HYDROCYCLONE

Abstract: A cyclone separator or hydrocyclone with good separation efficiency and large capacity comprises a substantially cyclindrical or slightly conical hollow body (1), the lower part of which terminates in an outlet opening (6) for liquid enriched with respect to solid particles, and in which the outlet (7) for purified liquid is defined between a centrally arranged body (11) and a guiding tube (2), and in which the liquid to be purified is introduced via a particularly designed nozzle (13).

Description: Hydrocyclone The present invention relates to a cyclone separator, preferably of the type being used -for separation of solid particles from a liquid medium. Such separators are often termed hydrocyclones. A short account of hydrocyclones is inter alia given in "Encyclopedia of Chemical Technology", 2nd. edition, volume 4 (pp 747 - 748) . Theoretically, a free vortex will exist in such a cyclone, resulting in large shear forces being developed in the sedimentation zone, hence such cyclones are not well suited for separation of flocculated matters or solid particles which easily are broken up. However, such cyclones are well suited for removal of fine particles at low or medium concentrations. Due to the shear forces existing in the vortex in a hydrocyclone, it is not only the centrifugal force which causes sepa¬ ration, but the form of the particles exert a certain effect. Hydrocyclones have hence been used in the wood pulp industry to cause a certain separation of fibres of different lengths. Normally, a hydrocyclone comprises a rotational-sym¬ metrical, elongated hollow body which under operation is arranged vertically, and the upper part of which is provided with at least one tangential inlet through which the liquid to be treated at high velocity is in¬ troduced, causing the formation of a vortex in the hydro¬ cyclone. In the upper part of the hydrocyclone a central opening exists, the cross-sectional area of which is larger .than the total cross-sectional area of the inlet open- Liricrs. Through the upper outlet opening the injected O PI liquid is fully or partly devoid of solid particles. In the lowest part of the hydrocyclone there is provided a central outlet opening, the cross-sectional area of which is less than the cross-sectional area of the inlet open¬ ing, which outlet opening serves as an outlet for a minor part of the injected liquid being enriched with respect to the solid matter. The rotational-symmetrical hollow body can be designed approximately conical along its entire length, as shown in US-PS No. 2 920 761, or be designed with a cylindrical upper part and with a conical lower part, as shown in NO-PS No. 144 128. In order to adapt hydrocyclones to different purposes, and in order to improve their effi¬ ciency, several modifications of hydrocyclones have been proposed, for instance with respect to the inlet for the liquid to be treated, as shown in the above-mentioned Norwegian patent, or by modifying the ourlet for the liquid portion enriched with solid matter, as shown in US-PS No. 4 309 238. Special designs of the outlet for the accept liquid are shown in US-PS No. 4 259 180 and FR-PS 1 518 253. Different variants of hydrocyclones are mentioned in the US-PS Nos. 4 265 470, 4 280 902, 4 305 825 and 4 267 048 as well as in US-PS No. 4 272 260, referring to a cyclone for separation of solid particles from gases. Common features of known cyclone separators and hydrocyclones, as described in the above-mentioned pat¬ ents, are that the outlet for the accept liquid consists of a central tube, the outlet opening of which normally being positioned below the level of the injected liquid. In order that the liquid shall be able to flow through the central outlet as an overflow, a substantial part of the volume of the cyclone will be occupied by rot¬ ating liquid layers. Due to the turning tendency at the OMPI lower conical inner wall of the hydrocyclone, turbul¬ ence will occur in the rotating liquid body disturbing the flow pattern, in turn resulting in decreased efficiency. Due to the central outlet of rotating liquid, a substan- tial part of the supplied kinetic energy will be lost as a consequence of friction losses. This because the leaving overflow only can have a rotational energy corre¬ sponding to the rotational velocity and the cross-section of inertia of the overflow. The angular velocity of the central overflow cannot be greater than in