Computational Granular Dynamics
By Thorsten Pöschel, T. Schwager. 2005
329 citations recorded by the source corpus.
Subfields: Computational Mechanics, Management, Monitoring, Policy and Law, Mechanics of Materials
View Paper: https://www.semanticscholar.org/paper/5bce143826370fcef69c2540a4ef5c043e7429c4
How researchers see this paper
The researchers whose trusted networks rank it highest, strongest advocate first. Every researcher gets a different order.
In Computational Mechanics
- Igor S. Aranson
- Lev S. Tsimring
- Stefan Luding
- J. Gray
- Jin Sun
- Marte Gutierrez
- Abdalsalam Mohamed
- S. Sundaresan
In Management, Monitoring, Policy and Law
In Mechanics of Materials
- Lev S. Tsimring
- Igor S. Aranson
- Stefan Luding
- Jin Sun
- S. Sundaresan
- Marte Gutierrez
- Abdalsalam Mohamed
Citations in the corpus
- Particle-based simulation of powder application in additive manufacturing (2016, unknown): “The interactions between spherical particles belonging to distinct composite particles are calculated by considering both contact forces and attractive particle interaction forces [36], [33].”
- A discrete element thermo-mechanical modelling of diffuse damage induced by thermal expansion mismatch of two-phase materials (2017, background): “The developed criterion assumes that fracture occurs if the computed tensile hydrostatic stress is higher than a threshold value σ : 1 3 trace(σ̄i) ≥ σ (14)”
- Patterns and collective behavior in granular media: Theoretical concepts (2005, background): “In the simplest case of identical frictionless spherical particles of radius d with fixed restitution coefficient e it assumes the following form (∂t + (v1 · ∇)) f((v1, r1, t) = I[f ] (2) with the binary collision integral I[f ] in the form I = d2 ∫ dv2 ∫ dn12Θ(−v12 · n12)|v12 · n12| × [χf(v1 ′′,…”
- Cohesive, frictional powders: contact models for tension (2008, methodology): “With tools from numerical integration, as nicely described in textbooks as [1,61,67], this is a straightforward exercise.”
- Coefficient of restitution and linear–dashpot model revisited (2007, unknown): “[5,6,8,15,11,19,22, 32], only the repulsive part of the force is used,”