2016
DOI: 10.1007/s11440-016-0496-y
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Unified modelling of granular media with Smoothed Particle Hydrodynamics

Abstract: In this paper, we present a unified numerical framework for granular modelling. A constitutive model capable of describing both quasi-static and dynamic behaviours of granular material is developed. Two types of particle interactions controlling the mechanical responses, frictional contact and collision, are considered by a hypoplastic model and a Bagnold-type rheology relation, respectively. The model makes no use of concepts like yield stress or flow initiation criterion. A smooth transition between the soli… Show more

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Cited by 83 publications
(48 citation statements)
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References 53 publications
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“…Its simplicity and robustness make it an ideal basic model to build more sophisticated models, e.g., critical state model and high-order model [5,8,9,13,30,31]. The failure surface is derived from the constitutive equation and likes that of DruckerPrager.…”
Section: Discussionmentioning
confidence: 99%
“…Its simplicity and robustness make it an ideal basic model to build more sophisticated models, e.g., critical state model and high-order model [5,8,9,13,30,31]. The failure surface is derived from the constitutive equation and likes that of DruckerPrager.…”
Section: Discussionmentioning
confidence: 99%
“…It is through I e that the model captures the effects of density and confining pressure on the strain-stress behaviour. Several forms for I e can be found in the literature [7,15,21,41], but in the present work, a different formulation for the critical state function I e is proposed:…”
Section: Constitutive Modelmentioning
confidence: 99%
“…However, in the interaction problems between dry granular flows and structures, the soil elements should stay in a critical state where the dilatancy is zero and the ignorance of the dilatancy in this study should not introduce much error. Additionally, even though the constitutive model accounts for the compressibility, the majority of existing numerical models can not satisfactorily reproduce the desired compressible behaviour due to numerical errors . Therefore, in the present study, the dry granular mass is modelled as an incompressible material with the governing equations as follows: dρdt=ρ·bold-italicv=0, dbold-italicvdt=1ρ·sans-serifσ+bold-italicg=1ρp+1ρ·bolds+bold-italicg. …”
Section: Mathematical Modelmentioning
confidence: 99%
“…Readers are referred to other works and He for the basis of SPH such as the smoothing kernels, the kernel approximation, and the particle approximation. Here, we focus on introducing the different part of our incompressible SPH scheme.…”
Section: Mathematical Modelmentioning
confidence: 99%
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