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dc.contributor.authorVashishtha, Ashish
dc.contributor.authorKhurana, Shashank
dc.date.accessioned2023-06-16T19:05:57Z
dc.date.available2023-06-16T19:05:57Z
dc.date.copyright2023
dc.date.issued2023-05-05
dc.identifier.citationVashishtha, A. & Khurana, S. (2023). Mach number dependence of flow instability around a spiked body. Proceedings from the 2nd International Conference on recent advances in fluid and thermal sciences, 2584, 020007. doi: 10.1063/5.0127721en_US
dc.identifier.urihttps://research.thea.ie/handle/20.500.12065/4532
dc.description.abstractA forward-facing aerospike have been identified as a passive flow control device for enhancing the aerodynamic efficiency and reducing the heat transfer in high-speed flows. In addition, it has been reported that the presence of a spike brings in unsteadiness in the form of oscillation and pulsation to the structure. Previous researchers have investigated the aerothermodynamic coefficients, together with offering a detailed explanation of the flow physics and associated unsteadiness, and their dependence on the spike's geometric characteristics (spike nose, and length-to-fore-body diameter ratio, L/D). This work focuses on ascertaining the role of flow speeds (free-stream Mach number), and their energy content, in governing the physics around a spiked body, which is yet to be established. Numerical investigation has been carried out using axisymmetric Navier-Stokes laminar flow solver for Mach number range of 2.0 to 7.0. A round-tip spike with flat-face cylindrical after-body have been simulated for spike length ratio of L/D=2.0, with spike diameter to fore-body diameter of 0.1. The flow unsteadiness has been analyzed with drag and pressure coefficients variation at different Mach numbers. It was found that the flow field around the spiked blunt nose behaves in pulsation mode at lower Mach numbers 2, 3 and transition to oscillatory mode at higher Mach numbers 5, 6 and 7, while remain almost stable at Mach 4. The limit of Strouhal Number for characterizing the pulsation and oscillation modes at various Mach numbers for spike length of L/D = 2 with flat after-body is observed as 0.2, however it may very well depend on other geometric parameters of spike and after-body.en_US
dc.formatPDFen_US
dc.language.isoengen_US
dc.publisherAIP Publishingen_US
dc.relation.ispartofAIP Conferenceen_US
dc.rightsAttribution-NonCommercial-NoDerivs 3.0 United States*
dc.rights.urihttp://creativecommons.org/licenses/by-nc-nd/3.0/us/*
dc.subjectEnergy Contenten_US
dc.subjectHeat Transferen_US
dc.subjectFluid Mechanicsen_US
dc.subjectFluid dynamicsen_US
dc.subjectAerodynamicsen_US
dc.subjectFlow controlen_US
dc.subjectFlow instabilitiesen_US
dc.titleMach number dependence of flow instability around a spiked bodyen_US
dc.typeinfo:eu-repo/semantics/conferenceObjecten_US
dc.conference.date2021-03-19
dc.conference.hostBITS Pilani, Dubai Campusen_US
dc.conference.locationDubai, United Arab Emiratesen_US
dc.contributor.affiliationengCore - SETU Carlowen_US
dc.description.peerreviewyesen_US
dc.identifier.doi10.1063/5.0127721en_US
dc.identifier.eissn1551-7616
dc.identifier.urlhttps://pubs.aip.org/aip/acp/article-abstract/2584/1/020007/2888905/Mach-number-dependence-of-flow-instability-around?redirectedFrom=fulltexten_US
dc.rights.accessrightsinfo:eu-repo/semantics/openAccessen_US
dc.subject.departmentengCORE - SETU Carlowen_US
dc.type.versioninfo:eu-repo/semantics/acceptedVersionen_US


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