postseismic deformation from the 1991 racha, georgia earthquake may 16, 2006 joel podgorski earth...
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Postseismic Deformation Postseismic Deformation from the 1991 Racha, from the 1991 Racha, Georgia EarthquakeGeorgia Earthquake
May 16, 2006May 16, 2006
Joel PodgorskiJoel Podgorski
Earth and Ocean SciencesEarth and Ocean Sciences
University of British ColumbiaUniversity of British Columbia
Purpose of studyPurpose of study
To determine if and how postseismic To determine if and how postseismic deformation has occurred following deformation has occurred following 1991 earthquake in Racha, Georgia1991 earthquake in Racha, Georgia
This information will provide This information will provide constraints on rheological constraints on rheological properties of lithosphere in Arabia-properties of lithosphere in Arabia-Eurasia continental collision zoneEurasia continental collision zone
OutlineOutline Racha earthquake and similar earthquakesRacha earthquake and similar earthquakes Tectonic settingTectonic setting GPS dataGPS data
• Racha rupture area and GPS sitesRacha rupture area and GPS sites
• data acquisition and analysisdata acquisition and analysis
• velocity decay in datavelocity decay in data
• correcting data for secular displacementcorrecting data for secular displacement Earthquake afterslipEarthquake afterslip
• afterslip processafterslip process
• inverse modelinginverse modeling
• modeling resultsmodeling results Viscoelastic relaxationViscoelastic relaxation
• viscoelasticity and modelingviscoelasticity and modeling
• modeling resultsmodeling results SummarySummary
Racha earthquake and similar Racha earthquake and similar earthquakesearthquakes
Racha earthquake, Georgia (April 29, 1991)Racha earthquake, Georgia (April 29, 1991)
• MMww=6.9 (same as Loma Prieta)=6.9 (same as Loma Prieta)
• Dip slip/thrust mechanismDip slip/thrust mechanism
• 3030˚ dip, hypocenter 6 km depth˚ dip, hypocenter 6 km depth
Similar thrust events:Similar thrust events:
• Chi-Chi, Taiwan (1999), MChi-Chi, Taiwan (1999), Mww=7.6, hypocenter =7.6, hypocenter
depth 8 km, dip 30depth 8 km, dip 30˚̊
• Northridge, California (1994), MNorthridge, California (1994), Mww=6.7, =6.7,
hypocenter depth 20 km, dip 45hypocenter depth 20 km, dip 45˚̊
• Loma Prieta, California (1989), MLoma Prieta, California (1989), Mww=6.9, =6.9,
hypocenter depth 16 km, dip 70hypocenter depth 16 km, dip 70˚̊
UP DIP
DOWN DIP
Setting
Greater Caucasus:Greater Caucasus:• 1000 km long, ~5000 1000 km long, ~5000
m highm high• middle of Alpine middle of Alpine
Himalayan fold beltHimalayan fold belt• uplift began 3.5 Ma uplift began 3.5 Ma
after collision of after collision of ArabiaArabia
Greater Caucasus
25 MM/YR
ARABIA
Racha rupture area and GPS sitesRacha rupture area and GPS sites
Racha Epicenter
Afterslip Plane
GPS Sites
GPS data acquisition and analysisGPS data acquisition and analysis
Data are from 8 sites for some or all of time Data are from 8 sites for some or all of time points: 1991.56 (~3 months after earthquake), points: 1991.56 (~3 months after earthquake), 1994.77, 1996.74, 1998.71, 2000.761994.77, 1996.74, 1998.71, 2000.76
Field work by collaborators at MITField work by collaborators at MIT Data analyzed at MIT with GAMIT/GLOBK software:Data analyzed at MIT with GAMIT/GLOBK software:
• Estimate site coordinates, satellite orbital Estimate site coordinates, satellite orbital parameters, atmospheric delay corrections, parameters, atmospheric delay corrections, and earth orientation parametersand earth orientation parameters
• Combine parameter estimates and covariances Combine parameter estimates and covariances and apply position and velocity constraints and apply position and velocity constraints from global core sites from global core sites
