• 专利附录
  • 专利说明
  • 权利要求
  • 类似技术
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    • 专利摘要:
    The present invention refers to a device for generating vortices in channels or conduits that allows the exploitation of the wingtip vortex that is formed in the aerodynamic profiles as a consequence of having a finite span. These aerodynamic profiles consist of one or two marginal edges from which the wingtip vortex detaches, causing an oscillatory movement to occur that subjects the particles traveling with the current to an up-down cycle. For this reason, the present invention has as a fundamental advantage that transverse speeds to the main current are produced, without hardly introducing pressure drops. (Machine-translation by Google Translate, not legally binding)
    公开号:ES2767024A1
    申请号:ES201831212
    申请日:2018-12-14
    公开日:2020-06-15
    发明作者:Martín Javier Dávila；Morales Alonso Fernández
    申请人:Universidad de Sevilla；
    IPC主号:
    专利说明:

    [0004] OBJECT OF THE INVENTION
    [0006] The present invention relates to a vortex generating device in channels or conduits that allows stable vortices to be generated along channels or conduits by using spindle bodies, so that the vortex produced has its axis of rotation parallel to the direction of the current. The device object of the present invention is applicable in fields where it is important to achieve an efficient agitation of fluids with the minimum energy consumption. In particular, it is applicable in organic crop growth processes in which the energy consumption necessary for the agitation of the crop represents one of the main operating costs, while its productivity is limited by the mixing capacity.
    [0008] BACKGROUND OF THE INVENTION
    [0010] Different in-line mixing systems are known in the state of the art, such as so-called static mixers, which incorporate different designs of solid elements, usually inside a duct. These elements produce a good mix of the flow due to a strong increase in the turbulent intensity, that is, the level of speed fluctuations with respect to the average speed of the flow. However, existing static mixers produce a high head loss (back pressure drop) in relation to the kinetic energy of the flow. Examples of static mixers are set out in the following patent documents: EP2433706, WO2010039162, CN202893218 and JPS5919524.
    [0012] Some static mixers are based on thin plates, but their behavior is very different from that of an aerodynamic profile, since either the angle of attack is very high (which produces the detachment of its boundary layer) or they are anchored by the edge leading or trailing edge to any of the duct walls, such as those described in patent applications with publication number US2006158961 or WO0062915.
    [0013] Other mixing systems are based on the generation of turbulent fluctuations through shear zones, as in the case of the jets or the mixing layers and can be more efficient than static mixers. Turbulent fluctuations are also generated in the cut zones, which allow the mixing of compounds in solution or of different fluids, as occurs in the device described in patent application US2010163114.
    [0015] In addition to the mentioned designs, there are other mixers in which a rotation current is generated without moving parts that could be called tangential mixers. Examples of this technique appear in patents ZA9802249, JP2012006013 and US2016250606. In these cases, in addition to the rotating current, an increase in turbulence intensity is usually sought. Another technique also based on the generation of twist in which a toroidal vortex is created to mix a region of fluid is described in patent US5823676.
    [0017] On the other hand, there are also other mechanical mixers with moving parts, such as propellers with axes parallel to the axis of the duct, which although they can be much more efficient than those mentioned above, are usually not suitable for use with liquid loaded with particles or in that biological species are cultivated and have high maintenance costs. These mixers can also produce a longitudinal vortex (with its axis parallel to the direction of the duct), with different levels of turbulence depending on whether, in addition to causing the current to rotate, it is also desired to achieve a transverse mixing of the moving fluids.
    [0019] The efficiency of these systems can be characterized by the level of agitation and mixing achieved, divided by the dimensionless coefficient of head loss. Depending on the objective sought, the level of agitation or mixing can be characterized in different ways, such as:
    [0021] a) The reduction in the dispersion of the concentration obtained with respect to the mean.
    [0022] b) The dispersion of the distance of different particles from a reference position, such as the central axis of the duct or the initial position of the particles.
