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・ Rays Snell ’ s Law Structure of the Earth ・ Seismic Waves Near-Field Terms (Static Displacements) Far-Field Terms (P, S, Surface waves) ・ Normal modes Free oscillations of the Earth II.1 Theoretical Seismology 2: Wave Propagation
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Seismic waves Faulting
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Homogeneous Earth
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Structure in the Earth Crust-Mantle Core-Mantle 440 km 660 km
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Snell’s Law Fermat’s Principle 11 22 sin 1 / sin 2 = n 21 Air Water Rays
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11 22 1 < 2 Ray Paths in a Layered Medium 11 22 1 > 2 S lower Faster Slower
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11 22 33 Ray Paths in a Layered Medium 1/ 1 1/ 2 1/ 3 Distance Time
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Andrija Mohorovicic (1857-1936) Found seismic discontinuity at 30 km depth in the Kupa Valley (Croatia). Mohorovicic discontinuity or ‘Moho’ Boundary between crust and mantle Moho
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Forward Branch Backward Branch
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Forward Branch Backward Branch Forward Branch Shadow Zone
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Forward Branch Backward Branch Forward Branch Shadow Zone PcP ・ 1912 Gutenberg observed shadow zone 105 o to 143 o ・ 1939 Jeffreys fixed depth of core at 2898 km (using PcP) Forward Branch Backward Branch Forward Branch P PcP PKP Shadow Zone
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PcP Core Reflections
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Aspects of Waves not Explained by Ray Theory ・ Different types of waves (P, S) ・ Surface Waves ・ Static Displacements ・ Frequency content Seismic Waves
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Wave Equation 1-D wave equation c = propagation speed Slinky: constant velocity wave propagation, no mass transfer, different from circulation eq.
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1-D Wave Equation LW 3.2.1 T = wave period = angular frequency Solution
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Wave Period and Wavelength wavelength 300 km Velocity 6 km/s Velocity = Wavelength / Period x t wavelength period Space Time period 50 s frequency = 1/period= 0.02 hz
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Body waves ( P ・ S ) 0.01 to 50 sec50 m to 500 km Surface waves 10 to 350 sec30 to 1000 km Free Oscillations 350 to 3600 sec1000 to 10000 km Static Displacements - PeriodWavelength
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3-D Wave Equation with Source sourcespatial 2nd derivative Solution Near-field Terms (Static Displacements) Far-field Terms (P, S Waves)
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Near-field terms ・ Static displacements ・ Only significant close to the fault ・ Source of tsunamis r/ r/ t →t → r/ r/
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Static Displacements Bei-Fung Bridge near Fung-Yan city, 1999 Chi-Chi, Taiwan earthquake
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Static displacements Co-seismic deformation of 2003 Tokachi-oki Earthquake (M8.0)
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Generation of Tsunami from Near-field Term
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Far-field Terms ・ Propagating Waves ・ No net displacement ・ P waves ・ S waves
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Surface Waves S Shearer, Fig. 8.1 Period (sec) Love Rayleigh
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January 26, 2001 Gujarat, India Earthquake (Mw7.7) Recorded in Japan at a distance of 57 o (6300 km) Love Waves vertical radial transverse Rayleigh Waves
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Normal Modes (Daishinji, Fukui Prefecture) Free Oscillations of the Earth 1960 Chile Earthquake Useful for studies of ・ Interior of the Earth ・ Largest earthquakes (Stein and Gellar 1978)
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Toroidal and Spheroidal Modes Toroidal Spheroidal Dahlen and Tromp Fig. 8.5, 8.17
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Natural Vibrations of the Earth Shearer Ch.8.6 Lay and Wallace, Ch. 4.6
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Houseman http://earth.leeds.ac.uk/~greg/?Sphar/index.html Free Oscillations l=1 m=1
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Houseman http://earth.leeds.ac.uk/~greg/?Sphar/index.html Free Oscillations l=1 m=2
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Houseman http://earth.leeds.ac.uk/~greg/?Sphar/index.html Free Oscillations l=1 m=3
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Summary Rays Earth structure causes complicated ray paths through the Earth (P, PKP, PcP) Wave theory explains ・ P and S waves ・ Static displacements ・ Surface waves Normal Modes The Earth rings like a bell at long periods
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Why are observed seismograms so messy ?
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Structure: Free Surface Earth is a not homogenous whole-space Free surface causes many complications - surface waves - reflections (pP, sP, sS)
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