Abstract
This paper deals with the stability of suspensions modelled as dusty gases for non-uniform
profiles of mass fraction of particles. It is known that a stationary uniform
fluidized bed may be unstable to small disturbances which grow until a secondary
instability develops forming bubbles that rise through the bed. Interactions between
particles are difficult to model and this makes it necessary to close the model with
some assumptions. However, in dilute fluidized beds which are characterized by a
low volume fraction of particles, interactions between particles are negligible and
this motivates the study of instabilities of suspensions by means of the dusty gas
equations, avoiding the problem of particular closures.We show in this work that suspensions blown to regions of higher concentration are
unstable to two-dimensional disturbances. An equation which governs this instability
is obtained. A physical mechanism is proposed to explain this instability and it is
related to the Rayleigh–Taylor one in the limit of long characteristic lengthscales
associated with the concentration profile. Finally, the evolution of this instability is
followed using a fully nonlinear numerical code showing the formation of streamers
and clusters of particles.
Publisher
Cambridge University Press (CUP)
Subject
Mechanical Engineering,Mechanics of Materials,Condensed Matter Physics
Cited by
10 articles.
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