Seismic Analysis of Large-Scale Piping Systems for the JNES ... - NRC
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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are made with time histories and Fourier spectra. Figure 4-16 through Figure 4-36 show plots <strong>for</strong><br />
<strong>the</strong>se comparisons. The time history plots are arranged with <strong>the</strong> test results shown at <strong>the</strong> top and<br />
<strong>the</strong> analytical results shown at <strong>the</strong> bottom, while <strong>the</strong> o<strong>the</strong>r plots show <strong>the</strong> test results and <strong>the</strong><br />
analytical results overlapped. In <strong>the</strong>se figures, red dots indicate <strong>the</strong> maxima while blue dots<br />
indicate <strong>the</strong> minima. A summary <strong>of</strong> <strong>the</strong>se comparisons are provided as follows.<br />
DM2-1:<br />
Comparisons <strong>for</strong> <strong>the</strong> DM2-1 test regarding <strong>the</strong> displacement D2, D4, and acceleration A2 are<br />
provided in Figure 4-16 through Figure 4-18. The overall shapes and <strong>the</strong> peak responses <strong>of</strong> <strong>the</strong><br />
time histories agree excellently between <strong>the</strong> test and <strong>the</strong> analysis, with a maximum peak<br />
difference <strong>of</strong> about 12% (over-predicted by <strong>the</strong> analysis). Since <strong>the</strong> input motions are <strong>the</strong><br />
smallest among <strong>the</strong> five tests, <strong>the</strong> responses are relatively small and <strong>the</strong>re<strong>for</strong>e <strong>the</strong> relative error<br />
may have been over shadowed by o<strong>the</strong>r uncertainties in <strong>the</strong> test and <strong>the</strong> analysis. The Fourier<br />
spectra comparisons show this point better. The Fourier spectra <strong>of</strong> <strong>the</strong> test displacements show a<br />
flat region <strong>for</strong> frequencies above 10 Hz, suggesting that white noise was recorded in <strong>the</strong> test. The<br />
white noise can also be identified as <strong>the</strong> small but non-trivial responses in <strong>the</strong> tails <strong>of</strong> <strong>the</strong> time<br />
histories from <strong>the</strong> test. The dominant responses, which are in <strong>the</strong> vicinity <strong>of</strong> 4~6 Hz, and <strong>the</strong><br />
nearby responses between 1~10 Hz compare especially well between <strong>the</strong> test and analysis. The<br />
displacement magnitudes at very low frequencies are between <strong>the</strong> peak responses at around 4~6<br />
Hz and <strong>the</strong> high frequency responses (white noise recorded in <strong>the</strong> test). The slight 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. As discussed previously, <strong>the</strong> baseline correction affects mainly <strong>the</strong> low frequency range.<br />
The low frequency content represents <strong>the</strong> gross shape or <strong>the</strong> slight skew <strong>of</strong> a time history and<br />
usually does not determine <strong>the</strong> major dynamic characteristics <strong>of</strong> a system. The response spectra<br />
<strong>of</strong> <strong>the</strong> acceleration A2 <strong>for</strong> <strong>the</strong> test and analysis match very well, with <strong>the</strong> test results having a<br />
slightly wider resonant region extending to <strong>the</strong> high frequency. The peaks are at a frequency <strong>of</strong><br />
about 5 Hz, which is between <strong>the</strong> input dominant frequency <strong>of</strong> 4.5 Hz and <strong>the</strong> piping system’s<br />
fundamental frequency <strong>of</strong> 6.09 Hz (6.3 Hz from test). The relative difference between <strong>the</strong><br />
maximum spectra responses is only about 0.3%, comparing to <strong>the</strong> relative difference <strong>of</strong> about 9%<br />
between <strong>the</strong> PGA’s (a borrowed term, meaning peak ground acceleration).<br />
DM2-2:<br />
Comparisons <strong>for</strong> <strong>the</strong> DM2-2 test regarding <strong>the</strong> displacement D2, D4, and acceleration A2 are<br />
provided in Figure 4-19 through Figure 4-21. The overall shapes and <strong>the</strong> peak responses <strong>of</strong> <strong>the</strong><br />
time histories agree excellently between <strong>the</strong> test and <strong>the</strong> analysis, with a maximum peak<br />
difference <strong>of</strong> about 10% (over-predicted by <strong>the</strong> analysis). Similarly to DM2-1, <strong>the</strong> Fourier<br />
spectra <strong>of</strong> <strong>the</strong> test displacements show a flat region <strong>for</strong> frequencies above 10 Hz, suggesting that<br />
white noise was recorded in <strong>the</strong> test, as can also be identified as <strong>the</strong> small but non-trivial<br />
responses in <strong>the</strong> tails <strong>of</strong> <strong>the</strong> time histories from <strong>the</strong> test. The dominant responses, which are in <strong>the</strong><br />
vicinity <strong>of</strong> 4~6 Hz, and nearby responses between 1~10 Hz compare especially well between <strong>the</strong><br />
test and analysis. Both <strong>the</strong> test and <strong>the</strong> analysis show a clear discontinuity around 1 Hz in <strong>the</strong><br />
Fourier spectra. The displacement magnitudes at very low frequencies are between <strong>the</strong> peak<br />
responses at around 4~6 Hz and <strong>the</strong> high frequency responses (white noise recorded in <strong>the</strong> test).<br />
The slight differences <strong>of</strong> <strong>the</strong> displacement responses at <strong>the</strong> low frequencies reflect <strong>the</strong> difference<br />
in <strong>the</strong> residual displacements and <strong>the</strong> overall shapes, and may be due to <strong>the</strong> baseline correction <strong>of</strong><br />
<strong>the</strong> input motions. In <strong>the</strong> frequency range <strong>of</strong> 0.1 to 1 Hz, <strong>the</strong> difference in D2 may indicate some<br />
plasticity in <strong>the</strong> elbow, which <strong>the</strong> analysis may not capture accurately. The response spectra <strong>of</strong><br />
<strong>the</strong> acceleration A2 <strong>for</strong> <strong>the</strong> test and analysis match very well, with <strong>the</strong> test results having a<br />
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