Dehghan, M., Basirat Tabrizi, H. (2014). Effects of coupling on turbulent gas-particle boundary layer flows at borderline volume fractions using kinetic theory. Journal of Heat and Mass Transfer Research(JHMTR), 1(1), 1-8. doi: 10.22075/jhmtr.2014.148

Maziar Dehghan; Hassan Basirat Tabrizi. "Effects of coupling on turbulent gas-particle boundary layer flows at borderline volume fractions using kinetic theory". Journal of Heat and Mass Transfer Research(JHMTR), 1, 1, 2014, 1-8. doi: 10.22075/jhmtr.2014.148

Dehghan, M., Basirat Tabrizi, H. (2014). 'Effects of coupling on turbulent gas-particle boundary layer flows at borderline volume fractions using kinetic theory', Journal of Heat and Mass Transfer Research(JHMTR), 1(1), pp. 1-8. doi: 10.22075/jhmtr.2014.148

Dehghan, M., Basirat Tabrizi, H. Effects of coupling on turbulent gas-particle boundary layer flows at borderline volume fractions using kinetic theory. Journal of Heat and Mass Transfer Research(JHMTR), 2014; 1(1): 1-8. doi: 10.22075/jhmtr.2014.148

Effects of coupling on turbulent gas-particle boundary layer flows at borderline volume fractions using kinetic theory

^{}Mechanical Engineering Department., Amirkabir University of Technology, Tehran, Iran

Receive Date: 11 July 2013,
Revise Date: 16 September 2013,
Accept Date: 27 October 2013

Abstract

This study is concerned with the prediction of particles’ velocity in a dilute turbulent gas-solid boundary layer flow using a fully Eulerian two-fluid model. The closures required for equations describing the particulate phase are derived from the kinetic theory of granular flows. Gas phase turbulence is modeled by one-equation model and solid phase turbulence by MLH theory. Results of one-way and two-way coupled approaches are compared with the available experimental and numerical results. Results show that one-way coupled approach is more efficient for particulate velocity prediction in dilute flows. But, if the gas-phase flow characteristics are desired, the twoway coupled approach should be used. Effects of free stream velocity on the coupling are discussed.

This study is concerned with the prediction of particles’ velocity in a dilute turbulent gas-solid boundary layer flow using a fully Eulerian two-fluid model. The closures required for equations describing the particulate phase are derived from the kinetic theory of granular flows. Gas phase turbulence is modeled by one-equation model and solid phase turbulence by MLH theory. Results of one-way and two-way coupled approaches are compared with the available experimental and numerical results. Results show that one-way coupled approach is more efficient for particulate velocity prediction in dilute flows. But, if the gas-phase flow characteristics are desired, the two-way coupled approach should be used. Effects of free stream velocity on the coupling are discussed.

Effects of coupling on turbulent gas-particle boundary layer flows at borderline volume fractions using kinetic theory

Maziar Dehghan,Hassan Basirat Tabrizi^{*}

Mechanical Engineering Departmen., Amirkabir University of Technology, Tehran, Iran

Journal of Heat and Mass Transfer Research 1 (2014) 1-7

1. Introduction

Gas-particle flows are frequently encountered in the natural environment and industrial processes, such as desert and sand storms, pollutions in industrial or urban regions, fluidized bed and pneumatic conveying of particles [1]. There are many parameters which determine the gas-particle flow characteristics; for example, particle mass loading rate ρp (Tsuji and Morikawa [2]), gravity g (Taniere et al. [3]), inter-particle spacing (Sato et al. [4]), particle volume fraction α_{p}(Elghobashi [5]), velocity gradient of the flow (Li et al. [6]).

Elghobashi [5] classified gas-solid flows when the solid volume fraction is less (dilute) or greater (dense) than 0.1%. When the flow is dilute, effect of presence of particle on the carrier fluid is negligible. The interaction in this regime is named one-way coupling. Also, a homogeneous model can be used in this regime same as the investigation done by Mirzaei and Dehghan [7]. When the flow is dense, the momentum transfer from particles to the carrier phase is large enough to modify the characteristics of the flow, and the interaction in this regime should be considered. This consideration could be done by using two-way coupling. Inter-particle and wall-particle collisions may be important in dense flows and considering the collisions leads the four-way coupling. But, this classification is questionable in borderline values of the solid volume fractions. In this study, it is desired to see which way of coupling is efficient for engineering purposes.