    [0024] On the other hand, the head loss coefficient is defined as the backwater pressure loss, divided by the kinetic energy of the average flow per unit volume. Most of the systems used today for in-line mixing produce a very high head loss, as the resulting flow is very turbulent and with many recirculation zones. Turbulent velocity fluctuations are very effective at mixing fluids, but at the same time they also have significant losses in momentum due to the so-called Reynolds apparent stress tensor. On the other hand, if the intensity of the turbulence is very low, the speed fluctuations are much less effective for the transport of mass, so in this case it is essential that the trajectories of the fluid particles are not parallel to the axis of the duct or channel. One procedure to achieve this is to generate waves on the surface of the channels, so that circular or elliptical trajectories appear that produce an effective agitation of the flow in the area near the free surface.
    [0026] In addition to the aforementioned drawbacks of other agitation and mixing systems, in some installations it is essential to maintain very demanding cleaning conditions, as is often the case with organic crops. In these cases, agitators with essentially flat blades or blades are usually used. This group of agitation systems could include propeller agitators (axial impellers) and the different types of paddle wheels.
    [0028] The channel or conduit vortex generating device of the present invention overcomes all of the above drawbacks.
    [0030] DESCRIPTION OF THE INVENTION
    [0032] The present invention relates to a vortex generating device in channels or conduits that favors the agitation of an essentially parallel current that flows through the conduit or channel that comprises side walls and a bottom or floor, generating wingtip vortices without a substantial increase in intensity of turbulence.
    [0034] The channel or conduit vortex generating device of the present invention is described in the claims, which are included herein by reference. Thus configured, the vortex generating device in channels or ducts comprises at least one flap shaped body or aerodynamic profile, anchored to one of the side walls or to the bottom of the channel or duct by the edge opposite the marginal edge of the fin or aerodynamic profile, or fixed to a first solid structure, which allows the controlled incorporation of intense wingtip vortices into the main flow of the duct or channel.
    [0036] Preferably, the at least one vane or aerodynamic profile is anchored to one of the side walls or to the bottom of the channel or duct by the edge opposite the marginal edge of the vane or aerodynamic profile, or anchored to the first solid structure to the channel or duct , by means of fixing means.
    [0038] The foundation of the vortex generating device in channels or ducts is the use of the wingtip vortex that forms at the marginal edges of the aerodynamic profiles as a consequence of the appearance of areas of greater and lesser relative pressure as they are large fused bodies. finite. In these aerodynamic profiles, the leading edge of the main current is defined as the leading edge and the downstream edge in the direction of the main current is the trailing edge. Aerodynamic profiles consist of one or two marginal edges, which are the lateral edges in the direction of the main current. The aerodynamic profile comprises a single marginal edge if it is attached directly to one of the duct or channel walls or if one of its lateral edges is out of the current.
    [0040] Thus configured, the vortex generating device in channels or conduits causes the wingtip vortex to detach from the marginal edge of a fin or aerodynamic profile and cause the appearance of an oscillatory movement that subjects the particles traveling with the current to an ascending-descending cycle. For this reason, the present invention has as a fundamental advantage that transverse speeds to the main current are produced without hardly introducing pressure losses, instead of from a strong increase in turbulent intensity through any other procedure, as known in the state of the art, which is key for the energy efficiency to be maximized.
    [0042] The channel or conduit vortex generating device of the present invention encourages the wingtip vortex, for which the angle between the fin or airfoil with the incident current should be reduced. In aerodynamics, the angle of attack of a longitudinal section of a body is defined as the angle between the incident current and the reference line of the longitudinal section of the body of the body, which in turn is the line that joins the leading edge with the trailing edge for the same longitudinal section of the fused body and that defines the so-called chord of the longitudinal section of the fused body. In order for a fin or aerodynamic profile to behave as a body fuse for at least one part of the body fuse the angle of attack must be reduced. For this reason, in the wing tip vortex generating device the minimum angle of attack of the fin or aerodynamic profile is between -20 ° and 20 °, since otherwise its boundary layer would completely detach and, as a consequence , the pressure differences would be much smaller and the hydraulic losses would be much higher, against the desired objective.
    [0044] An aerodynamic profile comprises a first lateral face defined between the leading edge and the trailing edge and a second lateral face defined between the leading edge and the trailing edge, so that, as a consequence of the operation of the aerodynamic profile as a body body there is a noticeable difference in pressure between the two lateral faces. The first side face or side face on which the overpressures occur is called intrados and the second side face or face on which a depression occurs with respect to the pressure of the incident current is called extradoses. This means that a finite-span aerodynamic profile produces wingtip vortices, since a favorable pressure gradient is generated from the intrados to the extrados, which in turn generates a current around the marginal edge called a rim current.
