Drag force of intermediate Reynolds number flow past mono- and bidisperse arrays of spheres
R. Beetstra
Faculty of Science & Technology, University of Twente, P.O. Box 217, 7500 AE Enschede, The Netherlands
Search for more papers by this authorCorresponding Author
M. A. van der Hoef
Faculty of Science & Technology, University of Twente, P.O. Box 217, 7500 AE Enschede, The Netherlands
Faculty of Science & Technology, University of Twente, P.O. Box 217, 7500 AE Enschede, The NetherlandsSearch for more papers by this authorJ. A. M. Kuipers
Faculty of Science & Technology, University of Twente, P.O. Box 217, 7500 AE Enschede, The Netherlands
Search for more papers by this authorR. Beetstra
Faculty of Science & Technology, University of Twente, P.O. Box 217, 7500 AE Enschede, The Netherlands
Search for more papers by this authorCorresponding Author
M. A. van der Hoef
Faculty of Science & Technology, University of Twente, P.O. Box 217, 7500 AE Enschede, The Netherlands
Faculty of Science & Technology, University of Twente, P.O. Box 217, 7500 AE Enschede, The NetherlandsSearch for more papers by this authorJ. A. M. Kuipers
Faculty of Science & Technology, University of Twente, P.O. Box 217, 7500 AE Enschede, The Netherlands
Search for more papers by this authorAbstract
Extensive lattice-Boltzmann simulations were performed to obtain the drag force for random arrays of monodisperse and bidisperse spheres. For the monodisperse systems, 35 different combinations of the Reynolds number Re (up to Re = 1,000) and packing fraction ϕ were studied, whereas for the bidisperse systems we also varied the diameter ratio (from 1:1.5 to 1:4) and composition, which brings the total number of different systems that we considered to 150. For monodisperse systems, the data was found to be markedly different from the Ergun equation and consistent with a correlation, based on similar type of simulations up to Re = 120. For bidisperse systems, it was found that the correction of the monodisperse drag force for bidispersity, which was derived for the limit Re = 0, also applies for higher-Reynolds numbers. On the basis of the data, a new drag law is suggested for general polydisperse systems, which is on average within 10% of the simulation data for Reynolds numbers up to 1,000, and diameter ratios up to 1:4. © 2007 American Institute of Chemical Engineers AIChE J, 2007.
Literature Cited
- 1 Ergun S. Fluid flow through packed columns. Chem Eng Proc. 1952; 48: 89.
- 2 Hill RJ,Koch DL,Ladd AJC. Moderate-Reynolds-number flows in ordered and random arrays of spheres. J Fluid Mech. 2001; 448: 243.
- 3 Kim S,Russel WB. Modeling of porous media by renormalization of the Stokes equation. J Fluid Mech. 1985; 154: 269.
- 4 Happel J,Brenner H. Low Reynolds Number Hydrodynamics. Dordrecht: Martinus Nijhoff; 1986.
- 5 Goldstein S. Concerning some solutions of the boundary layer equations in hydrodynamics. Proc Cambridge Philos Soc. 1929; 26: 1.
- 6 Clift R,Grace JR,Weber ME. Bubbles, Drops and Particles. New York: Academic Press; 1978.
- 7 Kaneda Y. The drag on a sparse random array of fixed spheres in flow at small but finite Reynolds number. J Fluid Mech. 1986; 167: 455.
- 8 Koch DL,Ladd AJC. Moderate Reynolds number flows through periodic and random arrays of aligned cylinders. J Fluid Mech. 1997; 349: 31.
- 9 Hill RJ,Koch DL,Ladd AJC. The first effects of fluid inertia on flow in ordered and random arrays of spheres. J Fluid Mech. 2001; 448: 213.
- 10 Di Felice R. Hydrodynamics of liquid fluidisation. Chem Eng Sci. 1995; 50: 1213.
- 11 Wen CY,Yu YH. Mechanics of fluidization. AIChE J. 1966; 62: 100.
- 12 Van der Hoef MA,Beetstra R,Kuipers JAM. Lattice Boltzmann simulations of low Reynolds number flow past mono- and bidisperse arrays of spheres: results for the permeability and drag force. J Fluid Mech. 2005; 528: 233.
- 13 Van der Hoef MA,van Sint Annaland M,Kuipers JAM. Computational fluid dynamics for dense gas-solid fluidized beds: a multi-scale modeling strategy. Chem Eng Sci. 2004; 59: 5157.