50% precision improvement 1991-1994 due to 50% precision improvement 1991-1994 due to increased satellite coverageincreased satellite coverage
Logarithmic versus linear fit to dataLogarithmic versus linear fit to data
Logarithmic fit indicative of afterslipLogarithmic fit indicative of afterslip Residuals to linear fit and log fit Residuals to linear fit and log fit
comparedcompared Sites showing better fit with Sites showing better fit with
logarithmic curve (misfit halved or logarithmic curve (misfit halved or better):better):
• LESO (N,E,Up)LESO (N,E,Up)
• KHUR (N)KHUR (N)
• SACC (E, Up)SACC (E, Up)
Data correction for secular Data correction for secular displacement: two optionsdisplacement: two options
Subtract 1996-2000 Subtract 1996-2000 velocitiesvelocities
• Assumption: Assumption: postseismic postseismic deformation deformation finished by 1996 – finished by 1996 – likely true if no likely true if no viscoelastic viscoelastic deformationdeformation
• Advantage: values Advantage: values based on actual based on actual measurementsmeasurements
Subtract predicted Subtract predicted MIT block model MIT block model velocitiesvelocities
• Based on 1988-2005 Based on 1988-2005 GPS measurements to GPS measurements to fit large-scale fit large-scale block model for block model for eastern eastern Mediterranean Mediterranean regionregion
• Advantage: data Advantage: data from entire from entire earthquake cycleearthquake cycle
• Disadvantage: rough Disadvantage: rough fit, not meant for fit, not meant for smaller scalesmaller scale
Earthquake afterslipEarthquake afterslip Motion on a fault after an earthquake due to Motion on a fault after an earthquake due to
stresses induced by the earthquakestresses induced by the earthquake Happens on coseismic fault; sometimes also on Happens on coseismic fault; sometimes also on
adjacent faultsadjacent faults Usually occurs where coseismic slip was at a Usually occurs where coseismic slip was at a
minimumminimum Occurs at shallow depths in zone of velocity Occurs at shallow depths in zone of velocity
strengtheningstrengthening Begins immediately after earthquake and can last Begins immediately after earthquake and can last
for several years – modeled as logarithmic decay for several years – modeled as logarithmic decay Examples of afterslipExamples of afterslip
• Chi-Chi: Chi-Chi: 16% of coseismic moment in 15 16% of coseismic moment in 15 months months
• Northridge: Northridge: 22% of coseismic moment in 2 22% of coseismic moment in 2 yearsyears
• Loma Prieta: Loma Prieta: 10% of coseismic moment in 5 10% of coseismic moment in 5 yearsyears
Afterslip inverse modelingAfterslip inverse modeling
Kinematic model inverting for fault Kinematic model inverting for fault displacement in an elastic half-space using displacement in an elastic half-space using displacements on Earth's surfacedisplacements on Earth's surface
Green‘s functions, Green‘s functions, GG, are calculated on each , are calculated on each fault tile to relate slip to each GPS fault tile to relate slip to each GPS displacementdisplacement
Smoothing parameter, Smoothing parameter, ßß, facilitates trade-off , facilitates trade-off between best fit to data and a smoothly between best fit to data and a smoothly varying solution by minimizing:varying solution by minimizing:
||||WW((GGss--dd)||)||22 + + ßß2 2 ||||LLss||||22
(misfit)(misfit) (roughness) (roughness)ssii is slip on each fault tileis slip on each fault tileddjj is displacement at each GPS site is displacement at each GPS site
L is the Laplacian operatorL is the Laplacian operatorWWTTWW = ∑ = ∑-1-1 (data covariance matrix) (data covariance matrix)
Fault plane resolution testsFault plane resolution tests Forward modeled checkerboard slip distribution to Forward modeled checkerboard slip distribution to
GPS sitesGPS sites Inverted for slip using forward modeled Inverted for slip using forward modeled