Giacinto et al. [8] studied the coupling effects for the first time. They investigated the behavior of particles based on a one-way model and a two-way model approaches. Also, they proposed a correlation for pressure drop arising from the particulate phase. Nasr and Ahmadi [9] studied the turbulence modulation due to its interaction with dispersed solid particles in a downward fully developed channel flow. They used the Eulerian framework for the gas-phase, whereas the Lagrangian approach was used for the particle-phase. The effect of turbulence on the flow-field was included via the standard k–ε model. Nasr et al. [10] studied the effects of particle–particle collisions and the two-way coupling on the dispersed and carrier phase turbulence fluctuations in a channel flow based on a DNS solution. They found when the particle collisions were neglected but the particle–fluid two-way coupling effects were accounted for, the two-way coupling and the particle normal fluctuating velocity decreased near the wall causing a decrease in the particle deposition velocity. In the case of the four-way coupling in which both inter-particle collisions and two-way coupling effects were present, it was found that the particle deposition velocity increased compared with the one-way coupling case. When the particle aerodynamic interactions were added to the four-way coupled case (termed six-way coupled case), no significant changes in the mean fluid and particle velocities and the fluid and particle fluctuating velocities were obtained.

Researchers investigate particles in particulate flows using two major approaches: Lagrangian and Eulerian. Lagrangian model traces the path of individual particles on their way through the flow field. This needs long computational time in comparison with Eulerian method. Eulerian approach is more efficient for engineering purpose but closure models are the shortcoming of the Eulerian approaches [11]. Closure relations for particulate flow have been derived from kinetic theory of granular flow in this study.

Similarities between non-uniform dense gases and particulate flows were a start point for developing the kinetic theory of granular flows. The kinetic theory of granular flow allows determination of pressure and viscosity of the solid particles by incorporating the flow, gas, and particle characteristics and properties [12, 13]. Lun et al. [14] applied the kinetic theory of granular flow for the first time. This model has been used and developed by researchers such as Sinclair and Jackson [15], Ding and and Gidaspow [16], Huilin et al. [13], Vejahati et al. [17], Dehghan and Basirat Tabrizi [18], and Yusof et al. [19].

Taniere et al. [3], Slater et al. [11], Wang and Levy [20, 21], and Dehghan and Basirat Tabrizi [18, 22] studied the turbulent boundary layer gas-particle flows. Taniere et al. [3] concentrated on the particle response to fluid turbulence in a dilute horizontal boundary layer. Slater et al. [11] used a one-way coupled method to predict the deposition rate of particles in the dilute region. Wang and Levy [20, 21] studied particle motion in a vertical boundary layer experimentally and numerically. They simulated the flow using the commercial ANSYS CFX-4 software based on the kinetic theory of granular flow. Dehghan and Basirat Tabrizi [18] studied on the modeling of a dilute turbulent gas-particle flows near the solid flat wall. They introduced a new inlet condition for the granular temperature balance equation. Also, they investigated the self similar profiles of particle velocity in the boundary layer which were independent of location and free stream velocity. Dehghan and Basirat Tabrizi [22] investigated the need of a turbulent model for a turbulent particulate phase and showed that the conventional turbulence models which are based on the conventional fluids are not suitable for particulate flows. However, they indicated that the results of a turbulent model for the particulate flow are more precise in comparison with a laminar model, especially near the wall.

In this study, one-way and two-way coupled approaches have been used to predict the experimental velocities of Wang and Levy [20, 21]. Motion of particles with 60 µm diameter (d_{p}) and 1680 kg/m^{3} material density (ρ_{mp}) at 0.6 and 1.0 kg/m^{3} particulate loading rates (ρ_{p}) and 20 and 30 m/s free stream velocities near a flat solid boundary was simulated numerically. These quantities were used on the basis of experiments of Wang and Levy [20, 21]. So, the volume fraction of particulate phase is in the borderline value. Eulerian-Eulerian two-fluid model was used to model the flow. Closure relations for particulate phase have been derived from the kinetic theory of granular flow. Effects of free stream velocity and way of coupling on the velocity of gas and particulate phases are investigated and the numerical simulations are compared with the available numerical and experimental data of Wang and Levy [20, 21].

