Journal
JOURNAL OF FLUID MECHANICS
Volume 629, Issue -, Pages 387-423Publisher
CAMBRIDGE UNIV PRESS
DOI: 10.1017/S0022112009006466
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Funding
- School of Architecture, Civil and Environmental Engineering
- European Research Community on Flow, Turbulence and Combustion (ERCOFTAC).
- NERC [NER/A/S/2003/00439, NE/EO03206/1]
- EPSRC Advanced Research Fellowship [GR/S50052/01, GR/S50069/01]
- Swiss National Science Foundation [200021-105193]
- Centre in Mobile Information and Communication Systems [5005-67322]
- Centre in Environmental Sciences [TRAMN/1]
- NERC [NE/E003206/1] Funding Source: UKRI
- Engineering and Physical Sciences Research Council [GR/S50069/01, GR/S50052/01] Funding Source: researchfish
- Natural Environment Research Council [NER/A/S/2003/00439, NE/E003206/1] Funding Source: researchfish
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Stratification patterns are formed when a bidisperse mixture of large tough grains and smaller more mobile particles is poured between parallel plates to form a heap. At low flow rates discrete avalanches flow down the free surface and are brought to rest by the propagation of shock waves. Experiments performed in this paper show that the larger particles are segregated to the top of the avalanche, where the velocity is greatest, and are transported to the flow front. Here the particles are overrun but may rise to the free surface again by size segregation to create a recirculating coarse-grained front. Once the front is established composite images show that there is a steady regime in which any additional large grains that reach the front are deposited. This flow is therefore analogous to finger formation in geophysical mass flows, where the larger less mobile particles are shouldered aside to spontaneously form static lateral levees rather than being removed by basal deposition in two dimensions. At the heart of all these phenomena is a dynamic feedback between the bulk flow and the evolving particle-size distribution within the avalanche. A fully coupled theory for such segregation-mobility feedback effects is beyond the scope of this paper. However, it is shown how to derive a simplified uncoupled travelling-wave solution for the avalanche motion and reconstruct the bulk two-dimensional flow field using assumed velocity profiles through the avalanche depth. This allows a simple hyperbolic segregation theory to be used to construct exact solutions for the particle concentration and for the recirculation within the bulk flow. Depending on the material composition and the strength of the segregation and deposition, there are three types of solution. The coarse-particle front grows in length if more large particles arrive than can be deposited. If there are fewer large grains and if the segregation Is strong enough, a breaking size-segregation wave forms at a unique position behind the front. It consists of two expansion fans, two shocks and a central 'eye' of constant concentration that are arranged in a 'lens-like' structure. Coarse grains just behind the front are recirculated, while those reaching the head are overrun and deposited. Upstream of the wave, the size distribution resembles a small-particle 'sandwich' with a raft of rapidly flowing large particles on top and a coarse deposited layer at the bottom, consistent with the experimental observations made here. If the segregation is weak, the central eye degenerates, and all the large particles are deposited without recirculation.
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