displacement vectorsdisplacement vectors
Modeled Afterslip Plane
SLIP INPUT
INVERSION OUTPUT
Racha Hypocenter
SURFACE
DEPTH
40 K
M
120 KM
Afterslip 1991-1994Afterslip 1991-1994 Subtracting 1996-2000Subtracting 1996-2000
• 90% error reduction90% error reduction
• 35% coseismic moment35% coseismic moment
max slip: 35 cmmax slip: 35 cm
Subtracting block Subtracting block modelmodel• 66% error reduction66% error reduction
• 28% coseismic moment28% coseismic moment
max slip: 45 cmmax slip: 45 cm
SURFACE
DOWN DIP
1991-1994 afterslip with coseimic slip 1991-1994 afterslip with coseimic slip distributionsdistributions
Using data subtracting 1996-2000 velocities
Using data subtracting block model
Coseismic model
DOWN DIP
SURFACE
Forward-modeled afterslip versus dataForward-modeled afterslip versus dataRed:Red: data with 1- data with 1-σσ errors (67% confidence interval) errors (67% confidence interval)Blue: modelBlue: model
Subtracting 1996-2000 Subtracting 1996-2000 velocitiesvelocities
Subtracting block modelSubtracting block model
Afterslip with seismicityAfterslip with seismicity• Afterslip plotted with first 2 months of Afterslip plotted with first 2 months of
aftershocksaftershocks Afterslip is from 3 months to 3 years after Afterslip is from 3 months to 3 years after
earthquakeearthquake
““shallow” aftershocks shallow” aftershocks beneath 1500m high Racha beneath 1500m high Racha RidgeRidge
QuickTimeª and aTIFF (LZW) decompressor
are needed to see this picture.
Afterslip 1994-1996Afterslip 1994-1996
Subtract 1996-2000Subtract 1996-2000
22% error reduction22% error reduction
max slip: 18 cmmax slip: 18 cm
Afterslip was likely not occurring after Afterslip was likely not occurring after 19941994
Subtract block Subtract block modelmodel
27% error reduction27% error reduction
ViscoelasticityViscoelasticity Viscoelasticity: elastic on short time Viscoelasticity: elastic on short time scale, viscous on long time scale (e.g. scale, viscous on long time scale (e.g. Earth's mantle)Earth's mantle)
Indication in lower lithosphere: seismic Indication in lower lithosphere: seismic attenuation and high heat flowattenuation and high heat flow
Maxwell viscoelastic material explained by:Maxwell viscoelastic material explained by:
ddε/dt = σ/2η + dσ/Edtε/dt = σ/2η + dσ/Edt
from which:from which:
σ = σσ = σ00exp(-Et/2η) exp(-Et/2η)
(stress decay at 0 strain rate)(stress decay at 0 strain rate)
where:where:
σ-stress, ε-strain, η-viscosity, E-Young's σ-stress, ε-strain, η-viscosity, E-Young's modulusmodulus
Viscoelastic modelingViscoelastic modeling Basis: P and S attenuation in lower crust Basis: P and S attenuation in lower crust of Caucasus of Caucasus
Used code to forward model response of Used code to forward model response of coseismic slip using different viscosities coseismic slip using different viscosities and layer thicknessesand layer thicknesses
Best model:Best model:
• 4e+17 Pa s for bottom 4e+17 Pa s for bottom
20 km of crust20 km of crust
• Only 21% error reduction Only 21% error reduction
Viscoelastic relaxation not responsible for Viscoelastic relaxation not responsible for early postseismic deformationearly postseismic deformation
SummarySummary Eight GPS sites produced sparse time series of nine-year Eight GPS sites produced sparse time series of nine-year
postseismic period of 1991 Racha earthquakepostseismic period of 1991 Racha earthquake Logarithmic decay in position measurements from three Logarithmic decay in position measurements from three
sites indicate postseismic deformationsites indicate postseismic deformation Two methods of correcting data for secular motions Two methods of correcting data for secular motions
produced similar afterslip inversions over 1991-1994:produced similar afterslip inversions over 1991-1994:
