Matches in SemOpenAlex for { <https://semopenalex.org/work/W2099221246> ?p ?o ?g. }
- W2099221246 endingPage "459" @default.
- W2099221246 startingPage "434" @default.
- W2099221246 abstract "A single bubble is placed in a solid-body rotating flow of silicon oil. From the measurement of its equilibrium position, lift and drag forces are determined. Five different silicon oils have been used, providing five different viscosities and Morton numbers. Experiments have been performed over a wide range of bubble Reynolds numbers (0.7 ≤ Re ≤ 380), Rossby numbers (0.58 ≤ Ro ≤ 26) and bubble aspect ratios (1 ≤ χ ≤ 3). For spherical bubbles, the drag coefficient at the first order is the same as that of clean spherical bubbles in a uniform flow. It noticeably increases with the local shear S = Ro −1 , following a Ro −5/2 power law. The lift coefficient tends to 0.5 for large Re numbers and rapidly decreases as Re tends to zero, in agreement with existing simulations. It becomes hardly measurable for Re approaching unity. When bubbles start to shrink with Re numbers decreasing slowly, drag and lift coefficients instantaneously follow their stationary curves versus Re . In the standard Eötvös–Reynolds diagram, the transitions from spherical to deformed shapes slightly differ from the uniform flow case, with asymmetric shapes appearing. The aspect ratio χ for deformed bubbles increases with the Weber number following a law which lies in between the two expressions derived from the potential flow theory by Moore ( J. Fluid Mech. , vol. 6, 1959, pp. 113–130) and Moore ( J. Fluid Mech. , vol. 23, 1965, pp. 749–766) at low- and moderate We , and the bubble orients with an angle between its minor axis and the direction of the flow that increases for low Ro . The drag coefficient increases with χ, to an extent which is well predicted by the Moore (1965) drag law at high Re and Ro . The lift coefficient is a function of both χ and Re . It increases linearly with (χ − 1) at high Re , in line with the inviscid theory, while in the intermediate range of Reynolds numbers, a decrease of lift with aspect ratio is observed. However, the deformation is not sufficient for a reversal of lift to occur." @default.
- W2099221246 created "2016-06-24" @default.
- W2099221246 creator A5010190747 @default.
- W2099221246 creator A5013451102 @default.
- W2099221246 creator A5083996939 @default.
- W2099221246 date "2011-07-19" @default.
- W2099221246 modified "2023-10-16" @default.
- W2099221246 title "Drag and lift forces on clean spherical and ellipsoidal bubbles in a solid-body rotating flow" @default.
- W2099221246 cites W1966983433 @default.
- W2099221246 cites W1969574061 @default.
- W2099221246 cites W1975944783 @default.
- W2099221246 cites W1981266929 @default.
- W2099221246 cites W1982487125 @default.
- W2099221246 cites W1992798196 @default.
- W2099221246 cites W1994936966 @default.
- W2099221246 cites W1996522799 @default.
- W2099221246 cites W2000108132 @default.
- W2099221246 cites W2015030561 @default.
- W2099221246 cites W2033093132 @default.
- W2099221246 cites W2038097455 @default.
- W2099221246 cites W2046135488 @default.
- W2099221246 cites W2047191809 @default.
- W2099221246 cites W2048735357 @default.
- W2099221246 cites W2049524580 @default.
- W2099221246 cites W2053038550 @default.
- W2099221246 cites W2057428581 @default.
- W2099221246 cites W2058833885 @default.
- W2099221246 cites W2060584020 @default.
- W2099221246 cites W2086936614 @default.
- W2099221246 cites W2097164075 @default.
- W2099221246 cites W2097281072 @default.
- W2099221246 cites W2099947840 @default.
- W2099221246 cites W2100055609 @default.
- W2099221246 cites W2119533737 @default.
- W2099221246 cites W2119823877 @default.
- W2099221246 cites W2132145594 @default.
- W2099221246 cites W2132428637 @default.
- W2099221246 cites W2134020148 @default.
- W2099221246 cites W2136599785 @default.
- W2099221246 cites W2147104524 @default.
- W2099221246 cites W2160897293 @default.
- W2099221246 cites W2169625305 @default.
- W2099221246 cites W4231302723 @default.
- W2099221246 cites W4240575290 @default.
- W2099221246 doi "https://doi.org/10.1017/jfm.2011.240" @default.
- W2099221246 hasPublicationYear "2011" @default.
- W2099221246 type Work @default.
- W2099221246 sameAs 2099221246 @default.
- W2099221246 citedByCount "78" @default.
- W2099221246 countsByYear W20992212462012 @default.
- W2099221246 countsByYear W20992212462013 @default.
- W2099221246 countsByYear W20992212462014 @default.
- W2099221246 countsByYear W20992212462015 @default.
- W2099221246 countsByYear W20992212462016 @default.
- W2099221246 countsByYear W20992212462017 @default.
- W2099221246 countsByYear W20992212462018 @default.
- W2099221246 countsByYear W20992212462019 @default.
- W2099221246 countsByYear W20992212462020 @default.
- W2099221246 countsByYear W20992212462021 @default.
- W2099221246 countsByYear W20992212462022 @default.
- W2099221246 countsByYear W20992212462023 @default.
- W2099221246 crossrefType "journal-article" @default.
- W2099221246 hasAuthorship W2099221246A5010190747 @default.
- W2099221246 hasAuthorship W2099221246A5013451102 @default.
- W2099221246 hasAuthorship W2099221246A5083996939 @default.
- W2099221246 hasBestOaLocation W20992212462 @default.
- W2099221246 hasConcept C107157880 @default.
- W2099221246 hasConcept C121332964 @default.
- W2099221246 hasConcept C124101348 @default.
- W2099221246 hasConcept C139002025 @default.
- W2099221246 hasConcept C150486481 @default.
- W2099221246 hasConcept C157915830 @default.
- W2099221246 hasConcept C182748727 @default.
- W2099221246 hasConcept C196558001 @default.
- W2099221246 hasConcept C41008148 @default.
- W2099221246 hasConcept C42652486 @default.
- W2099221246 hasConcept C57879066 @default.
- W2099221246 hasConcept C72117827 @default.
- W2099221246 hasConcept C72921944 @default.
- W2099221246 hasConcept C74650414 @default.
- W2099221246 hasConceptScore W2099221246C107157880 @default.
- W2099221246 hasConceptScore W2099221246C121332964 @default.
- W2099221246 hasConceptScore W2099221246C124101348 @default.
- W2099221246 hasConceptScore W2099221246C139002025 @default.
- W2099221246 hasConceptScore W2099221246C150486481 @default.
- W2099221246 hasConceptScore W2099221246C157915830 @default.
- W2099221246 hasConceptScore W2099221246C182748727 @default.
- W2099221246 hasConceptScore W2099221246C196558001 @default.
- W2099221246 hasConceptScore W2099221246C41008148 @default.
- W2099221246 hasConceptScore W2099221246C42652486 @default.
- W2099221246 hasConceptScore W2099221246C57879066 @default.
- W2099221246 hasConceptScore W2099221246C72117827 @default.
- W2099221246 hasConceptScore W2099221246C72921944 @default.
- W2099221246 hasConceptScore W2099221246C74650414 @default.
- W2099221246 hasLocation W20992212461 @default.
- W2099221246 hasLocation W20992212462 @default.
- W2099221246 hasLocation W20992212463 @default.
- W2099221246 hasLocation W20992212464 @default.