Balancing size and density segregation in bidisperse dense granular flows

Several experimental studies have illustrated a balance between the segregation forces arising due to size- and density-differences. However, no detailed studies have been carried out to quantify this balance. In 2014, by utilising discrete particle simulations, we presented a simple relationship be...

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Main Authors: Tunuguntla Deepak R., Thornton Anthony R.
Format: Article
Language:English
Published: EDP Sciences 2017-01-01
Series:EPJ Web of Conferences
Online Access:https://doi.org/10.1051/epjconf/201714003079
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spelling doaj-a17c1e82cd0d46809cda74ce0d21b6ee2021-08-02T07:45:35ZengEDP SciencesEPJ Web of Conferences2100-014X2017-01-011400307910.1051/epjconf/201714003079epjconf162567Balancing size and density segregation in bidisperse dense granular flowsTunuguntla Deepak R.0Thornton Anthony R.1Multi-Scale Mechanics Group, Dept. of Thermal and Fluid Engineering, University of TwenteMulti-Scale Mechanics Group, Dept. of Thermal and Fluid Engineering, University of TwenteSeveral experimental studies have illustrated a balance between the segregation forces arising due to size- and density-differences. However, no detailed studies have been carried out to quantify this balance. In 2014, by utilising discrete particle simulations, we presented a simple relationship between the particle size-and density-ratio, s^a=ρ^$s^a = \hat \rho$, where ‘a’ determines whether the partial pressure scales with the diameter, surface area or volume of the particle. For a 50:50 mix (in volume) of bidisperse granular mixtures, we found the partial pressure to scale with the volume of the particle, i.e. a = 3. Moreover, there also exists a range of size- and density-ratios that satisfy the relation s^3=ρ^$s^3 = \hat \rho$, where the bidisperse mixture remains homogeneously mixed. However, in this proceeding, we deviate from the conventional 50:50 mixes and consider a slightly extreme case of mixes, such as the 10:90 (in volume) mixes, which are often found in nature and industries. By doing so we observe that the partial pressure does not scale with the particle volume and, more importantly, the zero-segregation relation is not as simple as s^a=ρ^$s^a = \hat \rho$. However, there does exist a range of size- and density-ratios for which the mixture weakly segregates.https://doi.org/10.1051/epjconf/201714003079
collection DOAJ
language English
format Article
sources DOAJ
author Tunuguntla Deepak R.
Thornton Anthony R.
spellingShingle Tunuguntla Deepak R.
Thornton Anthony R.
Balancing size and density segregation in bidisperse dense granular flows
EPJ Web of Conferences
author_facet Tunuguntla Deepak R.
Thornton Anthony R.
author_sort Tunuguntla Deepak R.
title Balancing size and density segregation in bidisperse dense granular flows
title_short Balancing size and density segregation in bidisperse dense granular flows
title_full Balancing size and density segregation in bidisperse dense granular flows
title_fullStr Balancing size and density segregation in bidisperse dense granular flows
title_full_unstemmed Balancing size and density segregation in bidisperse dense granular flows
title_sort balancing size and density segregation in bidisperse dense granular flows
publisher EDP Sciences
series EPJ Web of Conferences
issn 2100-014X
publishDate 2017-01-01
description Several experimental studies have illustrated a balance between the segregation forces arising due to size- and density-differences. However, no detailed studies have been carried out to quantify this balance. In 2014, by utilising discrete particle simulations, we presented a simple relationship between the particle size-and density-ratio, s^a=ρ^$s^a = \hat \rho$, where ‘a’ determines whether the partial pressure scales with the diameter, surface area or volume of the particle. For a 50:50 mix (in volume) of bidisperse granular mixtures, we found the partial pressure to scale with the volume of the particle, i.e. a = 3. Moreover, there also exists a range of size- and density-ratios that satisfy the relation s^3=ρ^$s^3 = \hat \rho$, where the bidisperse mixture remains homogeneously mixed. However, in this proceeding, we deviate from the conventional 50:50 mixes and consider a slightly extreme case of mixes, such as the 10:90 (in volume) mixes, which are often found in nature and industries. By doing so we observe that the partial pressure does not scale with the particle volume and, more importantly, the zero-segregation relation is not as simple as s^a=ρ^$s^a = \hat \rho$. However, there does exist a range of size- and density-ratios for which the mixture weakly segregates.
url https://doi.org/10.1051/epjconf/201714003079
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