(223e) Evaluation of Spouted Bed Flow Instabilities Via High Speed Video and Pressure Fluctuations | AIChE

(223e) Evaluation of Spouted Bed Flow Instabilities Via High Speed Video and Pressure Fluctuations

Authors 

Breault, R. W., National Energy Technology Laboratory
Weber, J., National Energy Technology Laboratory
Yang, J., ORISE/ORAU

2017 AIChE Annual Meeting

Topic/Group: Fluidization and Fluid-Particle Systems

Tentative Session: Fundamentals of Fluidization I

Title: Evaluation of Spouted Bed Flow Instabilities
via High Speed Video and Pressure Fluctuations.

Authors:

Steven L. Rowan:       Steven.Rowan@netl.doe.gov

Jingsi J. Yang:            Jingsi.Yang@netl.doe.gov

Ronald W. Breault:     Ronald.Breault@netl.doe.gov

Justin M. Weber:         Justin.Weber@netl.doe.gov

Key Words: Fluidization, Spouted bed, Instability,
Cold Flow, Energy

Abstract:

 Spouted beds are a type of
gas-solid contacting process first introduced by Mathur and Gishler [1] in
1955.  The process, which is similar to fluidization, involves introducing gas
into the bottom of a dense packed bed of solid materials through a small
orifice.  The gas jet pushes up through the densely-packed particles, forming
an upwards moving core of entrained particles.  These entrained particles are
eventually ejected out of the top of the dense bed and fall into an annular
region outside of the central core area, forming a fountain-like structure
above the bed.  The particles located within the annular region recirculate
downwards towards the bottom of the bed, where they are eventually re-entrained
into the upwards moving gas core. This process is particularly well-suited to
processing of larger Geldart D particles that do not fluidize well using
traditional fluidized bed systems [2]. 

Under stable operating
conditions, the gas jet that forms the core of a spouted bed system will rise
vertically through the densely-packed bed of solids, however, under certain
flow conditions, the core will become unstable and take on more of a wavy, serpentine
path through the bed of solids.  Under even more extreme conditions, the gas
core can be seen to migrate from the center of the bed towards the outer wall,
bypassing the solids altogether.  Examples of these can be seen in Figure 1.

Figure 1:
Examples of gas behavior in a spouted bed (a) stable, (b) snake-like
instability, (c) gas bypassing.

            A
study has been conducted at the National Energy Technology Laboratory (NETL) to
explore the hydrodynamics of spouted bed systems, including the effects of
particle properties (size and density), bed geometry (nozzle size, cone angle),
spouting gas velocity, and static bed height on the dynamic stability of the
gas core.  By combining processing of high speed video with statistical and
deterministic chaos analysis of pressure fluctuations within the bed, it is
possible to identify the unstable operating regimes and develop an operational
envelop within which the hydrodynamics of the spouted bed are stable.  From
this, empirical expressions can be obtained for the minimum and maximum stable
spouting velocities as a function of the parameters listed above.

References

[1]        Mathur,
K. B., Gishler, P. E. 1955. A Technique for Contacting Gases With Coarse Solid
Particles, A.I.C.H.E. Journal, Vol.1, No. 2: 157-163.

[2]        Geldart,
d., Harnby, N., Wong, A.C. 1984. Fluidization of Cohesive Particles, Powder Technology
37, 25-37.

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