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1 <br />' San Luis Mine Phase Q, Raise 2 Design <br />' downstream face with basal sliding along the embattktrtent-liner interface. The lowest yield <br />accelerations computed for sliding wedge and rotational type failures of both embankment slopes <br />' are given in Figures 10 and 11. <br />4.6.2.3 Dynamic Displacements <br />' Average displacements calculated by the COE method are in excellent agreement with those <br />' calculated by the Makdisi and Seed Method. Displacement calculations computed using the Corps <br />of Engineers (COE) method utilized the upper bound envelope curve, presented in graphical form, <br />for all natural earthquake records processed except the unusually large ground motions recorded <br />' during the 1971 San Fernando earthquake. The record processed included numerous records of <br />events with M > 7.0, and should also produce conservative results for the event considered. <br />Displacement calculations which were computed using the Makdisi and Seed method incorporated <br />the use of the displacement envelope for a magnitude 7.5 earthquake within graphs which are <br />presented for calculating displacements. Thus, the displacement calculations using the Makdisi and <br />' Seed method have incorporated an earthquake with a slightly longer duration than the MCE for the <br />site and the resulting displacements should be conservative. Displacements calculated using the <br />method of Ambraseys and Menu included several levels of probability and these results should be <br />' the most accurate for the San Luis facility. <br />A$ shown in the calculations included as Appendix G, displacements calculated utilizing the three <br />' . methods are in good agreement. Displacements calculated by the COE method were generally the <br />largest and reflects the upper bound nature of the correlation presented and uncertainty in the <br />' velocity associated with the design ground motion. Displacements calculated lby the Makdisi and <br />Seed method are higher than those calculated by the Ambraseys and Menu metttod and reflect the <br />' use of the chart for a magnimde 7.5 earthquake. Displacements calculated fora 16 percent <br />probability of exceedence using the method of Ambraseys and Menu are in good agreement with <br />those calculated by the COE and Makdisi and Seed methods. <br />' For a peak ground acceleration of 0.6g arising from a M=7+ earthquake, the displacement along <br />' the critical potential failure surface for the downstream face is estimated to be on the order of 1-3 <br />ft. Under the same loading conditions, the displacement along the critical downstream face <br />rotational failure surface depicted on Figure I1 is estimated to be on the order of 1 to 1.5 ft. For <br />' the upstream face of the embankment raise and PGA=0.6g, the displacement estimated for both the <br />critical circular failure surface depicted on Figure 10 is on the order of 1 to 1.5 ft. <br /> <br />1 <br />u y 4-9 ro~ect o. <br />