Validation of Dimensionless Parameters for Distinguishing between Homogeneous and Bubbling Fluidizations ()

Kenya Kuwagi^{1}, Atsuto Kogane^{1}, Yui Sasaki^{1}, Hiroyuki Hirano^{2}

^{1}Department of Mechanical Systems Engineering, Okayama University of Science, Okayama, Japan.

^{2}Department of Applied Chemistry and Biotechnology, Okayama University of Science, Okayama, Japan.

**DOI: **10.4236/ojfd.2021.112006
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The difference between homogeneous and bubbling fluidization behaviors has been studied for the past 70 years, where several researchers have reported on the influence of interparticle forces in fluidization. Although interparticle forces such as van der Waals forces are evident in a real system, these forces are not the determinant in homogeneous fluidization, which can be simulated without any interparticle forces. In our previous study, the difference in fundamental mechanisms of the two fluidization states was analytically determined with a dimensionless gravity term, comprising the Reynolds number, Archimedes number, and density ratio. Nevertheless, some researchers insist that interparticle forces are dominant and a hydrodynamic force is not dominant. In this study, a dimensional analysis was applied to obtain a dominant parameter for distinguishing two fluidizations. Furthermore, some parameters were examined by comparing the experimental data in previous studies. The results indicated that hydrodynamic force is the dominant factor and the dimensionless gravity term is the dominant parameter in differentiating the two fluidized states.

Keywords

Bubbling Fluidization, Homogeneous Fluidization, Aggregative, Particulate, Dimensional Analysis

Share and Cite:

Kuwagi, K. , Kogane, A. , Sasaki, Y. and Hirano, H. (2021) Validation of Dimensionless Parameters for Distinguishing between Homogeneous and Bubbling Fluidizations. *Open Journal of Fluid Dynamics*, **11**, 81-97. doi: 10.4236/ojfd.2021.112006.

1. Introduction

1.1. Research Background

Fluidization can be observed in several natural phenomena such as avalanches, sandstorms, pyroclastic flows, and ground liquefaction. This characteristic is utilized in industrial processes as fluidized beds, where a balance between the drag and gravitational forces acting on the particle bed fluidizes the particles when the fluid velocity from the bottom wall exceeds a certain limit. The velocity at this instant is termed the minimum fluidization velocity, *u*_{mf}.

There are two kinds of fluidization: homogenous or particulate fluidization, where the particle bed expands homogeneously and bubbling or aggregative fluidization, where voids (bubbles) occur in the particle bed as the injected fluid velocity increases. Geldart [1] classified particles into Groups C, A, B, and D, in ascending order of particle size based on fluidization behavior. The powder bed of Group A homogeneously fluidized above the *u _{mf}*, and bubbles were observed at a certain fluid velocity, which is called the minimum bubbling fluidization velocity,

1.2. Literature Review

As summarized in Table 1, two approaches have been widely used to address the abovementioned issue. The first approach derives a discriminant equation to determine the criteria for the transition between homogeneous and bubbling fluidizations. The first discriminant equation was derived by Wilhelm and Kwauk [2], and numerous criteria have been proposed in the last 60 years [3] [4] [5] [6] [7]. Notably, most of these studies used Froude or Reynolds numbers based on the minimum fluidization velocity to estimate the fluidization state. Although the state of homogeneous or bubbling fluidization can be estimated under each condition, the estimation of the minimum bubbling fluidization velocity with these methods is difficult.

The second approach derives an equation to estimate the minimum bubbling fluidization velocity *u _{mb}*. Primarily, Geldart [1] derived the following simple equation:

${u}_{mb}=100{d}_{p}$. (1)

Subsequently, Abrahamsen and Geldart [8] obtained the following equation based on an extensive dataset:

${u}_{mb}=\frac{2.07{d}_{p}{\rho}_{f}^{0.06}}{{\mu}_{f}^{0.347}}\mathrm{exp}\left(0.716{F}_{45}\right)$, (2)

where *F*_{45} is the mass fraction of particles with diameters less than 45 μm. The equation derived by Abrahamsen and Geldart [8] is frequently used to study gas-fluidized beds. Although they used dimensional analysis, the derived equation was not expressed using dimensionless parameters. Kuwagi *et al.* [9] conducted a dimensional analysis using the governing equations of discrete element method (DEM) and computational fluid dynamics (CFD) coupling model [10] to describe the phenomenon of fluidization. They plotted the fluidization state

Table 1. Research on the difference between homogeneous and bubbling fluidization.