2. Analysis and Modeling

For two-dimensional turbulent gas flow in a boundary layer of a solid flat plate (figure 1), one can write:

(1)

(2)

(3)

U, u, and are instantaneous, mean, and fluctuating values, respectively. “1” is the upstream flow direction (the tangential direction to the plate). τ is the total stress tensor which is defined for incompressible fluids in the boundary layer of flat solid boundaries as:

(4)

is the turbulent (eddy) viscosity. One-equation model has been used for the gas-phase to model it [20]:

Figure 1. Schematic diagram of the problem

(5)

(6)

Here, k is turbulent kinetic, l denotes characteristic length of eddies which have the maximum portion of turbulent kinetic energy and l_{m} is the mixing length (Mixing Length Hypothesis):

(7)

Gas phase parameters and variables are written with no subscript for convenience. Subscript ‘p’ denotes particulate phase. Governing equations for the particulate phase are [12]:

(8)

(9)

The solid stress tensor (τ_{p}) is expressed in terms of the solid pressure (P_{p}), bulk viscosity (µ_{b}), and shear stress viscosity (µ_{s}) as [12]:

(10)

where I is unit matrix, µ_{b} is bulk viscosity of particulate phase, µ_{p} is shear viscosity of particulate phase, and B is drag coefficient which is required to couple the interface force for the two-way coupled approach. The interface momentum transfer coefficient will be as following when the porosity is greater than 0.8 [17]:

(11)

the porosity (α) represents gas-phase occupied area per the total area in any cross-section. The granular temperature (θ) is defined as a measure for the energy of the fluctuating velocity of the particles. The conservation equation of granular temperature is [12]:

(12)

(13)

Particulate phase pressure and shear viscosity have two important mechanisms in the dilute regimes, collisional and kinetic [24]:

(14)

Laminar shear viscosity is [25]:

(15)

“e” is the restitution coefficient of particles and e=1 is fully elastic. In this study, “e” is set to 0.95 [25]. Pressure of the particulate phase is [12]:

(16)

the first term on the RHS is the kinetic and the second one is the collisional part. “g_{0}” is the radial distribution function [12]:

(17)

(18)

(19)

µ_{b} is bulk viscosity, k_{p} is granular diffusion coefficient, and α_{p,max} is the maximum particle packing limit. Granular temperature dissipation and transfer between gas and particles are expressed as [12]:

(20)

(21)

Particles in turbulent flows have two types of motion: a) Random oscillations of individual particles, measured by the classical granular temperature; b) turbulence caused by the motion of clusters of particles. These two kinds of turbulence cause two kinds of mixing, mixing on the level of a particle and mixing on the level of clusters [26]. The expressed granular temperature theory is based on the laminar motion of particles. So, for considering the cluster-like motion of particles and effects of turbulent motion of particles, a model which considers the turbulent phenomena is required [11, 22, 26, 27]. Hence, the MLH (Mixing Length Hypothesis) theory was adopted for particulate phase in which equations are the same as those in the carrier phase and are described in equations 6 and 7.

It is assumed that gas phase had no-slip condition and zero turbulent kinetic energy on the solid boundary. Free stream condition at the entrance was considered. At the exit, Neumann-type boundary condition was adopted. Particulate phase had the same boundary conditions, except on the solid wall for tangential velocity and granular temperature which are as following [15]:

(22)

(23)

y-direction is normal to solid boundary, e_{w} is the restitution coefficient at the wall and is set to 0.75 [28]. Adopting lm at the solid wall equal to zero is not a realistic assumption for the particulate phase because of slip-velocity of particles. Hence, Neumann-type boundary condition for the mixing-length was adopted for the particulate phase at the wall [22].

These equations (1-23) describe one-way coupled approach. If one adds “-B(u-V_{p})” to the RHS of the equations (3), two-way coupled approach will yield. Finite-difference method [18, 22, 29, and 30] was used to solve equations (1-23). Pseudo-transient scheme was used to decouple the equations. Central difference in space and forward in time discretization with the second order of precision was applied to be more accurate. Non-uniform structured gird (figure 2) and artificial viscosity [18, 22] were used to save time with Compaq Visual FORTRAN 6.1 software.

