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DOE-STD-1024-92
As shown on Figures 2 through 5 and in Appendix A, the absolute
value of the ratio of the 85th/median is drastically different between
the two studies. The representative value at a peak ground
acceleration of 0.20g is about 3.5 for the EPRI study, and about 7.2
for the LLNL study without LLNL-AE5 and about 11.2 with LLNL-
AE5 included. In general, if LLNL-AE5 is excluded, the ratio for the
LLNL results decreases by about 20 to 40 percent;
The value of the ratio of the 85th/median is dependent on the
response spectral frequency. The ratio value increases as the
spectral frequency decreases, with a more drastic trend observed
for the EPRI data. The use of the lower frequency information is
complicated by the observation that the attenuation models selected
by the LLNL and EPRI studies result in different spectral shapes.
As discussed above, some attenuation models provide direct
spectral estimates while others are associated with standard
spectral shapes such as the Newmark/Hall spectral shape. These
two different approaches can be one of the factors which result in
larger ratio at the lower frequency; and
The difference between the LLNL and EPRI median hazard curves
is generally less than a factor of 2. This result is displayed on
Figure 6 for a peak ground acceleration of 0.20g for the LLNL
results including attenuation expert 5. Table 1 also provides
summary statistics for the ratio of the medians, broken down by
rock and soil site conditions, with and without LLNL-AE5. The
largest difference between the LLNL and EPRI medians is for soil
sites where the uncertainty in ratios is relatively large. This is
thought to reflect differences between the two studies regarding how
soil conditions could impact ground motion estimates.
Based on the review of this information, the approach selected for the
seismic hazard position is as follows: The trends in the ratio of the
LLNL/EPRI medians and individual LLNL or EPRI 85th/median can be
used to derive a pseudo-mean correction factor. Trends observed are
relatively stable, which result in the advantage that a specific correction
factor can be derived to result in consistent hazard estimates from site to
site. This is thought to be superior to the other approaches in that specific
reliance on the LLNL or EPRI 85th percentile hazard curves may not be
warranted given their extreme differences, and it is not necessary to derive
complex weighing methods to combine the two studies.
The derivation of the specific correction factor is built around the most
stable seismic hazard curves, the LLNL and EPRI median curves. A
decision was also required regarding the specific spectral frequency and
level of ground motion to base the correction factor on. The preferred
frequency would be one that shows a high degree of relative stability and
be of engineering significance, such as between 2.5 and 10 hertz.
15


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