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Laboratory(earthquakes:(Measuring(surface(displacements(with(high;speed(DIC(Vito%Rubino,%Nadia%Lapusta,%Ares%Rosakis%
California(Ins?tute(of(Technology(
The(full;field(displacement(clearly(shows(rela?ve(mo?on(on(the(two(sides(of(the(fault.(In(order(to(compute(strains,(we(denoise(the(displacement(field(using(the(tool(available( in(COSI;Corr,(based(on(Buades(et(al((2008).((
Research(goals(• ((Inves?gate(the(feasibility(of(dynamic(full;field(earthquake(measurements(from(space(through(laboratory(studies.(• ((First,(employ(digital(image(correla?on(techniques((such(as(VIC;2D(and(COSI;Corr)(to(study(the(final(sta?c(deforma?on(of(a(dynamic(crack(with(‘before’(and(‘aRer’(event(images(of(specimens(undergoing(dynamic(fric?onal(sliding.(• (Next,(extend(digital(image(correla?on(to(high(speed(photography(to(capture(dynamic(rupture(propaga?on.((
Specimen(configura?ons(
Sta?c(Measurements(San%Andreas%strike6slip%Fault,%Carrizo%Plain%(h>p://tharsisgallery.com/san6andres6fault6pictures)%
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Conclusions(and(Future(Work(• ((Successfully(characterized(full;field(sta?c(displacements(and(strain(of(a(dynamic(crack(with(digital(image(correla?on(techniques((COSI;Corr(and(VOC;2D).((• ((Performed(dynamic(measurements(by(coupling(high(speed(photography(and(digital(image(correla?on.((• ((Designing(experiments(to(study(poten?al(transi?on(to(supershear(speeds(due(to((favorable(heterogeneity.(
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• (((Study(discussed(in(this(poster:(interface(is(either(uniform(or(par?ally(glued(in(order(to(confine(the(rupture(before(it(reaches(the(ends(of(the(specimen.(• (((Ongoing(work:(interface(contains(a(patch(of(heterogeneity(with(lower(strength,(higher(stress,(or(pre;exis?ng(subcri?cal(crack.(The(aim(is(to(study(dynamic(triggering(of(a(secondary(rupture(on(a(patch(of(heterogeneity(and(explore(poten?al(transi?on(to(supershear(speeds((Liu(and(Lapusta,(2008).(
Displacement(field(u% Displacement(u(vs.(s% Strain(field(εxx%
Fault(parallel(displacement((((µm)( Fault(normal(displacement((((µm)(
εxx εyy εxy
Fault parallel displacement
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From(real(earthquakes(to(
Earthquakes(are(mimicked( in( the( laboratory(by( the(dynamic( rupture(propaga?ng(along(an(inclined(fric?onal(interface(formed(by(two(Homalite(quadrilateral(plates(under(compression((Xia( et( al.,( 2004).( The( sta?c( compressive( stress(P,( applied( to( the( test( specimen( assembly,(provides( resolved( shear( and( normal( stresses( on( the( fault,( simula?ng( tectonic( stresses(applied(to(a(strike;slip(fric?onal(fault(within(the(Earth’s(crust.(Dynamic(rupture( is(triggered(through(the(electrical(discharge(provided(by(a(NiCr(wire(filament.(((
Digital( (Image(Correla?on((DIC)(is(an(op?cal(method(to(measure(the(deforma?on(on(a(specimen(surface.(DIC(technique(iden?fies(gray(level(pa]erns(in(small(pixel(subsets(and(tracks(their(mo?on(during(deforma?on.(Two(methods(are(used(in(this(study:(VIC;2D((Correlated(Solu?ons(Inc.)(and(COSI;Corr((Leprince(et.(al,(2007).(Results(are(presented(for(COSI;Corr.((
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• Interface length (shown in frame): ~40 mm • Rupture goes through interface in t < 20 µs • Computed rupture speed: vr ~ 2.5 mm/µs • Compare to Homalite wave speeds: - cs = 1.29 mm/µs - cp = 2.61 mm/µs • Mach cone angle is given by: sin θ = cs / vr , θ ~ 30° • Mach cone will advance ~ 12.5 mm
Subset: 21 pixels Step: 1 pixels
Digital(Image(Correla?on((DIC)( Dynamic(Measurements(
laboratory(earthquakes(
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Large:(characteris?c(pa]ern(Small:(high(resolu?on(
• ((Subset(size:(32x32%• %%Step:(4(1 pixel ∼ 83 µm
42.6 mm
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Fault(Heterogenei?es(We(are(currently(inves?ga?ng(supershear(transi?on(by(dynamic(triggering(of(a(secondary(rupture(on(a(patch(of(heterogeneity,(such(as(a(preexis?ng(subcri?cal(crack(or(a(patch(of(higher(prestress,(to(extend(and(experimentally(validate(the(study(of(Liu(and(Lapusta,2008.((((
t = 29 µs
t = 37 µs
t = 41 µs
t = 50 µs
t = 30 µs
t = 35 µs
t = 40 µs
t = 45 µs
High-speed photoeleastic images from Mello et al, 2010.
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