, R , (often written A = 〈R R 〉) (Rallison & Hinch 1988). Higher order moments can be employed in more sophisticated representations (Lielens et al 1999;Ilg et al 2010). Figure 2: Bead-rod model for a polymer chain.…”
Section: General Approachmentioning
confidence: 99%
“…For constitutive equations inspired by molecular models, one option is to describe the polymer population by the conformation tensor, A, defined as the ensemble average of the tensorial product of the individual end-to-end vectors, R , (often written A = 〈R R 〉) (Rallison & Hinch 1988). Higher order moments can be employed in more sophisticated representations (Lielens et al 1999;Ilg et al 2010). Figure 2: Bead-rod model for a polymer chain.…”
Section: General Approachmentioning
confidence: 99%
“…Simulation of complex viscoelastic flows using bead-rod chain or bead-spring chain models with so many internal degrees of freedom is still not computationally feasible, and much recent work has been directed at developing simpler, closedform models that accurately capture or "coarse-grain" the macroscopic stressconformation hysteresis arising from molecular individualism on the microscale. The first models treated the additional stress arising from the strong local rate of deformation as explicitly viscous-like (see for example Rallison 1997, Verhoef et al 1998, whereas more recent models have attempted to capture the progressive changes in the average internal structure of the molecules during stretching and relaxation using additional scalar evolution equations (Lielens et al 1998, Lhuillier 2001. It remains to be seen which approach best describes kinematically complex "mixed" flows of polymer solutions containing regions of both strong elongation and shearing.…”
Section: Figure 14mentioning
confidence: 99%
“…Due to the very high computational cost of micro-macro simulations, another route which has been followed (see e.g. [14,16,22,32,33,35]) is to look for an approximate closure at the macroscopic level, namely a model of the form: 14) which is close to the microscopic model (1.7)-(1.8). Here M denotes an ensemble of macroscopic state variables that depend on time and space.…”
Section: Introductionmentioning
confidence: 99%