the remaining part of the cyclone, as the liquid would be exchanged with the liquid in sur¬ rounding layers, and hence cause a large secondary flow. Thus, said secondary flow is also one of the major defi¬ ciencies of prior art cyclones with a central outlet. Another deficiency of prior art cyclones consists in one or more tubular, elongated inlets with gradually reduced cross-sectional area. As the liquid velocity in said inlets will be high by optimum utilization of the cyclone, the pressure drop across the inlet will be high, due to friction against the wall in the inlet ducts. The pressure drop across the inlet and also the pressure drop across the cyclone will increase substantially with increasing viscosity. This energy loss reduces the rotational velocity and thereby the separating efficiency of the cyclone in re¬ spect to the inlet pressure. At high inlet velocity, the inlet diameter must be reduced, and for viscous liquids this can result in substantial losses. Cyclones with only one inlet will result in an uneven flow in the cyclone, a phenomenon being known from SF-PS 75 3027, in which long, curved inlet ducts with a tapered cross- section are shown. From another prior art, in which high liquid pressure energy is converted into kinetic energy with a minimum _QM?I loss, for instance in Pelton turbines, an entirely dif¬ ferent construction of the nozzle is used. Such techni¬ que is also known from drilling mud nozzles in drill heads used in drilling for oil, as such short nozzles give the optimum efficiency. The present cyclone separator or hydrocyclone differs inter alia from the prior art in that the inlets are designed with a short nozzle, the bore of which is less than the bore in front of and behind the nozzle. In this respect the invention is illustrated in Figs. 4 and 5 in the appended drawings. The nozzle 13 can. be made from a different and substanti¬ ally more wear resistant material, for instance hard metal, than the remaining part of the cyclone, thereby reducing the wear even at high velocities and a large number of particles in the inlet. In order to obtain an optimum inlet duct, the thickness D of the nozzle 13 must not exceed the diameter A in this section. The radius of curvature E of the nozzle 13 must not exceed 0,75 x A, and be less than 1,5 x A. The bore of the channel 5 in front of the nozzle 13 must have a section with a diameter C larger than 2 x A, and the bore of the channel 21 behind the nozzle, leading into the cyclone, must have a diameter B of at least 1,35 x A in order that a liquid layer shall not be formed in the channel behind the nozzle before the liquid jet has rea¬ ched the vortex forming chamber 4. The short nozzle 13 will result in a parallel directed jet of a diameter less than the diameter of the subsequent channel 21, hence friction against the wall in the channel 21 is avoided. The differential pressure across the hydrocyclone will thus be less viscosity dependent than for known cyclones. By adjusting the diameter A of the nozzle 13, the capa¬ city and the rate of separation for the cyclone may be adjusted simply by replacing the nozzles in the same OMPI manner as the capacity of a pump may be adjusted by al¬ tering the diameter of the impeller. Between the guiding tube 2 and the inner part 14 of the cylindrical body 1, a vortex forming chamber 4 is formed, into which the inlets for the liquids to be purified are introduced via the nozzles 13, as shown in Fig. 4. As apparent from Fig. 4, the inlets are tangentially directed in respect to the inner wall 14 of the cylindri- cal body 1, such that the introduced liquids is forced to rotation in the chamber 4, whereas the purified or accept liquid is discharged via the annular chamber 7 to the conical chamber 12, and further via the conical portion 10 and the rotation preventing portion 3. In using the hydrocyclone according to the invention, the liquid to be treated is pressure injected through the inlet nozzles 13, being made from a wear resistant material. Preferably the nozzles 13 are directed with a sloping angle such that the jets are lined side by side along the circumference. The introduced liquid is brought to a vigorous rotation in the chamber 4 and forms a downward cylindrically rotating layer 17 in contact with the inner wall 14. The liquid flows down along said wall until the rota¬ ting liquid is forced into the more conical portion 15, in which the liquid in the usual