3. Results and Discussion

Simulation is preformed based on a 71x141 grid. Also, a 121x201 grid is used to examine mesh dependency. Figure 2 compares the simulation results in the two grids. The maximum non-dimensional difference between results of these two grids is less than 3% for both gas and solid-phases. However, computational time of fine mesh increases in several orders.

Single-phase results of the gas phase are compared with the DNS result of Spalart [31] in figure 3. “k^{+}” is the non- dimensional kinetic turbulent energy, “δ” is the boundary layer thickness, and “y” is normal direction to the wall.

The numerical result of one-equation turbulence modeling is off at the peak of the kinetic energy curve. This type of error (being out of the peak of the turbulent

a)

b)

Figure 2. Used mesh (a) and mesh-dependency examination (b) (p: particulate-phase, g: gas-phase, x=0.5, U_{∞}= 30 m/s, d_{p}= 60 µm)

kinetic energy profile) is usual and originates from the modeling of turbulence phenomena instead of solving a complete and high resolution simulation (DNS). Overall, a good agreement between gas-phase simulation and the DNS can be seen.

Figure 4 shows results of one-way coupled approach in comparison with the numerical and experimental results of Wang and Levy [20, 21]. Results of current study are closer to the experiments than the previous simulation of Wang and Levy [21]. It is due to some simplification of commercial ANSYS CFX-4 code that has been used by Wang and Levy [21]. As it is discussed by Dehghan and Basirat Tabrizi [18], the accuracy of particulate phase results has a high dependency on the particulate viscosity definition and simulation. Away from the wall, drag term is dominating and velocity gradient vanishes. So, the velocity of particulates is not sensitive to the granular temperature and particulate viscosity values. The accuracy of results of gas and particulate phases has been verified.

Now, effects of coupling on the gas and particulate-phase velocities will be discussed. “2-W” in the following figures represents the two-way coupled approach.

Figures 5 and 6 show the particulate velocity results of one-way and two-way coupled approaches in comparison with experiments of Wang and Levy [21]. They could show a small discrepancy between the two

Figure 3. Gas-phase simulation in comparison with the DNS results of Spalart [27]

Figure 4. Examination of particulate phase simulation result accuracy (d_{p}=60 μm, particle loading rate ρ_{p}=1.0 kg/m^{3}, U_{∞}=30 m/s)

approaches. This is due to low volume fraction. Discrepancies between one-way and two-way approaches decrease by increasing the axial location (x-direction). Velocity results of the two-way coupled approach are higher than the one-way one. It is a result of coupling. When the two-way coupled approach is used, the simulated velocity of gas phase would increase since the particles are faster in the boundary layer and the code could consider the momentum enhancement of particles. Figures 7 and 8 are plotted for 20 m/s free stream velocity.

Figure 5. Results of particle velocity of one-way coupled approach in comparison with the two-way at x=0.25 and 0.75 m (ρ_{p}=1.0 kg/m^{3}, U_{∞}=30 m/s)

Figure 6. Results of particle velocity of one-way coupled approach in comparison with the two-way at x=0.5 and 1.0 m (ρ_{p}=1.0 kg/m^{3}, U_{∞}=30 m/s)

Figure 7. Results of particle velocity of one-way coupled approach in comparison with the two-way at x=0.25 and 0.75 m (ρ_{p}=1.0 kg/m^{3}, U_{∞}=20 m/s)

Figure 8. Results of particle velocity of one-way coupled approach in comparison with the two-way at x=0.5 and 1.0 m (ρ_{p}=1.0 kg/m^{3}, U_{∞}=20 m/s)

