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Finished and ongoing projects
Inversion of shallow seismic wavefield spectra
Additional topics
Osculation points in surface wave dispersion curves
Depending on the properties of the media the phase velocity dispersion
curves of Rayleigh waves may come close to each other.
This phenomenon is well known in the literature under the term "osculation
points".
E.g. the Stoneley mode at the core mantle boundary has contributions
from several overtones of spheroidal free modes.
The Stoneley mode changes the overtone index at every osculation point.
In shallow seismic media osculation points appear most often in
conjunction with low-velocity channels.
Here even the fundamental Rayleigh mode may become a pure channel mode.
In that case it is not observable at the surface.
The observed wavefield is purely due to higher-modes in these cases.
Modelling of recorded seismic waveforms is only possible if the source-time function is known in addition to subsurface structure. The usual sources in shallow seismics (hammer blow, small explosion) have time-constants within the period band of the recorded waveform. Since the time-function of these source is not known in advance and since it highly depends on the media, it must be derived from the data as well. However, simple onesided impulse-functions of finite duration fit the data well and allow to describe the source-time function with three unknowns only.
A proper tomographic inversion of phase traveltimes of shallow seismic Rayleigh waves is not known in the literature yet. This method will be applied to a tomographic dataset recorded at Bietigheim (Standort B). A model of the refractor topography is available from Stefan Hecht (2001). This shall be reproduced, at least qualitatively by phase-velocity maps.
Shallow seismic surveys have to deal with low-velocity channels in many cases, in particular in surveys on pavements. While these channels can be resolved with surface waves, the role of body-wave onsets is not clear. From ray-theory (high-frequency limit) refracted onsets are only expected for waves with apparent velocities larger than the velocity of the fast top layer. With band limited wave propagation, however, the fast direct wave dies out quickly after a few metres. At larger offsets refracted waves that have "tunneled" through the fast top structure contribute to the first visible arrivals. To exploit their traveltimes we need a physical concept of these phases in terms of propagating band-limited pulses, although they cannot be described as travelling waves within material that has seismic velocities larger than the apparent velocity of the waves.
In cases where the numbers of sources and receivers are badly balanced tomography is inappropriate to derive lateral heterogeneity. In these cases the direct application of the Laplace-Operator is promising (Friederich et al. 2000). Though this has never been tried with shallow-seismic field-data. Susanne Wölz (1999) recorded a unique dataset with extraordinary dense sampling of the wavefield. This may well serve as a test-case for the Laplace-Operator method.
last change: $Date: 2011-12-30 09:52:25 +0100 (Fr, 30 Dez 2011) $ $Revision: 10475 $