Earthquake Engineering GE / CEE - 479/679 Topic 13. Wave Propagation 2

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March 4, 2008 1 John Anderson: GE/CEE 479/679: Lecture 13 Earthquake Engineering GE / CEE - 479/679 Topic 13. Wave Propagation 2 John G. Anderson Professor of Geophysics

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Earthquake Engineering GE / CEE - 479/679 Topic 13. Wave Propagation 2. John G. Anderson Professor of Geophysics. Combining in F=ma. In this equation, X i is a body force acting on the point, if any. The Free Surface. SH. S-waves can have two polarizations: - PowerPoint PPT Presentation

Transcript of Earthquake Engineering GE / CEE - 479/679 Topic 13. Wave Propagation 2

Page 1: Earthquake Engineering GE / CEE - 479/679 Topic 13. Wave Propagation 2

March 4, 2008 1 John Anderson: GE/CEE 479/679: Lecture 13

Earthquake EngineeringGE / CEE - 479/679

Topic 13. Wave Propagation 2

John G. Anderson

Professor of Geophysics

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March 4, 2008 2 John Anderson: GE/CEE 479/679: Lecture 13

Combining in F=ma

• In this equation, Xi is a body force acting on the point, if any.

( ) iii

i Xuxt

uρμ

θμλρ +∇+

∂+=

∂ 22

2

23

2

22

2

21

22

x

u

x

u

x

uu

∂∂

+∂∂

+∂∂

=∇

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The Free Surface

• S-waves can have two polarizations:– SH - wave motion is parallel to

the surface. Causes only horizontal shaking.

– SV - wave motion is oriented to cause vertical motion on the surface.

• Amplitudes are approximately doubled

SH

SV

Motion in and out of the plane of this figure - hard to draw.

Motion perpendicular to the direction of propagation causes vertical motion of the free surface.

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Two Media in Contact

• This way of drawing is consistent with horizontal layers in the Earth.

• Lower velocities near the surface imply wave propagation direction is bent towards the vertical as the waves near the surface.

111 ,, βμρ

222 ,, βμρ

i1

i2

2

2

1

1 sinsin

ββii

=

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March 4, 2008 7 John Anderson: GE/CEE 479/679: Lecture 13

Two Media in Contact• For an incoming SV

wave, the situation gets even more complex.

• In this case, both P- and SV-waves are transmitted and reflected from the boundary.

• The P- and SV-waves are coupled by the deformation of the boundary.

1111 ,,, αβμρ

1222 ,,, αβμρ

i1

i2 i2

Incoming SVReflected SV

Transmitted SV

Transmitted P

Reflected Pj2

j1

Generalized Snell’s Law

2

2

1

1

2

2

1

1 sinsinsinsin

ααββjjii

===

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Realistic Earth Model

• Eventually, as the velocity increases with depth, rays are bent back towards the surface.

• Waves cannot penetrate into layers where β is too large.

111 ,, βμρ

222 ,, βμρ

i1

i2

2

2

1

1 sinsin

ββii

=

βi

psin

=

p is the “ray parameter. It is constant along the ray

β increases

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March 4, 2008 9 John Anderson: GE/CEE 479/679: Lecture 13

Body Waves: Discussion

• The travel time curves of body waves can be inverted to find the velocity structure of the path.

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March 4, 2008 10 John Anderson: GE/CEE 479/679: Lecture 13

Seismic Refraction

• Because velocity increases with depth, rays are bent back towards the surface.

• Apparent velocity at the array of sensors is the same as the velocity of the refracted ray along the top of the refracting layer.

• Records from a profile of sensors radial from an explosion can thus be inverted to find velocity with depth.

111 ,, βμρ

222 ,, βμρ

i1

i2

2

2

1

1 sinsin

ββii

=

βi

psin

=

p is constant along the ray

β increases

* ΔΔΔΔΔΔΔΔΔΔΔΔ

Refracted wave

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Realistic Earth Model

• Due to Snell’s law, energy gets trapped near the surface.

• This trapped energy organizes into surface waves.

