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Yang Fluidization, Solids Handling, and Processing

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576Fluidization, Solids Handling, and Processing

10.0EPILOGUE

Bubbling is the usual phenomenon in most accepted processes of fluidization. It has been demonstrated that species of fluidization with better G/S contacting are available by avoidance of bubbling. This chapter has offered certain tools for discriminating the homogeneous L/S fluidization on the one hand from the bubbling G/S fluidization on the other, in the form of the EMMS model, but this is by no means the only possible method. It has also revealed the significance of particle size choice or design in order to improve the fluidizing characteristics of a given species of fluidization through using the bed collapsing apparatus, but this, too, is by no means the only possible technique.

The message of significance is how to “particulatize” a G/S system which is otherwise aggregative.

NOTATIONS

A

Area; cross-sectional area, cm2

A

Frontal area of particle, cm2

x

= d p3 ρf g p/µ2, Archimedes number, dimensionless

Ar

A

Cross-sectional area based on particle terminal velocity, cm2

t

 

= A/At, reduced area, dimensionless

Bi

= hdp /k s, Biot number, dimensionless

Cp

Heat capacity of gas, cal/mol·oC

Cs

Heat capacity of solids, cal/gm·oC

dp

Particle diameter, cm

DDiffusivity, cm2/sec

E= Nu Pr-1/3/Ar or Sh Sc-1/3/Ar, effectiveness factor, dimensionless f Friction factor, dimensionless

g = 980 cm/sec2, acceleration of gravity

GMass flow rate of gas, mol/cm2·sec

h Heat transfer coefficient between particle and fluid, cal/sec·cm2·oC

HNonuniformity index, dimensionless

j = Nu Pr-1/3/Re or Sh Sc-1/3/Re, j-factor, dimensionless

kg

Thermal conductivity of gas, cal/cm·sec·oC

k

Thermal conductivity of solid, cal/cm·sec·oC

s

Mass velocity of liquid, gm/cm2·sec

L

Bubbleless Fluidization

577

mFixed bed pressure drop exponent, dimensionless

nFluidized bed expansion exponent, dimensionless

N

= (L/ρf A)(S/ρs A), liquid-solids velocity ratio, dimensionless

NH

Number of heat-transfer stages, dimensionless

Nu

= hdp /k g, Nusselt number, dimensionless

P

Pressure drop, gm-wt/cm2

Pr

= Cpµ/k g, Prandtl number, dimensionless

Re

= dp uρf /µ, Reynolds number, dimensionless

S

Mass velocity of solids, gm/cm2·sec

Sc

= µ/ρf Df, Schmidt number, dimensionless

Sh

= hDdp /Df , Sherwood number, dimensionless

Sy

Synergism number, dimensionless

T

Temperature, oC

u

Velocity, cm/sec

uo

Superficial fluid velocity, cm/sec

ud

Superficial solids velocity, cm/sec

umb

Superficial fluid velocity at incipient bubbling, cm/sec

uf,umf Superficial fluid velocity at incipient fluidization, cm/sec

up

Actual velocity of particle, cm/sec

us

Relative velocity between particle and fluid, cm/sec

ut

Terminal particle velocity, cm/sec

= u /ut , reduced velocity, dimensionless

= A´Z´, reduced volume, dimensionless

w

Particle population density, gm/cm2

x f

Weight fraction of fines in binary particle mixture, dimensionless

z

Distance, cm

zi

Location of point of inflection for fast fluidization, cm

Z

Height of fluidized bed, cm

Zo

Dimensionless distance in accelerative motion of particle;

 

characteristic length for fast fluidization voidage profile, cm

Zt

Height based on particle terminal velocity, cm

Z1

Dimensionless distance in heat transfer

= z/Z, reduced distance, dimensionless

τ

= GCp /SCs, flowing heat capacity ratio, dimensionless

ε

Voidage or void fraction, dimensionless

ε mf

Voidage at incipient fluidization, dimensionless

578 Fluidization, Solids Handling, and Processing

εo

Voidage of fixed bed, dimensionless

ν

Fractional heat recovery, dimensionless

θTime, sec

ΘDimensionless time in particle-fluid heat transfer; dimensionless subsidence time in bed collapsing test

µViscosity, gm/cm·sec

ρ

Density of solid, gm/cm3

s

Density of fluid, gm/cm3

ρ

f

 

ρ= ρs - ρf, effective density

Φo Dimensionless pressure drop in accelerative particle motion

REFERENCES

Chen, B., and Kwauk, M., Generalized Fluidization of Non-Ideal Systems, Proc. First Intern. Conf. Circulating Fluidized Bed, 127-132, Halifax, Canada (1985)

