Issue |
J. Phys. I France
Volume 7, Number 1, January 1997
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Page(s) | 39 - 80 | |
DOI | https://doi.org/10.1051/jp1:1997126 |
J. Phys. I France 7 (1997) 39-80
Stress propagation and Arching in Static Sandpiles
J.P. Wittmer1, M.E. Cates1 and P. Claudin21 Department of Physics and Astronomy, University of Edinburgh, JCMB King's Buildings, Mayfield Road, Edinburgh EH9 3JZ, UK
2 Cavendish Laboratory, Madingley Road, Cambridge CB3 OHE, Uk
(Received 17 June 1996, received in final form 19 September 1996, accepted 24 September 1996)
Abstract
We present a new approach to the modelling of stress propagation in static granular media, focussing on the conical sandpile
constructed from a point source. We view the medium as consisting of cohesionless hard particles held up by static frictional
forces; these are subject to microscopic indeterminacy which corresponds macroscopically to the fact that the equations of
stress continuity are incomplete - no strain variable can be defined. We propose that in general the continuity equations
should be closed by means of a constitutive relation (or relations) between different components of the (mesoscopically averaged)
stress tensor. The primary constitutive relation relates radial and vertical shear and normal stresses (in two dimensions,
this is all one needs). We argue that the constitutive relation(s) should be local, and should encode the construction history of the pile: this history determines the organization of the grains at a mesoscopic scale, and thereby the local relationship between
stresses. To the accuracy of published experiments, the pattern of stresses beneath a pile shows a scaling between piles of
different heights (RSF scaling) which severely limits the form the constitutive relation can take; various asymptotic features
of the stress patterns can be predicted on the basis of this scaling alone. To proceed further, one requires an explicit choice
of constitutive relation; we review some from the literature and present two new proposals. The first, the FPA (fixed principal
axes) model, assumes that the eigendirections (but not the eigenvalues) of the stress tensor are determined forever when a
material element is first buried. (This assumes, among other things, that subsequent loadings are not so large as to produce
slip deep inside the pile.) A macroscopic consequence of this mesoscopic assumption is that the principal axes have fixed
orientation in space: the major axis everywhere bisects the vertical and the free surface. As a result of this, stresses propagate along a nested
set of archlike structures within the pile, resulting in a minimum of the vertical normal stress beneath the apex of the pile, as seen experimentally ("the dip"). This experiment has not been
explained within previous continuum approaches; the appearance of arches within our model corroborates earlier physical arguments
(of S.F. Edwards and others) as to the origin of the dip, and places them on a more secure mathematical footing. The second
models is that of "oriented stress linearity" (OSL) which contains an adjustable parameter (one value of which corresponds
to FPA). For the general OSL case, the simple interpretation in terms of nested arches does not apply, though a dip is again
found over a finite parameter range. In three dimensions, the choice for the primary constitutive relation must be supplemented
by a secondary one; we have tried several, and find that the results for the stresses in a three-dimensional (conical) pile
do not depend much on which secondary closure is chosen. Three-dimensional results for the FPA model are in good semiquantitative
agreement with published experimental data on conical piles (including the dip); the data does not exclude, but nor does it
support, OSL parameters somewhat different from FPA. The modelling strategy we adopt, based on local, history-dependent constitutive
relations among stresses, leads to nontrivial predictions for piles which are prepared with a different construction history
from the normal one. We consider several such histories in which a pile is prepared and parts of it then removed and/or tilted.
Experiments along these lines could provide a searching test of the theory.
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