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Earthworms: multiscale (generalized wavelet?) analysis of the EGM96 gravity field model of the Earth

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Magnitude of slope is g(x,y) Locations of maxima of g(x,y) are positions of edges. These values of g(x,y), scaled by z/z0 , are magnitudes assigned to edges ... – PowerPoint PPT presentation

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Title: Earthworms: multiscale (generalized wavelet?) analysis of the EGM96 gravity field model of the Earth


1
Earthworms multiscale (generalized wavelet?)
analysis of the EGM96 gravity field model of the
Earth
  • Frank Horowitz1, Peter Hornby1, Gabriel
    Strykowski2, Fabio Boschetti1
  • 1CSIRO Exploration Mining, Perth, Australia
  • 2National Survey and Cadstre (KMS), Copenhagen,
    Denmark
  • http//www.ned.dem.csiro.au/HorowitzFrank

2
Overview
  • Edge detection on the EGM96 global geodetic
    gravity field
  • EGM96 is the geodetic communitys spherical
    harmonic model of the gravity field of the Earth,
    valid to degree and order 360 (roughly 30 minutes
    of arc)
  • For the spherical earth, the technique does not
    yield a "traditional" wavelet transform.
  • Still working on demonstrating whether
    construction preserves desirable properties of
    flat earth wavelet.

3
Overview (cont.)
  • Uses
  • Visualisation
  • Big picture tectonics
  • Corrections to global gravity models including
    error distributions
  • Source distributions?
  • Method of images (Kelvin transform)

4
Sources? Severity of problem
5
Theory
  • Flat earth wavelets from Green's function
  • potential
  • vertical acceleration

6
Theory (cont.)
  • Flat earth wavelets from Green's function
  • convolutional form
  • convolution kernel (Greens function)

7
Theory (cont.)
  • Flat earth wavelets from Green's function
  • smoothing/scaling function
  • on the line
  • On the plane

8
Theory (cont.)
  • Flat earth wavelets from Green's function
  • "mother" wavelet from derivative of smoothing
    function

9
Theory (cont.)
  • Flat earth wavelets from Green's function
  • different scales
  • Upward continuations are wavelet scale changes
    (Hornby et al. 1999)

10
Inverse wavelet transform
  • An interpretation of the wavelet transform as
    proportional to a possible source distribution

11
Spherical theory (1)
  • Green's function on sphere
  • Radial acceleration
  • Field due to mass distribution (in spherical
    harmonics)

12
Spherical theory (2)
  • Green's function on sphere
  • Radial acceleration
  • Field due to mass distribution (in spherical
    harmonics)

13
Wavelet scaling comparison
  • On flat earth
  • On spherical earth

14
Scaling on the sphere
Our gravity construction does NOT do this!
15
Spherical Smoother
16
Spherical wavelet?
17
Computing multiscale edges (flat earth)
  • Upward continue field to height z
  • Calculate horizontal derivatives as (vector
    valued) wavelet transform
  • Magnitude of slope is g(x,y)
  • Locations of maxima of g(x,y) are positions of
    edges
  • These values of g(x,y), scaled by z/z0 , are
    magnitudes assigned to edges

18
Computing multiscale edges on the sphere
  • Upward continue anomalous vertical acceleration
    field and horizontal derivatives to height h
    above reference ellipsoid using GRAVSOFT
    (Tscherning, et al. 1992) to evaluate T,zx T,zy
  • T is the anomalous potential, a subscripted comma
    denotes differentiation, and x, y and z are an
    orthonormal basis for a local tangent space
    denoting East(erly), North, and zenith
    respectively

19
Computing multiscale edges on the sphere (cont.)
  • Magnitude of slope is
  • Multiscale edges are defined as local maxima of g
  • These values of g, scaled by (R0h)/R0 , are
    magnitudes assigned to edges (mapped to color in
    the following)

20
Example Skeletonizations
21
Interlude Live demonstration
For one-on-one interactive demonstrations, see
Frank Horowitz and one of his Laptops of Doom
at the meeting. Or, play with the VRML model
yourself!
22
Supplementing Formal Error Statistics of EGM96 in
Local Area
  • Each spherical harmonic coefficient has
    associated distribution
  • Build cost function consisting of mismatch
    between edges from EGM96 (or successor) and edges
    from local survey (e.g. the AGSO dataset for
    Australia)
  • Search within distribution for best fitting set
    of coefficients
  • independent analysis of field
  • should ameliorate field translation problems

23
Example Australia Perturbed and Unperturbed
  • Worms derived from EGM96 mean valued coefficients
  • displayed in green
  • Worms derived from EGM96 coefficients, randomly
    drawn from within error distributions
  • displayed in red
  • Coincident worms
  • displayed in yellow

24
Conclusion
  • While we can prove our construction on the sphere
    does not yield a "traditional wavelet", the
    results exhibit the main practical
    characteristics of a spherical multiscale edge
    analysis.
  • We're still trying to recapture some of the
    useful properties of wavelets from our
    construction.
  • Problem Inverse transform might not be simple.
  • We might have lost the "horizontal gradient of
    magnitude is proportional to a dipole source
    distribution" property
  • Rats!
  • Signal processing operations?
  • Clearly the skeletonization has utility in
    qualitative and quantitative analysis of the
    gravity field itself.
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