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Seismic Analysis of Large-Scale Piping Systems for the JNES ... - NRC

Seismic Analysis of Large-Scale Piping Systems for the JNES ... - NRC

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DM4-2(2) (Restart):<br />

This analysis considered <strong>the</strong> plasticity developed during DM4-1 and DM4-2(1). Comparisons <strong>for</strong><br />

<strong>the</strong> DM4-2(2) with restart regarding <strong>the</strong> displacement D2, D4, and acceleration A2 are provided<br />

in Figure 4-28 through Figure 4-30. The overall shapes and <strong>the</strong> peak responses <strong>of</strong> <strong>the</strong> time<br />

histories agree generally well between <strong>the</strong> test and <strong>the</strong> analysis, with a maximum peak difference<br />

<strong>of</strong> about 6%. All response peaks in <strong>the</strong> time histories are under-predicted by <strong>the</strong> analysis. The<br />

analytical time histories appear to be slightly less damped than <strong>the</strong> test. In addition, <strong>the</strong> analytical<br />

time histories show some tendency that <strong>the</strong> responses are encapsulated within constant limits,<br />

which may imply that <strong>the</strong> mono multi-linear kinematic hardening model may result in strain<br />

shakedown <strong>for</strong> this level <strong>of</strong> input motions. The Fourier spectra <strong>of</strong> <strong>the</strong> test displacements show a<br />

flat region <strong>for</strong> frequencies above 20 Hz, suggesting white noise was recorded in <strong>the</strong> test. Unlike<br />

<strong>for</strong> tests DM2-1 and DM2-2, <strong>the</strong> white noise cannot be easily identified in <strong>the</strong> time histories<br />

because <strong>the</strong> white noise is about 4~5 magnitudes smaller than <strong>the</strong> peak response. The dominant<br />

responses, which are at a frequency <strong>of</strong> slightly less than 6 Hz, and most responses <strong>for</strong> frequencies<br />

between 1~20 Hz compare especially well between <strong>the</strong> test and analysis. Both <strong>the</strong> test and <strong>the</strong><br />

analysis show discontinuities at around 1 Hz and 10 Hz in <strong>the</strong> Fourier spectra. The differences <strong>of</strong><br />

<strong>the</strong> displacement responses at <strong>the</strong> low frequencies reflect <strong>the</strong> difference in <strong>the</strong> residual<br />

displacements and <strong>the</strong> overall shapes, and may be due to <strong>the</strong> baseline correction <strong>of</strong> <strong>the</strong> input<br />

motions. The response spectra <strong>of</strong> <strong>the</strong> acceleration A2 <strong>for</strong> <strong>the</strong> test and analysis match very well.<br />

The spectral response peaks are at a frequency <strong>of</strong> slightly less than 6 Hz, which is <strong>the</strong> same as <strong>the</strong><br />

input dominant frequency and close to <strong>the</strong> fundamental frequency <strong>of</strong> <strong>the</strong> pipe system (5.9 Hz<br />

from test DM4-2(2)). The relative difference <strong>of</strong> <strong>the</strong> maximum spectra responses is only about 5%<br />

(over-predicted by <strong>the</strong> analysis), comparing to <strong>the</strong> relative difference <strong>of</strong> about 6% <strong>of</strong> <strong>the</strong> PGA’s<br />

(under-predicted by <strong>the</strong> analysis).<br />

DM4-2(1) (Without Restart):<br />

This analysis did not consider any plasticity developed previously. Comparisons <strong>for</strong> <strong>the</strong> DM4-<br />

2(1) without restart regarding <strong>the</strong> displacement D2, D4, and acceleration A2 are provided in<br />

Figure 4-31 through Figure 4-33. Compared to DM4-2(1) with restart, no significant difference<br />

can be found <strong>for</strong> <strong>the</strong> various comparisons <strong>for</strong> this analysis, meaning that <strong>the</strong> previous plasticity<br />

accumulation does not have a significant impact on <strong>the</strong> displacement and <strong>the</strong> acceleration<br />

responses considered in <strong>the</strong> analysis.<br />

DM4-2(2) (Without Restart):<br />

This analysis did not consider any plasticity developed previously. Comparisons <strong>for</strong> <strong>the</strong> DM4-<br />

2(2) without restart regarding <strong>the</strong> displacement D2, D4, and acceleration A2 are provided in<br />

Figure 4-34 through Figure 4-36. Compared to DM4-2(2) with restart, no significant difference<br />

can be found <strong>for</strong> <strong>the</strong> various comparisons <strong>for</strong> this analysis, meaning that <strong>the</strong> previous plasticity<br />

accumulation does not have a significant impact on <strong>the</strong> displacement and <strong>the</strong> acceleration<br />

responses considered in <strong>the</strong> analysis.<br />

In summary, <strong>the</strong> comparisons <strong>of</strong> <strong>the</strong> piping system analyses <strong>of</strong> <strong>the</strong> design method confirmation<br />

tests demonstrated that displacement and acceleration time history responses were predicted with<br />

high accuracy, mostly within a maximum relative error <strong>of</strong> 10%. The analyses tend to overpredict<br />

<strong>the</strong> responses <strong>for</strong> low level input motions while somewhat under-predict <strong>the</strong> responses <strong>for</strong><br />

high level input motions. The analyses are capable to capture closely <strong>the</strong> dominant frequency<br />

content, in view <strong>of</strong> <strong>the</strong> Fourier spectra and response spectra. Major features in <strong>the</strong> Fourier spectra,<br />

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