2004
DOI: 10.1103/physreve.69.015301
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Oscillatory axial banding of particles suspended in a rotating fluid

Abstract: A nonviscous fluid, completely filling a tube rotating about its horizontal axis, contains a suspension of macroscopic particles. The particles are observed to distribute themselves spontaneously in bands distributed periodically along the axis, with a band separation dependent only on the tube radius and length. In many cases, the bands oscillate periodically between two interleaving patterns. We explain this banding phenomenon as arising from the excitation of inertial standing waves in the rotating fluid.

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Cited by 16 publications
(25 citation statements)
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“…waves propagating in opposite directions [13]. In dilute rotating suspensions of granulates, hydrodynamic effects may produce traveling waves of regions of accumulated grains [29][30][31].…”
Section: Traveling Rolls and Stripesmentioning
confidence: 99%
“…waves propagating in opposite directions [13]. In dilute rotating suspensions of granulates, hydrodynamic effects may produce traveling waves of regions of accumulated grains [29][30][31].…”
Section: Traveling Rolls and Stripesmentioning
confidence: 99%
“…Theoretical arguments and calculations [12][13][14]17,18,22,23 have been made to explain the observed flow patterns, but they made different assumptions and predictions. A generally accepted theoretical framework for the rotating suspension is yet to be obtained.…”
Section: Introductionmentioning
confidence: 98%
“…This pattern formation has been analyzed both theoretically and experimentally by Seiden et al [9][10][11], who explained the phenomenon as arising from the excitation of inertial waves in the regularly rotating fluid by the disturbance by the particles. The particle bands form due to the tendency of particles sedimenting in Stokes flow to attract one another into groups, thus creating a sink that draws in additional particles and causes further clustering.…”
Section: Introductionmentioning
confidence: 99%
“…Observations show that within a short time the granular particles accumulate into periodically spaced bands along the tube, with a characteristic periodic length approximately twice the diameter D of the tube. The observations indicate that the ends of the tube are situated either at the center of a band or halfway between two bands; as the length of the tube L is changed, the period adjusts itself around the characteristic period so that the length is equal to an integral number of half periods [1][2][3][4][5][6][7][8][9][10][11]. Figure 1 shows snapshots of stationary patterns observed when the tube length, L, is twice the characteristic periodic length, .…”
Section: Introductionmentioning
confidence: 99%