manner reverts and rotates upwards in a cylindrical layer 16, as indi¬ cated with arrows, and out via the annular chamber 7. The outer portion of the guiding tube 2 will, when the downward cylindrically rotating layer leaves the vortex forming chamber 4, smooth the surface of the rotating layer. In order that the outer wall 8 of the guiding tube 2 contributes as little as possible to the friction in the liquid and vortex formation, the guiding tube 2 is conically designed with a conicity of minimum 4 and maximum 10°. A part of the liquid OMPI 23 being enriched with respect to solids will be slowed down against the inner wall 14, and hence does not pos¬ sess sufficient rotational energy to be recarried upwards in the cyclone, and will consequently be carried against the apex of the cyclone and discharged via the outlet 6. The elongated part 1 of the cyclone separator has over a major part of its length a conicity which, with respect to the rotational velocity, only compensates for frictional loss against the inner wall 14. As mentioned, the lower part of the cyclone separator has a conical form 15 with a conicity such that invertion is effected, and the ro¬ tating liquid is carried upwards as a layer 16 within the layer 17 moving downwards in the direction of the outlet 7. It is within this part of the path through the separator that the separation mainly takes place, as in this region an absolute minimum of flow disturbance exists because the downward moving layer 17 rotates in the same dir¬ ection and with the same velocity, and because an cylin¬ drical air column 24 constitutes the surface of the layer 16. Said air column 24 is kept centrally in place in the cyclone of a parabolic shaped center stem 11 in order that the thickness of the layer 16 and hence the sedimentation distance shall be at a minimum. In common cyclones with a liquid filled center there will exist a liquid connection with small gravitational forces be¬ tween the reject and accept, and a "leakage" of particles from the reject to the accept will take place. This phenomenon is prevented by said air column 24. The centrally arranged center stem 11 must have a para¬ bolic form in order that the liquid in the center of the cyclone during the starting up of the same shall dis¬ appear from the central portion during the building-up of the air column 24. If the body 11 is of a different shape, a part of the liquid in " the center of the cyclone -flow¬ ing, in the direction of the overflow, will flow back to "BTJ £ the central portion of the cyclone and be mixed with gas in said portion, such that the building-up of the stable air column 24 centrally in the cyclone will not take place, The length of the substantially cylindrical part 1 is determined by the desired residence time in said part of the flow path, since in this part a minimum flow distur¬ bance will occur. In the outlet section 25 the purified rotating liquid is at first introduced into a section 12 with a cross-section giving minor alternations in the axial velocity, and thereafter into a section with incre¬ asing cross-sectional area 10, in which both the axial velocity and the rotational velocity are reduced and the remaining kinetic energy is converted into pressure energy. Finally, the purified liquid is introduced into a section with a rotation preventing device 3, in which the cross- section 10 is further increased. The flow of purified liquid will be axially directed and attain a reduced absolute velocity. The kinetic energy thus will be converted into pressure energy, which efficiently may be utilized for further transport of the purified liquid. In order to obtain the best possible results, the ratio between the diameters of the ascending layer 16, the descending layer 17 and the air column 24 must lie within well-defined values. Said values are not common for cyclones with several inlets. In practice this means that: 0,72D_^sD 2 ^-0,83 D-,. In order to obtain equilibrium between the ascending and the descending layers, optimum particle separation and recover as much energy as possible, the diameter of the paraboloid 11 must be: 0,4 D 3 ^D 1 ≤0,6 D 3 , OMPI and the focal length a, of the paraboloid 11 must be : 0 , 06 D, «Ξ a, ~S;0 , l D, . These ratios are not previously used or known from prior cyclones. As shown in Fig. 6, the guiding tube 2 is tapered with a lower sharp edge 20 with an angle in order not to form whirling at the outlet. The