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Periodic state of fluid flow and heat transfer in a lid-driven cavity due to an oscillating thin fin

机译:由于振荡的薄鳍片,流体在盖子驱动的空腔中流动和传热的周期性状态

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Results of a computational study of periodic laminar flow and heat transfer in a lid-driven square cavity due to an oscillating thin fin are presented. The lid moves from left to right and a thin fin is positioned normal to the right stationary wall. The length of the fin varies sinusoidally with its mean length and amplitude equal to 10% and 5% of the side of the cavity, respectively. Two Reynolds numbers of 100 and 1000 for a Pr = 1 fluid were considered. For a given convection time scale (t_(conv)), fin's oscillation periods (τ) were selected in order to cover both slow (TR = τ/t_(conv) > 1) and fast (τ/t_(conv) < 1) oscillation regimes, covering a Strouhal number range of 0.005-0.5. The periodic flow field for the case with Re = 1000 and TR = 10 is distinguished by the creation, lateral motion and subsequent wall impingement of a CCW rotating vortex within the lower half of the cavity. Periodic flow and thermal fields of the other nine cases studied were not as varied. Phase diagrams of the stream function and temperature vs. fin's length clearly exhibit the synchronous behavior of the system. Amplitude of fluctuations of the kinetic energy and temperature are very intense near the fin. As the fin oscillates slower, a greater portion of the cavity exhibits intense fluctuations. For slow to moderate oscillations, the maximum value of K_(amp) is observed to be greater for Re = 1000 in comparison to Re = 100. For fast oscillations, this behavior is reversed. The maximum values of the amplitude of fluctuations of temperature increase monotonically as the fin oscillates slower. The maximum values of θ_(amp) are greater for Re = 1000 compared to Re = 100. The amplitude of fluctuations of the mean Nusselt number on four walls increase as the fin oscillates slower.
机译:给出了由于振荡的薄翅片而导致的盖驱动方腔中周期性层流和传热的计算研究结果。盖子从左向右移动,薄鳍片垂直于右固定壁放置。鳍片的长度呈正弦变化,其平均长度和幅度分别等于腔侧面的10%和5%。考虑到Pr = 1流体的两个雷诺数分别为100和1000。对于给定的对流时间标度(t_(conv)),选择鳍的振荡周期(τ)以便同时涵盖慢速(TR =τ/ t_(conv)> 1)和快速(τ/ t_(conv)<1) )振荡状态,覆盖0.005-0.5的斯特劳哈尔数范围。对于Re = 1000和TR = 10的情况,周期性流场的特征在于腔体下半部的CCW旋转涡流的产生,横向运动和随后的壁撞击。其他九个案例的周期性流场和热场变化不大。流函数和温度与鳍片长度的相位图清楚地显示了系统的同步行为。在鳍片附近,动能和温度的波动幅度非常大。当鳍片振荡速度变慢时,空腔的大部分会出现剧烈的波动。对于慢到中等的振荡,与Re = 100相比,对于Re = 1000,观察到K_(amp)的最大值更大。对于快速振荡,此行为是相反的。随着鳍的振荡变慢,温度波动幅度的最大值单调增加。与Re = 100相比,Re = 1000的θ_(amp)最大值更大。随着鳍的振荡速度变慢,四壁平均Nusselt数的波动幅度增大。

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