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An experimental investigation of negative wakes behind spheres settling in a shear-thinning viscoelastic fluid

机译:剪切稀化粘弹性流体中球体沉降后负尾流的实验研究

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We present detailed experimental results examining "negative wakes" behind spheres settling along the centerline of a tube containing a viscoelastic aqueous polyacrylamide solution. Negative wakes are found for all Deborah numbers (2.43 less-than-or-equal-to De (gamma)(over-dot) less-than-or-equal-to 8.75) and sphere-to-tube aspect ratios (0.060 less-than-or-equal-to a/R less-than 0.396) examined. The wake structures are investigated using laser-Doppler velocimetry (LDV) to examine the centerline fluid velocity around the sphere and digital particle image velocimetry (DPIV) for full-field velocity profiles. For a fixed aspect ratio, the magnitude of the most negative velocity, U-min, in the wake is seen to increase with increasing De. Additionally, as the Deborah number becomes larger, the location of this minimum velocity shifts farther downstream. When normalized with the sphere radius and the steady state velocity of the sphere, the axial velocity profiles become self-similar to the point of the minimum velocity. Beyond this point, the wake structure varies weakly with aspect ratio and De, and it extends more than 20 radii downstream. Inertial effects at high Reynolds numbers are observed to shift the entire negative wake farther downstream. Using DPIV to investigate the transient kinematic response of the fluid to the initial acceleration of the sphere from rest, it is seen that the wake develops from the nonlinear fluid response at large strains. Measurements of the transient uniaxial extensional viscosity of this weakly strain-hardening fluid using a filament stretching rheometer show that the existence of a negative wake is consistent with theoretical arguments based on the opposing roles of extensional stresses and shearing stresses in the wake of the sphere. [References: 32]
机译:我们提出了详细的实验结果,研究了沿着包含粘弹性聚丙烯酰胺水溶液的管的中心线沉降的球体背后的“负尾流”。发现所有Deborah数的负尾迹(比De(γ)小2.43或小于8.75的Deγ)和球管长宽比(小于0.060) -等于或小于a / R小于0.396)。使用激光多普勒测速仪(LDV)来研究尾流结构,以检查围绕球体的中心线流体速度,并使用数字粒子图像测速仪(DPIV)来获得全场速度剖面。对于固定的宽高比,尾随时最大负速度U-min的大小随De的增加而增加。此外,随着Deborah数变大,此最小速度的位置向下游移动。当用球体半径和球体的稳态速度归一化时,轴向速度分布与最小速度的点自相似。超过这一点,尾流结构随长宽比和De的变化很小,并且向下游延伸超过20个半径。观察到高雷诺数的惯性效应使整个负尾流向下游移动。使用DPIV研究流体对静止状态下球体初始加速度的瞬态运动学响应,可以看出,尾流是由大应变下的非线性流体响应形成的。使用细丝拉伸流变仪对这种弱应变硬化流体的瞬态单轴拉伸粘度的测量结果表明,负尾流的存在与基于理论的论点相一致,这是基于球形尾流中拉伸应力和剪切应力的相反作用而得出的。 [参考:32]

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