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@ARTICLE{Brener:808658,
author = {Brener, Efim and Weikamp, Marc and Spatschek, Robert and
Bar-Sinai, Yohai and Bouchbinder, Eran},
title = {{D}ynamic {I}nstabilities of {F}rictional {S}liding at a
{B}imaterial {I}nterface},
journal = {Journal of the mechanics and physics of solids},
volume = {89},
issn = {0022-5096},
address = {Amsterdam [u.a.]},
publisher = {Elsevier Science},
reportid = {FZJ-2016-02291},
pages = {149 - 173},
year = {2016},
abstract = {Understanding the dynamic stability of bodies in frictional
contact steadily sliding one over the other is of basic
interest in various disciplines such as physics, solid
mechanics, materials science and geophysics. Here we report
on a two-dimensional linear stability analysis of a
deformable solid of a finite height H, steadily sliding on
top of a rigid solid within a generic rate-and-state
friction type constitutive framework, fully accounting for
elastodynamic effects. We derive the linear stability
spectrum, quantifying the interplay between stabilization
related to the frictional constitutive law and
destabilization related both to the elastodynamic
bi-material coupling between normal stress variations and
interfacial slip, and to finite size effects. The
stabilizing effects related to the frictional constitutive
law include velocity-strengthening friction (i.e. an
increase in frictional resistance with increasing slip
velocity, both instantaneous and under steady-state
conditions) and a regularized response to normal stress
variations. We first consider the small wave-number k limit
and demonstrate that homogeneous sliding in this case is
universally unstable, independent of the details of the
friction law. This universal instability is mediated by
propagating waveguide-like modes, whose fastest growing mode
is characterized by a wave-number satisfying
kH∼O(1)kH∼O(1) and by a growth rate that scales with
H−1. We then consider the limit kH→∞kH→∞ and
derive the stability phase diagram in this case. We show
that the dominant instability mode travels at nearly the
dilatational wave-speed in the opposite direction to the
sliding direction. In a certain parameter range this
instability is manifested through unstable modes at all
wave-numbers, yet the frictional response is shown to be
mathematically well-posed. Instability modes which travel at
nearly the shear wave-speed in the sliding direction also
exist in some range of physical parameters. Previous results
obtained in the quasi-static regime appear relevant only
within a narrow region of the parameter space. Finally, we
show that a finite-time regularized response to normal
stress variations, within the framework of generalized
rate-and-state friction models, tends to promote stability.
The relevance of our results to the rupture of bi-material
interfaces is briefly discussed},
cin = {PGI-2 / IEK-2},
ddc = {530},
cid = {I:(DE-Juel1)PGI-2-20110106 / I:(DE-Juel1)IEK-2-20101013},
pnm = {111 - Efficient and Flexible Power Plants (POF3-111) / 144
- Controlling Collective States (POF3-144)},
pid = {G:(DE-HGF)POF3-111 / G:(DE-HGF)POF3-144},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000374355900009},
doi = {10.1016/j.jmps.2016.01.009},
url = {https://juser.fz-juelich.de/record/808658},
}