on a three-dimensional (3-D) graph consisting of three dimensionless numbers—*Re*, *Ar*, and *ρ**. Thus, the following equation was derived from the boundary plane between homogeneous and bubbling fluidization states:

$R{e}_{mb}=0.263{\rho}^{\ast -0.553}A{r}^{0.612}.$ (3)

The derivation method is similar to that of Abrahamsen and Geldart [8] because the fitting equation was obtained from an extensive simulation and experimental data. In contrast, Kogane *et al.* [11] revealed that the dimensionless gravity term,
${F}_{G}^{*}=Ar/\left(R{e}^{2}{\rho}^{*}\right)$, distinguishing the two states of fluidization can be rewritten as

$R{e}_{mb}=0.297{\rho}^{\ast -1/2}A{r}^{1/2}$. (4)

1.3. Problems

Certain explanations have been proposed to adequately clarify the basic mechanisms that differentiate homogeneous and bubbling fluidization. Researchers [12] [13] have argued on the influence of interparticle forces and the insignificant effect of hydrodynamics. Although we can agree with this opinion when treating cohesive powders, Di Renzo and Di Maio [14] and Thornton *et al.* [15] have successfully simulated homogeneous fluidization without any cohesive forces. Thus, interparticle forces do not seem to be a determining parameter for fluidization. Nevertheless, we again emphasize on considering interparticle forces, such as van der Waals forces, during simulation of cohesive powder, *i.e.*, Group C of Geldart’s classification. In other words, interparticle forces are an additional distinguishing factor between the two fluidization states. In addition, homogeneous fluidization can occur in a liquid system with large particles, which is difficult to explain from the standpoint of cohesive forces.

In this study, we used larger particles, *i.e.*, Groups A, B, and D to determine the differences between the two fluidization states. The interparticle force includes a repulsion force resulting from the collision of particles, and the repulsion force can be calculated in a numerical simulation using softer springs to reduce computational time [10]. Nonetheless, the simulated results accurately described the real phenomenon for noncohesive fluidized particles [10]. Ye *et al.* [13] used a Hookean spring model with *k _{n}* = 7 or 3.5 N/m for calculating the repulsion force, whereas

Furthermore, as mentioned before, dimensional analysis has not been effectively utilized in previous studies for derivation of the discriminant equation to determine the criterion for transition between homogeneous and bubbling fluidizations. When the Froude number or Reynolds number is defined using the minimum fluidization velocity as a reference velocity, the dimensionless number is treated as a physical property, such as the Prandtl number. On the other hand, the velocity of the injected fluid, *i.e.*, the fluidizing velocity, can be used as a reference velocity for the dimensionless numbers. Valverde *et al.* [12] and Ye *et al.* [13] concluded that the criterion with the Froude number [2] fails to distinguish between the two fluidized states. In this study, we attempt to alter this perspective by defining the Froude number with the fluidizing velocity instead of the minimum fluidization velocity.

1.4. Purpose

The analogy between the dimensional and dimensionless simulations has already been presented [9]. In the study, a 3-D graph incorporating three dimensionless numbers—*Re*, *Ar*, and *ρ**—showed a clear boundary between the two states of fluidization. The dimensionless gravity term included these dimensionless numbers and clearly distinguished the two fluidization states in our previous study [11]. Furthermore, the results were in good agreement with prior experimental data. The definition of the dimensionless gravity term was examined in this study to form a basis of understanding and confirm the applicability of dimensional analysis on fluidization.

2. Analyses

2.1. Dimensional Analysis

The governing equations for the DEM-CFD coupling model [10] were assigned to equations describing the fluidization phenomenon.

Fluid phase:

$\frac{\partial \epsilon}{\partial t}+\frac{\partial}{\partial {x}_{i}}\left(\epsilon {u}_{i}\right)=0$, (5)

${\rho}_{f}\frac{\partial}{\partial t}\left(\epsilon {u}_{i}\right)+{\rho}_{f}\frac{\partial}{\partial {x}_{i}}\left(\epsilon {u}_{i}{u}_{j}\right)=-\epsilon \frac{\partial p}{\partial {x}_{i}}-\epsilon {f}_{pf}-{\rho}_{f}\epsilon g$. (6)

Particle phase:

${m}_{p}\frac{\text{d}v}{\text{d}t}=-{V}_{p}\nabla p+\left({F}_{pp}+{F}_{pf}\right)-{m}_{p}g$, (7)

$I\frac{\text{d}\omega}{\text{d}t}=\left|{F}_{t}\right|{r}_{p}$. (8)

There are two definitions of pressure: pressure perturbation, *p'*, and the summation of the pressure in the hydrostatic equilibrium and the pressure perturbation, *p*. Equations (6) and (7) are expressed with terms in relation to *p*.

