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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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