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