- 14 Blake, FE. Trans Am Inst Chem Engrs. 1922; 14: 415.
- 15 Kozeny J. Akad Wiss Wien Math.-naturw, Klasse. 1927; 136: 271.
- 16 Burke SP,Plummer WB. Gas flow through packed columns. Ind Eng Chem. 1928; 20: 1196.
- 17 Fand RM,Kim BYK,Lam ACC,Phan RT. Resistance to the flow of fluids through simple and complex porous media whose matrices are composed of randomly packed spheres. Trans ASME: J Fluids Eng. 1987; 109: 268.
- 18 Maier RS,Kroll DM,Davis HT,Bernard RS. Simulation of flow in bidisperse spheres packings. J Colloid Interface Sci. 1999; 217: 341.
- 19 Carman, PC. Fluid flow through granular beds. Trans Inst Chem Eng. 1937; 15: 150.
- 20 Kandhai D,Derksen JJ,van den Akker HEA. Interphase drag coefficients in gas-solid flows. AIChE J. 2003; 49: 1060.
- 21 Schlichting H. Boundary-Layer Theory. New York: McGraw-Hill Book Company; 1979.
- 22 Richardson JF,Zaki WN. Sedimentation and fluidisation. Part I. Trans Instn Chem Engrs. 1954; 39: 175.
- 23 Schiller L,Nauman A. A drag coefficient correlation. VDI Zeitung. 1935; 77: 318.
- 24 Di Felice R. On the voidage function in two-phase multiparticle systems. Int J Multiphase Flow. 1994; 20: 153.
- 25 Gidaspow D. Multiphase flow and fluidization: Continuum and kinetic theory descriptions. Boston: Academic Press; 1994.
- 26 Gibilaro LG,Di Felice R,Waldram SP,Foscolo PU. Generalized friction factor and drag coefficient correlations for fluid-particle interactions. Chem Eng Sci. 1985; 40: 1817.
- 27 Batchelor GK. Sedimentation in a dilute polydisperse system of interacting spheres. Part 1. General theory. J Fluid Mech. 1982; 119: 379.
- 28 Batchelor GK,Wen CS. Sedimentation in a dilute polydisperse system of interacting spheres. Part 2. Numerical results. J Fluid Mech. 1982; 124: 495.
- 29 Liang SC,Hong T,Fan LS. Effects of particle arrangements on the drag force of a particle in the intermediate flow regime. Int J Multiphase Flow. 1996; 22: 285.
- 30 Katoshevski D,Zhao B,Ziskind G,Bar-Ziv E. Experimental study of the drag force acting on a heated particle. J Aerosol Sci. 2001; 32: 73.
- 31 Zhu C,Lam K,Chu HH,Tang XD,Lui G. Drag forces of interacting spheres in power-law fluids. Mech Res Comm. 2003; 30: 651.
- 32 Patwardhan VS,Tien C. Sedimentation and liquid fluidization of solid particles of different sizes and density. Chem Eng Sci. 1985; 40: 1051.
- 33 Okayama Y,Doi A,Kawaguchi T,Tanaka T,Tsuji Y. Drag force model for fluidized bed of binary mixture of particles. Proceedings of the 5th World Congress on Particle Technology (WCPT5), Orlando, FL; April 23–27; 2006.
- 34
Succi S.
The lattice Boltzmann equation for fluid dynamics and beyond.
Oxford:
Clarendon Press;
2001.
10.1093/oso/9780198503989.001.0001 Google Scholar
- 35 Ladd, AJC. Numerical simulations of particulate suspensions via a discretized Boltzmann equation (Part I + II). J Fluid Mech. 1994; 271: 285.
- 36 Hasimoto H. On the periodic fundamental solutions of the Stokes equation and their application to viscous flow past a cubic array of spheres. J Fluid Mech. 1959; 5: 317.
- 37 White FM. Viscous fluid flow. pp 206–210. New York: McGraw-Hill; 1974.
- 38 Dallavalle JM. Micromeretics: the technology of fine particles. London: Pitman; 1948.
- 39 Turton R,Levenspiel O. A short note on the drag correlation for spheres. Powder Tech. 1986; 47: 83.
- 40 Beetstra R,van der Hoef MA,Kuipers JAM. Numerical study of segregation using a new drag force correlation for polydisperse systems derived from lattice Boltzman simulations. Chem Eng Sci. 2007; 62: 246.