・ Rays Snell ’ s Law Structure of the Earth ・ Seismic Waves
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Transcript of ・ Rays Snell ’ s Law Structure of the Earth ・ Seismic Waves
・ 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
Magnitude for Local Tsunami(Example)JMA Magnitude (Tsuboi, 1954) M=log 10A + 1.73 log10 Δ - 0.83 A : Half of maximum total amplitude [μm] Δ : Epicentral distance [km]
Seismic waves
Faulting
Travel Time and Distance
Homogeneous Earth
1
2
1 < 2
Ray Paths in a Layered Medium
1
2
1 > 2
S lower
Faster
Faster
Slower
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
1
2
3
Ray Paths in a Layered Medium
1/1
1/2
1/3
Distance
Time
Structure in the Earth
Crust-MantleCore-Mantle
440 km660 km
Forward Branch
Backward Branch
Forward Branch
Backward Branch
Forward Branch
Shadow Zone
Forward Branch
Backward Branch
Forward Branch
Shadow Zone
PcP
・ 1912 Gutenberg observed shadow zone 105o to 143o
・ 1939 Jeffreys fixed depth of core at 2898 km (using PcP)
ForwardBranch
BackwardBranch
ForwardBranch
PPcP
PKP
Shadow Zone
PcP
Core Reflections
Why are observed seismograms so complicated ?
Structure: Free Surface Earth is a not homogenous whole-space
Free surface causes many complications - surface waves - reflections (pP, sP, sS) depth phase
Surface Wave and Maximum Amplitude
Observed in Japan.Δ=57(deg)
Max Amp., 40 min after occurrence.
(Ms, 20 deg Δ 160 deg)≦ ≦
Seismogram of a distant earthquakeSeismogram of a distant earthquake
( LR: Rayleigh wave, LQ: Love wave )Fig.16
January 26, 2001 Gujarat, India Earthquake (Mw7.7)
Recorded in Japan at a distance of 57o (6300 km)
Love Waves
vertical
radial
transverse
Rayleigh Waves
Aspects of Waves not Explained by Ray Theory
・ Different types of waves (P, S) ・ Surface Waves ・ Static Displacements ・ Frequency content
Seismic Waves
Body waves ( P ・ S ) 0.01 to 50 sec 50 m to 500 km
Surface waves 10 to 350 sec 30 to 1000 km
Free Oscillations 350 to 3600 sec (6 min to 1 hour)
1000 to 10000 km
Static Displacements -
Period Wavelength
Static Displacements
Bei-Fung Bridge near Fung-Yan city, 1999 Chi-Chi, Taiwan earthquake
Static displacements
Co-seismic deformationof 2003 Tokachi-okiEarthquake (M8.0)
Houseman http://earth.leeds.ac.uk/~greg/?Sphar/index.html
Free Oscillations l=1 m=1
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
Thank you for your attention
Snell’s LawFermat’s Principle
1
2 sin 1 / sin 2 = n21
Air
Water
Rays
Wave Equation
21
2
21
12 1
tu
cxu
1-D wave equation c = propagation speed
Slinky: constant velocity wave propagation, no mass transfer, different from circulation eq.
1-D Wave Equation 21
2
21
12 1
tu
cxu
LW 3.2.1
2
T T = wave period = angular frequency
)]/(sin[),( cxtAtxu
Solution
Wave Period and Wavelength
wavelength 300 km
Velocity 6 km/s
Velocity = Wavelength / Period
x
t
wavelength
period
Space
Time
period 50 sfrequency = 1/period= 0.02 hz
)()()2(2
2
uuftu
3-D Wave Equation with Source source spatial 2nd derivative
Solution
dtM
rAtxu
r
r
N )(14
1),(/
/ 04 )(14
1)(14
1022022
rtMr
ArtMr
A ISIP
)(14
1)(14
10303
rtMr
ArtMr
A FSFP
Near-field Terms (Static Displacements)
Far-field Terms (P, S Waves)
Near-field terms
・ Static displacements
・ Only significant close to the fault
・ Source of tsunamis
r/ r/
t →r/ r/
Far-field Terms
・ Propagating Waves
・ No net displacement
・ P waves
・ S waves
)(14
1)(14
10303
rtMr
ArtMr
A FSFP
Surface Waves
S
Shearer, Fig. 8.1
Period (sec)
Love
RayleighGr
oup
Velo
city
(km
/sec
)
Generation of Tsunami from Near-field Term
Normal Modes Normal Modes
(Daishinji, Fukui Prefecture)(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)
Houseman http://earth.leeds.ac.uk/~greg/?Sphar/index.html
Free Oscillations l=1 m=2
Houseman http://earth.leeds.ac.uk/~greg/?Sphar/index.html
Free Oscillations l=1 m=3
Toroidal and Spheroidal Modes
ToroidalSpheroidal
Dahlen and Tromp Fig. 8.5, 8.17
Natural Vibrations of the Earth
Shearer Ch.8.6Shearer Ch.8.6Lay and Wallace, Ch. 4.6Lay and Wallace, Ch. 4.6