2000
DOI: 10.1103/physrevlett.84.4160
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Packing of Compressible Granular Materials

Abstract: 3D computer simulations and experiments are employed to study random packings of compressible spherical grains under external confining stress. In the rigid ball limit, we find a continuous transition in which the stress vanishes as (straight phi-straight phi(c))(beta), where straight phi is the (solid phase) volume density. The value of straight phi(c) depends on whether the grains interact via only normal forces (giving rise to random close packings) or by a combination of normal and friction generated trans… Show more

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Cited by 383 publications
(423 citation statements)
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“…where bulk ρ is tapped density, solid ρ is apparent particle density and c φ is the packing fraction for random loose packing [6], where the interaction is composed of both normal forces and transverse frictional forces, with a value of 0.6284, which is within the range generally obtained for spherical particles [22].…”
Section: Pelletsmentioning
confidence: 81%
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“…where bulk ρ is tapped density, solid ρ is apparent particle density and c φ is the packing fraction for random loose packing [6], where the interaction is composed of both normal forces and transverse frictional forces, with a value of 0.6284, which is within the range generally obtained for spherical particles [22].…”
Section: Pelletsmentioning
confidence: 81%
“…In summary, seeing as the most probable factors influencing the force distributions in this study are pellet deformation and/or fracture, it seems that, based on previous findings [6,8,10], which only took deformation and not fracture into account, the influence of deformation on MLP is greater than the other pellet types, as it was the only one to somewhat follow the trends seen in these studies, by exhibiting the least homogenous distribution within its pellet type at 10 MPa.…”
Section: Force Distributionsmentioning
confidence: 92%
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