HR: 1320h
AN: S43A-0986 [Abstracts]
TI: Elastic Nonlinear Response in Granular Media Under Resonance Conditions
AU: Jia, X
EM: jia@univ-mlv.fr
AF: Laboratoire de Physique des Mat‚riaux Divis‚s et des Interfaces, Universit‚ de Marne-la-Vall‚e, CNRS UMR
8108, Bƒtiment Lavoisier - Cit‚ Descartes, 5 boulevard Descartes - Champs sur Marne, Marne la Vall‚e, 77454
France
AU: * Johnson, P A
EM: paj@lanl.gov
AF: Laboratoire de Physique des Mat‚riaux Divis‚s et des Interfaces, Universit‚ de Marne-la-Vall‚e, CNRS UMR
8108, Bƒtiment Lavoisier - Cit‚ Descartes, 5 boulevard Descartes - Champs sur Marne, Marne la Vall‚e, 77454
France
AU: * Johnson, P A
EM: paj@lanl.gov
AF: Geophysics Group EES-11, Los Alamos National Laboratory of the University of California, MS D443, Los
Alamos, 87545
United States
AB:
We are studying the elastic linear and nonlinear behavior of granular media using dynamic wave methods. In the work
presented here, our goal is to quantify the elastic nonlinear response by applying wave resonance. Resonance studies are
desirable because they provide the means to easily study amplitude dependencies of elastic nonlinear behavior and thus to
characterize the physical nature of the elastic nonlinearity. This work has implications for a variety of topics, in
particular, the in situ nonlinear response of surface sediments. For this work we constructed an experimental cell in which
high sensitivity dynamic resonance studies were conducted using granular media under controlled effective pressure. We limit
our studies here to bulk modes but have the capability to employ shear waves as well. The granular media are composed of
glass beads held under pressure by a piston, while applying resonance waves from transducers as both the excitation and the
material probe. The container is closed with two fitted pistons and a normal load is applied to the granular sample across
the top piston. Force and displacement are measured directly. Resonant frequency sweeps with frequencies corresponding to
the fundamental bulk mode are applied to the longitudinal source transducer. The pore pressure in the system is 1 atm. The
glass beads used in our experiments are of diameter 0.5 mm, randomly deposited in a duralumin cylinder of diameter 30 mm and
height of 15 mm. This corresponds to a granular skeleton acoustic wave velocity of v ¦ 750m/s under 50 N of force [0.07 Mpa].
The loaded system gives fundamental mode resonances in the audio frequency band at half a wavelength where resonance
frequency is effective-pressure dependent. The volume fraction of glass beads thus obtained is found to be 0.63 ñ 0.01.
Plane-wave generating and detecting transducers of diameter 30 mm are placed on axis at the top and bottom of the cylindrical
container in direct contact with the glass beads. The wave signals are detected using a lock-in amplifier, and frequency
and amplitude are recorded on computer. Drive frequency is swept from below to above the resonance mode. A typical frequency
sweep is 3 kHz in width with a frequency sampling of 6 Hz. Frequency sweeps are applied at progressively increasing drive
voltages to test for nonlinear-dynamical induced modulus softening. The resonance frequency at peak amplitude corresponds
directly to modulus. We find significant elastic nonlinearity at all effective pressures, manifest by the fundamental-mode
resonance curves decreasing progressively, at progressively increasing drive level. This is equivalent to progressive
material softening with wave amplitude, meaning the wavespeed and modulus diminish. The wave dissipation simultaneously
increases (Johnson and Sutin 2004). For example, at 0.11 Mpa effective pressure the observed change in resonance frequency of
about 2.6% corresponds to a material bulk modulus decrease of about 5.2%. Strain amplitudes are 10-7-10-6. Thus, we would
predict that surface sediments should have significant elastic nonlinear response beginning at about 10-6 strain amplitude.
reference:
Johnson, P. and A. Sutin, Slow dynamics in diverse solids, J. Acoust. Soc Am., in press (2004).
DE: 6944 Nonlinear phenomena
DE: 7212 Earthquake ground motions and engineering
SC: Seismology [S]
MN: 2004 AGU Fall Meeting