Please use this identifier to cite or link to this item: https://open.uns.ac.rs/handle/123456789/4338
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dc.contributor.authorPopović M.en_US
dc.contributor.authorNesic M.en_US
dc.contributor.authorCiric-Kostic S.en_US
dc.contributor.authorŽivanov, M.en_US
dc.contributor.authorMarkushev D.en_US
dc.contributor.authorRabasovic M.en_US
dc.contributor.authorGalovic S.en_US
dc.date.accessioned2019-09-23T10:33:33Z-
dc.date.available2019-09-23T10:33:33Z-
dc.date.issued2016-12-01-
dc.identifier.issn0195928Xen_US
dc.identifier.urihttps://open.uns.ac.rs/handle/123456789/4338-
dc.description.abstract© 2016, Springer Science+Business Media New York. A minimum volume photoacoustic (PA) cell, employed as an acoustic resonator, is presented. A model of the PA cell transfer function, as a combination of two Helmholtz resonators, is derived. Frequency PA response is described as the product of theoretically derived pressure variation and the transfer function of the PA cell. The derived model is applied to the frequency PA measurements, performed on laser-sintered polyamide. It is shown that the derived model explains the occurrence of resonant peaks in the high-frequency domain (> 10 kHz), in both amplitude and phase measurements, obtained by a gas-microphone minimal volume PA cell. The implementation of the model in the growing possibilities of sample characterization using gas-microphone PA cell is discussed.en
dc.relation.ispartofInternational Journal of Thermophysicsen
dc.titleHelmholtz Resonances in Photoacoustic Experiment with Laser-Sintered Polyamide Including Thermal Memory of Samplesen_US
dc.typeJournal/Magazine Articleen_US
dc.identifier.doi10.1007/s10765-016-2124-3-
dc.identifier.scopus2-s2.0-84991268713-
dc.identifier.urlhttps://api.elsevier.com/content/abstract/scopus_id/84991268713-
dc.description.versionPublisheden_US
dc.relation.issue12en
dc.relation.volume37en
item.fulltextNo Fulltext-
item.grantfulltextnone-
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