However, Equations (6) and (7) can be expressed with terms in relation to *p'* as

${\rho}_{f}\frac{\partial}{\partial t}\left(\epsilon {u}_{i}\right)+{\rho}_{f}\frac{\partial}{\partial {x}_{i}}\left(\epsilon {u}_{i}{u}_{j}\right)=-\epsilon \frac{\partial {p}^{\prime}}{\partial {x}_{i}}-\epsilon {f}_{pf}$, (9)

${m}_{p}\frac{\text{d}v}{\text{d}t}=-{V}_{p}\nabla {p}^{\prime}+\left({F}_{pp}+{F}_{pf}\right)-\left({m}_{p}-{m}_{f}\right)g$. (10)

Thereafter, the following equations were derived by nondimensionalizing Equations (5)-(8).

Fluid phase:

$\frac{\partial \epsilon}{\partial T}+\frac{\partial}{\partial {X}_{i}}\left(\epsilon {U}_{i}\right)=0$, (11)

$\frac{\partial}{\partial T}\left(\epsilon {U}_{i}\right)+\frac{\partial}{\partial {X}_{i}}\left(\epsilon {U}_{i}{U}_{j}\right)=-\epsilon \frac{\partial P}{\partial {X}_{i}}-\epsilon {f}_{pf}^{*}-\frac{\epsilon}{F{r}^{2}}$. (12)

Particle phase:

$\frac{\text{D}V}{\text{d}T}=-\frac{1}{{\rho}^{*}}\nabla P+\left({F}_{pp}^{*}+{F}_{pf}^{*}\right)-\frac{Ga}{R{e}^{2}}\cdot \frac{g}{\left|g\right|}$, (13)

$\frac{\text{d}{\omega}^{*}}{\text{d}T}=\left|{F}_{t}^{*}\right|R$ (14)

Furthermore, Equations (9) and (10) can be rewritten as

$\frac{\partial}{\partial T}\left(\epsilon {U}_{i}\right)+\frac{\partial}{\partial {X}_{i}}\left(\epsilon {U}_{i}{U}_{j}\right)=-\epsilon \frac{\partial {P}^{\prime}}{\partial {X}_{i}}-\epsilon {f}_{pf}^{*}$, (15)

$\frac{\text{D}V}{\text{d}T}=-\frac{1}{{\rho}^{*}}\nabla {P}^{\prime}+\left({F}_{pp}^{*}+{F}_{pf}^{*}\right)-\frac{1}{{\rho}^{*}}\cdot \frac{Ar}{R{e}^{2}}\cdot \frac{g}{\left|g\right|}$. (16)

In addition, the following reference qualities were used in the nondimensionalization process:

$\begin{array}{l}{x}_{0}={d}_{p},\text{\hspace{0.17em}}\text{\hspace{0.17em}}{v}_{0}={u}_{0},\text{\hspace{0.17em}}\text{\hspace{0.17em}}{p}_{0}={\rho}_{f}{u}_{0}^{2},\text{\hspace{0.17em}}\text{\hspace{0.17em}}{t}_{0}=\frac{{d}_{p}}{{u}_{0}},\\ {f}_{0}=\frac{{\rho}_{f}{u}_{0}^{2}}{{d}_{p}},\text{\hspace{0.17em}}\text{\hspace{0.17em}}{F}_{0}=\frac{\pi}{6}{\rho}_{p}{d}_{p}^{2}{u}_{0}^{2},\text{\hspace{0.17em}}\text{\hspace{0.17em}}{\omega}_{0}=\frac{10{u}_{0}}{{d}_{p}}\end{array}$ (17)

Further details on the related nondimensionalization procedure can be found in our previous study [9]. The Archimedes number can be confused with the Galilei number [16]. However, the distinction between the two dimensionless numbers can be easily understood from the nondimensionalization procedure. The Archimedes number signifies the buoyancy force in the gravity term of the particle motion equation, whereas the Galilei number considers only the gravity force in the gravity term and the buoyancy as a static force, thus reflecting the total pressure in the expression.

2.2. Numerical Simulation

The fluidization behavior of homogeneous or bubbling fluidization was determined under each condition by performing a DEM-CFD simulation [11], as it was difficult to conduct numerous experiments under various conditions. The simulations were conducted with an in-house code. The accuracy of the simulation code used in this study has been validated in our previous study [9] [11]. The ratio of bed (container) size to particle size was chosen to be constant. The analysis domain is 200*d _{p}* in width, 700

2.3. Analysis Conditions

The simulation conditions are listed in Table 2 and Table 3.

