Abstract
This study presents the Probabilistic Seismic Demand Model (PSDM) and explores optimal intensity measures (IMs) for nuclear power plant (NPP) equipment when subjected to ground motions having high-frequency (HF) and low-frequency (LF) contents. To this end, the PSDM is first constructed in terms of the IM and the corresponding engineering demand parameter, and its outcomes are utilized to select the optimum IMs based on the satisfaction of certain essential properties (i.e., efficiency, practicality, and proficiency). Regarding earthquake excitation, different IMs (i.e., structure-independent and structure-dependent IMs) are studied. The results show that the most appropriate IMs for the seismic performance of the cabinet are velocity spectrum intensity and spectral accelerations for the structure-independent IMs and the structure-dependent IMs, respectively.
Moreover, fragility analysis is performed to assess the vulnerability of NPP equipment. The outcomes indicate that the cabinet is highly vulnerable to HF earthquakes as a consequence of response amplification. In addition, the selection of the earthquake IM has an important influence on the collapse capacity of the cabinet, and the fragility curves obtained from structure-dependent IMs are more reliable in comparison to those of structure-independent IMs.
Acronyms
ASI: | = | acceleration spectrum intensity |
DM: | = | demand measure |
DSI: | = | displacement spectrum intensity |
EDP: | = | engineering demand parameter |
FB: | = | front-to-back |
FEM: | = | finite element model |
HF: | = | high frequency |
IM: | = | intensity measure |
LF: | = | low frequency |
LS: | = | limit state |
NPP: | = | nuclear power plant |
PGA: | = | peak ground acceleration |
PGD: | = | peak ground displacement |
PGV: | = | peak ground velocity |
PSDM: | = | Probabilistic Seismic Demand Model |
SS: | = | side-to-side |
VSI: | = | velocity spectrum intensity |
Nomenclature
= | = | practical factor |
= | = | residual between the actual value and the predicted value |
= | = | natural frequencies from the experimental test |
= | = | natural frequencies from the numerical model |
= | = | magnitude |
= | = | total number of samples |
= | = | distance from the source to the site |
= | = | spectral acceleration at |
= | = | spectral displacement at |
= | = | spectral velocity at |
= | = | spectral acceleration at |
= | = | spectral displacement at |
= | = | spectral velocity at |
= | = | spectral acceleration at the frequency range (4 to 16 Hz) |
= | = | spectral velocity at the frequency range (4 to 16 Hz) |
= | = | spectral displacement at the frequency range (4 to 16 Hz) |
Greek
= | = | standard deviation/efficiency factor |
= | = | proficiency factor |
= | = | standard normal cumulative distribution function |
Acknowledgments
This work was supported by the Korea Institute of Energy Technology Evaluation and Planning and the Ministry of Trade, Industry & Energy of Korea (number 20171510101960) and by Gwangju University (KR) [2021].