Observational Seismology
Lecture 4 Surface Waves and Dispersion
GNH7/GG09/GEOL4002 EARTHQUAKE SEISMOLOGY AND EARTHQUAKE HAZARD Surface Wave Dispersion
GNH7/GG09/GEOL4002 EARTHQUAKE SEISMOLOGY AND EARTHQUAKE HAZARD Observations
stretched stretched dispersed
PS SS SSS wave packet surface waves
Body waves Impulsive, short period (but later arrivals are stretched out due to attenuation). Higher frequencies make waves “sharper”.
Surface waves Dispersed, arrive in wave packets. But note a wave packet might be a single wavelet (oceanic arrivals).
GNH7/GG09/GEOL4002 EARTHQUAKE SEISMOLOGY AND EARTHQUAKE HAZARD Reminder
Period T Phase velocity v = f λ Amp f – frequency = 1/T (s-1) λ - wavelength (m) t
But a whole spectrum of different period or frequency waves are emitted from an earthquake because earthquake rupture is a complex fracture process.
GNH7/GG09/GEOL4002 EARTHQUAKE SEISMOLOGY AND EARTHQUAKE HAZARD Body waves
Body waves all travel at the same velocity even if they are different frequencies, as travelling through the body of the Earth where velocity changes are gradual (except for major discontinuities).
Reminder
1/ 2 α ⎛ 4 ⎞ K S + µ. = ⎜ 3 ⎟ ⎜ ρ ⎟ ↓v increasing ⎝ ⎠
1/ 2 β ⎛µ ⎞ = ⎜ ⎟ ⎝ ρ ⎠
Velocity just depends on local elastic properties, e.g, of core or mantle
GNH7/GG09/GEOL4002 EARTHQUAKE SEISMOLOGY AND EARTHQUAKE HAZARD Types of surface waves
Love wave
Rayleigh wave
GNH7/GG09/GEOL4002 EARTHQUAKE SEISMOLOGY AND EARTHQUAKE HAZARD Surface waves
Surface waves travel close to surface
depth z Amplitude of surface waves decays exponentially with depth
Amplitude −Z Z0 A(z) = A0 e Characteristic depth Amplitude at surface of penetration
At Z = Z0 A(z) = A0 / e ~ A0 / 2 i.e., the amplitude at the characteristic depth of penetration is approx. half surface amplitude
GNH7/GG09/GEOL4002 EARTHQUAKE SEISMOLOGY AND EARTHQUAKE HAZARD Particle motion of Rayleigh waves rolling surface wave
Retrograde ellipse
amplitude decays -Z A = A /2 exponentially 0 0 with depth
Characteristic depth of penetration is proportional to wavelength of surface wave
Z0 ∝λ∝T ∝ 1/f - the longer wavelength the deeper it will penetrate e.g., for T = 20s, v ∼ 4km/s, then λ∼80km, c.f. lithospheric thickness
GNH7/GG09/GEOL4002 EARTHQUAKE SEISMOLOGY AND EARTHQUAKE HAZARD Dispersion Short T Long T Short λ Long λ High f Low f surface Low speed Moho lithosphere High speed
Penetrates deeply into high speed layer so will travel faster
So long period waves, as they penetrate deeply into the Earth travel at higher velocities; short period waves travel at slower velocities This is normal dispersion
GNH7/GG09/GEOL4002 EARTHQUAKE SEISMOLOGY AND EARTHQUAKE HAZARD Dispersion measured from seismograms
Surface waves are a complex superposition of simple harmonic waves. Complex because earthquake source and lithospheric structure are complex. Oceanic Dispersion Rayleigh wave
Long T This peak travels at group velocity vG arrives first
They travel at a group velocity because each peak can represent a group of S.H.M.
GNH7/GG09/GEOL4002 EARTHQUAKE SEISMOLOGY AND EARTHQUAKE HAZARD Types of dispersion a) v gradually increasing with depth v Long T arrives fist Long period travelling at high velocity
z Normal dispersion b) v gradually decreasing with depth v Short T arrives first
Long period travelling at low velocity z Reverse dispersion
GNH7/GG09/GEOL4002 EARTHQUAKE SEISMOLOGY AND EARTHQUAKE HAZARD Types of dispersion c) velocity constant v
z Impulsive arrival - all frequencies arrive together
GNH7/GG09/GEOL4002 EARTHQUAKE SEISMOLOGY AND EARTHQUAKE HAZARD Types of dispersion
P wave velocity d) Oceanic dispersion 1.5 4 6 8 v km/s water 1.5 km/s 10 km Moho 10 km sediments oceanic crust 6-8 km/s Not Sediments smooth particularly upper mantle 8 km/s z out layering sharp Large change in velocity in just 10 km - lots of dispersion 1) Lot of Rayleigh waves because big change in velocity in short depth. Wave train very dispersed. 2) Less Love waves because no distinct layering (no distinct Moho), thinner crust. (No shear waves in water anyway.)
GNH7/GG09/GEOL4002 EARTHQUAKE SEISMOLOGY AND EARTHQUAKE HAZARD Types of dispersion
e) Continental dispersion P wave velocity “Not seen” 68 sediments (ignore) v km/s upper crust Conrad 30 km lower crust Distinct mantle 30 km Moho z 1) Less Rayleigh because smaller change in velocity in greater depth. Continents do not provide big enough velocity difference for great dispersion. not so dispersed Some low frequency, long period responding to gradual increase in v beneath Moho Airy phase responding to 6 km/s thick continental crust GNH7/GG09/GEOL4002 EARTHQUAKE SEISMOLOGY AND EARTHQUAKE HAZARD Types of dispersion
d) Continental dispersion
Trapped SH Continental crust → crust 6 km/s waves distinct layer “trap” for Love waves mantle 8 km/s
Before advent of exploration and use of aftershock seismic arrays, surface waves were the main means for determining the structure of the lithosphere on a regional scale. Surface waves directly sample the lithosphere.
GNH7/GG09/GEOL4002 EARTHQUAKE SEISMOLOGY AND EARTHQUAKE HAZARD Dispersion
Note that phase and group velocity are strongly dependent on period especially at low frequency Note that the phase velocity is faster than the group velocity
GNH7/GG09/GEOL4002 EARTHQUAKE SEISMOLOGY AND EARTHQUAKE HAZARD