Again, it can be seen that two-way coupled approach has still little effects on the results. However, these effects are more sensible than the 30 m/s free stream velocity. By decreasing the free stream velocity, boundary layer will grow. This growth simultaneously occurs with velocity decrease, which decreases the order of viscous term in the Navier-Stokes equations for the particulate phase. Therefore, importance of viscous term will decrease in comparison with the drag term in the equation of motion. On the other hand, two-way coupled approach has a drag nature. In other words, when drag has a greater order of magnitude, the two-way coupled approach will be more important. Furthermore, as it was expected the results of the two-way coupled approach are closer to the experiments. An important parameter for engineering purposes is the computational time. The cost of the two-way coupled approach is very high in comparison with the achieved accuracy. In this study, simulation of a one-way coupled model lasts less than 72 hours for non-dimensional residuals lower than 0.001 on a PC with 3.12 GHz CPU and 4 GB RAM. But, the two-way coupled model needs more than 96 hours to achieve the same residuals of the one-way coupled model. Another matter arising from the two-way coupled approach is the tendency of the code to diverge. So, the code needs finer meshes and further numerical efforts to achieve the same residual of the one-way coupling.

From the presented discussion and results of the one-way and two-way models, one can conclude that the one-way coupled approach is more advantageous for engineering purposes in prediction particles velocity in such dilute conditions. Nevertheless, is it true for the carrying phase?

Figure 9 presents effects of the particulate loading rates (ρ_{p}= 1.0 and 0.6 kg/m^{3}) on the velocity of the carrier gas phase. It shows that particulate loading can modify the gas-phase velocity profile. To see effects of particulate phase on carrier phase more obviously, figure 8 has been drawn. Effect of particulate loading rate on the wall friction factor is not negligible even in such dilute conditions as it can be seen in figure 10. Friction factor in 1.0 kg/m^{3} and 0.6 kg/m^{3} loading rates increases 12% and 8% respectively in comparison with the clean gas flow. It is due to some simultaneous effects which affect gas-phase flow characteristics. From figure 8 one can see that

Figure 9. Effects of particulate loading rate on the gas-phase velocity in the boundary layer (ρ_{p}=0.0, 0.6, and1.0 kg/m^{3}, U_{∞}=30 m/s)

Figure 10. Effects of particulate loading rate on the wall friction factor (ρ_{p}=0.0, 0.6, and1.0 kg/m^{3}, U_{∞}=30 m/s)

the gas-phase velocity increases due to the particle existence. Simultaneously, boundary layer thickness attenuation occurs. These two simultaneous effects beside the high particle slip-velocity, which can be seen from figures 5-8, influence the gas-phase velocity more considerable. Therefore, the two-way coupled approach could be important in dealing with carrier gas-phase; while, it is not efficient for the particulate phase predictions for engineering purposes in such dilute flows.

4. Conclusion

Dilute turbulent gas-solid boundary layer flow has been studied numerically. Eulerian two-phase model based on the kinetic theory of granular flow has been used to model the flow. Turbulence of gas and solid phases has been modeled by the “k-l” and MLH models. Collisions have been considered via restitution coefficients (e and e_{w}). Costs and benefits of the way of coupling (one-way / two-way coupled approach) have been investigated on the simulations. Highlights of this study may be stated as following:

One-way approach is more advantageous among engineering purposes for particulate velocity predictions.

For the carrier phase, change in flow characteristics is considerable in comparison with the change of particulate velocity when the two-way coupled approach is used. So, when the gas-phase flow characteristics are needed, the two-way coupled approach should be applied.

At lower free stream velocity, the two-way coupled approach is more efficient for particulate phase simulations.

Boundary layer thickness attenuation, gas-phase velocity increase in the boundary layer, and high particle slip-velocity affect gas flow particularly near the wall.

To summarize, two-way coupled approach is not advantageous for such dilute flows, even in borderline volume fraction values (volume fractions near 0.1%). This is due to the computational costs and amount of achieved accuracy in the results. One-way coupled approach results are accurate enough for engineering purposes. For example in the current simulation, the two-way coupled approach needs up to 50% more computational time than the one-way for a same error limit and mesh size.

