Discrete Element Methods for the Study of Unconsolidated Granular
Materials through
Computational Modeling
A numerical code based on Discrete Element Modeling (DEM)
has been developed for computing the
response of particulate materials such as unconsolidated
granular materials, concentrated emulsions or fractured
rocks.
The systems under study in this project may be considered as
``unconsolidated'' aggregates of particulate materials which acquire
stiffness as a result of the applied stress. The constitutive
properties of such materials, which also include cohesionless soils,
industrial powders, droplets, foams
and colloidal suspensions,
are determined
mainly by interparticle contact properties such as friction and
viscoelastic response.
In DEM the
dynamical evolution of the particles is obtained by solving Newton's
equation for an assembly of spherical particles
constrained by a given external pressure.
In the case of granular materials, the particles
are modeled as viscoelastic
spheres of millimeter size
with different coefficients of friction. Interparticle
forces are computed using the principles of contact mechanics.
Full details are given in previous papers of the PI.
The normal force has the typical 3/2 power law
dependence on the overlap between two spheres in contact (Hertz force),
while the
transverse force depends linearly on the shear displacement between
the spheres, as well as on the value of the normal displacement
(Mindlin tangential elastic force).
An extra sliding condition is also added, according to
Coulomb friction.
Viscous dissipative forces are included in
the force acting between viscoelastic particles, proportional to the
relative normal and tangential
velocity of the particles.
This model is the starting point for our simulations. More complicated
interactions,
such as rolling friction or other forms of tangential elasticity,
will be incorporated at a later stage.
Results
A numerical code has been developed and tested for
the two-dimensional case and, preliminary, for three dimensions.
The code is written in Fortran 90 and is ready to be ported to a parallel
architecture.
Two dimensional case
We tested the code by performing
DEM simulations of systems of the order of $10000$
particles in serial computers.
Our calculations begin with a
numerical protocol designed to mimic the experimental procedure
used to prepare dense packed granular materials.
The simulations
begin with a gas of spherical particles located at random
positions in a periodically repeated cubic cell of side $L$.
At the outset, a series of
strain-controlled isotropic compressions and expansions are
applied until a volume fraction slightly below the critical
density is reached.
The system is then compressed and
extended slowly until a specified value of the stress and volume
fraction is achieved at static equilibrium.
The structure of packings depends in detail on the forces acting
between the grains.
In Figure 1 we show a typical micromechanical structure
of a packing of 10000 spherical disks.
We plot the forces between the particles as lines joining
the center of the particle.
The width of the lines represent the absolute value of the
interparticle forces. We show the case of a packing of identical
disks of 1 mm diameter (Fig. 1a)
and a
mixture composed of 5000 disk of 1 mm and 5000 disks of 1.5 mm (Fig. 1b).
The degree of crystallization and the difference
in the packing structure is obvious from the pictures.
We have further tested the code by conducting a simple numerical experiment
which measures the response of the granular packing to a
infinitesimal perturbation consisting of moving a grain in the center
of the packing. We monitor the stress relaxation as a function of time.
Figure 2 show snapshots of our simulations where
we plot
the stress as a function
of time. The color blue corresponds to particle under
compression (negative stress) and
purple corresponds to particles under extension (positive stress).
A movie of a simulation of the propagation os stress is available
here for
frictional spheres and frictionless spheres .
(a)
(b)
Fig. 1.
Example of microstructure obtained in DEM simulations
of a system of 10000 granular particles compressed at 10 MPa
showing the existance of force chains.
The lines between the particles corresponds to the interparticle
forces. (a) Monodisperse system showing crystalization and
(b) polydisperse system.
(a)
(b)
(c)
Fig. 2.
Evolution of the stress inside a granular packing
after a small perturbation is applied to the center of the system.
Three-dimensional results
We have also tested a preliminary version of the three-dimensional code
by developing
a thermodynamic formulation for slow granular matter
with
computer simulations.
The preliminary results of our first year of research
show very promising results.
Using the code developed under this grant
we have performed a preliminary
numerical study of a diffusion-mobility test for granular materials.
This work was published in Nature
and has received an
enthusiastic News & Views Editorial commentary
by B. Behringer.
Collaborators
Jorge Kurchan, ESPCI, Paris, Nicolas Gland, ENS, Paris,
Eugene Mananga, Won-Geun Kim.
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