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Microseismic Monitoring and Geomechanical Modelling of CO2 - bris

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3.4. SWS MEASUREMENTS AT WEYBURN<br />

eigenvalue minimisation analysis. Cluster analysis is performed to chose the best cluster <strong>of</strong> results,<br />

from which the best result is selected. To conduct the analysis I use the SHEar-wave Birefringence<br />

Analysis (SHEBA) algorithm developed by Teanby et al. (2004b).<br />

Figure 3.8 shows the results for an example event from the dataset. In panel (a), the seismograms<br />

are rotated into the ray frame. There should be no P-wave energy on the Sv <strong>and</strong> Sh components.<br />

Panel (b) shows the S-wave components rotated into radial <strong>and</strong> transverse components with respect<br />

to the initial source polarisation, both before <strong>and</strong> after the splitting correction. After correction, the<br />

transverse component should be minimised. Panel (c) shows the S-wave particle motion before <strong>and</strong><br />

after correction, <strong>and</strong> the fast <strong>and</strong> slow waveforms before <strong>and</strong> after correction. The particle motion<br />

should be linearised after the splitting correction, <strong>and</strong> the fast <strong>and</strong> slow waveforms should be similar.<br />

Panel (d) shows a contour plot <strong>of</strong> the energy on the transverse component after correction as a<br />

function <strong>of</strong> ψ <strong>and</strong> δt stacked for each <strong>of</strong> the 100 picked splitting analysis windows. An F-test is used<br />

to normalised this surface such that a value <strong>of</strong> 1 represents the 95% confidence interval. The cluster<br />

analysis is also displayed to the right <strong>of</strong> this panel. The upper cluster analysis panel shows the results<br />

(ψ <strong>and</strong> δV S ) <strong>of</strong> the splitting measurement for each <strong>of</strong> the splitting analysis windows. The lower cluster<br />

analysis panel maps the results for each window in ψ-δV S space, highlighting the clusters identified<br />

by SHEBA.<br />

Teanby et al. (2004b) provide a number <strong>of</strong> requirements that must be fulfilled if a splitting result<br />

is to be deemed reliable:<br />

• Well defined S-wave <strong>and</strong> successful rotation, with all the P-wave energy on the ‘c’ component<br />

((quasi-)parallel to the raypath), <strong>and</strong> S-wave energy on the ‘a’ <strong>and</strong> ‘b’ components (perpendicular<br />

to ‘c’).<br />

• Energy minimised on the transverse component after correction.<br />

• Linear S-wave particle motion after correction.<br />

• Good match between fast <strong>and</strong> slow waveforms.<br />

• Unique solution, with a well defined <strong>and</strong> small error ellipse.<br />

If a splitting measurement fulfils all <strong>of</strong> the above criteria then it is graded class A. Should it fulfil<br />

all but one <strong>of</strong> the above requirements it is graded class B. If it fails to satisfy two or more <strong>of</strong> these<br />

criteria, it is classed as C <strong>and</strong> considered to be unreliable.<br />

3.4.2 Splitting results for Weyburn<br />

Of the 688 possible splitting measurements (86 events × 8 receivers) only 72 provided class A <strong>and</strong> B<br />

results. This is a very low success rate for SWS analysis (compare with, for e.g., Al-Harrasi et al.,<br />

2010). There are two probable reasons for this. Firstly, the data generally has a very poor signalto-noise<br />

ratio. Secondly, many <strong>of</strong> the events are located close to the array (

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