    [0046] If the span of the profile is much greater than the maximum chord, the pressures on the intrados and the extrados are very uniform and the effect of the wingtip vortex on the support of said profile is reduced. Since in the present invention it is intended to intensify the wingtip vortex fins or profiles will be used aerodynamic in which the ratio between the sum of the surface of the intrados and the extrados of the fin or aerodynamic profile and the square of its maximum chord is less than 8. Therefore, in these profiles the span is of the same order of magnitude as the maximum chord.
    [0048] In the field of hydraulic engineering, the hydraulic diameter of a hydraulic duct or channel (DH) is defined as four times the area of its cross section (A) divided by the perimeter wetted by the fluid (p), which is the length of the contour of the section that is in contact with the fluid circulating through the conduit or channel:
    [0050] D h = 4 A / p
    [0052] In the case of circular ducts DH coincides with the internal diameter of the duct. In the case of ducts of square section DH coincides with the height of the duct. When a channel or duct has a section with a base, b, much greater than its height h, ( b >> h) the hydraulic diameter is of the order of the height of the duct, h, that is, the smallest of the dimensions that define the cross section.
    [0054] The losses of mechanical energy per unit of volume in a channel or conduit with a cross section of area A , which occur as a consequence of a section narrowing produced by the existence of a submerged device, where the area of the projection of the device on a plane perpendicular to the direction of the axis of the duct or channel is Ap, they can be determined as:
    [0058] Therefore, for the losses produced by the vortex generating device to be small in relation to the inertia of the fluid, it is necessary for Ap to be less than 0.5 times the section of the duct, A. Thus, the produced pressure loss coefficient, k, which is defined as:
    [0062] it will be much less than unity, which means that the losses produced by the device are negligible, thereby maximizing the efficiency of the process.
    [0063] On the other hand, so that the wingtip vortex is incorporated into the main flow of the duct or channel and therefore forms in an area where the energy dissipation is not high, it is convenient that the marginal edge of a fin or aerodynamic profile is not inside or near the boundary layers of the walls or bottom of the duct or channel. In most applications of industrial interest the flow is turbulent and the thickness of the boundary layer can be estimated as 5000 times the ratio of the kinematic viscosity to the average flow rate. Therefore, in order for the wingtip vortex not to dissipate rapidly, the minimum distance from the marginal edge of a fin or airfoil to the walls or bottom of the duct or channel should be greater than the result of multiplying 10,000 by the kinematic viscosity of the fluid and divide by average velocity in the channel or conduit.
    [0065] Furthermore, as an optional aspect of the invention, the marginal edge of a fin or aerofoil is at a minimum distance from the nearest solid wall greater than the hydraulic diameter of the duct or channel divided by 20, that is, the distance from the marginal edge from the fin or aerodynamic profile to the first solid structure or to a second solid structure is greater than the hydraulic diameter of the channel or duct divided by 20. In the event that the distance to the wall is less than that DH / 20 ratio, the wall would produce a strong interaction with the vortex, which would not efficiently achieve the desired objective.
    [0067] On the other hand, in order to obtain greater pressure differences between the extrados and the intrados of a fin or aerodynamic profile, it is convenient that the angle of attack that is defined for the different longitudinal sections increases from its root (central plane in the case of profiles with two marginal edges) towards one of its marginal edges, which is the area where the wingtip vortices form.
    [0069] For the same reason, to obtain greater pressure differences between the extrados and the intrados and at the same time avoid the boundary layer detachment, it is convenient that there is a certain curvature in the longitudinal section of a fin or aerodynamic profile, so it is convenient that the wingtip vortex generating device has a fin or aerodynamic profile with a longitudinal section in which the maximum height of the profile, called the maximum camber, is between 25% and 75% of its chord. These values exclude aerodynamic profiles in which the maximum camber is very close to the leading or trailing edge, which are more prone to have boundary layer detachment at the edges of the profile.
