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Earthquake
seismology
The San Andreas fault in the
Carrizo plain, California
Offset drainage along the San
Andreas fault, Wallace Creek,
California
Fence offset by the 1906 SanFrancisco earthquake
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Elastic strain
accumulation
(Most) faults are locked
between earthquakes
The area around faults
accumulates elastic strainGPS-derived velocities in Southern California (1992-2000). Velocities are shown with respect to North
America. The active faults of California are shown in
orange.
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The seismic
cycle
Between earthquakes:
Faults are locked
Area around faults accumulate deformation
During an earthquake: 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
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The seismic cycle
During an earthquake:
A fault slips suddenly
The deformation accumulated around the
fault is released
Stresses around the fault are modified
Between earthquakes:
Faults are locked
Area around faults accumulate deformation
Animation: R. Stein, USGS
Click for earthquake cycle animation
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Earthquake seismology Location of the earthquake (hypocenter)?
Frequency of similar earthquakes?
Focal mechanism? Rupture mechanism?
Size?
Intensity
Magnitude
Moment
Energy release
Earthquake triggering?
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Locating earthquakes
Difference in travel time
for P and S waves
increases with increasingepicentral distance:
tS=
D
VS
tP=
D
VP
" tS# t
P= D 1
VS
# 1V
P
$
%& '
()
VP= 5.85 km /s V
S= 3.38 km /s
" D = tS# t
P( )* 8.0
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Locating earthquakes
Errors:
Picking arrivals
Actual travel times are slightlydifferent from theoretical location
is dependent on the Earth model used
(global or local).
With at least 3 stations:
Calculate S-P time difference
Convert to distance
Draw circles centered on stations
Location = intersection of circles
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Earthquake focal
mechanisms
Earthquake = release ofaccumulated elastic energy bydisplacement on a fault
Problem: what type of fault motion? Case of a strike-slip fault: particle
motion due to fault slip:
Blue quadrants: particles pushedaway from the focus compressional first motion = UP
Red quadrants: particles pulled
towards the focus dilatationalfirst motion = DOWN
As a result, we obtain 4 quadrants:
2 compressional quadrants: firstmotion down
2 extensional quadrants: firstmotion up
dilatationalfirst motion
compressionalfirst motion
fault plane
auxiliary plane
compressional
quadrant
compressional
quadrant
extensional
quadrant
extensional
quadrant
tensionaxis
compressionaxis
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Earthquake focal
mechanisms
Earthquake = release of accumulated
elastic energy by displacement on a
fault
Problem: what type of fault motion?
Lets assume an earthquake on a
reverse fault:
Compressional / tensional quadrants
Compressional quadrant: surface ispulled down first motion DOWN
Tensional quadrant: surface is pushedup first motion UP
If we map first motion, we can find:
2 focal planes
P- and T-axis
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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.)
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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 earths structure =>
accuracy of focal mechanisms depend
on our knowledge of the Earth structure
(local, regional, global)
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Earthquake focalmechanisms
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:
The focal sphere:
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Earthquake focal mechanisms
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
reverse
normal
strike-slip
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Earthquake focal mechanisms
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Earthquake focal
mechanisms
Eastern Mediterranean
Earthquake focalmechanism illustrate:
Strike-slip faulting
Reverse faulting
Extensional faulting
Compare with GPSvelocities
(McClusky et al., JGR, 2000)
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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
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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
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Earthquake size
Shear forces on a faults
moment
Hookes law relates stress
and strain for elasticsolids: for shear,
proportionality factor isrigidity
MO= 2bF
"shear
= #$shear
with $shear
=
d
2band "
shear=
F
A=
F
L #W
% MO= Ad
Moment = rigidity x displacement x rupture area
F
-F
b
Rupture area:A = L x W
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Earthquake magnitude
1935: Richter worked on rankingearthquakes as a function of theirsize
First definition:
Maximum amplitude recordedat 100 km from the epicenter:
For local earthquakes: S-waveshave the largest amplitude
Correction for distance: (=angular epicentral distance indegrees)
Richter magnitude scale:
Open scale
Largest magnitude recorded =Chile, 1960, MW=9.6 (MS=8.3)
Negative magnitudes arepossible
ML=log10(Amax) + 3 log10- 2.92
nomogram used to compute magnitude quickly by eye
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Earthquake magnitude
ML = local magnitudes (~ 600 km from earthquake)
At larger distances: Using surface waves (they have the largest amplitude)
A=max. amplitude of vertical component in microns, T = period inseconds, D = angular distance in degrees.
