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Geology 5660/6660 Applied Geophysics 13 Jan 2014

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Presentation on theme: "Geology 5660/6660 Applied Geophysics 13 Jan 2014"— Presentation transcript:

1 Geology 5660/6660 Applied Geophysics 13 Jan 2014
Last time: Seismic Thought Exercise • Seismic Concepts:  Velocity is distance traveled per unit time, V = x/t  Different materials have different seismic velocities!  Introduced Wavefronts & Rays  Huygen’s Principle: Every point on a wavefront can be treated as a point source for the next generation of wavelets. The wavefront at time t = x/V later is a surface tangent to the furthest point on each of these. • Thought exercise: What do wavefronts look like for a slow layer over a fast layer? For fast over slow? Read for Wed 13 Jan: Burger 1-21 (Ch 1–2.1) © A.R. Lowry 2014

2 } Seismology (A Brief Introduction)
Four Important Types of Seismic Waves: (1) P (primary) wave (Velocity VP = 4 to 14 km/s) (2) S (secondary) wave (VS = 2/5 to 3/5 VP, or 0) (3) Surface Waves (Love, Rayleigh) V slightly < VS (4) Normal Modes (Resonant “Tones”, like a bell…)  continue for months after largest earthquakes  periods of minutes to a few hours “standing waves” } Body Waves Animation 0S3 from Lucien Saviot 0S3: (25.7 minutes) 2

3 P S Surface (Love) Surface (Rayleigh)

4 Seismic waves are strain waves that propagate in a medium…
The text begins with an analogy to ripples in a pond. There is similarity in that both are described by the wave equation; both involve stress & displacements that propagate as individual particles in the medium oscillate between potential and kinetic energy states… But, A major difference is rheology. Stress, displacement & strain in a solid continuum are governed by Hooke’s Law.

5 Elastic Rheology (Hooke’s Law):
Stress (= force per unit area)  and Strain (= change in shape)  are linearly related via  = c  where c is an elastic coefficient (a material property). Strain is a spatial derivative of displacement u described by (in 1-D),

6 A quick “review” of various strains and their elastic constants:
Uniaxial compression: Elongation (change in length l) (strain) xx yy Young’s modulus E:  = E applied  (elastic constant) Poisson’s ratio : (elastic constant) (0 <  < 0.5) For dilatation  (change in volume V/V0): Bulk modulus K = P/(where P is pressure) (strain) (elastic constant) applied s Rigidity modulus  = s/  = tan (elastic constant) (strain)


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