    [0071] In another particular embodiment of the invention, the at least one fin or aerodynamic profile of the vortex generating device in channels or ducts has the marginal edge substantially thicker than the average thickness of a fin or aerodynamic profile and is rounded to facilitate the formation of wingtip vortices. In the aeronautical industry, to reduce the formation of wingtip vortices, profiles are placed perpendicular to the blade, which are called wingtip devices. In contrast, for the device of the present invention, the edge The marginal edge is thickened to facilitate the formation of the wingtip vortex, which is why, in a fin or aerodynamic profile, the average value of the radius of curvature of the marginal edge is greater than the average thickness of said fin or aerodynamic profile.
    [0073] In summary the invention relates to the device claims included in this application, which are included herein by reference.
    [0075] The wingtip vortex generating device described above is applicable for agitation in various industrial equipment, such as tubular chemical reactors, tubular reagent mixing systems, tubular biological reactors, and open biological culture tanks. Their ability to generate transverse velocities from a parallel mainstream makes them also applicable for the resuspension of solid particles found at the bottom of channels, rivers, ports, docks and estuaries. Therefore, the invention also relates to a method of agitation in channels and ducts by generating vortices by means of the vortex generating device in channels or ducts described above.
    [0077] BRIEF DESCRIPTION OF THE DRAWINGS
    [0079] Figure 1 shows a perspective view of a channel or conduit of rectangular section with the vortex generator device in channels or conduits of the present invention anchored to one of the walls of a conduit. The leading edge, trailing edge, and marginal edge of the fin are shown, as well as the generated wingtip vortex.
    [0080] Figure 2 shows a longitudinal section of the channel or conduit vortex generating device of the present invention where the angle of attack is indicated in relation to the direction of the incident current, the chord and the maximum camber for that longitudinal section of said device .
    [0082] Figure 3 shows a longitudinal section of the channel or conduit vortex generating device of the present invention showing the typical pressure distribution in the intrados and extradoses of said device.
    [0084] Figure 4 shows a cross section of the channel or conduit vortex generating device of the present invention showing the pressure distribution in the intrados and extrados of said device and the rim current.
    [0086] Figure 5 shows a perspective view of a channel or conduit of rectangular section with the device of the present invention anchored to one of the walls, where the cross section of the channel or conduit and the projection of the device in the direction of the main current on a plane perpendicular to the axis of the duct.
    [0088] PREFERRED EMBODIMENT OF THE INVENTION.
    [0090] The references used in the figures of the channel or conduit vortex generating device of the present invention, which will be explained in detail below, are as follows:
    [0092] 1: flow with direction essentially parallel to the walls of the duct or channel.
    [0093] 2: canal or duct wall.
    [0094] 3: bottom of the canal or duct.
    [0095] 4: wingtip vortex generated by the profile.
    [0096] 5: fin or aerodynamic profile.
    [0097] 6: leading edge.
    [0098] 7: trailing edge.
    [0099] 8: marginal edge.
    [0100] 9: angle of attack.
    [0101] 10: rope.
    [0102] 11: maximum camber.
    [0103] 12: soffit.
    [0104] 13: extrados.
    [0105] 14: beading.
    [0106] 15: b.
    [0107] 16: h.
    [0108] 17: App.
    [0110] The behavior of a fuseled profile immersed in a flowing current is very well described for its applications in aeronautical engineering. The most important aerodynamic characteristics of a profile are its lift coefficient, CL, and its drag coefficient, CD, defined as
    [0114] - pv 2 S
    [0116] and
    [0118] (two),
    [0119] C = 7 - pv ¿S
    [0122] where L and D are, respectively, the lift forces and aerodynamic resistance on the profile and S is the wing surface.
    [0124] These two coefficients vary as a function of the Reynolds number, although it is generally sufficient to consider the asymptotic values for very high Reynolds numbers in fully developed turbulence. In addition, the coefficients also vary depending on the flap's angle of attack or aerodynamic profile. When the boundary layer on the profile is adhered and the wake that comes off the trailing edge is very narrow, the coefficient of aerodynamic resistance, CD , is much less than unity, since in this case the losses are produced by friction with profile walls, a generally negligible effect at high Reynolds numbers. In the same situation, the supporting coefficient, CL , is usually of a unity order, presenting an increasing dependence with the angle of attack, until for a certain critical angle the so-called lift crisis occurs, in which the boundary layer on the surface is detached before reaching the trailing edge. From this angle the lift of the aerodynamic profile is sharply reduced as the angle of attack increases as a consequence of the detachment of the boundary layer and of a smaller pressure difference between the intrados (overpressure face) and the extrados (depression). To achieve higher lift values, profiles with a certain thickness and curvature can be used, which allows the boundary layer to not come off for greater angles of attack.
