Earthquake seismology Fence offset by the 1906 San Francisco earthquake The San Andreas fault in the Carrizo plain, California Offset drainage along the San Andreas fault, Wallace Creek, California Elastic strain accumulation • GPS-derived velocities in Southern California (19922000). Velocities are shown with respect to North America. The active faults of California are shown in orange. • (Most) faults are locked between earthquakes The area around faults accumulates elastic strain The seismic cycle • Between earthquakes: – – • During an earthquake: – – • Faults are locked Area around faults accumulate deformation A fault slips suddenly The deformation accumulated around the fault is released After an earthquake: – – Stresses around the fault are modified Readjustments on the fault plane = aftershocks The seismic cycle Click for earthquake cycle animation Between earthquakes: – Faults are locked – Area around faults accumulate deformation Anim ation: R. Stein, USGS During an earthquake: – A fault slips suddenly – The deformation accumulated around the fault is released – Stresses around the fault are modified Earthquake seismology • • • • • Location of the earthquake (hypocenter)? Frequency of similar earthquakes? Focal mechanism? Rupture mechanism? Size? – – – – Intensity Magnitude Moment Energy release • Earthquake triggering? Locating earthquakes Difference in travel time for P and S waves increases with increasing epicentral distance: tS = D VS tP = D VP $1 1 ' " t S # t P = D& # ) V V % S P ( VP = 5.85 km / s " D = ( t S # t P ) * 8.0 VS = 3.38 km / s Locating earthquakes • With at least 3 stations: – – – – Calculate S-P time difference Convert to distance Draw circles centered on stations Location = intersection of circles • Errors: – Picking arrivals – Actual travel times are slightly different from theoretical ⇒ location is dependent on the Earth model used (global or local). Earthquake focal mechanisms • Earthquake = release of accumulated elastic energy by displacement on a fault • Problem: what type of fault motion? • Case of a strike-slip fault: particle motion due to fault slip: – Blue quadrants: particles pushed away from the focus ⇒ compressional first motion = UP – Red quadrants: particles pulled towards the focus ⇒ dilatational first motion = DOWN • As a result, we obtain 4 quadrants: – 2 compressional quadrants: first motion down – 2 extensional quadrants: first motion up compressional first motion dilatational first motion tension axis compression axis extensional quadrant compressional quadrant compressional quadrant extensional quadrant auxiliary plane fault plane Earthquake focal mechanisms • • • Earthquake = release of accumulated elastic energy by displacement on a fault Problem: what type of fault motion? Let’s assume an earthquake on a reverse fault: – Compressional / tensional quadrants – Compressional quadrant: surface is pulled down ⇒ first motion DOWN – Tensional quadrant: surface is pushed up ⇒ first motion UP • If we map first motion, we can find: – 2 focal planes – P- and T-axis Earthquake focal mechanisms • • • • Seismic rays travel away from the focus Each ray “samples” a dilatational or compressional quadrant around the focus Seismic stations at different distances record up or down first motions Rays along nodal planes? in cross-section focal mechanism (stereonet proj.) Earthquake focal mechanisms • The “focal sphere”: – Center = earthquake hypocenter – In each quadrant: first motion identical • Seismic stations are at the surface, (usually) not underground – Rays bend upward and eventually reaches a seismic station at the surface – The important parameter is the initial take-off angle – Take-off angle can be calculated knowing the earth’s structure => accuracy of focal mechanisms depend on our knowledge of the Earth structure (local, regional, global) The focal sphere: Earthquake focal mechanisms • Strike-slip faulting: – Vertical focal planes – Horizontal P-axis and T-axis • Other types of faulting: – Focal planes will have a dip – P-axis and T-axis will have a dip • For representation: focal sphere + stereographic projection of focal planes and P-T-axis ⇒ “Beach balls” In the horizontal plane: Earthquake focal mechanisms reverse • • • • Focal mechanisms define the type of faulting that occurred