APS March Meeting 2010
Volume 55, Number 2
Monday–Friday, March 15–19, 2010;
Portland, Oregon
Session T7: Avalanches in Condensed Matter
2:30 PM–5:30 PM,
Wednesday, March 17, 2010
Room: Portland Ballroom 254
Sponsoring
Units:
GSNP DCMP
Chair: Craig Maloney, Carnegie Mellon University
Abstract ID: BAPS.2010.MAR.T7.2
Abstract: T7.00002 : Physics of Earthquakes and Faults
3:06 PM–3:42 PM
Preview Abstract
Abstract
Author:
Yehuda Ben-Zion
(University of Southern California)
Detailed observations and theoretical results on brittle failure
events in individual fault zones point to three general dynamic
regimes [1]. The first is associated with broad range of
heterogeneities, little dynamic weakening during failure, power
law frequency-size statistics, and temporal clustering
of events. The second is associated with relatively-uniform
localized structures, significant dynamic weakening, and
quasi-periodic occurrence of characteristic system-size events.
For a range of conditions, the response can switch back and forth
between the forgoing two types of behavior. These dynamic
regimes, geometrical properties of slip, and observed
moment rate shapes can be explained by a simple model having two
tuning parameters: dynamic weakening and conservation of elastic
stress transfer during failure events [2]. The model can also
explain multiple aspects of deformation in volumetric regions,
including stress-strain curves, acoustic emissions and related
power spectra, with a continuous transition from brittle
to plastic behavior, and statistics of failure events in granular
media [3]. The results from the latter studies are in good
agreement with experimental data [4] and simulations with other
frameworks [5]. An extension of the model to include cohesion
changes during failure and healing phases of
deformation may account for transitions between solid and
granular phases of materials [6].\\[4pt]
[1] Y. Ben-Zion, \textit{Rev. Geophys.}, \textbf{46}, RG4006
(2008) and references therein.
\\[0pt]
[2] D.S. Fisher et al., Phys. Rev. Lett. \textbf{78, }4885
(1997); Y. Ben-Zion, and J.R. Rice, J. Geophys. Res.,
\textbf{98}, 14109, (1993). K.A. Dahmen et al., Phys. Rev. E 58,
1494 (1998). A.P. Mehta et al., Phys. Rev. E \textbf{73}, 056104
(2006).
\\[0pt]
[3] K.A. Dahmen, et al., \textit{Phys. Rev. Lett.}, \textbf{102},
175501, 2009. K.A.Dahmen, Y. Ben-Zion and J.T. Uhl, submitted, 2009.
\\[0pt]
[4] K.E. Daniels and N.W. Hayman, Journal of Geophysical
Research, \textbf{113} B11411 (2008). H. Jaeger, S.R. Nagel, R.P.
Behringer, Revs. Mod. Phys. \textbf{66}, 1259-1273 (1996) and
references therein.
\\[0pt]
[5] K. Chen \textit{et. al.,} Phys. Rev. A \textbf{43}, 625
(1991). M. Zaiser, Adv. Phys. \textbf{55}, 185 (2006); M.J. Alava
et al., Adv. Phys. \textbf{55}, (2006). E. Aharonov and D.
Sparks, Phys. Rev E, \textbf{60}, 6890-6896 (1999). E.
Aharonov and D. Sparks, J. Geophys. Res, \textbf{109}, B09306 (2004).
\\[0pt]
[6] Y. Ben-Zion, K. A. Dahmen and J.T. Uhl, submitted, 2009.
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2010.MAR.T7.2