2015
DOI: 10.1016/j.ijheatfluidflow.2015.05.006
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Experimental study on the flow regimes past a confined prism undergoing self-sustained oscillations

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Cited by 7 publications
(11 citation statements)
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“…For the lowest Reynolds number investigated (Re¼50) and the same channel-to-square width ratio than here, the critical density ratio was around 0.1. It is worth also remarking the work done by Reyes et al (2015), where the self-sustained oscillations of a square cylinder confined in channel were investigated at Reynolds numbers (based on the square width, too) ranging between 100 and 700, because they used the same channel-to-square width ratio than in the present study. For each Reynolds number they found a critical density ratio for which different oscillation regimes were found, going from no square motion at all (at Re¼100), to vibration around the equilibrium position with either the typical von Kármán streets downstream (at Re¼300) or with a chaotic wake (at Re ¼ 700).…”
Section: Introductionmentioning
confidence: 97%
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“…For the lowest Reynolds number investigated (Re¼50) and the same channel-to-square width ratio than here, the critical density ratio was around 0.1. It is worth also remarking the work done by Reyes et al (2015), where the self-sustained oscillations of a square cylinder confined in channel were investigated at Reynolds numbers (based on the square width, too) ranging between 100 and 700, because they used the same channel-to-square width ratio than in the present study. For each Reynolds number they found a critical density ratio for which different oscillation regimes were found, going from no square motion at all (at Re¼100), to vibration around the equilibrium position with either the typical von Kármán streets downstream (at Re¼300) or with a chaotic wake (at Re ¼ 700).…”
Section: Introductionmentioning
confidence: 97%
“…For each Reynolds number they found a critical density ratio for which different oscillation regimes were found, going from no square motion at all (at Re¼100), to vibration around the equilibrium position with either the typical von Kármán streets downstream (at Re¼300) or with a chaotic wake (at Re ¼ 700). However, when these Reynolds numbers used in Sánchez-Sanz and Velazquez (2009) and Reyes et al (2015) are re-calculated and based on the channel width, as it is in micromixing devices, they are higher than the typical micromixing Reynolds numbers, since the later are very small , usually lower than 100. Due to this, the VIV mixing mechanism seems not to be adequate for micromixing.…”
Section: Introductionmentioning
confidence: 99%
“…al. [54] the same problem is addressed with a crucial difference: in this case the prism is left to oscillate self selfsustainedly by tethering it with thin cables to the channel walls, but still, inside an isothermal channel. Three different prism to water densities are tested (different buoyancy forces).…”
Section: The Confined Cylinder Problemmentioning
confidence: 99%
“…The main objective of this experiment was to determine if any of the possible flow topologies resulting from flow induced vibrations found in [54] were suitable to enhance mixing. To find it out, temperature was chosen as scalar to be traced.…”
Section: Flow Induced Vibration Mixing Enhancementmentioning
confidence: 99%
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