Nomenclature

C

drag coefficient

d

diameter (m)

e

Restitution coefficient

I

unit matrix

K

turbulent kinetic energy

l

length scale

P

pressure

Re

Reynolds number

t

time

u, v

velocity

x, y

coordinate

Greek symbols

α

volume fraction

β

momentum transfer coefficient

γ

granular temperature dissipation

δ

boundary layer thickness

Θ

granular temperature

υ

kinematic viscosity

τ

stress tensor

µ

dynamic viscosity (Pa.s)

ρ

density (kgm-3)

Φ

energy transfer between phases

subscripts

coll

collision

D

drag

g

gas

i, j

indices

kin

kinetic

m

mixing-length

mp

material density

p

particulate phase

t

turbulent

w

wall

Superscripts

‘

fluctuating value

+

non-dimension value

T

transpose

References

[1]. Li J., H. Wang, Z. Liu, S. Chen, C. Zheng, An experimental study on turbulence modification in the near-wall boundary layer of a dilute gas-particle channel flow, Exp Fluids, 53, 1385–1403 (2012).

[2]. Y. Tsuji, Y. Morikawa, LDV measurements of an air-solid twophase flow in a horizontal pipe, J Fluid Mech., 120, 385–409 (1982).

[3]. A. Taniere, B. Oesterle, J.C. Monnier, On the behavior of solid particles in a horizontal boundary layer with turbulence and saltation effects. Experiments in Fluids, 23, 463-471 (1997).

[4]. Y. Sato, U. Fukuichi, K. Hishida, Effect of inter-particle spacing on turbulence modulation by Lagrangian PIV, Int J Heat Fluid Flow, 21, 554–561 (2000).

[6]. F. Li, H. Qi, C. You, Phase Doppler anemometry measurements and analysis of turbulence modulation in dilute gas–solid two phase shear flows, J Fluid Mech., 663, 434–455 (2010).

[7]. M. Mirzaei, M. Dehghan, Investigation of flow and heat transfer of nanofluid in microchannel with variable property approach, Heat Mass Transfer, 49, 1803-1811 (2013).

[8]. M. Di Giacinto, R. Piva, F. Sabetta., Two-way coupling effects in dilute gas-particle flows, ASME Transactions Journal of Fluids Engineering, 104, 304-311 (1982).

[9]. H. Nasr, G. Ahmadi, the effect of two-way coupling and inter particle collisions on turbulence modulation in a vertical channel flow, Int. J. Heat Fluid Flow, 28, 1507-1517 (2007).

[10]. H. Nasr, G. Ahmadi, J.B. McLaughin, A DNS study of effects of particle-particle collisions and two-way coupling on particle deposition and phase fluctuations, J. Fluid Mech., 640, p. 507-536 (2009).

[11]. S.A. Slater, A.D. Leeming, J.B. Young, Particle deposition from two-dimentional turbulent gas flows. Int. J. Multiphase Flow, 29, 721-750 (2003).

[12]. D. Gidaspow, Multiphase flow and fluidization: continuum and kinetic theory descriptions, Boston: Academic press, (1994).

[13]. L. Huilin, D. Gidaspow, J. Bouillard, L. Wenti, Hydrodynamics simulation of gas-solid flow in a riser using kinetic theory of granular flow. chemical Engineering Journal, 95, 1-13 (2003).

[14]. C.K.K. Lun, S.B. Savage, D.J. Jefferey, N. Chepurniy, Kinetic theories for granular flow: inelastic particles in Couette flow and slightly inelastic particles in a general flow field. J. Fluid Mechanics, 140, 223-256 (1984).

[15]. J.L Sinclair, R. Jackson, Gas-particle flow in a vertical pipe with particle-particle interactions. AIChE J., 35, 1473-1486 (1989).

[16]. J. Ding, D. Gidaspow, A bubbling fluidization model using kinetic theory of granular flow. AIChE J., 36, 523-538 (1990).

[17]. F. Vejahati, N. Mahinpey, N. Ellis, M.B. Nikoo, CFD simulation of gas–solid bubbling fluidized bed: A new method for adjusting drag law, Canadian J. Chem. Eng., 87 (1), 19-30 (2009).

[18]. M. Dehghan, H. Basirat Tabrizi, On near-wall behavior of particles in a dilute turbulent gas–solid flow using kinetic theory of granular flows, Powder Technology, 224, 273–280 (2012).

[19]. R. Yusuf, B. Halvorsen, M.C. Melaaen, Computational fluid dynamic simulation of ethylene hydrogenation in a fluidised bed of porous catalyst particles, Canadian J. Chem. Eng., 90 (3), 544-557 (2012).

