Matches in SemOpenAlex for { <https://semopenalex.org/work/W4386132896> ?p ?o ?g. }
- W4386132896 endingPage "103958" @default.
- W4386132896 startingPage "103958" @default.
- W4386132896 abstract "The purpose of this study is to develop a reduced-order model (ROM) for the prediction of vortex-induced vibration of an elastically mounted circular cylinder constrained to oscillate purely in-line with a uniform free stream. The fluid force in the streamwise direction was modeled by an extended version of Morison’s equation that comprises an inviscid inertial component opposing the cylinder acceleration, a viscous drag component proportional to the square of the relative velocity of the free stream and the oscillating cylinder, and a wake drag component representing the excitation from vortex shedding. A van der Pol equation was employed to model the oscillating wake drag component. The coupling between the oscillating wake and the oscillating cylinder was accomplished by forcing the wake oscillator with a term proportional to either the acceleration or the velocity of the cylinder. The ROM parameters were tuned against data from numerical solutions of the full system of non-linear equations governing the fluid and cylinder motions for a cylinder with a mass ratio of 10 and a Reynolds number of 180. The results showed that acceleration forcing can predict well the amplitude response when the ROM is properly tuned, whereas velocity forcing leads to underestimation of the amplitude response. In addition, acceleration forcing can predict satisfactorily the magnitude of the total streamwise force and of the wake drag. However, the trend in the frequency response was not well predicted by acceleration forcing, which was predicted more satisfactorily by velocity forcing. Both acceleration and velocity forcing predicted satisfactorily the phase lag between the wake drag and the cylinder displacement. Predictions with the calibrated ROM at different mass ratios captured well the amplitude response as a function of the reduced velocity, including the narrowing of the range where relatively high amplitudes occur, as in the full numerical simulations. Linear stability analysis based on the ROM equations indicated that the interaction between the fluid and the vibrating cylinder has the characteristics of nonlinear resonance, where the selection of the common frequency of the system is sensitive to nonlinearities, which cannot be faithfully captured by the van der Pol wake oscillator." @default.
- W4386132896 created "2023-08-25" @default.
- W4386132896 creator A5021066144 @default.
- W4386132896 creator A5057757758 @default.
- W4386132896 creator A5073270631 @default.
- W4386132896 creator A5091427665 @default.
- W4386132896 date "2023-10-01" @default.
- W4386132896 modified "2023-10-18" @default.
- W4386132896 title "Aspects of vortex-induced in-line vibration at low Reynolds numbers: Simulation and prediction by a reduced-order model" @default.
- W4386132896 cites W1478048485 @default.
- W4386132896 cites W1975882045 @default.
- W4386132896 cites W1979048468 @default.
- W4386132896 cites W1980906192 @default.
- W4386132896 cites W1985839812 @default.
- W4386132896 cites W1989659923 @default.
- W4386132896 cites W2043014996 @default.
- W4386132896 cites W2044305809 @default.
- W4386132896 cites W2045308943 @default.
- W4386132896 cites W2047542720 @default.
- W4386132896 cites W2057079320 @default.
- W4386132896 cites W2060711624 @default.
- W4386132896 cites W2062842814 @default.
- W4386132896 cites W2063824742 @default.
- W4386132896 cites W2098840252 @default.
- W4386132896 cites W2105837825 @default.
- W4386132896 cites W2147814840 @default.
- W4386132896 cites W2170254912 @default.
- W4386132896 cites W2212704950 @default.
- W4386132896 cites W2338871146 @default.
- W4386132896 cites W2609167807 @default.
- W4386132896 cites W2803715485 @default.
- W4386132896 cites W2921396373 @default.
- W4386132896 cites W2968095281 @default.
- W4386132896 cites W2997703243 @default.
- W4386132896 cites W3083575487 @default.
- W4386132896 cites W3110117645 @default.
- W4386132896 cites W3208305521 @default.
- W4386132896 cites W4280514069 @default.
- W4386132896 doi "https://doi.org/10.1016/j.jfluidstructs.2023.103958" @default.
- W4386132896 hasPublicationYear "2023" @default.
- W4386132896 type Work @default.
- W4386132896 citedByCount "0" @default.
- W4386132896 crossrefType "journal-article" @default.
- W4386132896 hasAuthorship W4386132896A5021066144 @default.
- W4386132896 hasAuthorship W4386132896A5057757758 @default.
- W4386132896 hasAuthorship W4386132896A5073270631 @default.
- W4386132896 hasAuthorship W4386132896A5091427665 @default.
- W4386132896 hasBestOaLocation W43861328961 @default.
- W4386132896 hasConcept C10599892 @default.
- W4386132896 hasConcept C117896860 @default.
- W4386132896 hasConcept C120665830 @default.
- W4386132896 hasConcept C121332964 @default.
- W4386132896 hasConcept C122312997 @default.
- W4386132896 hasConcept C140820882 @default.
- W4386132896 hasConcept C178760647 @default.
- W4386132896 hasConcept C180205008 @default.
- W4386132896 hasConcept C182748727 @default.
- W4386132896 hasConcept C190840664 @default.
- W4386132896 hasConcept C196558001 @default.
- W4386132896 hasConcept C197115733 @default.
- W4386132896 hasConcept C198394728 @default.
- W4386132896 hasConcept C203311528 @default.
- W4386132896 hasConcept C24890656 @default.
- W4386132896 hasConcept C2524010 @default.
- W4386132896 hasConcept C33923547 @default.
- W4386132896 hasConcept C48939323 @default.
- W4386132896 hasConcept C57879066 @default.
- W4386132896 hasConcept C72117827 @default.
- W4386132896 hasConcept C72921944 @default.
- W4386132896 hasConcept C74650414 @default.
- W4386132896 hasConcept C86252789 @default.
- W4386132896 hasConcept C91586092 @default.
- W4386132896 hasConceptScore W4386132896C10599892 @default.
- W4386132896 hasConceptScore W4386132896C117896860 @default.
- W4386132896 hasConceptScore W4386132896C120665830 @default.
- W4386132896 hasConceptScore W4386132896C121332964 @default.
- W4386132896 hasConceptScore W4386132896C122312997 @default.
- W4386132896 hasConceptScore W4386132896C140820882 @default.
- W4386132896 hasConceptScore W4386132896C178760647 @default.
- W4386132896 hasConceptScore W4386132896C180205008 @default.
- W4386132896 hasConceptScore W4386132896C182748727 @default.
- W4386132896 hasConceptScore W4386132896C190840664 @default.
- W4386132896 hasConceptScore W4386132896C196558001 @default.
- W4386132896 hasConceptScore W4386132896C197115733 @default.
- W4386132896 hasConceptScore W4386132896C198394728 @default.
- W4386132896 hasConceptScore W4386132896C203311528 @default.
- W4386132896 hasConceptScore W4386132896C24890656 @default.
- W4386132896 hasConceptScore W4386132896C2524010 @default.
- W4386132896 hasConceptScore W4386132896C33923547 @default.
- W4386132896 hasConceptScore W4386132896C48939323 @default.
- W4386132896 hasConceptScore W4386132896C57879066 @default.
- W4386132896 hasConceptScore W4386132896C72117827 @default.
- W4386132896 hasConceptScore W4386132896C72921944 @default.
- W4386132896 hasConceptScore W4386132896C74650414 @default.
- W4386132896 hasConceptScore W4386132896C86252789 @default.
- W4386132896 hasConceptScore W4386132896C91586092 @default.
- W4386132896 hasLocation W43861328961 @default.
- W4386132896 hasOpenAccess W4386132896 @default.