    [0126] As explained previously, to increase the intensity of the wingtip vortex that is produced on a profile, it is convenient that the pressure difference between intrados and extrados is high throughout the entire chord of the fin or aerodynamic profile. As a consequence of the aforementioned, the aerodynamic profile should work with high angles of attack, but without reaching the critical value at which the lift crisis occurs due to the detachment of the boundary layer.
    [0128] The type of vortex that emerges from the marginal edge of the fin or aerodynamic profile can be modeled as a cylindrical vortex, which in the case of a current from a channel or conduit would have an axis essentially parallel to the axis of the same channel or conduit.
    [0130] Cylindrical vortex models such as Rankine's vortex or Burgers' vortex are often used in specialized literature ( Dávila J. & Hunt JCR 2001 Settling of small particles near vortices and in turbulence. J. Fluid Mech. 440, 117-145 ). These models describe a dependency of the azimuth velocity (around the axis of the vortex) as a function of the distance from the axis of the vortex.
    [0132] The most important parameters of the cylindrical vortices are their viscous radius, Rv, and the vortex circulation. The first of these parameters determines the distance to the axis of the vortex at which the azimuth speed is maximum. When the Reynolds number is high, the viscous radius is very small (typically on the order of a millimeter) and the vortex circulation is approximately constant. From the point of view of agitation it is important that the circulation of the vortex is high, which as it is very related to high values of the fin lift coefficient or aerodynamic profile and the angle of attack.
    [0134] The technical problem that the present invention solves is to favor the agitation of an essentially parallel current (1) that flows through a conduit or a channel formed by side walls (2) and a bottom or hearth (3) (FIG. 1). To do this, recourse is made to the generation of wingtip vortices (4) through the use of fins or aerodynamic profiles, without a substantial increase in turbulence intensity.
    [0136] For this, the channel or duct vortex generator device of the present invention comprises at least one fin or aerodynamic profile (5), anchored to one of the side walls (2) or to the bottom (3) of the channel or duct by the edge opposite the marginal edge (8) of the fin or aerodynamic profile (5), or anchored to a first solid structure, by means of fixing means, so that the controlled incorporation of intense wingtip vortices (4) occurs ) to the main flow (1) of the duct or channel.
    [0138] The basis of the device is the use of the wingtip vortex (4) that is formed in the aerodynamic profiles (5) as a consequence of having a finite wingspan. In these profiles, the leading edge (1) is defined as the leading edge (6) and the leading edge (7) is the downstream edge in the direction of the current (1) (FIG. one). These profiles consist of one or two marginal edges (8), which are the lateral edges in the direction of the main current (1). The profiles will have a single marginal edge when it is fixed directly to one of the solid walls of the duct or channel, or one of its sides protrudes through the surface in a channel or duct.
    [0140] The wingtip vortex (4) detaches from the marginal edge (8) of the fin or aerodynamic profile (5) and causes the appearance of an oscillatory movement that subjects the particles traveling with the current to an up-down cycle . For this reason, the present invention has as a fundamental advantage that transverse speeds to the main current are produced without hardly introducing pressure losses, instead of from a strong increase in turbulent intensity by any other procedure, which is key for that energy efficiency can be maximized.
    [0141] The designed device, therefore, tries to promote the wingtip vortex (4), for which the angle of attack of the fin or aerodynamic profile must be small, since otherwise the boundary layer would be detached and, as As a consequence, the bearing force would be much lower and hydraulic losses would be much higher, against the intended objective. Therefore, the angle of attack must be between -20 ° and 20 °. As shown in Fig. 2, the angle of attack of a longitudinal section (9) is that formed by the incident current with the reference line of a fused body, which is the line that joins the leading edge of the at least one wing or aerodynamic profile with the edge of exit and that defines the so-called chord (10) of the fin or aerodynamic profile (5) in said longitudinal section (FIG. 2).
