scholarly journals SEISMIC LOSS ANALYSIS OF A CODE‑DESIGNED INFILLED RC BUILDING ACCOUNTING FOR INFILL MODEL CLASS UNCERTAINTY

2021 ◽  
Author(s):  
Fabio Romano ◽  
Mohammad S. Alam ◽  
Maria Zucconi ◽  
Marco Faggella ◽  
Andre R. Barbosa ◽  
...  
2020 ◽  
Vol 19 (1) ◽  
pp. 429-462
Author(s):  
Fabio Romano ◽  
Mohammad S. Alam ◽  
Maria Zucconi ◽  
Marco Faggella ◽  
Andre R. Barbosa ◽  
...  

2020 ◽  
Author(s):  
Maria Zucconi ◽  
Marco Bovo ◽  
Fabio Romano ◽  
Barbara Ferracuti

2018 ◽  
Vol 177 ◽  
pp. 707-723 ◽  
Author(s):  
Fabio Romano ◽  
Marco Faggella ◽  
Rosario Gigliotti ◽  
Maria Zucconi ◽  
Barbara Ferracuti

2014 ◽  
Vol 580-583 ◽  
pp. 1763-1766
Author(s):  
Li Na Xian ◽  
Xiao Ying Ou

Incorporating the probability of seismic hazard, expected annual earthquake loss with different collapse margin ratio (CMR) has been studied in this paper. Nonlinear simulation models of reinforced concrete (RC) frames were analyzed using incremental dynamic analysis (IDA) under continuous earthquake intensity. The analytic results from four examples of RC frames show that the expected annual loss has negative correlation with theCMRof the concerned structures, and seismic loss basically decreases with increasingCMRat given ground motion intensity. The proposed idea herein could be regarded as a promising improvement on the quantification of earthquake loss estimation by utilizingCMRof structures.


Author(s):  
P.E. Batson

Use of the STEM to obtain precise electronic information has been hampered by the lack of energy loss analysis capable of a resolution and accuracy comparable to the 0.3eV energy width of the Field Emission Source. Recent work by Park, et. al. and earlier by Crewe, et. al. have promised magnetic sector devices that are capable of about 0.75eV resolution at collection angles (about 15mR) which are great enough to allow efficient use of the STEM probe current. These devices are also capable of 0.3eV resolution at smaller collection angles (4-5mR). The problem that arises, however, lies in the fact that, even with the collection efficiency approaching 1.0, several minutes of collection time are necessary for a good definition of a typical core loss or electronic transition. This is a result of the relatively small total beam current (1-10nA) that is available in the dedicated STEM. During this acquisition time, the STEM acceleration voltage may fluctuate by as much as 0.5-1.0V.


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