CFD and experimental studies of reactive pulsing flow in environmentally-based trickle-bed reactors
Introduction
Two-phase flow in TBRs has been intensively studied both in the realm of fluid dynamics and in the domain of chemical reaction engineering. The gas–liquid cocurrent flow in these packed-bed reactors found common applications in the petrochemical industry, where hydrotreating reactions of the various petroleum fractions play a major role (Al-Dahhan et al., 1997). More recently, the unprecedented number of publications devoted to biochemical processes as well as advanced oxidation processes have envisaged TBRs for the purification of wastewaters and gases polluted with toxic organic compounds, using a bed of immobilized bacteria or the chemical catalyst, respectively (Bhargava et al., 2006). As trickle-beds are governed by different hydrodynamic states, the literature has primarily reported on trickle and pulse flow regimes in view of the fact that these contacting patterns are conventionally encountered in commercial-scale trickle-beds. Our case-study follows up the long-standing interest on the environmental applications of trickle-beds in catalytic wet oxidation to realize theoretically and experimentally the advantages of the convective nature of liquid disturbances that grow into pulses in TBRs (Ayude et al., 2007, Guo and Al-Dahhan, 2005).
The comprehensive understanding on the nature and characteristics of the hydrodynamics in those flow regimes and the transition between them is ultimately recognized to push forward the oxidation conversions. In order to accomplish such a task, precise tools are required for the identification of the flow pattern and the reaction behavior. Important emphasis is being put nowadays on advanced Computational Fluid Dynamics codes to deal with an accurate prediction of the trickle-to-pulse flow transition, which is a key feature of major importance in the characterization of flow pattern apart from the quantification of phase holdups, two-phase frictional pressure drop, and mass fluxes. Here, we focus on the development of a phenomenological framework that enables to assess how catalytic wet oxidation can be promoted when the trickle flow state evolve to forced pulse flow regimes. The pulsing hydrodynamic regime is attained at severe flow conditions, where sharp, structured, and traveling disturbances of high liquid payloads substitute the low interaction regime achieved under trickling flow conditions. As long as pulsing flows affect the heat and mass transfer rates, and thus reaction rates, hence it is necessary to grasp how superior the detoxification of phenol-like pollutants can be advanced, and this may be cited as the motivation cause for the current work.
Section snippets
Previous work
On the flow regime transition from trickle to pulse, valuable attempts have been made to identify such dynamic multiphase flow events within the trickle-bed reactors. A microelectrode technique has been used by Latifi et al. (1992) to determine the flow regime transition in trickle-bed reactors, though a detailed information on frequency distribution in a pulse flow regime. Nonlinear time series analysis was also studied to characterize flow regime transitions in bubble columns and
Governing flow equations
Transport phenomena such as interfacial momentum transfer is integrated into Eulerian CFD model, resulting from the volume averaging of the continuity and momentum equations and solved for a three-dimensional representation of the bed at an unsteady state. In Euler–Euler mathematical approach, both continuous and dispersed phases are considered as interpenetrating continuous media (Lopes and Quinta-Ferreira, 2008). The CFD model equations were implemented in commercial software FLUENT and only
Optimization of mesh and time step
Under pulsing flow conditions, the process methodology encompassed by liquid flow modulation confers distinct hydrodynamic features with respect to the steady-state operation. Our periodic workflow experiments can be described as a mode of process, in which the system is forced to operate continuously in a transient mode. This experimental technique did not exhibit a seamless flow pattern, but rather consisted of scattered loads of liquid pockets that can a priori eliminate the in situ
Conclusions
A state-of-the-art CFD model was developed to simulate the periodic operation for the catalytic abatement of phenol-like pollutants in a trickle-bed reactor. Several numerical simulations were performed to evaluate on how the ON–OFF liquid flow modulations can improve the detoxification of liquid effluents by catalytic wet oxidation. The effect of oxidation temperature as well as the influence of gas and liquid flow rates has been investigated comparatively under different flow regimes.
Nomenclature
- C1ε, C2ε
k−ε model parameters: 1.44, 1.92
- C
specie concentration, ppm
- d
particle nominal diameter, m
- E1, E2
Ergun's constants
gravitational acceleration, 9.81 ms2
- G
gas mass flux, kg/m2 s
- GkL
generation rate of turbulent kinetic energy
- k
k−ε model kinetic energy
- Kqp
interphase momentum exchange coefficient
- L
liquid mass flux, kg/m2 s
- p
pressure, bar
interaction force between phases p and q
- s
complex frequency of wave equation
- Sq,i
source mass of specie i for phase q, ppm
- Sq,h
source term containing volumetric reaction
Acknowledgment
The authors gratefully acknowledge the financial support of Fundação para a Ciência e Tecnologia, Portugal.
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