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首页> 外文期刊>Journal of Fluid Mechanics >The measurement of the shear-induced particle and fluid tracer diffusivities in concentrated suspensions by a novel method
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The measurement of the shear-induced particle and fluid tracer diffusivities in concentrated suspensions by a novel method

机译:用一种新方法测量浓悬液中剪切诱导的颗粒和流体示踪剂的扩散率

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The shear-induced particle self-diffusivity in a concentrated suspension (20%-50% solids volume fraction) of non-colloidal spheres (90 mu m average diameter) was measured using a new correlation technique. This method is based on the correlation between the positions of tracer particles in successive images and can be used to determine the self-diffusivity in non-colloidal suspensions for different time scales. These self-diffusivities were measured in the velocity gradient and vorticity directions in a narrow-gap Couette device for values of the strain gamma Delta t ranging from 0.05 to 0.5, where gamma is the applied shear rate and Delta t is the correlation time. In both directions, the diffusive displacements scaled linearly with gamma Delta t over the range given above and the corresponding diffusivities were found to be in good agreement with the experimental results of Leighton & Acrivos (1987a) and of Phan & Leighton (1993), even though these earlier studies were performed at much larger values of gamma Delta t. The self-diffusivity in the velocity gradient direction was found to be about 1.7 times larger than in the vorticity direction. The technique was also used to determine the shear-induced fluid tracer by measuring the mean square displacement of 31.5 mu m diameter tracer particles dispersed in concentrated suspensions (30%-50% solids volume fraction) of much larger spheres (325 mu m average diameter). These fluid diffusivities were found to be 0.7 times the corresponding particle diffusivities when both were scaled with gamma a(2) (2a = 325 mu m). [References: 13]
机译:使用一种新的相关技术测量了非胶体球(平均直径90微米)的浓缩悬浮液(固体体积分数为20%-50%)中的剪切诱导颗粒自扩散性。该方法基于连续图像中示踪剂颗粒位置之间的相关性,可用于确定不同时间范围内非胶体悬浮液的自扩散性。这些自扩散是在窄间隙Couette装置中沿速度梯度和涡度方向测量的,其应变γδt的值在0.05到0.5之间,其中γ是施加的剪切速率,而δt是相关时间。在两个方向上,扩散位移都在上述范围内与γδt成线性比例关系,并且相应的扩散率与Leighton&Acrivos(1987a)和Phan&Leighton(1993)的实验结果非常吻合。尽管这些早期研究是在更大的γδt值下进行的。发现在速度梯度方向上的自扩散是在涡度方向上的约1.7倍。通过测量分散在更大球体(平均直径325μm)的浓缩悬浮液(30%-50%固体体积分数)中的直径31.5μm示踪剂颗粒的均方位移,该技术还用于确定剪切诱导的流体示踪剂)。当两个流体的扩散系数均按伽马a(2)(2a = 325μm)缩放时,发现它们的流体扩散系数是相应粒子扩散系数的0.7倍。 [参考:13]

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