Abstract

Abstract

Highlights

  • Granular flows exhibit several intriguing phenomena that distinguish them fromNewtonian fluids, such as the presence of pressure-dependent arrest and flow onset criteria leading to rate-independent and rate-dependent flows, and a dilute gas-like907 A18-2 I

  • This study examines the flow of dense granular materials under external shear stress and pressure using discrete element method simulations

  • Where η0{H} is a fourth-rank viscosity tensor. We adapt this rheological framework to model granular rheology through the following assumptions that will be demonstrated to hold true in the present simulations: (1) the flow is homogeneous with a constant stretch history (Noll 1962); and (2) the flow is planar and isochoric, i.e. D is characterized by two dominant eigenvalues and tr(D) = 0

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Summary

Introduction

Newtonian fluids, such as the presence of pressure-dependent arrest and flow onset (yield) criteria leading to rate-independent and rate-dependent flows, and a dilute gas-like. A detailed discussion of such viscoplastic models can be found in a recent review (Goddard 2014) These rheological models have successfully predicted granular flow profiles in a remarkable number of geometries (MiDi 2004), several rheological effects remain unexplained, such as surface curvature in free-surface flows (Couturier et al 2011; McElwaine, Takagi & Huppert 2012), negative rod climbing effects (Boyer, Pouliquen & Guazzelli 2011b), anomalous stress profile in Couette flows (Mehandia, Gutam & Nott 2012), and the observation of shear-free sheets in split-bottom Couette flows (Depken et al 2007). We describe fully stress-controlled discrete element method (DEM) simulations in both rate-independent and rate-dependent regimes This simulation method enables the evolution of all strain degrees of freedom of a fully periodic representative volume element of granular material in response to external applied shear stress and pressure.

Rheological model
Constant stress simulations
Bulk deformation
Contact mechanics
Simulation details
Evolution towards viscometric flow
Model calibration
Flow functions: η1 and κ1
Flow functions: η2 and κ2
Flow function: η3
Granular flow-induced dilation
Normal stress differences and their microstructural origins
Second normal stress difference
First normal stress difference
Conclusions

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