Strain localization and the onset of dynamic weakening in granular fault gouge Steven Smith 1,...
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Transcript of Strain localization and the onset of dynamic weakening in granular fault gouge Steven Smith 1,...
Strain localization and the onset of dynamic weakening in granular fault gouge
Steven Smith1, Stefan Nielsen1, Giulio Di Toro1,2
INGV, Rome1; University of Padova2
This research is funded by the European Research Council http://erc.europa.eu/
Talk outline• Exploring the rheology of granular fault gouges
during rapid (earthquake) shear – motivations
• Experimentally reproducing “earthquake-like” slip pulses in fault gouges
• Feedback between strain localization and weakening in fault gouges at coseismic slip rates
• Conclusions
Chester & Goldsby, SCEC Ann. Rpt., 2003Chester & Chester, Tectonophys. 1998
Motivation: In mature fault zones, large displacements (including coseismically) are often localized in granular fault rocks (e.g. gouges)
cohesivecataclasites
incohesivecataclasites
20 m
Localizedslip zone5 mm
Punchbowl Fault
How does dynamic stress evolve in the presence of granular fault rocks during coseismic slip?
One approach: experimentally deform granular fault rocks using combined
high slip rates and high normal stresses
Future experimental work IThe machine at INGV
SHIVA, Italy, July 2009SHIVA apparatus at
INGV, Rome
5 cm
Axial Load
RotaryMotion
n < 60 MPaSlip velocity < 6.5 m s-1
Standard “solid” samples
Outer ring
Inner ring
65 mm
Incohesive gouge(5 g of calcite gouge,
<250 µm)
Purpose-built sample holder for use with incohesive gouges
Stationary side(normal load)
Tested up to 30 MPa σn and 3 m s-1 slip velocity.Ongoing tests with various gouges: calcite, dolomite, quartz, clays
Rotary side50 mm
High velocity “slide-hold-slide” experiments: feedback between localization and strength in fault gouges
0 1 2 2 3 4
SLIDE 1 SLIDE 21 min. HOLD
Slip (m)
Shea
r str
ess
(MPa
)
0
10
5
1 m s-1, 8.5 MPa
SOLID CYLINDERS OFCALCITE MARBLE
Slide 2: Much faster weakening
as in solid rocks
0
1
Slip
vel
ocity
(m s
-1)
Slip velocity
Shear stress
Slide 1: Prolonged
strengthening phase
G2
Strengthening phase during Slide 1 accounts in some cases for >50% of experimental “fracture energy”
Strengthening phase
Weakeningphase
Onset ofdynamic weakening
0 1 20.2 m
G2G1
Slip (m)
Shea
r str
ess
(MPa
)
0
10
5
1 m s-1, 8.5 MPa
0
0.05
0.1
0.15
0.2
0.25
0.3
0 5 10 15 20 25 30
Str
en
gth
en
ing
ph
ase
(m
)
Normal Stress (MPa)
0
0.05
0.1
0.15
0.2
0.25
0.3
0 5 10 15 20 25 30
Str
en
gth
en
ing
ph
ase
(m
)
Normal Stress (MPa)
Strengthening phase is shorter at higher normal stress (acceleration the same in each experiment)
2 mm thick gouge layers
1.5 mm thick gouge layers
Solid cylinders of calcite marble
Slide 2
Stre
ngth
enin
g ph
ase
(m)
Normal Stress (MPa)
0
2
4
6
8
10
0 0.2 0.4 0.6 0.8 1
She
ar
stre
ss (
MP
a)
Slip velocity (m s-1)
Velocity at which weakening initiates (Vcrit) during Slide 1 is relatively high
Slide 1
Vcrit:0.8 m s-1
Slide 2
Vcrit:0.1 m s-1
Weakening
WeakeningStrengthening
Starting material: incohesive calcite gouge derived from Carrara marble (<250 µm size fraction)
55 mm
1 mm
Minimal grain size reduction
Incipient localization to boundary-parallel shear band 100 – 200 µm wide precedes weakening
1 mm
100 µm
Laterally continuous shear bandparallel to layer boundaries (Y-shear)
Fine-grainedshear band
Within 100 µm-wide shear band, multiple short and anastomosing slip surfaces have formed, flanked by “welded” layers of calcite grains (local
heating within shear band...?).
100 µm wideshear band
10 µm
Cohesive, “welded” layer of calcite grains around micro-slip surface
1 µm
Small pores related to CO2 degassing
Prominent, single slip surface 2-3 µm wide surrounded by a zone of dynamically recrystallized calcite – this slip surface is stable with
increasing slip and is reactivated following hold period
Slip surface
0.5 mm Zone of dynamically recrystallizedand indurated calcite (Smith et al 2013, Geology)
Conclusions
• Confined calcite gouges show significant early phase of strengthening during acceleration to high velocity (influenced by normal stress, layer thickness, grain size...)
• Weakening initiates by formation of a locally hot shear band. Continued localization during weakening leads to a single, discrete slip surface that is reactivated during Slide 2.
• In nature, fresh gouge is probably generated during every rupture event by e.g. dynamic fracturing and wear processes. Therefore, localization is expected to be an important process in the dynamic strength evolution of faults.