    [0143] As a consequence of the profile working as a fused body, there is a notable pressure difference between the two sides of the wing or aerodynamic profile (5) (FIG. 3). The face on which the overpressures occur is called intrados (12) and the face on which a depression occurs with respect to the pressure of the incident current is called extrados (13). This allows us to explain why a finite-span aerodynamic profile (5) produces wingtip vortices, since from the intrados (12) towards the extrados (13) a favorable pressure gradient is generated, which in turn generates a current around of the marginal edge (8) called rim current (14), as indicated in FIG. Four.
    [0145] If the span of the profile is much greater than the maximum chord, the pressures on the intrados (12) and the extrados (13) are very uniform and the effect of the wingtip vortex (4) on the support of said profile is reduced. Since in the present invention it is intended to intensify the wingtip vortex (4), fins or aerodynamic profiles will be used in which the quotient between the sum of the surface of the intrados (12) and the extrados (13) of the fin or aerodynamic profile and the square of its maximum chord (10) is less than 8. Therefore, in these profiles the span is of the same order of magnitude as the maximum chord.
    [0147] In the field of hydraulic engineering, the hydraulic diameter of a hydraulic duct or channel (DH) is defined as four times the area of its cross section (A) divided by the perimeter wetted by the fluid (p), which is the length of the contour of the section that is in contact with the fluid circulating through the conduit or channel: D H 4 A / p (3)
    [0149] In the case of circular ducts, DH coincides with the inner diameter of the duct. In the case of ducts with a square section, it coincides with the height of the duct. When a channel or duct has a section with a base, b (13), much greater than its height h (14), (b >> h) the hydraulic diameter is of the order of the height of the duct, h, that is, the smallest of the dimensions that define the cross section (FIG. 5).
    [0151] The mechanical energy losses per unit of volume in a channel or conduit with a cross section of area A, which occur as a consequence of a section narrowing caused by the existence of a submerged device whose area Ap, of the projection of the device ( 15) on a plane perpendicular to the direction of the axis of the duct or channel (FIG. 5), can be determined as
    [0156] Therefore, for the losses produced by the vortex generating device to be small in relation to the inertia of the fluid, it is necessary that Ap be less than 0.5 times the section of the duct, A. Thus, the loss coefficient of produced load, k, defined as
    [0160] it will be much less than unity, which means that the losses produced by the device are negligible, thereby maximizing the efficiency of the process.
    [0162] EXAMPLE OF PRACTICAL IMPLEMENTATION OF THE INVENTION
    [0164] In the attached figures a practical embodiment of the invention is shown, where the device requires the supply of a flow of the gas or liquid to be stirred. This flow must be high enough so that the Reynolds number associated with the flow around the profiles that form the vortex generating device is high. On the other hand, the number of fins or profiles and / or their surface will be increased if necessary to reach agitation levels required for each specific application. Likewise, the angle of attack, the chord or the curvature of the profiles will be increased if more agitation is required.
    [0166] The flow rate of the fluid to be agitated must be as homogeneous as possible upstream of the aerodynamic profiles to avoid boundary layer detachments near the leading edge.
    [0168] The materials in which the vortex generating device can be manufactured are multiple (metal, plastic, composites, etc.), the choice of material being fundamentally dependent on the specific application in which the device is to be used.
    [0170] Figures 1 and 2 show the diagram of a prototype installed in a hydrodynamic channel or conduit with walls (2) and sole (3), in which an aerodynamic profile with parallel sides has been attached to the bottom of said channel or conduit. (4) by the edge opposite its marginal edge (8). This prototype has worked with water velocities of the incident stream of between 0.3 and 0.5 m / s. The width of the profile has been 15 cm, the length of its marginal edge also 15 cm and its average thickness 4 mm. Tests have been carried out in a range of angles of attack (9) of the aerodynamic profile (5) between 0 ° and 20 °. The marginal edge of the profile was at a distance to the nearest wall equivalent to 0.5 times the hydraulic diameter of the duct, which in this case was 30 cm.
    [0172] For the hydrodynamic channel or conduit the thickness of the boundary layers of the walls can be estimated at 5000 times the kinematic viscosity of the fluid (water) and divided by average velocity. In this case, the thickness is therefore of the order of one centimeter, so that the marginal edge of the fin does not interact with these areas of high energy dissipation.
