Introduction to Seismology: Surface Waves - PowerPoint PPT Presentation

1 / 23
About This Presentation
Title:

Introduction to Seismology: Surface Waves

Description:

Geometry for Love & Rayleigh Wave Motion. The Earth Rings Like a Bell: ... Time between bounces is given by pX(p), where p is the ray parameter. ... – PowerPoint PPT presentation

Number of Views:460
Avg rating:3.0/5.0
Slides: 24
Provided by: michaelw81
Category:

less

Transcript and Presenter's Notes

Title: Introduction to Seismology: Surface Waves


1
Introduction to SeismologySurface Waves
  • Wednesday, November 16, 2005
  • Jesse Lawrence
  • Office Munk Room 209
  • Email jlawrence_at_ucsd.edu
  • Webhttp//titan.ucsd.edu/classes/ITS/

2
Surface Waves
3
Geometry for Love Rayleigh Wave Motion
4
The Earth Rings Like a Bell
5
Rayleigh Wave Displacement as a Function of Depth
6
Horizontal Vertical Rayleigh Wave Motions
7
Love Waves
  • Constructive interference of SH wave multiples.
  • Destructive interference occurs at all but a few
    specific times at a given location
  • Time between bounces is given by pX(p), where p
    is the ray parameter.
  • The phase velocity is given by
  • c 1/p k/?
  • Phase velocity is dependent upon frequency, which
    causes dispersion.

X(t)
8
Love Waves Continued
  • Constructive interference of SH wave multiples.
  • When phase velocity varies by frequency
    (dispersion) interference occurs, making energy
    travel at a different velocity called the group
    velocity
  • With some math

X(t)
9
Love Waves Continued
T
Group Velocity
Phase Velocity
  • Phase Velocity
  • c k/?
  • Group Velocity

SSS
SS
S
X
10
Love Wave Geometry
  • Love waves occur because incoming SH waves are
    trapped within a Layer
  • In other words the layer acts as a waveguide.
  • interference between incoming and layer-reflected
    waves.
  • This only happens at just the right angle of
    incidence
  • This angle is defined by the modes of Earths
    geometry.

11
Love Wave Geometry
12
Love Wave Dispersion
  • Dispersion occurs because longer-period waves
    sample more of the halfspace, and travel at
    faster velocities.

13
Displacement of Love Waves
  • A Love Wave oscillates as cos(kxr?1z) in a layer,
    but decays exponentially as exp(-kxr?2z) in the
    halfspace below.
  • The vertical sensitivities of the modes are the
    eigenfunctions.

14
Modes
15
Phase v. Group Velocity
  • Sum two harmonic waves with slightly different
    frequency and wavenumbers
  • u(x,t) cos(?1t-k1x) cos(?2t-k2x)

16
Phase v. Group Velocity
  • Phase Velocity
  • c(?) ?/k(?)
  • ? 1/period, k 1/wavelength
  • c(?) is distance/time
  • Group Velocity
  • U(?) d?/dk
  • U(?) distance/time

17
Fundamental Mode Love Wave Group Phase
Velocities
18
Love Wave Group Dispersion
19
Love Wave Group Dispersion
  • Filter a single wave at a bunch of different
    frequencies/periods.
  • Longer periods arrive earlier than shorter ones.

20
Walvis Ridge Rayleigh wave group velocity
  • Group velocity is lower on the ridge than off the
    ridge because of a shallow low velocity layer at
    85 km depth.

21
East Pacific Rise Phase Velocities
22
Phase Velocity Oceanic Plate Age
Dispersion curves as function of age
Inverted structure
  • Higher velocities for older oceanic plates
  • Thick, cold lithosphere leads to higher
    velocities

23
Global Surface Wave Maps
Write a Comment
User Comments (0)
About PowerShow.com