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Technical Papers

Probabilistic Seismic Demand Model and Seismic Fragility Analysis of NPP Equipment Subjected to High- and Low-Frequency Earthquakes

ORCID Icon, , ORCID Icon, , , & ORCID Icon show all
Pages 1327-1346 | Received 08 Mar 2020, Accepted 15 Apr 2021, Published online: 09 Jul 2021
 

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.

APPENDIX

Details of selected earthquakes are given in and .

TABLE A.I High-Frequency Earthquakes

TABLE A.II Low-Frequency Earthquakes

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

B ==

practical factor

ei ==

residual between the actual value and the predicted value

fexp ==

natural frequencies from the experimental test

fnum ==

natural frequencies from the numerical model

M ==

magnitude

N ==

total number of samples

R ==

distance from the source to the site

SaT1 ==

spectral acceleration at T1

SdT1 ==

spectral displacement at T1

SvT1 ==

spectral velocity at T1

Sa10 ==

spectral acceleration at T10

Sd10 ==

spectral displacement at T10

Sv10 ==

spectral velocity at T10

Sa416 ==

spectral acceleration at the frequency range (4 to 16 Hz)

Sv416 ==

spectral velocity at the frequency range (4 to 16 Hz)

Sd416 ==

spectral displacement at the frequency range (4 to 16 Hz)

Greek

βDM|IM ==

standard deviation/efficiency factor

ζ ==

proficiency factor

Φ. ==

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].

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