3. Results and Discussion

3.1. Comparison of Estimation Equations

Equations (3) and (4) were compared with Equations (1) and (2) to be rewritten with dimensional numbers (physical properties) as follows:

Table 2. Properties of particles.

Table 3. Properties of fluids.

${u}_{mb}=\frac{1.06{d}_{p}^{0.836}{\rho}_{f}^{0.165}}{{\mu}_{f}^{0.224}}\times \frac{{\left({\rho}_{p}-{\rho}_{f}\right)}^{0.612}}{{\rho}_{p}^{0.553}}$ (18)

${u}_{mb}=0.930{d}_{p}^{0.5}{\left(1-\frac{{\rho}_{f}}{{\rho}_{p}}\right)}^{0.5}$. (19)

The indices of *d _{p}*,

3.2. Comparisons of Criteria

Certain equations from Table 1 were compared using our simulated data. The distribution of the Froude number *Fr _{mf}* based on

Figure 1. Relationship between Froude numbers based on *u _{mf}* [2] and fluidization behaviors.

Table 4. Comparison of property indices in*u _{mb}* equations.

*Fr _{mf}* < 0.1. The experimental data obtained from the literature [16] [17] [18] [19] are indicated with vacant symbols in Figure 1. The boundary between the two fluidization states ranged from 10

The values of *U _{e}* −

Furthermore, Figure 3 shows the discrimination number *D _{n}* proposed by Liu

Figure 2. Relationship between the criterion of Foscolo and Gibilaro [6] and fluidization behaviors.

Figure 3. Relationship between discrimination number [7] and fluidization behaviors.

The values of the dimensionless gravity term
${F}_{G}^{*}$ proposed by the present authors [11] are illustrated in Figure 4. Both *Fr _{mf}* and

In this study, we considered a Froude number based on *u*_{0} instead of *u*_{mf} [2], and the results are plotted in Figure 5. In contrast to the results shown in Figure 1,

Figure 4. Relationship between dimensionless gravity term [11] and fluidization behaviors.

Figure 5. Relationship between Froude numbers based on fluidizing velocity, *u*_{0}, and fluidization behaviors.

the homogeneous and bubbling fluidizations were well separated by a boundary value of 0.1. Moreover, this result is similar to that presented in Figure 4. Furthermore, the relationship between *Fr* and
${F}_{G}^{*}$ can be expressed using the dimensionless numbers as

$Fr=\frac{R{e}^{2}}{Ga}$ (20)

${F}_{G}^{*}=\frac{Ar}{R{e}^{2}{\rho}^{*}}$. (21)

These equations correspond to the expressions of gravity in Equations (13) and (16). Therefore, both *Fr* and
${F}_{G}^{*}$ were derived from the dimensionless governing equations discussed earlier, and the distinction is highlighted from the treatment of pressure, *i.e.*, *p* or *p*', as shown in Equations (7) and (10). Notably, *Fr* comprises two dimensionless numbers, whereas
${F}_{G}^{*}$ comprises three dimensionless numbers. The dimensional analysis requires three dimensionless parameters [9], and
${F}_{G}^{*}$ satisfies this condition but *Fr* does not. Nevertheless, *Fr* can distinguish the two fluidization states, as shown in Figure 5, and the reason has to be clarified with further studies.

3.3. Accuracy of Estimation Equation

The estimation equation for *u _{mb}* was quantitatively verified by comparing the experimental values with that referred from the literature [16] [17] [18] [19]. The values calculated using Equations (2), (3), and (4) are presented in Figure 6, Figure 8 and Figure 9, respectively. In addition, the values calculated using the equation of Foscolo and Gibilaro [6] are presented in Figure 7. In each figure, the ordinate indicates the calculated value, whereas the abscissa indicates the experimental value.

Figure 6. Comparison of *u _{mb}* values predicted by equation of Abrahamsen and Geldart [8] (Equation (2)) with experimental data.

Figure 7. Comparison of *u _{mb}* values predicted by equation of Foscolo and Gibilaro [6] with experimental data.

