Matches in SemOpenAlex for { <https://semopenalex.org/work/W2809567882> ?p ?o ?g. }
- W2809567882 endingPage "65" @default.
- W2809567882 startingPage "46" @default.
- W2809567882 abstract "Finite-time Lyapunov Exponents (FTLE) can, through suitable choice of integration parameters, capture not only convecting coherent structures in compressible turbulent flows but also propagating dilatational components. This semi-Lagrangian approach thus provides an implicit sliding decomposition technique to connect hydrodynamic and acoustic features, and furthermore facilitates a direct examination of individual time-local events such as intermittency, which are often obscured by statistical techniques. The FTLE method yields attracting (also designated stable or backward-integrated) and repelling (unstable or forward-integrated) structures. In this paper, we show that FTLE offers substantial additional analysis capability in compressible flows over corresponding incompressible situations. Not only does the method establish a connection between attracting structures and the acoustic field, it also offers an effective means to elucidate finer details of the governing dynamics. This is achieved by leveraging repelling structures, as well as negative FTLE magnitudes, which complement the positive values in incompressible flows. The test bed considered is a free shear layer, specifically a validated Large-Eddy Simulation of a Mach 0.9 jet, where hydrodynamic and acoustic components interact with each other in an intricate manner. The implications of attracting and repelling FTLE structures are found to depend on whether they arise in the core turbulent region or in regions where the acoustic energy dominates. In turbulent regions, attracting structures correlate well with lower frequency acoustic components propagating downstream but repelling structures isolate the higher frequency components of the principal vortex dynamics. On the other hand, away from the highly turbulent regions, attracting structures continue to be associated with the (relatively weaker) coherent vortices while repelling structures gradually capture more of the acoustic energy and show higher correlation with the Eulerian dilatation. The joint FTLE field, defined as the difference between attracting and repelling FTLE coefficients, also reveals crucial aspects of the underlying physics. In particular, it captures hydrodynamic features at time scales representative of convection, which are shown to induce and modulate acoustic events within the potential core as they relate to entrainment and vortex interactions. In compressible flows, therefore, proper interpretation of the different components of the FTLE enables a rich, time-accurate connection between different temporal events." @default.
- W2809567882 created "2018-06-29" @default.
- W2809567882 creator A5037915614 @default.
- W2809567882 creator A5082589597 @default.
- W2809567882 date "2018-09-01" @default.
- W2809567882 modified "2023-09-25" @default.
- W2809567882 title "Analysis of compressible free shear layers with finite-time Lyapunov exponents" @default.
- W2809567882 cites W1965612527 @default.
- W2809567882 cites W1966397236 @default.
- W2809567882 cites W1977966552 @default.
- W2809567882 cites W1979176272 @default.
- W2809567882 cites W1981202981 @default.
- W2809567882 cites W1990963754 @default.
- W2809567882 cites W2007221293 @default.
- W2809567882 cites W2021467891 @default.
- W2809567882 cites W2026835270 @default.
- W2809567882 cites W2041274917 @default.
- W2809567882 cites W2043200311 @default.
- W2809567882 cites W2057260009 @default.
- W2809567882 cites W2057393236 @default.
- W2809567882 cites W2064915294 @default.
- W2809567882 cites W2066590884 @default.
- W2809567882 cites W2067153599 @default.
- W2809567882 cites W2068658646 @default.
- W2809567882 cites W2072980307 @default.
- W2809567882 cites W2074294125 @default.
- W2809567882 cites W2082578031 @default.
- W2809567882 cites W2083449273 @default.
- W2809567882 cites W2084755618 @default.
- W2809567882 cites W2110360252 @default.
- W2809567882 cites W2111405281 @default.
- W2809567882 cites W2112548197 @default.
- W2809567882 cites W2123739111 @default.
- W2809567882 cites W2134475147 @default.
- W2809567882 cites W2144836076 @default.
- W2809567882 cites W2145130735 @default.
- W2809567882 cites W2148302906 @default.
- W2809567882 cites W2152481940 @default.
- W2809567882 cites W2166875775 @default.
- W2809567882 cites W2169561174 @default.
- W2809567882 cites W2309317873 @default.
- W2809567882 cites W2345613619 @default.
- W2809567882 cites W2393515624 @default.
- W2809567882 cites W2469382904 @default.
- W2809567882 cites W2496614598 @default.
- W2809567882 cites W2508597397 @default.
- W2809567882 cites W2528471251 @default.
- W2809567882 cites W3021394930 @default.
- W2809567882 cites W3098800800 @default.
- W2809567882 cites W3105167274 @default.
- W2809567882 cites W4245037559 @default.
- W2809567882 doi "https://doi.org/10.1016/j.compfluid.2018.04.030" @default.
- W2809567882 hasPublicationYear "2018" @default.
- W2809567882 type Work @default.
- W2809567882 sameAs 2809567882 @default.
- W2809567882 citedByCount "2" @default.
- W2809567882 countsByYear W28095678822019 @default.
- W2809567882 countsByYear W28095678822023 @default.
- W2809567882 crossrefType "journal-article" @default.
- W2809567882 hasAuthorship W2809567882A5037915614 @default.
- W2809567882 hasAuthorship W2809567882A5082589597 @default.
- W2809567882 hasBestOaLocation W28095678821 @default.
- W2809567882 hasConcept C121332964 @default.
- W2809567882 hasConcept C121448008 @default.
- W2809567882 hasConcept C121864883 @default.
- W2809567882 hasConcept C140820882 @default.
- W2809567882 hasConcept C158622935 @default.
- W2809567882 hasConcept C165231844 @default.
- W2809567882 hasConcept C191544260 @default.
- W2809567882 hasConcept C196558001 @default.
- W2809567882 hasConcept C2780388094 @default.
- W2809567882 hasConcept C38349280 @default.
- W2809567882 hasConcept C5192115 @default.
- W2809567882 hasConcept C57879066 @default.
- W2809567882 hasConcept C62520636 @default.
- W2809567882 hasConcept C74650414 @default.
- W2809567882 hasConcept C84655787 @default.
- W2809567882 hasConceptScore W2809567882C121332964 @default.
- W2809567882 hasConceptScore W2809567882C121448008 @default.
- W2809567882 hasConceptScore W2809567882C121864883 @default.
- W2809567882 hasConceptScore W2809567882C140820882 @default.
- W2809567882 hasConceptScore W2809567882C158622935 @default.
- W2809567882 hasConceptScore W2809567882C165231844 @default.
- W2809567882 hasConceptScore W2809567882C191544260 @default.
- W2809567882 hasConceptScore W2809567882C196558001 @default.
- W2809567882 hasConceptScore W2809567882C2780388094 @default.
- W2809567882 hasConceptScore W2809567882C38349280 @default.
- W2809567882 hasConceptScore W2809567882C5192115 @default.
- W2809567882 hasConceptScore W2809567882C57879066 @default.
- W2809567882 hasConceptScore W2809567882C62520636 @default.
- W2809567882 hasConceptScore W2809567882C74650414 @default.
- W2809567882 hasConceptScore W2809567882C84655787 @default.
- W2809567882 hasLocation W28095678821 @default.
- W2809567882 hasOpenAccess W2809567882 @default.
- W2809567882 hasPrimaryLocation W28095678821 @default.
- W2809567882 hasRelatedWork W1965571475 @default.
- W2809567882 hasRelatedWork W1997121297 @default.
- W2809567882 hasRelatedWork W2046781374 @default.