2019
DOI: 10.1016/j.jnnfm.2019.03.003
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DNS and LST stability analysis of Oldroyd-B fluid in a flow between two parallel plates

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Cited by 18 publications
(15 citation statements)
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“…A similar non-monotonic behaviour of with has been obtained for elasto-inertial wall mode instabilities in plane Poiseuille flow of Oldroyd-B (Sadanandan & Sureshkumar 2002; Brandi et al. 2019) and FENE-P (Zhang et al. 2013) fluids.…”
Section: Neutral Stability Curvessupporting
confidence: 69%
See 1 more Smart Citation
“…A similar non-monotonic behaviour of with has been obtained for elasto-inertial wall mode instabilities in plane Poiseuille flow of Oldroyd-B (Sadanandan & Sureshkumar 2002; Brandi et al. 2019) and FENE-P (Zhang et al. 2013) fluids.…”
Section: Neutral Stability Curvessupporting
confidence: 69%
“…(2013) using the FENE-P model which, like the FENE-CR model, accounts for the finite extensibility of polymer chains. The recent effort of Brandi, Mendonça & Souza (2019) also explored the role of elasticity on the TS (wall) mode using the Oldroyd-B model, focusing on smaller range of (). Both linear stability analysis (using a shooting procedure) and direct numerical simulations (DNS) were used to analyse the unstable flow structures corresponding to the wall mode, and good agreement was found between the two.…”
Section: Introductionmentioning
confidence: 99%
“…A fim de simplificar o problema e eliminar o tratamento da pressão na equação do momento, utiliza-se a formulação vorticidade-velocidade [2]. A vorticidade ω z , em coordenadas bidimensionais, é matematicamente definida como…”
Section: Formulação Raiz Quadrada-conformaçãounclassified
“…Este trabalho, em particular, dedica-se à investigação da estabilidade hidrodinâmica do escoamento [2], com o objetivo de prever mudanças que ocorram no regime de escoamento laminar de um fluido levando-o potencialmente ao regime turbulento. Este processo é conhecido como transição laminar-turbulenta, e ainda não é completamente estabelecido, principalmente para escoamentos não-Newtonianos.…”
Section: Introductionunclassified
“…This rich phenomenology can also be interpreted as an explanation of the well-known shear-thinning effect through the following sequence of comprehensive arguments. (1) The strain rate of the flow stretches the polymers in the axial direction, a phenomenon also known from earlier literature; (2) Such an extension causes contraction in the radial direction, due to the resistance to elongation exerted by restoring force between the ends of the polymer molecules; (3) This triggers a nonzero negative correlation between the x−component and r−component of the end-to-end polymer vector, resulting in an elastic shear stress (τ 12 ) to develop; (4) Since there is no strain rate at the pipe center, this correlation is zero due to the liberty of the ends of the polymers to be at random motion; (5) Due the increase of the elastic modulus with respect to r, a feature of the FENE-P model, the stretching rate with respect to r slows down, giving rise to convexity of C 11 (i.e., C 11rr < 0), which in turn causes concavity in τ 12 ; (6) The points in (3), (4) and (5) imply that the divergence of elastic shearstress, i.e, the resistive force contribution to the flow by the polymers decreases with r; (7) The driving force, i.e., the pressure gradient, which is balanced completely by the Newtonian viscous force and elastic force, is a constant; (8) Since the elastic force decrease radially, the Newtonian viscous force should increase with r; (9) Finally, this is achieved by enhancing strain rate owing to the fact that the dynamic viscosity of the solvent is a constant, thus increasing the flow rate. The last point in this sequence could be perceived as shear-thinning by introducing a variable viscosity as a factoring function together with ∇ 2 U , which balances the total dissipation.…”
mentioning
confidence: 99%