• shallow aseismic afterslipshallow aseismic afterslip
• 65-90% error reduction65-90% error reduction
• ~30% of coseismic moment~30% of coseismic moment No evidence for afterslip post-1994No evidence for afterslip post-1994 No evidence for viscoelastic relaxation in 1991-1994No evidence for viscoelastic relaxation in 1991-1994 Afterslip dominated Racha deformation as anticipated by Afterslip dominated Racha deformation as anticipated by
studies of similar earthquakesstudies of similar earthquakes A viscoelastic layer may be in the lower lithosphere, but A viscoelastic layer may be in the lower lithosphere, but
Racha event not strong enough to activate itRacha event not strong enough to activate it
Thank YouThank You
Velocity calculation from raw dataVelocity calculation from raw data
Displacements found by Displacements found by differencing measurements differencing measurements relative to station SACC relative to station SACC located near fault on footwalllocated near fault on footwall
Secular displacements corrected Secular displacements corrected by subtracting velocities from by subtracting velocities from the 1996-2000 time periodthe 1996-2000 time period
Errors found by summing squares Errors found by summing squares of errors used in differencing of errors used in differencing measurementsmeasurements
Fault afterslipFault afterslip Inverse modeling in an elastic half-Inverse modeling in an elastic half-space with Poisson‘s ratio of 0.25space with Poisson‘s ratio of 0.25
Green‘s functions, Green‘s functions, GG, are calculated , are calculated on each fault slip tileon each fault slip tile
Roughness, Roughness, LL, of inversion result is , of inversion result is minimized by applying smoothing minimized by applying smoothing factor, factor, ßß, and minimizing weighted , and minimizing weighted residual sum of squares (WRSS):residual sum of squares (WRSS):
||||WW((GsGs--dd)||)||22 + + ßß2 2 ||||LsLs||||22
where:where:
ssii is slip on each fault tileis slip on each fault tile
ddjj is displacement at each GPS is displacement at each GPS sitesite
WWTTWW = ∑ = ∑-1-1 (data covariance matrix) (data covariance matrix)
Determine smoothingDetermine smoothing
Choose Choose smoothing smoothing where where curvature of curvature of misfit vs. misfit vs. roughness roughness graph is graph is greatestgreatest
Afterslip fault planes & Afterslip fault planes & aftershocksaftershocks
Afterslip inversion resultAfterslip inversion result
Smoothing = 5.8Smoothing = 5.8
EQEQ
slipslip
Smoothing = 10.0Smoothing = 10.0
Comparison of inversion and dataComparison of inversion and data(BLUE: model, RED: data)(BLUE: model, RED: data)
All stationsAll stations Close up near Close up near faultfault
Viscoelastic relaxation codeViscoelastic relaxation code
Code forward models response of Code forward models response of earth to earthquake stressesearth to earthquake stresses
Uses spherical layers with Uses spherical layers with variable density, bulk modulus, variable density, bulk modulus, shear modulus, and viscosityshear modulus, and viscosity
Calculates spherical harmonic Calculates spherical harmonic expansion of spheroidal and expansion of spheroidal and toroidal motion components toroidal motion components
Viscoelastic relaxation vs. fault Viscoelastic relaxation vs. fault afterslip afterslip
Viscosity = 10Viscosity = 101717 Pa s (below Pa s (below 16km)16km)
Things to do…Things to do…
Confirm that investigating only Confirm that investigating only 1991-1994 is adequate1991-1994 is adequate
Do more modeling of Do more modeling of viscoelastic relaxation to gain viscoelastic relaxation to gain clearer picture of what clearer picture of what viscosity is needed to fit dataviscosity is needed to fit data
Perhaps try viscoelastic Perhaps try viscoelastic modeling of 1994-1996 modeling of 1994-1996 deformationdeformation