The present invention relates to a device for injecting a fluid or mixture of fluids, liquid or gaseous, into a rotating fluidized bed, for increasing the momentum and energy that the fluid can transfer to the solid particles rotating in a rotating fluidized bed in order to increase their speed of rotation.
Methods in which solid particles are in suspension in a fluid and thereby form a fluidized bed through which this fluid passes, are well known. When the fluid is injected tangentially to the cylindrical wall of a cylindrical reactor, it can transfer part of its kinetic energy to the solid particles to make them rotate, and if the energy transfered is sufficient, this rotational movement produces a centrifugal force which can maintain the fluidized bed along the cylindrical wall of the reactor, thereby forming a rotating fluidized bed, whereof the surface is approximately an inverted truncated cone, if the cylindrical reactor is vertical. Such a method is the subject of Belgian patent application No. 2004/0186, filed 14 Apr. 2004, in the name of the same inventor.
However, when a fluid jet is injected at high speed into a large reactor, it is rapidly slowed down by its expansion in the reactor, thereby limiting its ability to transfer a significant momentum to the solid particles. This is why, unless other mechanical means are used to rotate the fluidized bed, it is necessary to have a very high fluid flow rate to transfer to the solid particles the momentum necessary to maintain a sufficient speed of rotation to maintain them along the cylindrical wall of the reactor, and if the fluid density is much lower than the density of the particles, the devices for centrally removing these fluids may become very bulky.
The present invention, to improve the efficiency of transfer of momentum and kinetic energy between a fluid jet and solid particles in suspension in a rotating fluidized bed, comprises deflectors, inside the rotating fluidized bed, appropriately profiled and arranged close to the fluid injectors, for the mixing of the injected fluid with a limited quantity of solid particles, while channeling it, in order to prevent or reduce its expansion in the reactor before it has transferred a substantial quantity of its kinetic energy to the solid particles. This device is suitable for using fluids that are much lighter than the solid particles, and for injecting a fluid at high speed into the reactor without losing a large part of its kinetic energy on account of its expansion in the reactor. An application of this application is described in a Belgian patent application, in the name of the same inventor, filed on the same day as the present application.
The present invention may also apply to a horizontal reactor. In this case, the speed of injection of the fluid into the reactor, its flow rate and the efficiency of transfer of its kinetic energy, must be sufficient to impart a speed of rotation to the fluidized bed producing a sufficient centrifugal force to maintain it against the cylindrical wall of the upper part of the reactor.
These side deflectors, together with the injectors, bound access passages or corridors of width (7), through which streams (8) of solid particles in suspension in the rotating fluidized bed can enter these spaces (6) and mix with the fluid jets (4). The convergence or divergence limited by the deflectors in the first part of these spaces (6) prevents or limits the expansion of the fluid jets, whereof the pressure may decrease to preserve a substantial part of their speed while they accelerate the streams (8) of solid particles. The fluid streams (9) then slow down in the divergent part of these spaces or corridors (6) and their pressure can rise to reach the reactor pressure. Due to inertia, the solid particles slow down less and may have a tangential outlet speed close to or even higher than that of the fluids which will therefore have yielded to them a large part of their kinetic energy.
If the length of the space (6) and its minimum cross section (10) are such that the injected fluids can yield such a large part of their energy to the solid particles that their speed at the outlet of said space may decrease excessively, the injection pressure and hence their energy must increase to enable the fluids to escape via the outlet (11), despite the considerable slowdown caused by the solid particles. This pressure increase is transferred into the access passages or corridors (7) and decreases the inlet speed therein of the solid particles, whereof the concentration increases and whereof the flow rate decreases, accordingly decreasing the quantity of energy that they can absorb, in order to obtain an equilibrium of energy transfer depending on the dimensions of these spaces (6), and the speeds and densities of the solid particles and of the fluids. To avoid this slowdown of the solid particles in the access passages or corridors (7), the length of these spaces (6) must be shorter insofar as the ratios of the width (3) or cross section of the injectors to the width (7) or cross section of the access passages are low, so that the fluids still have a speed substantially higher than that of the particles at the outlet (11). In contrast, the quantity of energy transferred to the solid particles will be greater if these ratios of cross sections are lower and if the length of these spaces (6) is higher, the optimum depending on the operating conditions and objectives.
Simplified calculations show that these dimensions allow for wide variations in the operating conditions enabling the fluids to yield at least three-quarters of their kinetic energy, in order to obtain a sufficient transfer of momentum to the solid particles by very light fluids, without excessively increasing their flow rate, by injecting these fluids at high speed.
The figure also shows the cross section (11) of the surface of the rotating fluidized bed, the solid particles symbolized by small arrows (12) indicating their travel direction, the cross section of central deflectors (13), bounding longitudinal slits for centrally sucking out the fluids (14) to remove them from the reactor, the curvature (15) of these central deflectors ensuring the separation between the solid particles and the fluid before its removal.
The injectors are separated by transversal rings or fractions of rings (20) running along the side wall (1) of the reactor and the side deflectors (19) are inserted between these rings, leaving an access corridor for the streams of solid particles, symbolized by the black arrows (21). These rings or fractions of rings may be transversal fins or helical turns oriented in order to make the solid particles rise along the side wall of the reactor. They may also be hollow and serve as a fluid distributor to the injectors connected thereto.
The transfers of energy and momentum between fluids and solid particles strongly depend on the type and size of the particles. However, simplified calculations show, as an indicative example, that for solid particles with a density 700 times higher than the fluid density, with a ratio of the cross section of the access corridors (7) to the injectors of 3 to 4 and an outlet (11) cross section equal to or greater than the sum of the cross sections of the access corridors and the injectors, the fluids can be injected at a speed 5 to 15 times higher than the average speed of rotation of the solid particles, and transfer at least 75% of their kinetic energy to said particles, if the space (5) is sufficiently long with regard to the size of the particles.
Number | Date | Country | Kind |
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2004/0613 | Dec 2004 | BE | national |
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/EP05/56640 | 12/9/2005 | WO | 00 | 3/25/2008 |