Using body-waves (P-waves)
Ms mb relationship:
MS= log10(Amax/T)+1.66 log10+ 3.3
mb = log10(Amax/T)+0.01 + 5.9
mb = 0.56 MS+ 2.9
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Earthquake magnitude
2/TR 2/TD
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
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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-designedbuildings. Can cause major damage to poorlyconstructed buildings over small regions.
6.1-6.9: Can be destructive in areas up to about 100kilometers across where people live.
7.0-7.9: Major earthquake. Can cause serious damageover larger areas.
8 or greater: Great earthquake. Can cause seriousdamage in areas several hundred kilometers across.
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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 andlength than smaller ones
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Energy release
Energy release:
Increase of one level of
magnitude corresponds to:
Amplitude increase: 101 = 10
Energy increase: 101.5
30 Energy release increases very
rapidly with magnitude
log10 E= 4.4 +1.5MS
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Largest Earthquakes in the World Since 1900
1. Chile - 1960 05 22 - 9.5 (Ms = 8.5)
2. Prince William Sound, Alaska - 1964 03 28 - 9.2 (Ms = 8.3)
3. Off the West Coast of Northern Sumatra - 2004 12 26 - 9.0
4. Kamchatka - 1952 11 04 - 9.05. Off the Coast of Ecuador - 1906 01 31 - 8.8
6. Northern Sumatra, Indonesia - 2005 03 28 - 8.7
7. Rat Islands, Alaska - 1965 02 04 - 8.7
8. Andreanof Islands, Alaska - 1957 03 09 - 8.6
9. Assam - Tibet - 1950 08 15 - 8.6
10. Kuril Islands - 1963 10 13 - 8.5
11. Banda Sea, Indonesia - 1938 02 01 - 8.5
12. Chile-Argentina Border - 1922 11 11 - 8.5
Visit: http://neic.usgs.gov/
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Earthquake
frequency
There are far more small earthquakesthan large ones
Many small earthquakes are not
detected Gutenberg-Richter law:
Linear relationship betweenlog[number of earthquakes] andmagnitude:
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 hazardstudies
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Earthquake
frequency
The USGS estimates that several
million earthquakes occur in the
world each year. Many goundetected 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
Major 7 - 7.9 18
Strong 6 - 6.9 120
Moderate 5 - 5.9 800
Light 4 - 4.9 6,200 (estimated)
Minor 3 - 3.9 49,000 (estimated)
Very Minor < 3.0Magnitude 2 - 3: about 1,000 per day
Magnitude 1 - 2: about 8,000 per day
Frequency of occurrence of earthquakes based on observations since 1900
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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
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Seismic hazard Earthquake damage:
Ground acceleration, ing(up to 2g)
Secondary effects: liquefaction, landslides, fires, etc
Seismic risk= seismic hazard vulnerability
Seismic hazard = seismic potential (When? Where? Whatsize?) 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 givenacceleration for a given time period
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Seismic potential
Derived from Gutemberg-Richter law, tailored forthe are under study
Requires earthquakecatalogb value
Can be complemented byinformation on activefault: geometry, slip rate
Can be complemented bygeodetic information:strain rate
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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
hyp othetical SAF earthquake (K. Olsen, UCSB)
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Final result: seismic hazard maps
Peak acceleration that has a 2% probability to be exceeded in 50 years
Compare New Madrid and California!
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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 accumulatedover 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
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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.