Matches in SemOpenAlex for { <https://semopenalex.org/work/W182362231> ?p ?o ?g. }
- W182362231 abstract "The current response spectrum method, based on the principle of superposition, is the principal method for seismic analysis of structures. It has been widely adopted by seismic design codes all over the world, although it is limited to linear systems. The progresses of the method are summarized in this paper. The limitations and the shortcomings of the method are pointed out. In current response spectrum method, the initial stiffness matrix of a structure is adopted in traditional modal analysis, but the effects of the structure deformations on the stiffness matrix are not considered yet. In fact, behavior of long span spatial structures under dynamic loads is higher nonliear and much complex. As an example, an long span arch structure is analyzed for revealing the effects of the geometrical nonlinearity and comparison in the paper. The numerical results show that there are obvious differences between two groups of vibration modes and corresponding periods obtained from the deformed and the undeformed structure configurations. Therefore, it is theoretically irrational to describe overall dynamic responses of a long span spatial structure by means of linear vibration mode theory. And also only a general damping ratio of a structure is usually employed in the troditional spectrum response analysis, instead of multi-material damping ratios, in almost all seismic design codes. If a structure is composed of different materials or/and installed more than one type of dampers, there are of couse several different damping ratios in the structure. The damping matrix in motion equations is no longer a classical damping matrix. As a result, the free vibration characters will be obviously different from one of the structure composed of the same material or/and without dampers. Apparently, the traditional response spectrum method fails to cope with the dynamic problems of a structure composed of different materials or/and installed dampers. The current develop situation of the nonlinear normal mode theory and its application are also introduced in this paper. The current effective analysis method for nonlinear dynamic equations is the well-known step by step integration method, named time-history method. However, it is difficult for wide application because of unacceptable time consumption, especially in analysis of large-scale buildings or spatial structures. The nonlinear mode theory is simple and effective for interpreting the complex nonlinear dynamic phenomenon. Then the nonlinear mode theory is still a developing vibration" @default.
- W182362231 created "2016-06-24" @default.
- W182362231 creator A5069954293 @default.
- W182362231 creator A5073216396 @default.
- W182362231 date "2009-12-01" @default.
- W182362231 modified "2023-09-24" @default.
- W182362231 title "Response Spectrum Analysis Methods for Spatial Structures" @default.
- W182362231 cites W1815946177 @default.
- W182362231 cites W1965679139 @default.
- W182362231 cites W1971956088 @default.
- W182362231 cites W2000339543 @default.
- W182362231 cites W2135737547 @default.
- W182362231 cites W2141285159 @default.
- W182362231 cites W2167825703 @default.
- W182362231 cites W2171525677 @default.
- W182362231 hasPublicationYear "2009" @default.
- W182362231 type Work @default.
- W182362231 sameAs 182362231 @default.
- W182362231 citedByCount "1" @default.
- W182362231 countsByYear W1823622312019 @default.
- W182362231 crossrefType "journal-article" @default.
- W182362231 hasAuthorship W182362231A5069954293 @default.
- W182362231 hasAuthorship W182362231A5073216396 @default.
- W182362231 hasConcept C104286136 @default.
- W182362231 hasConcept C106487976 @default.
- W182362231 hasConcept C121332964 @default.
- W182362231 hasConcept C124139854 @default.
- W182362231 hasConcept C127413603 @default.
- W182362231 hasConcept C134306372 @default.
- W182362231 hasConcept C135628077 @default.
- W182362231 hasConcept C140096630 @default.
- W182362231 hasConcept C14198674 @default.
- W182362231 hasConcept C158622935 @default.
- W182362231 hasConcept C159985019 @default.
- W182362231 hasConcept C178736951 @default.
- W182362231 hasConcept C182358397 @default.
- W182362231 hasConcept C192562407 @default.
- W182362231 hasConcept C198394728 @default.
- W182362231 hasConcept C200239387 @default.
- W182362231 hasConcept C24890656 @default.
- W182362231 hasConcept C27753989 @default.
- W182362231 hasConcept C2777256427 @default.
- W182362231 hasConcept C2778753569 @default.
- W182362231 hasConcept C2779372316 @default.
- W182362231 hasConcept C32758168 @default.
- W182362231 hasConcept C33923547 @default.
- W182362231 hasConcept C56625316 @default.
- W182362231 hasConcept C62520636 @default.
- W182362231 hasConcept C66938386 @default.
- W182362231 hasConceptScore W182362231C104286136 @default.
- W182362231 hasConceptScore W182362231C106487976 @default.
- W182362231 hasConceptScore W182362231C121332964 @default.
- W182362231 hasConceptScore W182362231C124139854 @default.
- W182362231 hasConceptScore W182362231C127413603 @default.
- W182362231 hasConceptScore W182362231C134306372 @default.
- W182362231 hasConceptScore W182362231C135628077 @default.
- W182362231 hasConceptScore W182362231C140096630 @default.
- W182362231 hasConceptScore W182362231C14198674 @default.
- W182362231 hasConceptScore W182362231C158622935 @default.
- W182362231 hasConceptScore W182362231C159985019 @default.
- W182362231 hasConceptScore W182362231C178736951 @default.
- W182362231 hasConceptScore W182362231C182358397 @default.
- W182362231 hasConceptScore W182362231C192562407 @default.
- W182362231 hasConceptScore W182362231C198394728 @default.
- W182362231 hasConceptScore W182362231C200239387 @default.
- W182362231 hasConceptScore W182362231C24890656 @default.
- W182362231 hasConceptScore W182362231C27753989 @default.
- W182362231 hasConceptScore W182362231C2777256427 @default.
- W182362231 hasConceptScore W182362231C2778753569 @default.
- W182362231 hasConceptScore W182362231C2779372316 @default.
- W182362231 hasConceptScore W182362231C32758168 @default.
- W182362231 hasConceptScore W182362231C33923547 @default.
- W182362231 hasConceptScore W182362231C56625316 @default.
- W182362231 hasConceptScore W182362231C62520636 @default.
- W182362231 hasConceptScore W182362231C66938386 @default.
- W182362231 hasLocation W1823622311 @default.
- W182362231 hasOpenAccess W182362231 @default.
- W182362231 hasPrimaryLocation W1823622311 @default.
- W182362231 hasRelatedWork W1972363719 @default.
- W182362231 hasRelatedWork W1990874358 @default.
- W182362231 hasRelatedWork W2027729466 @default.
- W182362231 hasRelatedWork W2029673997 @default.
- W182362231 hasRelatedWork W2074768976 @default.
- W182362231 hasRelatedWork W2165006972 @default.
- W182362231 hasRelatedWork W2181950393 @default.
- W182362231 hasRelatedWork W2312608705 @default.
- W182362231 hasRelatedWork W2471118430 @default.
- W182362231 hasRelatedWork W2504315294 @default.
- W182362231 hasRelatedWork W2739164721 @default.
- W182362231 hasRelatedWork W2799635418 @default.
- W182362231 hasRelatedWork W2810890931 @default.
- W182362231 hasRelatedWork W2908731063 @default.
- W182362231 hasRelatedWork W3048397592 @default.
- W182362231 hasRelatedWork W3092730898 @default.
- W182362231 hasRelatedWork W3126695950 @default.
- W182362231 hasRelatedWork W3177375991 @default.
- W182362231 hasRelatedWork W617252999 @default.
- W182362231 hasRelatedWork W1800369453 @default.
- W182362231 isParatext "false" @default.
- W182362231 isRetracted "false" @default.