Surface Wave Tomography - Seismology - Lecture Notes, Study notes of Geology

Lecturer has discussed the following key points in these Lecture Notes : Surface Wave Tomography, Love Waves, Raleigh Waves, Sinusoidal-Acoustic, Evanescence Wave, Different Modes, Travel, Projector, Model Perturbation, Sensitivity Kernel

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Continents: Qucik review. Surface wave Tomography
Love waves-SH
Raleigh waves-P-SV
Sinusoidal-acoustic
๏ƒจEvanescence wave ๐ด ๐‘ง โˆ—eโˆ’ฮทฯ‰z
low frequency wave is more sensitive to deep structure. Therefore, low frequency wave should
arrive earlier than high frequency wave.
๏ƒจDifferent modes: Fundamental and Higher modes/overtones.
Surface wave Tomography
Recall from the travel time tomography:
๐’…=๐‘จ๐’Ž
(1)
where ๐’…, is the data; ๐‘จ, is the projector; and ๐’Ž is the model.
๐’…๐’Š= ๐‘ฎ๐’Š ๐’“ ๐ ๐’“ ๐’…๐’“
๐’—๐’๐’๐’–๐’Ž๐’†
(2)
Where ๐’…๐’Š is the observation; ๐‘ฎ๐’Š ๐’“ is greenโ€™s function/kernel (Sensitivity kernel) e.g. travel time
tomography; and ๐ ๐’“ is the model perturbation.
๐œน๐’•=๐‘ป๐’๐’ƒ๐’” โˆ’๐‘ป๐’“๐’†๐’‡ = โˆ†๐’”๐’…๐’
๐’‘๐’‚๐’•๐’‰ Integration over the ray path
(3)
Slower,
increasing ฮป
decreasing ฯ‰
Sensitivity kernel
wavespeed
decreasing ฯ‰
ฯ‰
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Continents: Qucik review. Surface wave Tomography Love waves-SH Raleigh waves-P-SV Sinusoidal-acoustic

๏ƒจEvanescence wave ๐ด ๐‘ง โˆ— eโˆ’ฮทฯ‰^ z

low frequency wave is more sensitive to deep structure. Therefore, low frequency wave should

arrive earlier than high frequency wave.

๏ƒจDifferent modes: Fundamental and Higher modes/overtones.

Surface wave Tomography

Recall from the travel time tomography:

๐’… = ๐‘จ๐’Ž (1)

where ๐’… , is the data; ๐‘จ , is the projector; and ๐’Ž is the model.

๐’—๐’๐’๐’–๐’Ž๐’†

Where ๐’…๐’Š is the observation; ๐‘ฎ๐’Š ๐’“ is greenโ€™s function/kernel (Sensitivity kernel) e.g. travel time

tomography; and ๐ ๐’“ is the model perturbation.

๐œน๐’• = ๐‘ป๐’๐’ƒ๐’” โˆ’ ๐‘ป๐’“๐’†๐’‡ = (^) ๐’‘๐’‚๐’•๐’‰ โˆ†๐’”๐’…๐’Integration over the ray path (3)

Slower, increasing ฮป

decreasing ฯ‰

Sensitivity kernel

wavespeed

decreasing ฯ‰

ฯ‰

2

When we do surface wave tomography, we measure the phase (or group) velocity:๏ค ci

for an earthquake i. As with the body wave tomography, we will look at perturbations between the model and the data:

๐‘ค๐‘Ž๐‘ฃ๐‘’๐‘  ๐‘๐‘Ž๐‘ก โ„Ž

๐ด๐‘‡^ ๐‘‘ = ๐ด๐‘‡^ ๐ด๐‘š

(๐ด๐‘‡^ ๐ด)โˆ’^1 ๐ดโˆ’^1 ๐‘‘ = ๐‘š

Those phase velocity maps are first constructed for a particular frequency. But, because of the evanescence of the surface waves, we can see what frequency is sensitive to a particular depth.

Convert ๏ท to z. To do so, we look at the sensitivity kernel for different frequencies. We use

๏‚ถ c ๏‚ถ๏ข

and we get

๐‘ค๐‘Ž๐‘ฃ๐‘’๐‘  ๐‘๐‘Ž๐‘ก โ„Ž

is a phase velocity map of particular frequency ๐œ”.

receiver Source

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Figure: Sensitivity of 1-D waveform inversions to focal depths. The effects of varying focal depth for two events: (a) focal depth 2 km (b) focal depth 9 km. Fits of final synthetic (dashed) to observed (solid) seismograms for shifts in focal depths of 10-50 km are shown on the left and the corresponding inversion velocity models (thin lines) are shown on the right along with the velocity model for the correct depth (thick line). The misfit and maximum frequency achieved by the waveform inversion are denoted to the right of each waveform fit. Maggi, Alessia & Priestley, Keith Surface waveform tomography of the Turkish-Iranian plateau. Geophysical Journal International 160 (3), 1068-1080. doi: 10.1111/j.1365-246X.2005.02505.x

Updated by: Sami Alsaadan Sources: April 20,2005 by Sophie Michelet โ€œAn Introdution to Seismology, Earthquakes, And Earth Structureโ€ by Stein &Wysession (2007).

Figure removed due to copyright restrictions.