during the earthquake. The actual fault plane is ambiguous Focal mechanisms can combine these types of faulting. Focal mechanisms in an actively deforming area contain information about the strain regime normal strike-slip Earthquake focal mechanisms Earthquake focal mechanisms • Eastern Mediterranean • Earthquake focal mechanism illustrate: – Strike-slip faulting – Reverse faulting – Extensional faulting • Compare with GPS velocities (McClusky et al., JGR, 2000) Earthquake rupture • • • An earthquake usually breaks a segment of a fault The rupture does not always reach the surface The earthquake is followed by aftershocks: – Readjustments on the rupture plane – Help define the rupture plane Animation http://www.scecdc.scec.org/northreq.html Northridge earthquake, January 1994, M=7.2 Earthquake rupture • • • Time and space history of a rupture, example of the Northridge earthquake Slip on the rupture plane is not homogeneous Asperities and barriers Animation D. Wald, http://www.scecdc.scec.org/northrup.html Earthquake size -F • Shear forces on a faults ⇒ moment • Hooke’s law relates stress and strain for elastic solids: for shear, proportionality factor is rigidity µ b F Rupture area: A = L x W MO = 2bF " shear = µ # $shear with $shear = d 2b and " shear = F F = A L #W % MO = µAd Moment = rigidity x displacement x rupture area ! Earthquake magnitude • • 1935: Richter worked on ranking earthquakes as a function of their size First definition: – “Maximum amplitude recorded at 100 km from the epicenter”: ML=log10(Amax) + 3 log10Δ - 2.92 – For local earthquakes: S-waves have the largest amplitude – Correction for distance: Δ (= angular epicentral distance in degrees) • Richter magnitude scale: • • • Open scale Largest magnitude recorded = Chile, 1960, MW=9.6 (MS=8.3) Negative magnitudes are possible… nomogram used to compute magnitude quickly by eye Earthquake magnitude • ML = local magnitudes (~ 600 km from earthquake) • At larger distances: – Using surface waves (they have the largest amplitude) MS = log10(Amax/T)+1.66 log10Δ + 3.3 A=max. amplitude of vertical component in microns, T = period in seconds, D = angular distance in degrees. – Using body-waves (P-waves) mb = log10(Amax/T)+0.01 Δ + 5.9 – Ms – mb relationship: mb = 0.56 MS + 2.9 Earthquake magnitude • • • • Spectrum of seismogram gives spectral amplitude at all frequencies Static moment = amplitude at low frequencies Corner frequency depends on duration of rupture time TD and and rise time TR Above corner frequency – there is destructive interference – Shaking cannot get higher amplitude but continues in time longer • As a result: – Ms saturates at 8.3 – mb saturates at 6.2 • Use of moment magnitude: MW = (2/3) log10MO – 10.7 2/TR 2/TD Earthquake magnitude • Less than 3.5: Generally not felt, but recorded. • 3.5-5.4: Often felt, but rarely causes damage. • Under 6.0: At most slight damage to well-designed buildings. Can cause major damage to poorly constructed buildings over small regions. • 6.1-6.9: Can be destructive in areas up to about 100 kilometers across where people live. • 7.0-7.9: Major earthquake. Can cause serious damage over larger areas. • 8 or greater: Great earthquake. Can cause serious damage in areas several hundred kilometers across. Earthquake size • Logarithmic relationship between magnitude and: – Coseismic displacement: M5=1 cm, M8=10m – Rupture length: M5=1 km, M8=400 km • Large earthquakes have a MUCH LARGER rupture displacement and length than smaller ones Energy release • Energy release: log10 E = 4.4 + 1.5M S • Increase of one level of magnitude corresponds to: ! ⇒ Amplitude increase: 101 = 10 ⇒ Energy increase: 101.5 ≈ 30 • Energy release increases very rapidly with magnitude Largest Earthquakes in the World Since 1900 1. 2. 3. 4. 5. 6. 7. 8. 9. 10. 11. 