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engineers; (2) requisite input includes standard geotechnical parameters that are obtained during<br />
routine foundation investigations; and (3) the methods have been coded in straightforward,<br />
efficient computer programs that allow for sensitivity studies of various design options.<br />
For use in determining the seismic stability of slopes, limit equilibrium analyses are modified<br />
slightly with the addition of a permanent lateral body force that is the product of a seismic<br />
coefficient and the mass of the soil bounded by the potential slip. The seismic coefficient<br />
(usually designated as k h or N h ) is specified as a fraction of the peak horizontal acceleration, due<br />
to the fact that the lateral inertial force is applied for only a short time interval during transient<br />
earthquake loading. Seismic coefficients are commonly specified as roughly 1 / 3 to 1 / 2 of the peak<br />
horizontal acceleration value (Seed 1979; Marcuson et al. 1992; CDMG 1997).<br />
In most cases involving soils that do not exhibit strength loss after the peak strength has been<br />
mobilized, common pseudostatic, rigid body methods of evaluation will generally suffice for<br />
evaluating the stability of slopes. These methods are well established in the literature (Kramer<br />
1996). Although they are useful for indicating an approximate level of seismic stability in terms<br />
of a factor of safety against failure, pseudostatic methods suffer from several potentially<br />
important limitations. These are: (1) they do not indicate the range of slope deformations that<br />
may be associated with various factors of safety; (2) the influence of excess pore pressure<br />
generation on the strength of the soils is incorporated in only a very simplified, “decoupled”<br />
manner; (3) progressive deformations that may result due to cyclic loading at stresses less than<br />
those required to reduce specific factors of safety to unity are not modeled; (4) strain softening<br />
behavior for liquefiable soils or sensitive clays is not directly accounted for, and (5) the dynamic<br />
behavior of the slide mass is not accounted for (Kramer and Smith 1997).<br />
7.2.3 Analysis of the “Post-Earthquake” Factor of Safety for Slopes<br />
Traditional slope stability analyses for seismic conditions depend on the overall pseudo-static<br />
factor of safety to indicate whether the slope will remain in equilibrium. While these stability<br />
analyses do not provide explicit information on the magnitude of seismically-induced<br />
deformations, one would expect that slopes with greater pseudo-static stability would be less<br />
prone to movement. Therefore, the factor of safety based on this procedure might provide a<br />
useful index. As previously mentioned, the pseudostatic methods are particularly useful for cases<br />
involving competent soils that do not lose significant strength during shaking. These methods are<br />
not, however, well suited for analysis involving liquefiable sandy soils and sensitive fine-grained<br />
soils that experience a reduction of strength during seismic loading.<br />
In order to evaluate the seismic stability of slopes involving liquefiable soils using standard limit<br />
equilibrium methods, the residual undrained shear strength of the soil can be estimated based on<br />
standard geotechnical parameters such as the penetration resistance of the soil based on in situ<br />
tests (Figures 4-3 and 4-4). The shear strengths provided in these two figures are applicable only<br />
if the seismic loading was sufficient to liquefy sandy soil. Once the residual shear strength of the<br />
sandy soil has been estimated, the layer is now modeled in a manner similar to that of an<br />
undrained cohesive soil. The dynamic stability (sometimes termed the post-earthquake stability)<br />
of the slope can now be assessed. While these equilibrium analyses are relatively simple to<br />
perform, this technique for evaluating seismic stability is still based on rigid body mechanics and<br />
thus suffers from the same shortcomings as the pseudostatic method.<br />
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