2007
DOI: 10.1103/physreve.75.025302
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Transition from laminar to turbulent drag in flow due to a vibrating quartz fork

Abstract: Flow due to a commercially available vibrating quartz fork is studied in gaseous helium, He I and He II, over a wide range of temperatures and pressures. On increasing the driving force applied to the fork, the drag changes in character from laminar (characterized by a linear drive vs velocity dependence) to turbulent (characterized by a quadratic drive vs velocity dependence). We characterize this transition by a critical Reynolds number Recrdelta=Ucrdelta/nu, where Ucr is the critical velocity, nu stands for… Show more

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Cited by 60 publications
(43 citation statements)
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“…30, chapter 5). We note also the critical velocity for the formation of a classical turbulent wake behind an oscillating structure: in the case when the viscous penetration depth is greater than the size of the structure (low frequency), the critical velocity is given by putting the Reynolds number equal to unity; in the opposite limit, it is given in order of magnitude by (31,32):…”
Section: The Development Of Quantum Turbulencementioning
confidence: 99%
“…30, chapter 5). We note also the critical velocity for the formation of a classical turbulent wake behind an oscillating structure: in the case when the viscous penetration depth is greater than the size of the structure (low frequency), the critical velocity is given by putting the Reynolds number equal to unity; in the opposite limit, it is given in order of magnitude by (31,32):…”
Section: The Development Of Quantum Turbulencementioning
confidence: 99%
“…Additional experiments in water at room temperature (dynamically similar to the ones in normal helium) using the Baker visualization technique [25] and Kalliroscope [26] have proved that the observed change in the drag force is indeed associated with turbulence [27]. In the normal helium liquid and helium gas, which both behave as classical fluids of low kinematic viscosity, the obtained critical velocities conform to the expected scaling law of v c ∝ √ νω, see [28,29]. When the same data are plotted in terms of the drag coefficient, an unexpected feature is seen for the data taken in the superfluid, esp.…”
Section: Efm11mentioning
confidence: 89%
“…6, where the calibration procedure and the potential of the fork used as thermometer or pressure gauge has been considered in detail. Moreover, if driven in the nonlinear flow regime, it serves as an excellent tool to study the crossover from the laminar drag regime (characterized by a linear drive versus velocity dependence) to the turbulent drag regime (characterized by a quadratic drive versus velocity dependence) in both classical viscous fluids [7] and quantum fluids [8].…”
Section: Introductionmentioning
confidence: 99%