111 ,, βμρ

222 ,, βμρ

i1

i2

2

2

1

1 sinsin

ββii

=

β increases

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March 4, 2008 15 John Anderson: GE/CEE 479/679: Lecture 13

Four types of seismic wavesBody WavesP Waves Compressional, Primary

S Waves Shear, Secondary

Surface WavesLove Waves

Rayleigh Waves

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March 4, 2008 16 John Anderson: GE/CEE 479/679: Lecture 13

Surface Waves

• Love waves: trapped SH energy.

• Rayleigh waves: combination of trapped P- and SV- energy.

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Surface Waves

• For surface waves, geometrical spreading is changed.– For body waves, spreading is ~1/r.– For surface waves, spreading is ~1/r0.5.

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Surface Waves: Discussion

• Body waves are not dispersed.• Surface waves are dispersed, meaning that

different frequencies travel at different speeds.• Typically, low frequencies travel faster. These

have a longer wavelength, and penetrate deeper into the Earth, where velocities are faster.

• Typically, Love waves travel faster than Rayleigh waves.

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Surface Waves

• Surface wave dispersion curves can be inverted to find the velocity structure of the path crossed by the surface waves.

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Surface Waves: Discussion• Particle motion in S-waves is normal to the direction of

propagation.

• This is also true of Love waves.

• However, Love waves would show changes in phase along the direction of propagation that would not appear in vertically propagating S waves.

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Surface Waves: Discussion

• Motion of Rayleigh waves is “retrograde elliptical”.

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Site Response

• What is site response

• What causes it

• What are it’s characteristics.

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Classic example of site effect : Mexico City

• Mexico City, Mexico

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Figure 2

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Physics of Site Response

• Layer over half space

• Multiple layers over half space

• Basins

• Topography

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Multiple flat layers

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Basins: major phenomena

• Amplification

• Energy trapped

• Conversion to surface waves at basin edge

• Longer duration

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• Basin edge

• Kobe, Japan earthquake disaster.

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Liu and Heaton, ~1980

Study of strong motion from the San Fernando earthquake.

Published in Bull. Seism. Soc. Am.

Demonstration of a basin effect.

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Site Characterization• Goal: characterize the average effect of geology on strong motion,

and use this to improve predictions.

• The shallow geology is an almost miniscule part of the total path from the earthquake to the station.

• However, it has a strong effect on the ground motions, because it is the closest to the station.

• Geophysical measurements, using wave propagation techniques, are used to measure near-surface site characteristics.

• Also need to know basin geometry, depth.

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March 4, 2008 45 John Anderson: GE/CEE 479/679: Lecture 13

Geotechnical Site Classification

• Many schemes to classify the site.

• Encroaching into the territory that Prof. Siddharthan will discuss later.

• But it’s good to introduce the subject from the viewpoint of the seismologist.

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Seed and Idriss (1982)

• 1. Rock sites• 2. Stiff soil sites (< 60 m deep)• 3. Deep cohesionless soil sites (> 75 m deep)• 4. Sites underlain by soft to medium stiff clays

Problem with this approach:Does not recognize that the spectral shape also depends on the earthquake magnitude.

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Geotechnical Classification Schemes

• Geology– Material on a geological map

• For example, for California one simple approach is the “QTM” approach, using the age of the material.

• Q = Quaternary• T = Tertiary• M = Mesozoic

– Whether the location is “erosion-dominated” or “sedimentation-dominated” (rock, soil)

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NEHRP Category

Description Shear velocity

(m/s)

A Hard rock >1500

B Firm to hard rock 760-1500

C Dense soil, soft rock 360-760

D Stiff soil 180-360

E Soft soil <180

F Special studies soils

NEHRP ClassificationShear velocity of near-surface materials

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Empirical site response and comparison with measured site conditions at ANSS sites in the

Reno area

Pancha, Anderson, Biasi, Anooshepor, Louie

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March 4, 2008 50 John Anderson: GE/CEE 479/679: Lecture 13

Results from Pancha’s ReMi studies in the Central Truckee Meadows

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Figure 1a

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Figure 3

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Figure 1b

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Figure 5

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Alternate Figure 9

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Figure 3

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Figure 2

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Figure 6

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OLD Figure 7