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Yang Fluidization, Solids Handling, and Processing

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point to the middle section of a three-section reducer. A considerable amount of CO is generated between reaction of C and FeO, which fluidizes the two top sections by continuous flow. Division into the two fluidized sections helps the establishment of a solids concentration gradient (dilute in the top section, and dense in the lower section) which tends to suppress longitudinal mixing. Only the lowest of the three-section reducer is semifluidized through jigging, in which only the last traces of CO are evolved.

All the CO resulting from the pseudo solid-solid reaction is conducted, together with entrained char, from the top fluidized section through a constriction, in which the high-velocity gas flow prevents backflow, to a transport combustor, where the CO is burned to CO2 with preheated air, along with as much of the char as is called for by heat balance to maintain the endothermic FeO-C reaction. The heated recycled char is separated from the off gas at the top of this transport combustor in a hot cyclone and is returned as a thermal carrier to the lower part of the lowest jigged section, while the hot flue gas from the transport combustor is used to preheat the incoming air in a recuperator.

In the top fluidized section, where the first portion of FeO reduction, that is, prereduction, takes place, the lighter coke particles are elutriated from the heavier ore particles. The lower fluidized section is sized for adequate FeO-C mixing in order to maximize contacting of the reacting solids. Then, in the lowest section, where vestigial amounts of CO are evolved, solids are semi-fluidized through jigging to effect an additional stage of coke upflow in order to denude the powdered metallic iron product of its accompanying char.

Jigging is produced by a gas oscillation generator, which could be either mechanical or electromagnetic, separated from the bottom of the jigged section first by a solids knockout hopper and then by a thermal break, which is essentially a packed-bed heat regenerator. To protect further the gas oscillation generator from hot gases, a cooler is interposed between it and the thermal break.

The process proposed in Fig. 42 uses powdered iron ore directly without prior treatment such as sintering or pelletization as called for in the case of the blast furnace, and powdered coke or coal without prior gasification. Jigging through gas oscillation replaces expensive gas recycling which calls for first cooling and then reheating, often accompanied by unavoidable carbon deposition through the Bouduord reaction.

556 Fluidization, Solids Handling, and Processing

8.0PARTICLES WHICH QUALIFY FOR BUBBLELESS OPERATION

Whether or not a solid powder qualifies for bubbleless gas/solid contacting depends greatly on its fluidizing characteristics, which may be determined in a bed collapsing apparatus which automatically tracks the subsiding bed surface of the collapsing bed by means of an optical-fiber probe (Qin and Liu, 1985). Modeling of the collapsing process (Tung and Kwauk, 1982; Yang, Tung and Kwauk, 1985; Tung, Yang, Xia, Zheng, Yang and Kwauk, 1989) resulted in a dimensionless number to quantify the fluidizing characteristics of powders. Certain binary and ternary solid mixtures have been shown to demonstrate synergistic actions in improving the fluidization characteristics of the component particles, implying the significance of particle size design.

8.1Powder Characterization

Broadly speaking, for G/S systems, three modes of particle-fluid contacting may be recognized to take place simultaneously as shown in Fig. 43: bubbles containing sparsely disseminated particles, emulsion of densely suspended particles, and defluidized (transient as well as persistent) particles not fully suspended hydrodynamically by the flowing gas. For all intents and purposes, it is desirable to suppress bubbles and to prevent defluidization.

When the gas, which is fluidizing a powder exhibiting all these modes of contacting, is turned off abruptly, the fluidized bed will collapse and subside in three consecutive stages, as shown in Fig. 44 (Yang, Tung and Kwauk, 1985):

(i)A rapid initial stage for bubble escape

(ii)An intermediate stage of hindered sedimentation with constant velocity of the dense emulsion of mobile particles, and

(iii)A final decelerating stage of solids consolidation for the incompletely suspended particles.

Thus, the random spatial distribution of the three modes of particlefluid contacting is transformed into the ordered, temporal sequence of the three stages of the sedigraph.

