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               Topography effects
               Topography of the site can also have a noticeable effect on amplification of ground motion.
               The strong motion shown in Figure 4.3 was recorded on a rocky ridge connected to the
               Pacoima Dam, and is characterized by a peak acceleration of 1.17g, one of the highest ever
               recorded. Many people argued that this was mainly the result of a topographic amplification,
               although other interpretations were also suggested (Reiter, 1991).
                 The major parameter of the problem appears to be the steepness of the ridges; it can be
               shown that the displacement amplification at the crest of an essentially triangular hill is equal
               to 2/v, where vπis the angle formed by the ridges; therefore the amplification increases as the
               ridge becomes steeper. Observed amplifications at the crest (with respect to the base) range
               from 2 to 20, whereas theoretical predictions are generally much less (3 to 4), possibly due to
               the influence of three-dimensional effects and ridge to ridge interaction. Topography effects
               are discussed, among others, by Finn (1991) and Kramer (1996). Due to the complexity of the
               subject, it is generally considered as not mature enough to be included in code provisions. The
               Recommendations of the French Association for Earthquake Engineering (AFPS, 1990)
               appear to be the only document of regulatory character that has adopted rather detailed rules
               for the calculation of the topographic amplification factor.

               Spatial variability of ground motion
               While the smallest dimension of common structures such as buildings is usually small enough
               that the ground motion can be assumed to be the same along the entire plan of the structure, in
               elongated structures, such as long bridges and pipelines, a rather significant variability of the
               ground motion may occur, particularly whenever the large plan dimensions are combined with
               irregularities in the soil profile. The local spatial variation or incoherence of ground motion is
               mainly due to
               ●travelling wave effects, wherein non-vertical seismic waves reach different points of the
                 structure at different times (time delay effect);
               ●scattering (reflection, refraction) of seismic waves caused by inhomogeneities along the
                 travel path;
               ●local soil filtering and amplification of the motion.

               The coherency of two ground motions is a measure of correlation of amplitudes and phase
               angles at different frequencies. Ground motions recorded by dense arrays of accelerographs
               have shown that coherency decreases with increasing distance and increasing frequency of
               motion (Clough and Penzien, 1993; Kramer, 1996).


                                         4.2.5 Assessment of seismic hazard
               Analysis of seismic hazard (resulting from strong motions) is the basis for defining seismic
               loading for design purposes, more particularly for deriving the design response spectrum,
               discussed in more detail in Section 4.3.2.
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