Abstract

Numerical simulations of granular flows with Navier–Stokes type models emerged in the last decade, challenging the well established depth-averaged models. The structure of these equations allows for extension to general rheologies based on complex and realistic constitutive models. Substantial effort has been put into describing the effect of the shear rate, i.e. the magnitude of the velocity gradient, on the shear stress. Here we analyse the effect of the deformation type. We apply the theories of Mohr–Coulomb and Matsuoka–Nakai to calculate the stresses under different deformation types and compare results to the theory of Drucker–Prager, which is formulated independently of the deformation type. This model is particularly relevant because it is the basis for many granular rheologies, such as the μ ( I ) –rheology. All models have been implemented into the open-source toolkit OpenFOAM® for a practical application. We found that, within the context of these models, the deformation type has a large influence on the stress. However, for the geometries considered here, these differences are limited to specific zones which have little influence on the landslide kinematics. Finally we are able to give indicators on when the deformation type should be considered in modelling of landslides and when it can be neglected.

Highlights

  • Dense granular flows are substantial parts of many natural hazards, such as avalanches, landslides, debris flows and lahars

  • The first models for granular materials stem from geotechnics and applications in the soil mechanics community, with the earliest examples of a mathematical description being in the 19th century, when Charles-Augustin de Coulomb formulated his famous friction law, based on the rules found earlier by Guillaume Amontons

  • Using the approach of Schaeffer [14], almost arbitrary yield surfaces can be expressed as non-Newtonian viscosities and implemented into the incompressible Navier–Stokes Equations

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Summary

Introduction

Dense granular flows are substantial parts of many natural hazards, such as avalanches, landslides, debris flows and lahars. The first models for granular materials stem from geotechnics and applications in the soil mechanics community, with the earliest examples of a mathematical description being in the 19th century, when Charles-Augustin de Coulomb formulated his famous friction law Matsuoka and Nakai [6] proposed a smoother version of the Mohr–Coulomb criterion, the Matsuoka–Nakai (MN) failure criterion. It has gained a lot of popularity, as it improved numerical stability as well as physical accuracy. All developments were merged into modern constitutive models for quasi-static granular materials, such as the hardening-soil-model [5], Severn-Trent-sand [7], SaniSand [8], Hypoplasticity [9,10] or Barodesy [11,12,13]

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