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Pulsatile flow past an oscillating cylinder

机译:脉动流经过振荡缸

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摘要

A fundamental study to characterize the flow around an oscillating cylinder in a pulsatile flow environment is investigated. This work is motivated by a new proposed design of the total artificial lung (TAL), which is envisioned to provide better gas exchange. The Navier–Stokes computations in a moving frame of reference were performed to compute the dynamic flow field surrounding the cylinder. Cylinder oscillations and pulsatile free-stream velocity were represented by two sinusoidal waves with amplitudes A and B and frequencies ωc and ω, respectively. The Keulegan–Carpenter number (Kc=Uo∕Dωc) was used to describe the frequency of the oscillating cylinder while the pulsatile free-stream velocity was fixed by imposing ω∕Kc=1 for all cases investigated. The parameters of interest and their values were amplitude (0.5D<A<D), the Keulegan–Carpenter number (0.33<Kc<1), and the Reynolds number (5<Re<20) corresponding to operating conditions of the TAL. It was observed that an increase in amplitude and a decrease in Kc are associated with an increase in vorticity (up to 246%) for every Re suggesting that mixing could be enhanced by the proposed TAL design. The drag coefficient was found to decrease for higher amplitudes and lower Kc for all cases investigated. In some cases the drag coefficient values were found to be lower than the stationary cylinder values (A=0.5, Kc=0.3, and Re=10 and 20). A lock-in phenomenon (cylinder oscillating frequency matched the vortex shedding frequency) was found when Kc=1 for all cases. This lock-in condition was attributed to be the cause of the rise in drag observed in that operating regime. For optimal performance of the modified TAL design it is recommended to operate the device at higher fiber oscillation amplitudes and lower Kc (avoiding the lock-in regime).
机译:研究了表征脉动流动环境中摆动圆柱体周围流动的基础研究。这项工作是由总人工肺(TAL)的新提议设计推动的,该设计旨在提供更好的气体交换。在参考运动的框架中进行了Navier–Stokes计算,以计算圆柱周围的动态流场。圆柱振动和脉动自由流速度分别由两个正弦波表示,振幅分别为A和B,频率为ωc和ω。 Keulegan-Carpenter数(Kc = Uo ∕Dωc)用来描述振荡筒的频率,而通过对所有研究情况施加ω∕ Kc = 1来固定脉动自由流速度。感兴趣的参数及其值是振幅(0.5D

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