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Modification of turbulent channel flow by passive and additive devices.

机译:通过被动和附加装置修改湍流通道。

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Three devices are examined independently in this study: increasing the Reynolds number (passive device), injection of high molecular weight long-chain polymers (additive device), and introduction of micelle rods (additive device). This experimental investigation focuses on how the velocity statistics in a turbulent channel flow are modified by these devices. Two optical measurement techniques, laser Doppler velocimetry (LDV) and particle-image velocimetry (PIV), are used to obtain accurate measurements of the instantaneous fluctuating velocities in a 5.08 cm {dollar}times{dollar} 61.0 cm rectangular channel.; A two-component laser Doppler velocimeter, with high spatial and temporal resolution, was used to measure the instantaneous streamwise and normal velocities for six different Reynolds numbers; {dollar}Resb{lcub}b{rcub}{dollar} = 5100, 9200, 12400, 20300, 31200, and 48800 (based on the bulk velocity and half-height of the channel). Results are presented comparing the streamwise mean velocity, the root-mean-square of the streamwise and normal velocity fluctuations, Reynolds shear stresses, and the streamwise and normal power spectral density functions. The ideas of inner and outer scaling are supported by the measurements. Scaling of the power spectral density function of the streamwise and normal velocity fluctuations shows that the energy contributed by large frequencies increases with increasing Reynolds number, indicating larger contributions from smaller turbulence structures.; In this investigation, the instantaneous streamwise and normal velocity fluctuations were measured with LDV over a large range of drag reductions (10% to 69%) and polymer concentrations (0.25 ppm to 50 ppm) for {dollar}Resb{lcub}b{rcub} simeq{dollar} 20300. The polymer used was Percol 727, a copolymer of polyacrylamide and sodium-acrylate. Comparisons of the turbulence statistics obtained for the different polymer solutions were made to measurements for water at the same Reynolds number. The velocity statistics were found to be quite different for low drag-reduction ({dollar}{dollar}60%).; Solutions of surfactants in water can be formulated so that rod-shaped micelles are created, which can reduce the drag over what would be experienced with a Newtonian fluid flowing turbulently at the same rate. A solution of 2000 ppm tallow-(tris-hydroxyethyl)-ammonium acetate (or Ethoquad T/13/50) and sodium salicylate is investigated in this study. The instantaneous streamwise and normal velocity fluctuations were measured using LDV for four different Reynolds numbers; {dollar}Resb{lcub}b{rcub}{dollar} = 13300, 19100, 3200, and 49100. For a fixed volumetric flow the pressure drop is reduced by 62 to 76 per cent when compared to a Newtonian flow with an equal wall viscosity. Measurements were made of the mean streamwise velocity, the root-mean-square of the streamwise and normal fluctuating velocities, the Reynolds shear stress, and the spectral density function of the fluctuating velocity in the streamwise direction. (Abstract shortened by UMI.)
机译:在这项研究中,对三种装置进行了独立检查:增加雷诺数(无源装置),注射高分子量长链聚合物(添加物装置)和引入胶束棒(添加物装置)。这项实验研究的重点是这些设备如何修改湍流通道中的速度统计数据。激光多普勒测速仪(LDV)和粒子图像测速仪(PIV)两种光学测量技术用于获得5.08厘米{美元}倍{美元} 61.0厘米矩形通道中瞬时波动速度的精确测量值。具有高时空分辨率的两分量激光多普勒测速仪用于测量六个不同雷诺数的瞬时流向和法向速度。 {dollar} Resb {lcub} b {rcub} {dollar} = 5100、9200、12400、20300、31200和48800(基于通道的整体速度和半高)。给出了比较流向平均速度,流向和法向速度波动的均方根,雷诺剪切应力以及流向和法向功率谱密度函数的结果。测量支持内部和外部缩放的想法。流向和法向速度波动的功率谱密度函数的缩放显示,大频率贡献的能量随雷诺数的增加而增加,表明较小湍流结构的贡献更大。在这项研究中,对于{美元} Resb {lcub} b {rcub,在较大的减阻(10%至69%)和聚合物浓度(0.25 ppm至50 ppm)的大范围内,用LDV测量了瞬时的流速和法向速度波动。 } simeq {dollar} 20300。所用的聚合物是Percol 727,它是聚丙烯酰胺和丙烯酸钠的共聚物。比较了不同聚合物溶液获得的湍流统计数据,以比较雷诺数相同时的水含量。速度统计数据在低减阻方面有很大不同({dollar} {dollar} 60%)。可以配制表面活性剂在水中的溶液,以便形成棒状胶束,这可以减少以相同速率湍流流动的牛顿流体所经历的阻力。在这项研究中研究了2000 ppm牛脂-(三羟乙基)-乙酸铵(或Ethoquad T / 13/50)和水杨酸钠的溶液。对于四个不同的雷诺数,使用LDV测量了瞬时的瞬时水流和法向速度波动。 {dollar} Resb {lcub} b {rcub} {dollar} = 13300、19100、3200和49100。对于固定体积流量,与等壁牛顿流相比,压降降低了62%至76%粘度。对平均流速,流速和法向波动速度的均方根,雷诺剪切应力以及沿流速方向的波动速度的频谱密度函数进行了测量。 (摘要由UMI缩短。)

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