    [0174] As shown in figure 5, to ensure a minimum pressure drop in this prototype, the projection of the section of the profile in the direction of the current had an area between 0 and 20 cm2.
    权利要求:
    Claims (7)
    [1]
    1. Vortex generator device in channels or conduits comprising:
    - at least one channel or conduit through which a fluid (1) circulates comprising a kinematic viscosity and an average velocity of the fluid (1) in the channel or conduit, where the channel or conduit comprises at least two walls (2) and a background (3),
    - at least one fin or aerodynamic profile (5) where the fluid (1) falls, which in turn comprises a face on which overpressures are produced due to the incidence of the fluid (1), or intrados (12), and a face on which depressions occur with respect to the overpressures in the intrados (12), or extrados (13), and a maximum chord (10),
    where the at least one fin or aerodynamic profile (5) is fixed to one of the walls (2) or to the bottom (3) of the channel or conduit by means of an edge opposite to a marginal edge (8) of the fin or aerodynamic profile (5), or is fixed to a first solid structure, characterized in that it has the following design characteristics:
    • the angle of attack of said fin or aerodynamic profile (5) is between -20 ° and 20 °;
    • the quotient between the sum of the surface of the intrados (12) and the extrados (13) of the fin or aerodynamic profile (5) and the square of its maximum chord (10) is less than 8, and
    • the distance from the marginal edge (8) of the fin or aerodynamic profile (5) to one of the at least two walls (2) or to the bottom of the channel or duct, whichever is the least, is greater than the result of multiplying 10000 by the kinematic viscosity of the fluid (1) and divide by the average speed of the fluid (1) in the channel or conduit.
    [2]
    2. Vortex generating device in channels or ducts according to claim 1 characterized in that the channel or duct comprises a hydraulic diameter and also the distance from the marginal edge (8) of the fin or aerodynamic profile (5) to the first structure solid or to a second solid structure is greater than the hydraulic diameter of the channel or conduit divided by 20.
    [3]
    3. Vortex generating device in channels or conduits according to any one of the preceding claims, characterized in that the channel or conduit comprises an axis and a cross section, where the quotient between an area of the projection of the at least one wing or aerodynamic profile (5) on a plane perpendicular to the direction of the axis of the channel or conduit and the cross-sectional area of the channel or conduit is less than 0.5.
    [4]
    4. Vortex generating device in channels or ducts according to any of the preceding claims, characterized in that the at least one fin or aerodynamic profile (5) comprises a root where the at least one fin or aerodynamic profile (5) comprises an angle of increasing attack from its root to the marginal edge (8).
    [5]
    5. Device for generating vortices in channels or ducts according to any of the preceding claims, characterized in that the at least one wing or aerodynamic profile (5) has, in one of its longitudinal sections, a maximum camber (11) between 25 % and 75% of its maximum chord (10).
    [6]
    6. Vortex generating device in channels or ducts according to any of the preceding claims characterized in that the marginal edge of the at least one fin or aerodynamic profile (5) comprises a radius of curvature and the at least one fin or aerodynamic profile (5) comprises an average thickness, where an average value of the radius of curvature of the marginal edge (8) is greater than the average thickness of said fin or aerodynamic profile (5).
    [7]
    7. Method of agitation in channels and ducts by generating vortices by means of the vortex generator device in channels or ducts of any of the preceding claims.
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    同族专利:
    公开号 | 公开日
    EP3878545A1|2021-09-15|
    ES2767024B2|2021-09-17|
    US20220016585A1|2022-01-20|
    WO2020120818A1|2020-06-18|
    AU2019398483A1|2021-07-08|
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    EP19894824.2A| EP3878545A1|2018-12-14|2019-12-12|Device for generating vortices in channels or pipes|
    US17/312,297| US20220016585A1|2018-12-14|2019-12-12|Device for generating vortices in channels or pipes|
    AU2019398483A| AU2019398483A1|2018-12-14|2019-12-12|Device for generating vortices in channels or pipes|
    PCT/ES2019/070842| WO2020120818A1|2018-12-14|2019-12-12|Device for generating vortices in channels or pipes|
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