Coulson, J. M., and Richardson, J. F., “Sedimentation,” Vol. 2, Chemical Engineering, McGraw-Hill, 2nd Ed. (1968); 3rd Ed. (1978)

Deng, Y., and Kwauk, M., “Levitation of Discrete Particles in Oscillating Liquids,” Chem. Eng. Sci., 45(2):483–490 (1990)

Geldart, D., “The Effect of Particle Size and Size Distribution on the Behavior of Gas-Fluidized Beds,” Powder Technol., 6:201–205 (1972)

Geldart, D., “Types of Fluidization,” Powder Technol., 7:285–290 (1973)

Houghton, G., “The Behavior of Particles in a Sinusoidal Velocity Field,” Proc. Roy. Soc., A272:33–43 (1963)

Houghton, G., “Digital Computer Simulation of Fluttering Lift in the Desert Locust,” Nature 201, pp. 568–570; “Effect of Variation in Lift Coefficient, Phase Angle and Waveform on Fluttering Lift in the Desert Locust,” Nature 202, pp. 870–872; “Simulation of Fluttering Lift in a Bird, Locust, Moth, Fly and Bee,” Nature 202, pp. 1183–1185; “Fluttering Flight Mechanisms in Insects and Birds,” Nature 204, pp. 447–449; “Generalized Hovering-Flight Correlation for Insects,” Nature 204, pp. 666–668 (1964)

Houghton, G., “Particle Trajectories and Terminal Velocities in Vertically Oscillating Fluids,” Can. J. Chem. Eng., 44:90-95 (1966)

Houghton, G., “Velocity Retardation of Particles in Oscillating Fluids,” Chem. Eng. Sci., 23:287-288 (1968)

Kramers, H., “Heat Transfer from Spheres to Flowing Media,” Physica, 12:61 (1946)

Bubbleless Fluidization

579

Krantz, W. B., Carley, J. F., and Al-taweel, A. M., “Levittion of Solid Spheres in Pulsating Liquids,” Ind. Eng. Chem. Fund., 12:391-396 (1973)

Kwauk, M., “Fluidized Calcination of Aluminum Ore for Pre-Desilication,” (unpubl.),

Inst. Chem. Metall., 1964-11–6 (1964c)

Kwauk, M., and Tai, D. -W., “Transport Processes in Dilute-Phase Fluidization as Applied to Chemical Metallurgy,” (I). Transport Coefficient and System Pressure Drop as Criteria for Selecting Dilute-Phase Operations; (II). Application of Dilute-Phase Technique to Heat Transfer, (in Chinese, with Eng. abs.), Acta Metallurgica Sinica, 7:264–280; 391–408 (1964)

Kwauk, M., “Particulate Fluidization in Chemical Metallurgy,” Scientia Sinica, 16:407 (1973)

Kwauk, M., “Fluidized Leaching and Washing,” (in Chinese), Science Press, Beijing (1979a)

Kwauk, M., :Fluidized Roasting of Oxidic Chinese Iron Ores,” Scientia Sinica, 22:1265 (1979b); repr. Intern. Chem. Eng., 21:95–115 (1981)

Kwauk, M., “The Jigged Reducer,” (unpubl.); (i) 1979; (ii) 1981; (iii) 1983; Inst. Chem. Metall.

Kwauk, M., and Wang, Y., Fluidized Leaching and Washing, Chem. E. Symp,. Ser. No. 63, paper D4/BB/1-21 (1981)

Kwauk, M., Wang, N., Li, Y. Chen, B., and Shen, Z., “Fast Fluidization at ICM,”

Proc. First Intern. Conf. Circulating Fluidized Bed, p. 33–62, Halifax, Canada (1985)

Kwauk, M., Fluidization—Idealized and Bubbleless, with Applications, Science Press, Beijing, and Ellis Horwood, U. K. (1992)

Kwauk, M., “Fast Fluidization,” Advances in Chemical Engineering, (M. Kwauk, ed.), Vol. 20, Academic Press, U.S.A. (1994)

Li, J., Tung, Y., and Kwauk, M., “Fast Fluidization at ICM,” (i) Method of Energy Minimization in Multi-Scale Modeling of Two-Phase Flow; (ii) Energy Transport and Regime Transition in Particle-Fluid Two-Phase Flow; (iii) Axial Voidage Profiles of Fast Fluidized Beds in Different Operating Regions, Second International Conference on Circulating Fluidized Beds, p. 75, 89, 193, Compiegne, France (1988)

Li, J., and Kwauk, M., “Particle-Fluid Two-Phase Flow, The Energy-Minimization Multi-Scale Method,” Metallurgical Industry Press, Beijing (1994)

Li, Y., and Kwauk, M., “The Dynamics of Fast Fluidization,” Third Intern. Conf. Fluidization, p. 537–544, Henniker, U.S.A. (1980)