As shown in Figure 6, the values calculated using Equation (2) were in poor agreement with the experimental values for the liquid system (blue circles) because Abrahamsen and Geldart [8] obtained their equation based on data of fluidizing fine powder under gas flow. As shown in Figure 7, the equation of Foscolo and Gibilaro [6] provided a better correlation in the case of the liquid system, but the overall variance was large. Moreover, a considerable agreement can be observed in Figure 8 because Equation (3) was obtained from an extensive dataset comprising 3-D flow regime map [9], including that of a liquid system. Figure 9 displays another disagreement for the liquid system owing to its larger particle diameters and higher fluidizing velocities, *i.e.*, high Reynolds numbers. As the dimensionless gravity term in our study was derived by assuming Stokes flow, we used the modified dimensionless gravity term [11]. However, the dimensionless gravity term should be used to determine the fundamental mechanisms differentiating between homogeneous and bubbling fluidizations. Regardless, the disagreement is unimportant in terms of analyzing the fundamental mechanisms of the two fluidization behaviors.

The deviation from the experimental data is summarized in Table 5. Although Equation (3) can be applied to a wide range of conditions including liquid systems, its application in fine powders without modification is difficult. In Figure 9, the deviation between the predicted and experimental values broadened as *u _{mb}* increased; a large

Figure 8. Comparison of *u _{mb}* values predicted by equation of Kuwagi

Table 5. Deviation from experimental data.

Figure 9. Comparison of *u _{mb}* values predicted by equation of Kogane

4. Conclusions

In this study, the distinct fundamental mechanisms of the homogeneous and bubbling fluidization behaviors were determined using a dimensionless gravity term that was derived to distinguish the two fluidization states as per our previous report [11]. The dimensionless gravity term was validated with results of prior research.

The estimation equations for dimensional analysis were derived from a 3-D flow regime map and the dimensionless gravity term was compared with the criteria reported in previous studies. A comparative analysis on the indices of physical properties confirmed that our derived equations were almost equivalent to the equations established in prior research. Thus, the dimensionless gravity term is signified as a dominant parameter for distinguishing between homogeneous and bubbling fluidization. In addition, the dimensionless gravity term was expressed in the dimensionless governing equations. In comparison to interparticle forces, the results of the current research indicated that hydrodynamic force is the most important and dominant factor in differentiating the two fluidized states. However, interparticle forces, such as cohesive and repulsion forces and the effect of particle inertia can be considered as additional factors to demonstrate more accurate simulations. Notably, the distinction between the two fluidization states can be simulated and observed without considering these additional factors as well.

Furthermore, the estimation equations were compared with existing discriminant equations. The minimum bubbling fluidization velocities estimated in the current study were consistent with the experimental data, and the estimation equations accurately distinguished the two fluidization behaviors.

Nomenclature

*Ar* Archimedes number, –

*d _{p}* diameter of particle, m

*f _{pf}* particle-fluid interaction force per unit volume, N/m

${f}_{pf}^{*}$ dimensionless particle-fluid interaction force, –

*F _{pp}* particle-particle interaction force, N

${F}_{pp}^{*}$ dimensionless particle-particle interaction force, –

*F _{pf}* particle-fluid interaction force, N

${F}_{pf}^{*}$ dimensionless particle-fluid interaction force, –

*Fr* Froude number, –

*F _{t }*tangential soft sphere interaction at contact, N

${F}_{t}^{*}$ dimensionless tangential soft sphere interaction at contact, –

*g* gravitational acceleration, m/s^{2}

*Ga*Galilei number, –

*I *inertial moment of particle, kg·m^{2}

*m _{ }*mass, kg

*p _{ }*pressure, Pa

*p' _{ }*pressure perturbation, Pa

*P _{ }*dimensionless pressure, –

*P' *dimensionless pressure perturbation, –

*r _{p}* radius of particle, m

*R* dimensionless radius of particle, –

*Re* particle Reynolds number, –

*t*time, s

*T *dimensionless time, –

*u*fluid velocity, m/s

*U *dimensionless fluid velocity, –

*u*_{0}fluidizing velocity, m/s

*u _{t}*terminal velocity, m/s

*v*particle velocity, m/s

*V *dimensionless particle velocity, –

*V _{p}*volume of particle, m

*x*coordinate, m

*X *dimensionless coordinate, –

*ε* voidage, –

*μ* viscosity, Pa·s

*ρ* density, kg/m^{3 }

*ρ*^{*} density ratio (=*ρ _{p}*/

*ω* angular velocity, rad/s

*ω*^{*} dimensionless angular velocity

Subscripts

*f* fluid

*mf* minimum fluidization

*mb* minimum bubbling fluidization

*o* arbitrary reference quality

*p* particle

Conflicts of Interest

The authors declare no conflicts of interest regarding the publication of this paper.

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