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Volumn 184, Issue 3, 2013, Pages 628-637

Simulations of driven overdamped frictionless hard spheres

Author keywords

Deformation; Event driven; Geometry; Granular; Hard spheres; Overdamped

Indexed keywords

CONTACT FORCES; DRIVING FORCES; EQUATION OF MOTION; EVENT DRIVEN; EVENT-DRIVEN APPROACH; EVENT-DRIVEN SIMULATIONS; EXTERNAL FORCE; GEOMETRIC INFORMATION; GRANULAR; HARD SPHERES; HIGH-PRECISION; HYDRODYNAMIC INTERACTION; JAMMED PACKINGS; OVERDAMPED; UNDERLYING NETWORKS;

EID: 84872049942     PISSN: 00104655     EISSN: None     Source Type: Journal    
DOI: 10.1016/j.cpc.2012.10.020     Document Type: Article
Times cited : (29)

References (25)
  • 7
    • 84872009076 scopus 로고    scopus 로고
    • J. Chem. Phys. 131 2009 024504
    • (2009) J. Chem. Phys. , pp. 024504
  • 23
    • 84872033012 scopus 로고    scopus 로고
    • f 0 〉 is the eigenvector associated with the zero eigenvalue of N, it can be calculated via diagonalization, for instance
    • f 0 〉 is the eigenvector associated with the zero eigenvalue of N, it can be calculated via diagonalization, for instance
  • 24
    • 84872021808 scopus 로고    scopus 로고
    • Such patches can be hyperstatic, i.e., over-constrained. Physically these patches move as solid blocks, until they break. In our approach these patches are difficult to deal with (although it can be done), as they lead to zero modes in the spectrum of N, which renders Eq. (11) difficult to solve numerically. We avoid this problem by adding polydispersity
    • Such patches can be hyperstatic, i.e., over-constrained. Physically these patches move as solid blocks, until they break. In our approach these patches are difficult to deal with (although it can be done), as they lead to zero modes in the spectrum of N, which renders Eq. (11) difficult to solve numerically. We avoid this problem by adding polydispersity


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.