Liu, D., Liu, J., Li, T., and Kwauk, M., “Shallow-Fluid-Bed Tubular Heat Exchanger,” Fifth Int. Fluidization Conf., p. 401–408, Elsinore, Denmark (1986)

580 Fluidization, Solids Handling, and Processing

Liu, K., “Particle Motion in Standing Waves in Gaseous Medium,” (in Chinese, unpubl.), Inst. Chem. Metall. (1981)

Qian, Z., and Kwauk, M., “Computer Application in Characterizing Fluidization by the Bed Collapsing Method,” Tenth Intern. CODATA Conf., Ottawa (1986)

Qin, S., and Liu, G., “Application of Optical Fibers to Measurement and Display of Fluidized Systems,” Proc. China-Jpn. Fluidization Symp., p. 258–266, Hangzhou, China (1982)

Qin, S., and Liu, G., “Automatic Surface Tracking for Collapsing Fluidized Bed,” Sec. China-Japan Fluidization Symp ., Kunming, Elsevier, p. 468 (1985)

Reh, L., “Calcination von Aluminumhydroxid in einer zirkulierenden Wirbelschicht,” Chem. Eng.-Tech., 42:447–451 (1970)

Reh, L., “Fluidized Bed Processing,” Chem. Eng. Prog. 67:58–63 (1971)

Reh, L., “Calcining Aluminum Trihydrate in a Circulating Fluid Bed, a New Technique of High Thermal Efficiency, Metallurges,” Rev. Activ., 1972(15):58–60 (1972)

Reh, L., “The Circulating Fluid Bed Reactor—A Key to Efficient Gas-Solid Processing,” Proc. First Intern. Conf. Circulating Fluidized Bed, p. 105– 118, Halifax, Canada (1985)

Squires, A. M., “Applications of Fluidized Beds in Coal Technology,” lecture, Intern. School on Heat and Mass Transfer Problems in Future Energy Production, Dubrovnik, Yugoslavia (1975a)

Squires, A. M., “Gasification of Coal in High-Velocity Fluidized Beds,” loc. cit. (1975b)

Squires, A. M., “The City College Clean Fuels Institute:” Programs for (i) Gasification of Coal in High-Velocity Fluidized Beds; (ii) Hot Gas Cleaning,

Symp. Clean Fuels from Coal, I.G.T., Chicago (1975c)

Squires, A. M., The Story of Fluid Catalytic Cracking: “The First Circulating Fluid Bed,” Proc. First Intern. Conf. Circulating Fluidized Bed, p. 1–19 (1985)

Treybal, R. E., Mass Transfer Operations, McGraw-Hill, 1st Ed. (1955); 2nd Ed. (1968); 3rd Ed. (1980)

Tung, Y., and Kwauk, M., Dynamics of Collapsing Fluidized Beds, China-Jpn. Fluidization Symp ., Hangzhou, China (1982), Science Press, Beijing, and Gordon Breach, New York, p. 155–166

Tung, Y., Li, J., Zhang, J., and Kwauk, M., “Preliminary Experiments on Radial Voidage Distribution in Fast Fluidization,” Fourth Nat. Conf. Fluidization, Lanzhou, China (1987)

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581

Tung, Y., Li, J., and Kwauk, M., “Radial Voidage Profiles in a Fast Fluidized Bed,”

Proc. of Third China-Jpn. Symp. on Fluidization, p. 139, Beijing, China (1988)

Tung, Y., Yang, Z., Xia, Y., Zheng, W., Yang, Y., and Kwauk, M., “Assessing Fluidizing Characteristics of Powders,” Sixth Int. Fluidization Conf., Banff, Canada (1989)

Tunstall, E. B., and Houghton, G., “Retardation of Falling Spheres by Hydrodynamic Oscillation,” Chem. Eng. Sci,. 23:1067–1081 (1968)

Van Oeveren, R. M., and Houghton, G., “Levitation and Countergravity Motion of Spheres by Nonuniform Hydrodynamic Oscillation,” Chem. Eng. Sci., 26:1958–1961 (1971)

Wang, N., Li, Y., Zheng, X., and Kwauk, M., “Voidage Profiling for Fast Fluidization,” First Intern. Conf. Circulating Fluidized Beds, Halifax, Canada (1985)

Wilhelm, R. H., and Kwauk, M., “Fluidization of Solid Particles,” Chem. Eng. Prog., 44:201–218 (1948)

Yan, Z., Yao, J., and Liu, S., “Turbulence in Grid Zone of Fluidized Reactor,”

Proc. China-Jpn. Fluidization Symp., Hangzhou, China, p. 100–111 (1982)

Yan, Z., Yao, J. Z., Wang, W. L., Liu, S. J., and Kwauk, M., “Cocurrent Shallow Multistage Fluid-Bed Reactor,” Third Intern. Conf. Fluidization , Kashikojima, Japan, p. 607–614 (1983)

