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Civil-Comp Proceedings
ISSN 1759-3433 CCP: 77
PROCEEDINGS OF THE NINTH INTERNATIONAL CONFERENCE ON CIVIL AND STRUCTURAL ENGINEERING COMPUTING Edited by: B.H.V. Topping
Paper 105
Site Effect Induced in the El-Asnam (Algeria) Earthquake of 10 October 10 1980 K. Tounsi+* and M. Hammoutène*
+Department of Earthquake Engineering, National Center of Earthquake Engineering Applied Research, Algiers, Algeria
, "Site Effect Induced in the El-Asnam (Algeria) Earthquake of 10 October 10 1980", in B.H.V. Topping, (Editor), "Proceedings of the Ninth International Conference on Civil and Structural Engineering Computing", Civil-Comp Press, Stirlingshire, UK, Paper 105, 2003. doi:10.4203/ccp.77.105
Keywords: site effect, local geological conditions, Thomson-Haskell method, amplification, wave propagation, El-Asnam earthquake, response spectrum.
Summary
When an earthquake occurs, the measured motion on the surface is considered as the
result of three effects : the source mechanism, propagation path and the influence of
geological and topographical local conditions [1,4]. The different observations and
theoretical studies performed previously make possible to distinguish three kinds of site
effects : effect of the geological strata and their geometry, topography effects and
effects induced by the lateral discontinuities of the local structure of the ground.
The strong recent earthquakes, in particular those of Michoacan "Mexico City" (1985),
Armenia (1988) and California (1989), highlighted the important influence of the
geological conditions on the level and the characteristics of the ground motion, and also
on the induced damage.
The purpose of the present study is to perform a model [6] in order to investigate the effect of the local geology. In this frame, an analytical approach based on the Thomson-Haskell's method is adopted [1,2,3,5] and El-Asnam earthquake of October 10th, 1980 is considered. A numerical investigation is performed to analyse the local conditions site effects on the P, SV and SH propagating waves. The bedrock motion is simulated using a technique based on the empirical Green functions. To simulate the principal event of El-Asnam earthquake at the bedrock, the aftershock of November 8th (ML=5.6), having a similar focal mechanism with the major event, is considered as Green function. The obtained transfer functions in the frequency domain for El-Asnam's site show that the height and width of the peaks are controlled by the attenuation. The module of the transfer functions can be in excess of 10 for certain frequencies, and that whereas the amplification of S wave is dominant in the frequency range 1 to 10 Hz, the amplification of P waves is dominant above 10 Hz. Below, 1 Hz, the sedimentary structure has little effect upon either P or S waves. The surface's seismograms are obtained by the convolution of the calculated transfer function with the simulated seismograms at the bottom of the array. The results highlight important variations of the amplitudes of the motion for points located in free surface compared to the points located in-depth. The PGA at the surface presents an amplification of 1.5 to 5 times the bedrock's one. This is confirmed by the calculation of the response spectra for acceleration and displacement where, on the average, the surface spectra are about 3 times greater than the bottom spectra, although the ratio can be as large as 10. The obtained accelerations are compatible with the results obtained by the performed observations in-situ. This study shows the importance of the geological and geotechnical structure of the ground and the need to take into account, in an aseismic strategy, the site effects of structural origin for El-Asnam site. References
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