Download Advances in Geophysics, Vol. 32 by Renata Dmowska (ed.), Barry Saltzman (ed.) PDF

By Renata Dmowska (ed.), Barry Saltzman (ed.)

ISBN-10: 0120188325

ISBN-13: 9780120188321

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1986) and Sileny (1986, 1989) to distinguish between double-couple and non-double-couple mechnism for small mine tremors in Czechoslovakia; their results are briefly described below. Seismic moment tensor inversion is the most general approach to pointsource representation. It requires fewer but higher-quality waveform data. This approach could possibly provide a conclusive answer to the growing interest as to whether certain mine tremors are nonshearing events. 2. Non-Double-Couple Mechanism There is considerable similarity between volcanic seismicity and mineinduced seismicity in the sense that both types of seismic activity are responses 26 SLAWOMIR J.

Williams and Arabasz (1989) have noted that the majority of the dilatational events can be fitted with a double-couple normal faulting mechanism if they occurred above mine level. Figure 15, reproduced from Williams and Arabasz (1989), demonstrates the dramatic influence of depth, usually the least constrained parameter in location procedure, on the fault-plane solution. In the Gentry Mountain area the vast majority of the largest events located by Wong et al. (1989) were characterized by a non-double-couple, possibly implosional, mechanism and were determined to be predominantly below mine level.

FIG. 18. Radiation patterns of P waves (A) and vertical component of S waves (B) generated by combined shear-implosive sources with the implosion/shear ratio from 0 to 20% for P waves and from 0 to 100% for S waves. Equal-area projection of the whole focal sphere with the upper hemisphere in the center is used. n pattern. The shadowed areas correspond to compression (A) and down motion (B). ) compression disappears almost completely. The S-wave radiation, on the other hand, is much less sensitive to the presence of the implosive component.

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