1965
DOI: 10.1139/p65-122
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Particle Motions in Sheared Suspensions: Xvi. Orientations of Rods and Disks in Hyperbolic and Other Flows

Abstract: The angular velocity of a body of revolution suspended in a viscous fluid undergoing slow arbitrary shear Row is given. Integrated equations are derived for the orientation of its axis, directly in terms of the vorticity and dilatation components, for any flow in which the vorticity is parallel to a principal axis of dilatation; these are analogous to the equations for motion of a spheroid in Couette flow with an electric field parallel or perpendicular to the vorticity. The flows considered include examples o… Show more

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Cited by 26 publications
(1 citation statement)
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“…To describe the particle rotation, a spherical coordinate system with spherical angles 0 and 0 can conveniently be used as shown in Figure 2. If an ellipsoid of revolution with principal semi-axes b1 and b2 = b3 is taken, then the rate change of these spherical angles (ø and 0), which completely describes the three-dimensional particle rotation, can be expressed as [61] Integration of Equation (29) shows that the rotation is periodic, and the period of rotation can be easily seen as:…”
Section: Jeffery's Modelmentioning
confidence: 99%
“…To describe the particle rotation, a spherical coordinate system with spherical angles 0 and 0 can conveniently be used as shown in Figure 2. If an ellipsoid of revolution with principal semi-axes b1 and b2 = b3 is taken, then the rate change of these spherical angles (ø and 0), which completely describes the three-dimensional particle rotation, can be expressed as [61] Integration of Equation (29) shows that the rotation is periodic, and the period of rotation can be easily seen as:…”
Section: Jeffery's Modelmentioning
confidence: 99%