Matches in SemOpenAlex for { <https://semopenalex.org/work/W1992508612> ?p ?o ?g. }
- W1992508612 endingPage "1075" @default.
- W1992508612 startingPage "1064" @default.
- W1992508612 abstract "Compressible isothermal-wall channel flows are studied with direct numerical simulation and large-eddy simulation tools. Computations are carried out using a high-order, low-dissipation, bandwidth-optimized weighted essentially nonoscillatory numerical scheme to describe the hyperbolic terms of the Navier–Stokes equations. Periodic supersonic channel flow direct numerical simulation (, , , and ) is used to validate the procedure and the numerical scheme; a new subgrid term contribution based on pressure drop is proposed for the driving term required in momentum and energy equations for large-eddy simulation. Coherent structures of the flowfield are analyzed with scatter plots, criterion, and vorticity fields. As expected, the strong Reynolds analogy is not valid for this nonadiabatic flow. Streaks and horseshoe-like structures are highlighted and detailed. The authors propose a scenario for the formation of horseshoe-like structures. With large-eddy simulation tools, a dynamic procedure to evaluate the turbulent Prandtl number is required because results are found more accurate and computations more stable. Wall temperature and pressure impact are also emphasized on the normalized van Driest velocity profile in the logarithmic region. The classical log law is recovered: with , and a constant depending on and . An analog law is also recovered for the normalized temperature with the maximum of the Prandtl number . An a priori study on mesh requirements determination for a large range of pressure levels is realized through highly near-wall resolved large-eddy simulation." @default.
- W1992508612 created "2016-06-24" @default.
- W1992508612 creator A5005191950 @default.
- W1992508612 creator A5013015930 @default.
- W1992508612 date "2013-09-01" @default.
- W1992508612 modified "2023-09-26" @default.
- W1992508612 title "Direct Numerical Simulation and Large-Eddy Simulation of Supersonic Channel Flow" @default.
- W1992508612 cites W1654446976 @default.
- W1992508612 cites W1964321515 @default.
- W1992508612 cites W2007872098 @default.
- W1992508612 cites W2022249960 @default.
- W1992508612 cites W2028314523 @default.
- W1992508612 cites W2029921733 @default.
- W1992508612 cites W2032632004 @default.
- W1992508612 cites W2057393236 @default.
- W1992508612 cites W2058116430 @default.
- W1992508612 cites W2067138631 @default.
- W1992508612 cites W2071492522 @default.
- W1992508612 cites W2072281465 @default.
- W1992508612 cites W2074447412 @default.
- W1992508612 cites W2086209713 @default.
- W1992508612 cites W2091312969 @default.
- W1992508612 cites W2092566323 @default.
- W1992508612 cites W2109275518 @default.
- W1992508612 cites W2123157681 @default.
- W1992508612 cites W2131537960 @default.
- W1992508612 cites W2135483806 @default.
- W1992508612 cites W2141077768 @default.
- W1992508612 cites W2147591989 @default.
- W1992508612 cites W2168795429 @default.
- W1992508612 cites W2173763669 @default.
- W1992508612 cites W3010292040 @default.
- W1992508612 cites W4246101744 @default.
- W1992508612 cites W4250066299 @default.
- W1992508612 cites W78226598 @default.
- W1992508612 doi "https://doi.org/10.2514/1.b34777" @default.
- W1992508612 hasPublicationYear "2013" @default.
- W1992508612 type Work @default.
- W1992508612 sameAs 1992508612 @default.
- W1992508612 citedByCount "9" @default.
- W1992508612 countsByYear W19925086122015 @default.
- W1992508612 countsByYear W19925086122016 @default.
- W1992508612 countsByYear W19925086122017 @default.
- W1992508612 countsByYear W19925086122020 @default.
- W1992508612 countsByYear W19925086122022 @default.
- W1992508612 crossrefType "journal-article" @default.
- W1992508612 hasAuthorship W1992508612A5005191950 @default.
- W1992508612 hasAuthorship W1992508612A5013015930 @default.
- W1992508612 hasConcept C121332964 @default.
- W1992508612 hasConcept C121448008 @default.
- W1992508612 hasConcept C121864883 @default.
- W1992508612 hasConcept C130230704 @default.
- W1992508612 hasConcept C140820882 @default.
- W1992508612 hasConcept C165231844 @default.
- W1992508612 hasConcept C181824747 @default.
- W1992508612 hasConcept C182748727 @default.
- W1992508612 hasConcept C18533594 @default.
- W1992508612 hasConcept C196558001 @default.
- W1992508612 hasConcept C200114574 @default.
- W1992508612 hasConcept C205991772 @default.
- W1992508612 hasConcept C32526432 @default.
- W1992508612 hasConcept C500300565 @default.
- W1992508612 hasConcept C50517652 @default.
- W1992508612 hasConcept C57879066 @default.
- W1992508612 hasConcept C72687893 @default.
- W1992508612 hasConcept C74650414 @default.
- W1992508612 hasConcept C89881335 @default.
- W1992508612 hasConceptScore W1992508612C121332964 @default.
- W1992508612 hasConceptScore W1992508612C121448008 @default.
- W1992508612 hasConceptScore W1992508612C121864883 @default.
- W1992508612 hasConceptScore W1992508612C130230704 @default.
- W1992508612 hasConceptScore W1992508612C140820882 @default.
- W1992508612 hasConceptScore W1992508612C165231844 @default.
- W1992508612 hasConceptScore W1992508612C181824747 @default.
- W1992508612 hasConceptScore W1992508612C182748727 @default.
- W1992508612 hasConceptScore W1992508612C18533594 @default.
- W1992508612 hasConceptScore W1992508612C196558001 @default.
- W1992508612 hasConceptScore W1992508612C200114574 @default.
- W1992508612 hasConceptScore W1992508612C205991772 @default.
- W1992508612 hasConceptScore W1992508612C32526432 @default.
- W1992508612 hasConceptScore W1992508612C500300565 @default.
- W1992508612 hasConceptScore W1992508612C50517652 @default.
- W1992508612 hasConceptScore W1992508612C57879066 @default.
- W1992508612 hasConceptScore W1992508612C72687893 @default.
- W1992508612 hasConceptScore W1992508612C74650414 @default.
- W1992508612 hasConceptScore W1992508612C89881335 @default.
- W1992508612 hasIssue "5" @default.
- W1992508612 hasLocation W19925086121 @default.
- W1992508612 hasLocation W19925086122 @default.
- W1992508612 hasOpenAccess W1992508612 @default.
- W1992508612 hasPrimaryLocation W19925086121 @default.
- W1992508612 hasRelatedWork W176552594 @default.
- W1992508612 hasRelatedWork W1766475506 @default.
- W1992508612 hasRelatedWork W2025499724 @default.
- W1992508612 hasRelatedWork W2094332773 @default.
- W1992508612 hasRelatedWork W2567447833 @default.
- W1992508612 hasRelatedWork W2739459952 @default.
- W1992508612 hasRelatedWork W3123831362 @default.