Rayleigh-Taylor instability in size-bidisperse isodense granular flow down an incline

Size-bidisperse granular material flowing down a rough incline, or chute, may develop a Rayleigh-Taylor instability even when the two particle species have the same density. Unlike fluid instability, which occurs under quiescent conditions, the granular material must be flowing for the instability to occur. Initially, size segregation results in a monodisperse layer of large particles above a monodisperse layer of small particles with an interfacial layer of mixed particles that has a higher volume fraction and, hence, is denser than the monodisperse layers above and below it. The interfacial layer destabilizes via a Rayleigh-Taylor instability and forms dense descending plumes of mixed particles and ascending plumes of less dense pure small particles. As a result of these plumes, the upper layer of large particles breaks and accumulates above the descending plumes; the small-particle plumes reach the free surface. The instability evolves into persistent longitudinal rolls corresponding to streamwise bands, or stripes, of small and large particles at the free surface. The appearance of the instability depends on the particle and mixture properties as well as the flow conditions. In all cases, the propensity for the appearance of the instability and subsequent band formation can be traced back to the total particle volume fraction, or packing density, in the mixed-particle layer, which depends on the particle size ratio, fraction of each particle species, and thickness of the flow.

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Publication Details

Journal
Physical review. E
Published
2025-12-23
DOI
https://doi.org/10.1103/xtjj-rlr4
Primary Topic
Granular flow and fluidized beds
Type
article
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article

Rayleigh-Taylor instability in size-bidisperse isodense granular flow down an incline

Umberto D’Ortona, Richard M. Lueptow, Nathalie Thomas
Physical review. E
Granular flow and fluidized beds
article

Rayleigh-Taylor instability in size-bidisperse isodense granular flow down an incline

Umberto D’Ortona, Richard M. Lueptow, Nathalie Thomas
article en

Abstract

Size-bidisperse granular material flowing down a rough incline, or chute, may develop a Rayleigh-Taylor instability even when the two particle species have the same density. Unlike fluid instability, which occurs under quiescent conditions, the granular material must be flowing for the instability to occur. Initially, size segregation results in a monodisperse layer of large particles above a monodisperse layer of small particles with an interfacial layer of mixed particles that has a higher volume fraction and, hence, is denser than the monodisperse layers above and below it. The interfacial layer destabilizes via a Rayleigh-Taylor instability and forms dense descending plumes of mixed particles and ascending plumes of less dense pure small particles. As a result of these plumes, the upper layer of large particles breaks and accumulates above the descending plumes; the small-particle plumes reach the free surface. The instability evolves into persistent longitudinal rolls corresponding to streamwise bands, or stripes, of small and large particles at the free surface. The appearance of the instability depends on the particle and mixture properties as well as the flow conditions. In all cases, the propensity for the appearance of the instability and subsequent band formation can be traced back to the total particle volume fraction, or packing density, in the mixed-particle layer, which depends on the particle size ratio, fraction of each particle species, and thickness of the flow.

Physical review. EVol. 113(2)
Northwestern University (US), Aix-Marseille Université (FR), Laboratoire de Mécanique, Modélisation & Procédés Propres (FR), Château Gombert (FR), Institut Universitaire des Systèmes Thermiques Industriels (FR)
Openalex Percentile: Top 70%
Granular flow and fluidized beds
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Rayleigh-Taylor instability in size-bidisperse isodense granular flow down an incline — Umberto D’Ortona, Richard M. Lueptow, et al. · Physical review. E (2025) | TGRS Research Map | TGRS