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The cause of oscillations of the large-scale circulation of turbulent Rayleigh-B{\'e}nard convection

机译:湍流大规模循环振荡的原因   Rayleigh-B {\'e} nard对流

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摘要

In agreement with a recent experimental discovery by Xia et. al. (2009), wealso find a sloshing mode in experiments on the large-scale circulation (LSC)of turbulent Rayleigh-Benard convection in a cylindrical sample of aspect ratioone. The sloshing mode has the same frequency as the torsional oscillationdiscovered by Funfschilling and Ahlers (2004). We show that both modes can bedescribed by an extension of a model developed previously [Brown and Ahlers(2008)] which consists of permitting a lateral displacement of the LSCcirculation plane away from the vertical center line of the sample as well as avariation in displacements with height (such displacements had been excluded inthe original model). Pressure gradients produced by the side wall of thecontainer on average center the plane of the LSC so that it prefers to reachits longest diameter. If the LSC is displaced away from this diameter, thewalls provide a restoring force. Turbulent fluctuations drive the LSC away fromthe central alignment, and combined with the restoring force they lead tooscillations. These oscillations are advected along with the LSC. This modelpredicts the correct wavenumber and phase of the oscillations, as well asestimates of the frequency, amplitude, and probability distributions of thedisplacements.
机译:与Xia等人最近的实验发现相一致。等(2009),我们还发现了在宽高比为圆柱形的样品中湍流瑞利-贝纳德对流的大规模循环(LSC)实验中的晃荡模式。晃动模式的频率与Funfschilling和Ahlers(2004)发现的扭转振动的频率相同。我们表明,这两种模式都可以通过先前开发的模型的扩展来描述[Brown and Ahlers(2008)],该模型包括允许LSC循环平面的横向位移远离样品的垂直中心线以及位移随高度(原始模型中不包括此类位移)。容器侧壁平均产生的压力梯度位于LSC平面的中心,因此它倾向于达到最长的直径。如果LSC偏离此直径,则壁会提供恢复力。湍流的波动使LSC偏离中心对准,并与恢复力相结合,导致过分振荡。这些振荡与LSC一起发生。该模型可预测正确的振荡波数和相位,并估计位移的频率,幅度和概率分布。

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