Effects of Corner Radii on Vortex-Induced Vibration With Forced Convection Heat Transfer From Angled Tandem-Cylinder at Low Re

Yuvraj Sarout, Md. Islam, I. Janajreh
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引用次数: 1

Abstract

Flow-induced vibration (FIV) of the modified tandem-cylinder with a change in corner radii has been investigated in a laminar flow regime with Re = 150 and Pr = 0.7. The corner radius (r: corner radii, R: cylinder characteristic length) r* = 0, 0.5, 0.75 and 1 are used at a constant angle of attack of 45°. The cylinders are allowed to vibrate in transverse direction while restricted in axial direction with spacing ratio L/D = 4. Computation is carried out with a fixed mass ratio m* = 10 and varying reduced velocity Ur = 2 ∼ 10. Constant heating is provided by keeping boundary at a constant temperature. The two-dimensional incompressible Navier-Stokes equations and energy equation are coupled together. Navier-Stokes equations are used with FIV equation of elastically supported cylinder to have flow solutions. Lock-in phenomenon for most of the configuration is occurring at Ur = 6 where vibrational amplitude for most of the configuration is peaked. At Ur = 6 for square cylinder, pseudo ‘2P’ can be observed in the wake of r* = 0. Vortices at Ur = 6 are not merged properly to form a definite type of vortex shedding, although in further downstream weak 2S vortex shedding can be observed. Heating of cylinder is affected by various parameters such as corner radii and spacing ratio with other factors such as early flow separation, reattachment, and vibrational amplitude. Maximum values of Average Nusselt number Nuavg is at Ur = 6 for circular cylinder, whereas minimum lies at Ur = 2 for square downstream cylinder. Results give a deep insight into heat transfer getting changed by changing different parameters and will make a base for future study of tube bundles in heat exchangers with FIV.
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角半径对低雷诺数下斜置圆柱强制对流换热涡激振动的影响
在Re = 150, Pr = 0.7的层流流态下,研究了改进型串联式圆柱体随转角半径变化的流激振动。角半径(r:角半径,r:圆柱体特征长度)r* = 0、0.5、0.75、1在攻角恒定为45°时使用。圆柱横向允许振动,轴向限制振动,间距比L/D = 4。计算采用固定质量比m* = 10和变减速速度Ur = 2 ~ 10进行。通过保持边界温度恒定,可以提供恒定的加热。将二维不可压缩Navier-Stokes方程和能量方程耦合在一起。将Navier-Stokes方程与弹性支撑柱体的FIV方程结合,得到了流动解。大多数构型的锁定现象发生在Ur = 6处,大多数构型的振动幅度达到峰值。当方形圆柱Ur = 6时,在r* = 0的尾迹处可以观察到伪2P。在Ur = 6处的涡没有完全合并,形成一种明确的涡脱落类型,但在更远的下游可以观察到微弱的2S涡脱落。筒体加热受转角半径、间距比等参数的影响,还受早期流动分离、再附着、振动幅度等因素的影响。平均努塞尔数Nuavg的最大值为圆形柱体的Ur = 6,最小值为方形下游柱体的Ur = 2。研究结果深入揭示了不同参数对换热特性的影响,为今后换热器管束的研究奠定了基础。
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