[20]. J. Wang, E.K. Levy, Particle motions and distributions in turbulent boundary layer of air-particle flow past a vertical flat plate. Experimental Thermal and Fluid science, 27, 845-853 (2003).

[21]. J. Wang, E.K. Levy, Particle behavior in the turbulent boundary layer of a dilute gas-partilce flow past a flat plate. Experimental Thermal and Fluid science, 30, 473-483 (2006).

[22]. M. Dehghan, H. Basirat Tabrizi, Turbulence effects on the granular model of particle motion in a boundary layer flow, Canadian J. Chem. Eng., 92, 189–195 (2014).

[24]. S. Dartevelle, Numerical and granulometric approaches to geophysical granular flows, PhD thesis, Department of Geological and Mining Engineering, Michigan Technological University: Houghton, (2003).

[25]. V.S. Syamlal, W. Rogers, T.J. O'Brien, MFIX documentation: volume I, theory guide: National Technical information service, Springfield, (1993).

[26]. D. Gidaspow, J. Jung, R.K. Singh, Hydrodynamics of fluidization using kinetic theory: an emerging paradigm 2002 Flour-Daniel lecture. Powder Technology, 148, 123-141 (2004).

[27]. Y. Cheng, F. Wei , Y. Guo, Y. Jin, CFD simulation of hydrodynamics in the entrance region of a downer. Chemical Engineering Science, 56(4), 1687-1696 (2001).

[28]. A.H. Govan, G.F. Hewitt, C.F. Ngan, Particle motion in the turbulent pipe flow. Int. J. Multiphase Flow, 15, 471-481 (1989).

[29]. M. Dehghan, M. Mirzaei, A. Mohammadzadeh, Numerical formulation and simulation of a non-Newtonian magnetic fluid flow in the boundary layer of a stretching sheet, Journal of Modeling in Engineering 11 (34), 73-82 (2013).

[30]. M. Dehghan, M. Mirzaei, M.S. Valipour, S. Saedodin, Flow of a non-Newtonian fluid over a linearly moving sheet at a transient state; new similarity variable and numerical solution scheme, Journal of Modeling in Engineering, (2014) (accepted manuscript).

[31]. P.R. Spalart, Direct numerical simulation of turbulent boundary layer up to Reθ=1410. J. Fluid Mechanics, 187, 61-98 (1988).

References

[1]. Li J., H. Wang, Z. Liu, S. Chen, C. Zheng, An experimental study on turbulence modification in the near-wall boundary layer of a dilute gas-particle channel flow, Exp Fluids, 53, 1385–1403 (2012).

[2]. Y. Tsuji, Y. Morikawa, LDV measurements of an air-solid twophase flow in a horizontal pipe, J Fluid Mech., 120, 385–409 (1982).

[3]. A. Taniere, B. Oesterle, J.C. Monnier, On the behavior of solid particles in a horizontal boundary layer with turbulence and saltation effects. Experiments in Fluids, 23, 463-471 (1997).

[4]. Y. Sato, U. Fukuichi, K. Hishida, Effect of inter-particle spacing on turbulence modulation by Lagrangian PIV, Int J Heat Fluid Flow, 21, 554–561 (2000).

[6]. F. Li, H. Qi, C. You, Phase Doppler anemometry measurements and analysis of turbulence modulation in dilute gas–solid two phase shear flows, J Fluid Mech., 663, 434–455 (2010).

[7]. M. Mirzaei, M. Dehghan, Investigation of flow and heat transfer of nanofluid in microchannel with variable property approach, Heat Mass Transfer, 49, 1803-1811 (2013).

[8]. M. Di Giacinto, R. Piva, F. Sabetta., Two-way coupling effects in dilute gas-particle flows, ASME Transactions Journal of Fluids Engineering, 104, 304-311 (1982).

[9]. H. Nasr, G. Ahmadi, the effect of two-way coupling and inter particle collisions on turbulence modulation in a vertical channel flow, Int. J. Heat Fluid Flow, 28, 1507-1517 (2007).

[10]. H. Nasr, G. Ahmadi, J.B. McLaughin, A DNS study of effects of particle-particle collisions and two-way coupling on particle deposition and phase fluctuations, J. Fluid Mech., 640, p. 507-536 (2009).

