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DC poleHodnotaJazyk
dc.contributor.authorYanovych, Vitalii
dc.contributor.authorDuda, Daniel
dc.contributor.authorUruba, Václav
dc.contributor.authorKosiak, Pavlo
dc.contributor.authorHoráček, Vít
dc.date.accessioned2023-03-20T11:00:16Z-
dc.date.available2023-03-20T11:00:16Z-
dc.date.issued2022
dc.identifier.citationYANOVYCH, V. DUDA, D. URUBA, V. KOSIAK, P. HORÁČEK, V. Turbulence topology behind different sections of the wind turbine blade. In MATEC Web of Conferences Volume 367 (2022) 21st Conference on Power System Engineering. Plzeň: EPD Sciences, 2022. s. nestránkováno. ISBN: neuvedeno , ISSN: 2261-236Xcs
dc.identifier.issn2261-236X
dc.identifier.urihttp://hdl.handle.net/11025/51721
dc.format9 s.cs
dc.format.mimetypeapplication/pdf
dc.language.isoenen
dc.publisherEPD Sciencesen
dc.relation.ispartofseriesLecture Notes in Artificial Intelligenceen
dc.rights© CC BY-NC-ND 4.0en
dc.titleTurbulence topology behind different sections of the wind turbine bladeen
dc.typekonferenční příspěvekcs
dc.typeConferenceObjecten
dc.rights.accessopenAccessen
dc.type.versionpublishedVersionen
dc.description.abstract-translatedThis work aimed to investigate the turbulence characteristics behind different parts of the wind turbine blade. Airfoils S807, S813, S817, and S803, which characterize the shape of the blade at different lengths, were selected for estimation. During the experiment, the chord-based Reynolds number was 2.6×105, while the angle of attack was zero. Measuring crosssections were placed behind the trailing edge at x·c-1≈0.2, 0.4 and 1.0. For the determination flow topology, we used a Hotwire anemometry with a split fiber probe 55R55 and a miniature X-wire probe 55P64. The obtained data allowed us to determine and compare the evolution of the wake behind different types of airfoils in streamwise and spanwise directions. Thus, the largest and smallest velocity deficit located behind S817 and S803 airfoils, respectively. This trend is also evident in the Normalized Reynolds shear stress distributions. Finally, we determined the spectrum and calculated the Integral length scale, the Taylor and Kolmogorov microscale of turbulent flow. According to the results, profile S817 contributes to the formation of a flow with a large scale of turbulence, while the S803 is contrary.en
dc.subject.translatedHot Wire Anemometryen
dc.subject.translatedAirfoilen
dc.subject.translatedwakeen
dc.subject.translatedWind Turbineen
dc.subject.translatedStructure of turbulenceen
dc.identifier.doi10.1051/matecconf/202236700023
dc.type.statusPeer-revieweden
dc.identifier.obd43936974
dc.project.IDEF19_073/0016931/Zvyšování kvality interních grantových schémat na ZČUcs
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