Yang, Z., Tung, Y., and Kwauk, M., “Characterizing Fluidization by the Bed Collapsing Method,” Chem. Eng. Commun., 39:217–232 (1985)

9

Industrial Applications

of Three-Phase

Fluidization Systems

Jack Reese, Ellen M. Silva, Shang-Tian Yang,

and Liang-Shih Fan

1.0INTRODUCTION

Three-phase fluidization systems offer the flexibility of a wide range of operation conditions and contacting modes and are finding increased industrial applications in reacting and physical processing schemes. This is primarily due to the increased use of three-phase fluidization systems in the rapidly growing biotechnology field, but application in other areas abound as well. Successful application of three-phase fluidization systems lies in the comprehensive understanding of the complex transport phenomena mechanisms and associated reaction parameters. For the past 30 years, large research efforts have been put forth to characterize and predict the complex behavior of three-phase systems; however, a complete understanding and the ability to reliably scale up three-phase fluidization systems have yet to be achieved.

582

Three-Phase Fluidization Systems 583

The term three-phase fluidization, in this chapter, is taken as a system consisting of a gas, liquid, and solid phase, wherein the solid phase is in a non-stationary state, and includes three-phase slurry bubble columns, three-phase fluidized beds, and three-phase flotation columns, but excludes three-phase fixed bed systems. The individual phases in threephase fluidization systems can be reactants, products, catalysts, or inert. For example, in the hydrotreating of light gas oils, the solid phase is catalyst, and the liquid and gas phases are either reactants or products; in the bleaching of paper pulp, the solid phase is both reactant and product, and the gas phase is a reactant while the liquid phase is inert; in anaerobic fermentation, the gas phase results from the biological activity, the liquid phase is product, and the solid is either a biological carrier or the microorganism itself.

The important inherent differences in the operating characteristics between fixed bed systems and fluidization systems as given by Fan (1989) are summarized here. Fixed bed systems produce high reactant conversions for reaction kinetics favoring plug flow patterns because of the small axial dispersion of phases and low macromixing present in such reactors. Fixed bed systems offer the advantage of high controllability over product selectivity for complex reactions and low solids attrition and consumption, permitting the use of precious metals as catalysts. In fluidization systems, high macromixing with large axial dispersion is prevalent which produces high reactant conversions for reaction kinetics favoring completely mixed flow patterns. The high mixing in fluidization systems also yields uniformity in the temperature throughout the system and ease in temperature control. The non-stationary nature of the particles in a fluidization system allow for ease in continuous catalyst replacement and, hence, minimum flow maldistribution.

Fan (1989) provided a detailed historical development of threephase fluidization systems in reactor applications. Only a brief review of the significant accomplishments and the economic factors affecting the development of three-phase reactors will be provided here. Table 1 provides the important contributions in the application of three-phase fluidization systems for the past several decades. The direct liquefaction of coal to produce liquid fuels was the first commercial reactor application of three-phase fluidization systems, with development having occurred from the mid-1920’s throughout the 1940’s. A large effort was put forth at this time in Europe for the production of liquid fuels from coal as a direct

584 Fluidization, Solids Handling, and Processing

result of the need for such fuels during World War I and II. The commercial production of liquid fuels from direct coal liquefaction peaked at an average annual production of 4.2 million tons of primarily aviation fuel (Donath, 1963). At the end of the war, the direct production of liquid fuels from coal was phased out. Another important process which was developed during and prior to the 1940’s is the application of a three-phase reactor for the reactions known as Fischer-Tropsch (F-T) synthesis. These reactions produce liquid fuels via indirect coal liquefaction involving hydrogen and synthesis gas derived from coal gasification, in the presence of a catalyst. The peak production for the liquid phase F-T synthesis occurred in the early 1950’s at a daily production rate of 11.5 tons of liquid fuels (Kolbel and Ralek, 1980). Fischer-Tropsch synthesis ceased in the mid-1960’s because of the availability of relatively cheap crude oil. However, renewed interest in F-T synthesis in the early 1970’s, caused by the oil shortages of the time, lead to further studies in the commercial scale production of liquid fuels via F-T synthesis in slurry bubble column reactors. This development has continued throughout the 1980’s and into the 1990’s.

Table 1. Industrial Development and Application of Three-Phase

Fluidization Systems

 

 

Decade

Application

 

 

1940's

Coal liquefaction, Fischer-Tropsch synthesis

1950's

Catalytic synthesis of chemicals

1960's

Hydrotreatment of petroleum resids

1970's

Environmental applications

1980's

Biotechnology application

1990's

Biotechnology / Chemical synthesis

 

 

 

 

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