[11]. S.A. Slater, A.D. Leeming, J.B. Young, Particle deposition from two-dimentional turbulent gas flows. Int. J. Multiphase Flow, 29, 721-750 (2003).

[12]. D. Gidaspow, Multiphase flow and fluidization: continuum and kinetic theory descriptions, Boston: Academic press, (1994).

[13]. L. Huilin, D. Gidaspow, J. Bouillard, L. Wenti, Hydrodynamics simulation of gas-solid flow in a riser using kinetic theory of granular flow. chemical Engineering Journal, 95, 1-13 (2003).

[14]. C.K.K. Lun, S.B. Savage, D.J. Jefferey, N. Chepurniy, Kinetic theories for granular flow: inelastic particles in Couette flow and slightly inelastic particles in a general flow field. J. Fluid Mechanics, 140, 223-256 (1984).

[15]. J.L Sinclair, R. Jackson, Gas-particle flow in a vertical pipe with particle-particle interactions. AIChE J., 35, 1473-1486 (1989).

[16]. J. Ding, D. Gidaspow, A bubbling fluidization model using kinetic theory of granular flow. AIChE J., 36, 523-538 (1990).

[17]. F. Vejahati, N. Mahinpey, N. Ellis, M.B. Nikoo, CFD simulation of gas–solid bubbling fluidized bed: A new method for adjusting drag law, Canadian J. Chem. Eng., 87 (1), 19-30 (2009).

[18]. M. Dehghan, H. Basirat Tabrizi, On near-wall behavior of particles in a dilute turbulent gas–solid flow using kinetic theory of granular flows, Powder Technology, 224, 273–280 (2012).

[19]. R. Yusuf, B. Halvorsen, M.C. Melaaen, Computational fluid dynamic simulation of ethylene hydrogenation in a fluidised bed of porous catalyst particles, Canadian J. Chem. Eng., 90 (3), 544-557 (2012).

[20]. J. Wang, E.K. Levy, Particle motions and distributions in turbulent boundary layer of air-particle flow past a vertical flat plate. Experimental Thermal and Fluid science, 27, 845-853 (2003).

[21]. J. Wang, E.K. Levy, Particle behavior in the turbulent boundary layer of a dilute gas-partilce flow past a flat plate. Experimental Thermal and Fluid science, 30, 473-483 (2006).

[22]. M. Dehghan, H. Basirat Tabrizi, Turbulence effects on the granular model of particle motion in a boundary layer flow, Canadian J. Chem. Eng., 92, 189–195 (2014).

[24]. S. Dartevelle, Numerical and granulometric approaches to geophysical granular flows, PhD thesis, Department of Geological and Mining Engineering, Michigan Technological University: Houghton, (2003).

[25]. V.S. Syamlal, W. Rogers, T.J. O'Brien, MFIX documentation: volume I, theory guide: National Technical information service, Springfield, (1993).

[26]. D. Gidaspow, J. Jung, R.K. Singh, Hydrodynamics of fluidization using kinetic theory: an emerging paradigm 2002 Flour-Daniel lecture. Powder Technology, 148, 123-141 (2004).

[27]. Y. Cheng, F. Wei , Y. Guo, Y. Jin, CFD simulation of hydrodynamics in the entrance region of a downer. Chemical Engineering Science, 56(4), 1687-1696 (2001).

[28]. A.H. Govan, G.F. Hewitt, C.F. Ngan, Particle motion in the turbulent pipe flow. Int. J. Multiphase Flow, 15, 471-481 (1989).

[29]. M. Dehghan, M. Mirzaei, A. Mohammadzadeh, Numerical formulation and simulation of a non-Newtonian magnetic fluid flow in the boundary layer of a stretching sheet, Journal of Modeling in Engineering 11 (34), 73-82 (2013).

[30]. M. Dehghan, M. Mirzaei, M.S. Valipour, S. Saedodin, Flow of a non-Newtonian fluid over a linearly moving sheet at a transient state; new similarity variable and numerical solution scheme, Journal of Modeling in Engineering, (2014) (accepted manuscript).

[31]. P.R. Spalart, Direct numerical simulation of turbulent boundary layer up to Reθ=1410. J. Fluid Mechanics, 187, 61-98 (1988).