Effective drag coefficient correlation for coarse coal particle fluidization in transitional flow regime
Graphical abstract
Introduction
Liquid–solid fluidized beds have extensive applications in industrial production, such as polymerization, food processing, metallurgical processing, and wastewater treatment (Galvin et al., 2018; Jameson et al., 2020; Lu et al., 2016; Sowmeyan and Swaminathan, 2008; Trivedi et al., 2006; Zhu et al., 2000). Among these processes, high solid particle mixing rates, which are mainly controlled by the quality of particle fluidization, are inherently required to improve the interphase heat and mass transfer rate (Fosu et al., 2015; Zhu et al., 2000). Accordingly, to improve the performance of liquid–solid fluidized beds, an insight into the hydrodynamic characteristics of these systems is critical.
Over the last few decades, despite their wide application, liquid–solid systems have received limited attention compared with gas–solid systems, which usually have many heterogeneous flow structures (Xie et al., 2021; Zhu et al., 2016). In liquid–solid fluidized beds, however, a low solid–fluid density ratio can easily lead to particle entrainment, especially small and light particles; thus, severe heterogeneous fluidization seems improbable under normal operating conditions. In contrast, the homogeneous fluidization of liquid–solid fluidized beds has been frequently observed (Wang et al., 2010). Nevertheless, it should be noted that heterogeneous liquid–solid flow behaviors, such as particle clustering, bubbling, and velocity fluctuations, do occur (Chen and Zhu, 2008; Esteghamatian et al., 2017, 2018; Kasat et al., 2008; Kramer et al., 2020; Sardeshpande et al., 2009, 2010; Song et al., 2019a, 2019b). As early as 1995, heterogeneous fluidization in liquid–solid fluidization systems had been reported by Di Felice (1995). In these systems, the degree of heterogeneity has been attributed to the particle morphology, particle size distribution, and fluid–solid density ratio.
Generally, experimental and numerical simulation approaches have been used in previous studies to investigate the liquid–solid flow characteristics. Based on advanced experimental measurement techniques, such as particle image velocimetry (Reddy et al., 2013; Peng et al., 2014), electrical resistance tomography (Razzak et al., 2007, 2009, Razzak et al., 2010; Zbib et al., 2018a, 2018b), and laser Doppler anemometry (Mathiesen et al., 2000), the particle phase distributions can be visualized. The characterized particle concentration, particle velocity, and particle clusters can aid in clarifying the fluidization mechanism and provide guidance for optimizing fluidized beds. However, the experimental data may be extremely dependent on the specific experimental method. As a result, the experimentation cost usually hinders obtaining a variety of experimental data.
Recently, the modeling and simulation of liquid–solid fluidized beds have been performed through computational fluid dynamics (CFD) to investigate the hydrodynamic characteristics, particularly for the purpose of scaling up. Although experiments are still required to validate the CFD model, numerical simulations allow particle scale characterization. For liquid–solid fluidized beds, the typically reported numerical techniques can be classified into Eulerian and Lagrangian approaches according to the treatment of the solid phase. In particular, the computational fluid dynamics–discrete element method (CFD–DEM) can provide a detailed description of the particle scale information based on the analysis of forces acting on individual particles (Liu et al., 2017; Zhu et al., 2007). In the past few decades, various numerical simulations have been performed to investigate the hydrodynamic behaviors of liquid–solid fluidized beds under different flow regimes (Lettieri et al., 2006), to explore flow stability (Ghatage et al., 2014; Ramesh et al., 2018; Zbib et al., 2018a, 2018b), and to study the homogeneous and heterogeneous fluidization phenomena (Fan et al., 2010; Mazzei and Lettieri, 2008). Such qualitative and quantitative studies have also afforded considerable amounts of important basic data derived by investigating the effects of liquid superficial velocity, physical properties of solid particles and liquids, and the structure of fluidized beds (Cornelissen et al., 2007; Dadashi et al., 2014; Hua et al., 2020; Wang et al., 2012; Ye et al., 2017). Additionally, the importance of liquid–particle and particle–particle interactions has been confirmed by many researchers (Luo et al., 2019; Koerich et al.,2018; Wu and Yang, 2019; Xie and Luo, 2018; Yu et al., 2016). In terms of numerical simulation, it is necessary to choose the interphase force model carefully because it can considerably influence the two-phase flow behavior (Visuri et al., 2012). In transitional flow regimes, many interphase drag models are available; however, each has its own character and application scope.
This study aims to investigate the hydrodynamic behavior of a liquid–solid fluidized bed applied to coarse coal separation. The three-dimensional (3D) fluidized bed was operated in the intermediate flow regime, and the expansion experiments and CFD simulations were implemented considering different particle densities, particle sizes, and liquid velocities. Based on the measured experimental data, a drag relationship was developed; thereafter, the drag coefficient correlation was incorporated into liquid–solid two-phase flow model to predict the bed expansion height. To the best knowledge of the authors, the obtained experimental data and simulation results can improve the understanding of liquid–solid fluidized beds with coarse particles.
Section snippets
Theory and modeling
In fixed and fluidized beds, the fluid passes through a dense porous medium, generally accompanied by a pressure drop, which may arise from two main factors: frictional loss and inertia. Fluid flow regimes usually have profound effects on pressure drop characteristics. For example, the pressure drop fluctuation is caused by local changes in the porosity of the fluidized bed. According to the well-known Ergun equation (Ergun, 1952), the pressure drop calculation formula has the following form:
Experimental setup and materials
The laboratory-scale fluidized bed apparatus was made of transparent plexiglass with a length, width, and height of 100, 20, and 1000 mm, respectively. Raw coal from the Tunlan coal preparation plant in Shanxi Province was crushed by a laboratory jaw crusher and then sieved to produce five large size fractions (0.375 ± 0.125, 0.60 ± 0.10, 0.85 ± 0.15, 1.25 ± 0.25, and 1.75 ± 0.25 mm). These were further subdivided according to different densities using the ZnCl2 heavy liquid method. As a
Bed expansion height and porosity
As mentioned above, the particle fluidization experiments were performed by varying the coal particle sizes, coal particle densities, and water superficial rates. In total, 183 fluidization experimental datasets were derived in this study. Fig. 1, Fig. 2, Fig. 3 show the bed expansion ratio at different water superficial velocities and particle densities in each size fraction. The bed expansion ratio exhibits different trends with the increase in water superficial velocity. As an example, in
Conclusions
In this study, the fluidization of coarse coal particles in a liquid–solid fluidized bed was studied through experiments and CFD simulations. Numerous expansion experiments were performed at varying particle densities, particle sizes, and fluid superficial velocities. It is found that the bed expansion ratio practically has a distinct linearly increasing tendency under low water superficial velocity conditions. When the flow velocity exceeds the critical value, however, the bed expansion height
CRediT authorship contribution statement
Le Xie: Conceptualization, Experiment, Methodology, Software, Writing - original draft. Dongdong Wang: Experiment, Writing - review & editing. Huaifa Wang: Supervision, Project administration, Writing - review & editing, Funding acquisition.
Declaration of competing interest
The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.
Acknowledgement
The authors are grateful for the financial support from the Natural Science Foundation of Hunan Province (No. 2018JJ2482).
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