12. Chile - 1960 05 22 - 9.5 (Ms = 8.5) Prince William Sound, Alaska - 1964 03 28 - 9.2 (Ms = 8.3) Off the West Coast of Northern Sumatra - 2004 12 26 - 9.0 Kamchatka - 1952 11 04 - 9.0 Off the Coast of Ecuador - 1906 01 31 - 8.8 Northern Sumatra, Indonesia - 2005 03 28 - 8.7 Rat Islands, Alaska - 1965 02 04 - 8.7 Andreanof Islands, Alaska - 1957 03 09 - 8.6 Assam - Tibet - 1950 08 15 - 8.6 Kuril Islands - 1963 10 13 - 8.5 Banda Sea, Indonesia - 1938 02 01 - 8.5 Chile-Argentina Border - 1922 11 11 - 8.5 Visit: http://neic.usgs.gov/ Earthquake frequency • There are far more small earthquakes than large ones • Many small earthquakes are not detected • Gutenberg-Richter law: – Linear relationship between log[number of earthquakes] and magnitude: LogN = a – b x M – Slope = ‘b-value’ • Worldwide average is 1.0 • May vary regionally • Lab. experiments show: – – High stress ⇒ low b (less small eqs) Low stress ⇒ high b (more small eqs) • Empirical tool for seismic hazard studies Earthquake frequency The USGS estimates that several million earthquakes occur in the world each year. Many go undetected because they hit remote areas or have very small magnitudes. The NEIC now locates about 50 earthquakes each day, or about 20,000 a year. Earthquake information: http://neic.usgs.gov/ Descriptor Magnitude Average Annually Great 8 and higher 1 M ajor 7 - 7.9 18 Strong 6 - 6.9 120 M oderate 5 - 5.9 800 Light 4 - 4.9 6,200 (estimated) M inor 3 - 3.9 49,000 (estimated) Very M inor < 3.0 M agnitude 2 - 3: about 1,000 per day M agnitude 1 - 2: about 8,000 per day Frequency of occurrence of earthquakes based on observations since 1900 Intensity • • • Qualitative description of earthquake size Based on damage assessment ⇒ Mercalli scale Can be severely biased – – – • Area with local amplification of seismic waves or secondary effects such as liquefaction Subjective reports from people Depends on vulnerability Often the only information available for historical earthquakes Seismic hazard • Earthquake damage: – Ground acceleration, in g (up to 2 g) – Secondary effects: liquefaction, landslides, fires, etc • Seismic risk = seismic hazard ⊗ vulnerability • Seismic hazard = seismic potential (When? Where? What size?) ⊗ propagation of seismic waves – Seismic potential = probability for an earthquake of a given size to occur – Propagation = attenuation of seismic waves, site response • Seismic hazard = probability to exceed a given acceleration for a given time period Seismic potential • Derived from GutembergRichter law, tailored for the are under study • Requires earthquake catalog ⇒ b value • Can be complemented by information on active fault: geometry, slip rate • Can be complemented by geodetic information: strain rate Attenuation • Amplitude of seismic waves is attenuated: – Geometric attenuation – Intrinsic attenuation – Attenuation relationship: determined empirically • Many different attenuation relationships are available: – Quantity of available data – Geological nature of the terrain: amplification or damping Site response • Ground acceleration decreases with distance, but can vary by a factor of 10 for 2 sites at the same distance to an earthquake ⇒ site response • Site response depends on geological factors: – Softness of soil or rocks near the surface: ground motion amplified by soft rocks – Sediment thickness above bedrock: ground motion amplified by thick sediments Snapshots of simulated wave propagation in the LA area for the hypothetical SAF earthquake (K. Olsen, UCSB) Final result: seismic hazard maps • Peak acceleration that has a 2% probability to be exceeded in 50 years • Compare New Madrid and California! What have we learned? • • • Active faults are (usually) locked between earthquakes, while the area around them is accumulating elastic strain. An earthquake is the sudden release of the elastic strain accumulated over decades. The earthquake results in: – A rupture, that may sometimes reach the surface – Seismic waves, that propagate away from the rupture area • Using seismic wave, one can figure out: – – – – • The location of the earthquake The type of fault motion (focal mechanism) The magnitude of the event (energy released) The slip distribution on the rupture plane Magnitude scale: – Is not linear but power law – Gutemberg-Richter law: N = a –b M • Earthquake hazard depends on source, attenuation, and site response What have we learned? • One can use seismic waves generated artificially to image deep structures: – Seismic reflection: • Receiver and source close • Arrivals describe hyperbolas – Seismic refraction: • Receiver and source far apart • Arrivals describe straight lines • Data collection, processing (increase SNR and remove artefacts), interpretation • Applications: oil exploration, sequence stratigraphy, etc.