Review and extension of normal force models for the Discrete Element Method
H. Kruggel-Emden, E. Simsek, S. Rickelt, S. Wirtz, V. Scherer
Department of Energy Plant Technology
Ruhr-Universitaet Bochum, Universitaetsstrasse 150,
D-44780 Bochum,
Germany
Source : http://cat.inist.fr/?aModele=afficheN&cpsidt=20126261
Abstract
For the simulation of dense granular systems the Discrete Element Method based on a soft-sphere approach is commonly used. In such
simulations collisions between particles take a finite time. The equations of motion are applied for each particle and solved numerically. Therefore
models for the forces acting between particles in contact need to be specified. In this paper the focus is set on normal contacts. Based on
macroscopic and microscopic accessible parameters like coefficient of restitution, collision time, force, displacement and displacement rate a wide
range of commonly used force schemes are reviewed. Results obtained from these commonly used models are compared to experimental data on
collisions of different metal alloys, ice and marble as reported in literature. Due to obvious limitations extensions are presented. The new extended
models based on linear and non-linear models are compared to experimental data and their accuracy and applicability are discussed.
© 2006 Elsevier B.V. All rights reserved
Introduction
Several phenomena in nature as well as many industrial
applications involve static or dynamic granular assemblies.
Depending on the physical background the number of particles
being involved in these assemblies differs largely. Whereas
laboratory scale experiments usually involve small numbers of
particles, industrial applications like silos may contain several
cubic meters of granular material in which the particle number
may easily exceed the order of 109 per cubic meter. Phenomena
related to nature like avalanches often incorporate hundreds of
tons of granular material therefore involving even larger
quantities of particles.
In general, simulations provide a feasible alternative to
experimental investigations. Their better reproducibility, less
demand for time and reduced costs are advantageous. In recent
years modeling and simulation of particle assemblies have been
difficult due to their enormous demand of computer power.
With advances in computer processing speed and due to parallel
computing the field of industrial applications is nowadays
accessible by numerical simulations [1–3].
A very promising approach for modeling particle systems is
the Discrete Element Method. It provides a way of simulating
systems of an arbitrary number of particles by modeling each
particle and its interactions with the surrounding, individually.
Depending on the density of the granular system two different
approaches are applicable. In low density systems like granular
gases the Event Driven (ED) Discrete Element Method [4] is
most feasible. Here it can be assumed, that the collision time is
of much lower magnitude than the mean free flight time and
collisions higher than binary ones are excluded. In case that
these assumptions are violated the Molecular Dynamics (MD)
Discrete Element Approach [5] finds application. Originally this
approach was designed for the simulation of particles on the
atomic and molecular level. By definition of pairwise potentials
information on the thermodynamics of fluids were accessible
otherwise only available by statistical means [6,7]. To perform a
MD simulation the initial conditions of the particle system need
to be specified.
The full text can be downloaded from : http://cat.inist.fr/?aModele=afficheN&cpsidt=20126261