angle of said tapering must be 25 ^£ jS35 , and the thickness must be ,02 D 3 ^e^0,04 D 3 , Tn relation to prior art hydrocyclones, a smaller pres¬ sure drop over the cyclone is obtained, and it is equ¬ ally effective at large absolute pressures, such that for several purposes no auxiliary pumps are necessary for an optional subsequent treatment of the purified liquid. Tests have shown that, compared with conventional hydro¬ cyclones, the present hydrocyclone, under equal condi¬ tions, will remove particles of a size down to 2 - 3 um, whereas conventional hydrocyclones will separate partic¬ les down to 7 - 8 um by equal cyclone diameter and pressure drop. However, the flow through the present cyclone will be twice that of a conventional cyclone with the same inlet diameter and the same internal dia¬ meter. In total, the present cyclone exhibits substantially improved properties. Enclosed performance data for part¬ icles in sea water are shown. The number if particles in the shown ranges was deter¬ mined by means of a "Coulter Counter TAII" before and after a cyclone of the present invention, with a dia¬ meter of approximately 7,6 cm. The capacity of the cyclone was 150 1/min with a pres- sure drop of 2,1 bar. 10 Coulter Counter TAII Liquid: Sea water Place: NUTEC, Bergen Before After cyclone cyclone Efficiency % Particle Number of Number of Percentage Accumulated diameter particles particles of particles percentage per ml per ml removed greater than 1.0-1.25 22436 17072 23.9 75.4 1.25-1.6 10578 8095 23.5 76.7 1.6-2.0 6268 4357 30.5 78.1 2.0-2.5 4651 2971 36.1 79.5 2.5-3.2 2765 1529 44.7 81.6 3.2-4.0 1727 759 56.1 83.8 4.0-5.1 1084 299 72.4 86.0 5.1-6.4 707 107 84.9 87.6 6.4-8.0 423 58 86.3 88.1 8.0-10.1 233 26 88.8 88.6 10.1-12.7 100 9 91.0 88.5 12.7-16.0 39 6 84.6 87.1 16.0-20.2 19 3 81.2 88.8 20.2-25.2 2 0 100.0 100.0 25.2-32 1 0 100.0 100.0 5 ! ■ -: - ■ -

Claims: C l a i s: 1. Cyclone separator or hydrocyclone for separation of solid particles from a liquid comprising a substantially cylindrical or slightly conical hollow body (1) , the lower part of which, at least internally, is conically tapered and terminates in an opening (6) for discharge of liquid enriched with respect to solid particles, and wherein the upper end of the hollow body (1) is provided with at least one inlet opening (5) and an annular outlet (7) for purified liquid, c h a r a c t e r i z e d in that the inlet (5) is provided with a short nozzle (13) , and where the diameter of the inlet in front of the nozzle (13) has a bore larger or equal to two times the bore (A) of the nozzle (13) , and in which the diameter (B) of the channel behind the nozzle (13) has a diameter of at least 1,3 times the bore (A) of the nozzle (13) , and that the length (D) of the nozzle is not larger than the diameter (A) of the nozzle, and that the radius of curvature (E) of the nozzle is less than 1,5 times and larger than 0,75 times the diameter (A) of the nozzle (13) , and that the annular outlet (7) is defined between a centrally arranged body (11) and an annular guiding tube (2) having an external diameter (D 2 ) , which in respect to the inner diameter (D-.) of the cyclone is in the range 0,72 (D 3 ) and 0,83 (D- . 2. Hydrocyclone according to claim 1, c h a r a c t e r- i z e d in that the centrally arranged body (11) has the form of a paraboloid with a diameter (D, ) , which in respect to the inner diameter (D ) of the cyclone is in the range 0,4 (D 3 ) and 0,6 (D- . 3. Hydrocyclone according to claim 2, c h a r a c t e r¬ i z e d in that the body (11) has a focal distance which i. is greater than 0,06 (D,) and less than 0,1 (D, ) . 4. Hydrocyclone according to the claims 1 - 3, -£U T £ OMPI c h a r a c t e r i z e d in that the annular guiding tube (2) is conically shaped with the larger diameter within the cyclone and with a conicity in the range 4° - 10°. 5. Hydrocyclone according to the claims 1 . - 4, c h a r a c t e r i z e d in that the annular guiding tube (2) is designed with a lower sharp edge (20) in which the angle ct» is in the range 25 - 35 . 6. Hydrocyclone according to the claims 1 - 5, c h a r a c t e r i z e d in that the tube (2) has a wall thickness in the range 0,02 (D ) and 0,04 (D_) . "gJ l

Inventors: FLADBY TRON-HALVARD, HOVIND LEIF, FLADBY, TRON-HALVARD, HOVIND, LEIF
Applicants: ANDRESEN J H TITECH, TITECH, JOH., H., ANDRESEN
Application year: 1984
Main classification: B04C5
IPC codes: B04C5, D21D5