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Non-Newtonian stress, collisional dissipation and heat flux in the shear flow of inelastic disks: a reduction via Grad’s moment method
The non-Newtonian stress tensor, collisional dissipation rate and heat flux in the plane shear flow of smooth inelastic disks are analysed from the Grad-level moment equations using the anisotropic Gaussian as a reference. For steady uniform shear flow, the balance equation for the second moment of...
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Published in: | Journal of fluid mechanics 2014-10, Vol.757, p.251-296 |
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Main Authors: | , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | The non-Newtonian stress tensor, collisional dissipation rate and heat flux in the plane shear flow of smooth inelastic disks are analysed from the Grad-level moment equations using the anisotropic Gaussian as a reference. For steady uniform shear flow, the balance equation for the second moment of velocity fluctuations is solved semi-analytically, yielding closed-form expressions for the shear viscosity
$\def \xmlpi #1{}\def \mathsfbi #1{\boldsymbol {\mathsf {#1}}}\let \le =\leqslant \let \leq =\leqslant \let \ge =\geqslant \let \geq =\geqslant \def \Pr {\mathit {Pr}}\def \Fr {\mathit {Fr}}\def \Rey {\mathit {Re}}\mu $
, pressure
$p$
, first normal stress difference
${\mathcal{N}}_1$
and dissipation rate
${\mathcal{D}}$
as functions of (i) density or area fraction
$\nu $
, (ii) restitution coefficient
$e$
, (iii) dimensionless shear rate
$R$
, (iv) temperature anisotropy
$\eta $
(the difference between the principal eigenvalues of the second-moment tensor) and (v) angle
$\phi $
between the principal directions of the shear tensor and the second-moment tensor. The last two parameters are zero at the Navier–Stokes order, recovering the known exact transport coefficients from the present analysis in the limit
$\eta ,\phi \to 0$
, and are therefore measures of the non-Newtonian rheology of the medium. An exact analytical solution for leading-order moment equations is given, which helped to determine the scaling relations of
$R$
,
$\eta $
and
$\phi $
with inelasticity. We show that the terms at super-Burnett order must be retained for a quantitative prediction of transport coefficients, especially at moderate to large densities for small values of the restitution coefficient (
$e \ll 1$
). Particle simulation data for a sheared inelastic hard-disk system are compared with theoretical results, with good agreement for
$p$
,
$\mu $
and
${\mathcal{N}}_1$
over a range of densities spanning from the dilute to close to the freezing point. In contrast, the predictions from a constitutive model at Navier–Stokes order are found to deviate significantly from both the simulation and the moment theory even at moderate values of the restitution coefficient (
$e\sim 0.9$
). Lastly, a generalized Fourier law for the granular heat flux, which vanishes identically in the uniform shear state, is derived for a dilute granular gas by analysing the non-uniform shear flow via an expansion around the anisotropic Gaussian state. We show that the gradient of the deviatoric part of the |
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ISSN: | 0022-1120 1469-7645 |
DOI: | 10.1017/jfm.2014.489 |