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Steady and time-periodic blowing/suction perturbations in a turbulent channel flow

机译:湍流通道中的稳态和时间周期吹气/吸气扰动

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摘要

Direct Numerical Simulations (DNS) of an incompressible turbulent channel flow with given local perturbations at the walls are performed. Steady and time-periodic blowing/suction are applied by means of narrow spanwise slots located at the lower and upper walls. Our previous investigations on time-periodic blowing/suction (Araya et al. (2008) [13,14] and Araya (2008) [15]) have revealed the existence of a characteristic forcing frequency of f?=0.64 or f+=0.044. At this frequency, the largest local increases of the skin friction in the region downstream from the slots, followed by the highest augmentation of the Stanton number, were achieved. In this study, we seek to compare the different effects of constant blowing/suction with time-periodic blowing/suction on the flow and thermal fields. For the cyclical perturbation, the normal disturbing velocity is varied sinusoidally in time at the characteristic frequency of f?=0.64. In both cases, the forcing amplitude, Ao, is fixed to 0.025. The Reynolds number of the unperturbed case is Reτ=394 and the molecular Prandtl number is Pr=0.71. Isothermal conditions are assumed for the lower wall (hot) and the upper wall (cold), respectively. For the forcing amplitude considered, steady disturbances induce higher modifications on the mean time quantities than time-periodic blowing/suction does. In addition, the effects of steady perturbations were observed to last longer downstream. However, time-periodic blowing/suction disturbances at the characteristic forcing frequency of f+=0.044 have been demonstrated to be more effective in promoting local pressure fluctuations despite its short-distance influence. Furthermore, the energy spectra analysis of fluctuations indicates that time-periodic perturbations at this forcing frequency would be more efficient to excite the very small scales in a turbulent channel flow than by steady disturbances at the same forcing amplitude.
机译:对壁上具有给定局部扰动的不可压缩湍流通道流进行直接数值模拟(DNS)。通过位于下壁和上壁的狭窄翼展方向缝隙,进行稳定的吹扫和定时吹/吸。我们之前对时间周期吹气/吸气的研究(Araya等人(2008)[13,14]和Araya(2008)[15])发现存在特征强迫频率f?= 0.64或f + = 0.044。 。在该频率下,在缝隙下游区域中皮肤摩擦的最大局部增加,随后是斯坦顿数的最大增加。在这项研究中,我们试图比较恒定吹气/吸气与时间周期吹气/吸气对流场和热场的不同影响。对于周期性扰动,正常的干扰速度在特征频率f 1 = 0.64时随时间呈正弦变化。在这两种情况下,强制振幅Ao都固定为0.025。无扰动情况的雷诺数为Reτ= 394,分子的Prandtl数为Pr = 0.71。假定下壁(热)和上壁(冷)的等温条件。对于考虑的强迫幅度,稳定干扰比平均时间吹气/吸气对平均时间量的影响更大。此外,观察到稳定扰动的影响在下游持续更长的时间。然而,已经证明,在特征强迫频率为f + = 0.044的时间周期内,吹气/吸气扰动尽管具有短距离影响,但在促进局部压力波动方面更为有效。此外,波动的能谱分析表明,在相同强迫幅度下,在该强迫频率下的时间周期扰动比在稳态强迫扰动下激发湍流中很小的尺度更有效。

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