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Figure 45 shows the instrument used for automatic tracking of the surface of the collapsing bed, inclusive of a computer for data acquisition and on-line analysis. The fluidized bed, 5 cm in diameter and 120 cm high, is provided with a high pressure-drop gas distributor to insure uniform gas flow. Below the distributor is a specially designed knife valve operated by a solenoid for quick gas shufoff. An optical-fiber probe, consisting of two separate sets of projector and receiver fibers, respectively, for illumination and for reception of reflected light, is used for rapid tracking and recording of the subsiding bed surface.

Figure 46 shows a typical bed collapsing curve traced by the instrument described above.

The entire determination, from gas shutoff to printout from the computer, rarely exceeds 3 to 4 minutes for normal solids. And since all measurements are taken by the instrument, they are not subject to personal error of observation. The size of solids test sample is of the order of a kilogram or less.

Figure 43. The three modes of particle-fluid contacting in G\S fluidization.

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Figure 45. Instrument for automatic surface tracking and data processing. (Yang, Tung, and Kwauk, 1985.)

560 Fluidization, Solids Handling, and Processing

Figure 46. Typical bed collapse curve traced by optical-fiber probe tracking instrument (solids:alumina A66, 140–280 microns). (Yang, Tung, and Kwauk, 1985.)

Not all powders exhibit all the three stages described above, as shown in Fig. 47. Depending on the presence or absence of the above stages, a three-digit qualitative designation has been formulated:

100 Bubble-escape stage only

123Three stages: bubble escape, hindered sedimentation and solids consolidation

020 Hindered sedimentation only

023 Hindered sedimentation plus solids consolidation

Bubbleless Fluidization

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562 Fluidization, Solids Handling, and Processing

Mathematical modeling of the three-stage bed collapsing process led to a more quantitative characterization of powders, in the form of a dimensionless number called the dimensionless subsidence time:

 

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To test the viability of Θ in quantifying fluidizing characteristics, it is plotted against the ratio of incipient bubbling velocity to incipient fluidization velocity, umb/umf, the latter being calculated after Geldart (1972). Figure 48 shows that a linear relation exists between ln(umb/umf) and θ¼ as represented by the following empirical relation

ln(umb /umf) = 4 Θ¼

The straight line starts from Θ = 0 and umb /umf = 1, and extends without limit towards the upper right-hand corner. The value of umb /umf = 1 obviously signifies bubbling. The corresponding value of Θ is zero, for which stages 1 and 2 of the bed collapsing process take place almost instantaneously. As the fluidizing characteristics improve, the value of umb/umf becomes progressively greater than unity, signifying particulate expansion. The corresponding value of Θ also increases, showing a slower bed collapsing process. As the curve tends toward even larger values of Θ, the characteristics of particulate fluidization becomes more predominant.

8.2Improving Fluidization by Particle Size Adjustment

Catalyst powders with carefully specified particle size distribution have been known to possess good fluidization characteristics. Generally, addition of fine particles to coarse particles tends to improve the latter’s fluidization characteristics. Experiments were thus conducted on binary particle mixtures, each consisting of a fairly close particle size distribution.

Figure 49 shows a set of bed collapsing curves for a Geldart Group A- A (for Geldart’s classification of solid particles, see Geldart, 1972, 1973) binary solids mixture, two closely sized alumina powders, of average particle diameter 104 and 66 microns, respectively. The curve on the extreme left with 0% fines represents the pure coarse component, which is

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barely Group A in fluidizing characteristics, as can be seen from its very brief stage 2. The curve on the extreme right, representing the 100% fine component, demonstrates pronounced Group A, or “123,” fluidizing characteristics with a long stage 2. Curves with intermediate compositions are shown in their ordered locations between the purely coarse and purely fine components.

Figure 48. Plot: umb/umf versus Θ¼. (Yang, Tung, and Kwauk, 1985.)

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