Seismology Orals
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Transcript of Seismology Orals
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INTRODUCTION to
SEISMOLOGY
Ashley Shuler
Orals Prep 2008-2009
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What is Seismology?
The study of wave propagation and what it tells usabout the structure of the Earth and the physics ofEarths deep interior.
We study earthquakes which radiate seismicwaves that travel throughout the Earth, causingground motion that is measured on sensitiveinstruments. Sometimes we use explosions (activevs. passive source).
Seismology has many applications includinghazards, exploration and nuclear monitoring.
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Where Do Earthquakes Occur?
Earthquakes occur on faults and along plateboundaries.
The earths surface is composed of a smallnumber of rigid plates that drift slowly over
geologic time. Their relative motions along theirboundaries give rise to earthquakes.
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Types of Faults
Just as there are 3 kinds ofplate boundaries, there are 3types of faults.
Normal faults occur in
extensional environments(rifts, mid-ocean ridges).Thrust faults occur in
compressive environments(subduction zones), andstrike-slip faults occur intransform environments.
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Earthquakes are not point sources, but occur
along planes. Earthquakes have a finiterupture velocity, which is generally .8*shear
velocity.
There hypocenter is where the earthquake
begins. The epicenter is the surface
projection of the hypocenter.
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Earthquake Sources
Earthquakes are double-couple sources.
Different types of earthquakes produce differentradiation patterns and have different momenttensors. These differences can be visually
displayed with focal mechanisms.
They are made from the radiation pattern of P-waves. They are plotted on the lower hemisphereof an imaginary sphere surrounding the source.
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Focalmechanisms are
made from thefirst motions ofearthquakes.
There is some
ambiguityconcerningwhich plane isthe true fault
plane. Moreinformation isneeded.
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Elastic Rebound Theory
Earthquakes arecaused by the slowaccumulation ofshear stress and
strain that issuddenly released bymotion along a fault
(producingpermanentdisplacement).
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Stress and Strain
Stress is the internalforces between partsof a medium. Strainis related todeformation. Thesequantities are linkedby a constitutive
relationship, andthrough elasticparameters.
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Some math
Homogeneous
equation of motion
Vector equation
Solutions give the P
and S wavevelocities (dependent
on density and
elastic parameters)
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Body Waves
Body waves travel through volumes of the Earth(P and S waves).
P waves have displacement in the direction ofpropagation (compressional). S waves have
displacement perpendicular to the direction ofpropagation (shear) - can be broken down into SVand SH.
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Surface Waves
Surface waves are confined to the free surface. Rayleigh waves are radially polarized and are
caused by the interaction of P and SV waves at thefree surface.
Love waves are transversely polarized and aretrapped in a surface low-velocity layer.
Compared to body waves, they travel slower andhave less amplitude decay.
Surface wave velocities are frequency dependent(dispersion). In general, longer period wavestravel faster because they feel deeper.
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Phase Identification on
Seismograms P wave first,
mostly onvertial.
S wave later,on horizontals.
Love wavelater on
transverse. Rayleigh wave
last on verticaland radial.
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Waveform Notes
In a seismogram, we are seeing a convolution ofthe source-time function with the Earth responseand the instrument response.
We see body wave phases which travel at certainvelocities, and surface waves which travel atdifferent speeds depending on frequency.
Phase velocity - speed of single phase (frequency)
Group velocity - speed of wave packet (envelope)
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Normal Modes
Any finite solid willresonate at certainvibration frequencies.
The Earth hasspheroidal andtoroidal modes.
Any wave motionwithin the Earth maybe expressed as a sumof normal modes withdifferent excitations.This representation isunique.
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Ray Theory (good approximation, but doesnt fit everything)
We often consider rays
instead of wavefronts.Rays are perpendicularto wavefronts and obeySnells Law (sin
theta/v=constant) Because compressional
and shear velocitiesincrease as a function of
depth, rays turn. If there is a low-velocity
zone, we can getshadows.
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Travel-time curves
Traveltime curvesare created by
picking phases from
seismograms
recorded at varying
distances.
These tell us about
Earth structure.
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What happens at boundaries?
Waves can be transmitted or reflected atboundaries. The reflection and transmission
coefficients depend on density, wave speed,
and angle of incidence. Waves can also be converted. P can convert to
SV and vice versa.
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The amplitudes of waves change as they
propagate. If the area increases, the
amplitudes decrease (geometrical
spreading).
The amplitudes also depend on the
impedance (product of density and
wavespeeds).
Energy is also lost to attenuation through
anelastic processes such as internal friction.
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Magnitude Scales
First done in 1935 by Richter. The Richter scalewas empirical, and not related to the source. It
saturated at high magnitudes.
Today we use the moment scale (moment is the
product of rigidity, displacement, and fault area).
A M7 earthquake releases 32 times more energy
than a M6 earthquake, and 1000 times more
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Gutenberg-Richter Relationship
There is a relationshipbetween the magnitudeand the total number ofearthquakes in any
given region and time. Log N = A -bM
B is typically 1. Thismeans that there are 10
M3 earthquakes forevery M4 earthquake,etc.
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Seismic Intensity
Another measure isintensity, whichdescribes localshaking as determined
by damage tostructures andperceptions of peoplewho experienced theearthquake.
This is measured onthe Mercalli scalefrom I to XII.
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Earth Structure
Seismology allowed us to determine thepresence of the core (absence of direct Pand S arrivals at source-receiver distancesgreater than 100 degrees).
It also allowed us to determine the presenceof a solid inner core (reflections from innercore boundary in shadow zone).
We know the outer core is liquid because itcasts shadows in S-waves (shear waves donot propagate in fluids).
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P and S wave velocities Rapid velocity increases in
upper mantle, transition zonewith mineralogical phasechanges (410 and 660 km),gradual increase to CMB
At CMB, P wave velocitydrops and S velocity goes tozero. P velocity increases withdepth due to increased
pressure/temperatue P and S wave velocities
increase with depth in innercore
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Reflection Seismology
Mostly used in oceans andindustry.
Large numbers of sources
and receivers at short,regularly spaced intervals.
Looking for changes in
velocity or density
Will be discussed by Milena!
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Tomography
We often want to inverttraveltimes or full waveforms toget 3-D velocity structures.
This is complicated by noise,
limited data, nonuniformdistribution of sources/receivers,location/timing errors.
In tomography, we set up a grid,
and the travel time is the sum ofthe product of distance and1/velocity through each gridpointon the raypath from source to
receiver.
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Earthquake Location
Earthquakes are treated as pointsources during location.
A location can be approximatedusing S-P traveltimes at a few
stations. From this guess of location,
depth and origin time, wecompare the predicted arrival
times to observed. Perturb andIterate.
There are tradeoffs betweendepth and origin time.
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Instrumentation
Early seismographs were pendulums sensitive toground motion (velocity).
Modern seismographs are electromagnetic masseson a spring. The voltage required to keep the massin place is proportional to velocity.
We use broadband seismometers with a broaddynamic range.
Earthquakes are detected and located within a fewminutes of occurring in many cases. Digital data isfreely shared among many nations. There isexcellent global coverage that is always improving(both permanent and temporary stations).
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Can we predict earthquakes?
Only in a long-term statistical sense (ie 30%
chance of having M7 or greater in the next
10 years) Many seismologists doubt we will ever be
able to predict earthquakes within a
potential evacuation period - too complex,too many variables