剪切和电场中的粒子行为:IV.非旋转椭球悬浮液的粘度

C.E. Chaffey , S.G. Mason
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引用次数: 23

摘要

Jeffery关于非相互作用的椭球体在缓慢剪切流中的悬浮液中能量耗散的计算,推广到Couette流中的长形椭球体,当它们被外部扭矩阻止旋转时,椭球轴垂直于流体涡度。固有粘度系数(自由旋转球体为2.5)对于固定球体为4,对于平行于流体流线的长杆为2,对于垂直于流线的长杆则变得无限大。它总是超过自由旋转的最小值。这样的悬架提供了具有非对称应力张量的流体的可实现模型。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Particle behavior in shear and electric fields: IV. The viscosity of suspensions of nonrotating ellipsoids

Jeffery's calculation of the energy dissipation in a suspension of noninteracting spheroids undergoing slow shear flow is extended for prolate spheroids in Couette flow, when they are prevented from rotating by an external torque, the spheroid axes being perpendicular to the fluid vorticity. The intrinsic-viscosity coefficient (2.5 for freely rotating spheres) is 4 for fixed spheres and 2 for long rods parallel to the fluid streamlines, and becomes indefinitely large for long rods perpendicular to the streamlines. It always exceeds the minimum value for free rotation. A suspension such as this provides a realizable model of a fluid having an unsymmetric stress tensor.

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