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Some features of the acceleration impulse response function

dc.contributor.authorIwanaga, M. K. [UNESP]
dc.contributor.authorBrennan, M. J. [UNESP]
dc.contributor.authorTang, B.
dc.contributor.authorScussel, O. [UNESP]
dc.contributor.authorAlmeida, F. C.L. [UNESP]
dc.contributor.institutionUniversidade Estadual Paulista (Unesp)
dc.contributor.institutionDalian University of Technology
dc.date.accessioned2021-06-25T10:48:28Z
dc.date.available2021-06-25T10:48:28Z
dc.date.issued2021-01-01
dc.description.abstractImpulse response functions (IRFs) and frequency response functions (FRFs) are fundamental quantities that describe the dynamic behaviour of a linear vibrating system in the time and frequency domains respectively. The acceleration IRF is of particular concern in this paper, because unlike the displacement and velocity IRFs it contains a Delta function as well as a decaying oscillation. The origin of this Delta function is shown to be due to the causality constraint rather than the system. To illustrate the characteristics of the IRFs and FRFs, simulations are presented for a single-degree-of-freedom system, and are supported by some laboratory experimental work. The acceleration IRF is partitioned into the impulse component (Delta function for the simulations) and the oscillatory component. They are separately transformed to the frequency domain to illustrate their effects in the accelerance FRFs for both simulated and measured data.en
dc.description.affiliationDepartment of Mechanical Engineering UNESP-FEIS
dc.description.affiliationInstitute of Internal Combustion Engine Dalian University of Technology
dc.description.affiliationFaculty of Science and Engineering UNESP-FCE
dc.description.affiliationDepartment of Mechanical Engineering UNESP-FEB
dc.description.affiliationUnespDepartment of Mechanical Engineering UNESP-FEIS
dc.description.affiliationUnespFaculty of Science and Engineering UNESP-FCE
dc.description.affiliationUnespDepartment of Mechanical Engineering UNESP-FEB
dc.description.sponsorshipNational Outstanding Youth Science Fund Project of National Natural Science Foundation of China
dc.description.sponsorshipFundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP)
dc.description.sponsorshipConselho Nacional de Desenvolvimento Científico e Tecnológico (CNPq)
dc.description.sponsorshipIdNational Outstanding Youth Science Fund Project of National Natural Science Foundation of China: 11672058
dc.description.sponsorshipIdFAPESP: 2013/50412-3
dc.description.sponsorshipIdFAPESP: 2017/14432-0
dc.description.sponsorshipIdFAPESP: 2017/16953-8
dc.description.sponsorshipIdCNPq: 88887.374001/2019-00
dc.format.extent169-177
dc.identifierhttp://dx.doi.org/10.1007/s11012-020-01265-4
dc.identifier.citationMeccanica, v. 56, n. 1, p. 169-177, 2021.
dc.identifier.doi10.1007/s11012-020-01265-4
dc.identifier.issn1572-9648
dc.identifier.issn0025-6455
dc.identifier.scopus2-s2.0-85098695738
dc.identifier.urihttp://hdl.handle.net/11449/207067
dc.language.isoeng
dc.relation.ispartofMeccanica
dc.sourceScopus
dc.subjectElectrodynamic shaker
dc.subjectFourier transform
dc.subjectFrequency response functions
dc.subjectHeaviside function
dc.subjectImpulse response functions
dc.titleSome features of the acceleration impulse response functionen
dc.typeArtigopt
dspace.entity.typePublication
relation.isDepartmentOfPublicationc94031d3-1184-4720-a3d6-062c562bd372
relation.isDepartmentOfPublication.latestForDiscoveryc94031d3-1184-4720-a3d6-062c562bd372
unesp.author.orcid0000-0003-4333-6439[1]
unesp.departmentEngenharia Mecânica - FEBpt
unesp.departmentEngenharia Mecânica - FEISpt

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