The present invention belongs to the field of injection of a fog capable of decontaminating air and solid surfaces of objects, and is particularly related to a new, simpler nozzle which injects a cone-shaped rotating fog volume.
Currently, the use of spray nozzles capable of spraying one or more liquids in the form of small-sized particles for various applications such as firefighting, decontamination tasks, cleaning industrial waste, etc., among others, is well-known. In particular, the decontamination of public facilities and critical infrastructures has recently gained a great importance due to worldwide situation created by the Covid-19 pandemic.
Up to very recently, nozzles used were only useful for surface decontamination, as the size of the particles generated was too large to produce a relevant decontamination in terms of airborne contaminant particles. Moreover, the very small size of certain pollutant particles means that, even when they are “laying on” a surface, any weak air flow can raise them up into the air. This is the case, for example, for viruses such as Covid-19. So, when using conventional cleaning nozzles that emit large liquid particles, the flow created around each particle when it hits the surface could cause viruses around its point of impact onto the surface to be re-suspended up into the air, subsequently falling back down onto the same or other surfaces nearby. In short, it is clear that conventional decontamination nozzles are not efficient.
The inventors of the present application have recently discovered that the generation of a fog with a droplet size distribution with a large submicrometric fraction, for example between 0.1 μm and 20 μm, which is also injected under pressure, therefore tending to form a conical fog jet with a large axial velocity gradient, and which also has a tangential component, leads to the appearance of a Venturi effect which causes airborne pollutant particles in the air to be absorbed by the fog. The inventors of the present application describe this cleaning procedure in detail in document EP3406317A1. Furthermore, the small size of the particles emitted by this nozzle avoids the appearance of strong flows when they fall on a surface, thus avoiding the re-suspension in the air of very small contaminant particles such as viruses and so on. Furthermore, the inventors of the present application describe in document EP3395449A1 a new fog cone generation nozzle capable of carrying out the procedure described in the previous paragraph.
In effect, this new nozzle generates a spiral cone of fog made up of submicron-sized particles that can be used for the purpose of simultaneously decontaminating air and surfaces. As can be seen in
As it can be seen, the configuration of the nozzle described in document EP3395449A1 is quite complex and is composed of a large number of parts. Moreover, the intricately shaped parts, such as the spiral module, require the use of excessively long and complicated manufacturing processes.
In short, there is currently a need in the technical field for nozzles capable of emitting a rotating cone-shaped fog, whose configuration is simpler and whose component parts require less manufacturing effort.
The nozzle of the present invention solves the above problems thanks to a novel design that reduces the number of parts and their complexity, while maintaining the ability to generate a rotating conical flow of fog at the outlet. In addition, the new design described in this document makes it possible to select, during assembly, the magnitude of the rotational effect of the conical fog jet generated.
In this document, the “axial axis” refers to the main central axis of the nozzle, the overall shape of which may be cylindrical.
In this document, the term “forward” refers to the main direction of liquid flow along the axial axis from an inlet end of the nozzle to an outlet end of the nozzle. That is, the outlet end of the nozzle is located at a front side thereof, while the inlet end of the nozzle is located at a rear side of the nozzle.
In this document, the term “transverse” refers to a plane perpendicular to the axial axis of the nozzle of the invention. In turn, the “cross section” of a specific element, unless otherwise indicated, refers to a section perpendicular to a main axis of said element. For example, in the case of the radial arms, their cross section is perpendicular to the main direction along which said radial arms extend.
The present invention describes an improved fog injection nozzle for emitting a rotating conical flow of fog formed by liquid particles suspended in a gas. This nozzle comprises a body provided with a first axial cylindrical cavity traversed by an axial liquid conduit connected at its rear end to a pressurized liquid inlet port. A pressurized gas inlet port is also connected to said first cavity by means of a radial conduit. The nozzle further comprises a cylindrical block that covers a front side of the first cavity and that is provided with a central axial conduit connected to the front end of the axial liquid conduit. The body comprises a second axial cylindrical cavity for mixing liquid and gas arranged on the front side of the cylindrical block. The nozzle further comprises an outlet pin located in an axial outlet passage of the nozzle which is attached to a front side of the second cavity. A front end of the outlet pin comprises an axial stem provided with a flare located at the front end of said axial nozzle outlet duct, such that the flare guides the flow of liquid and gas to generate a conical flow of fog. In turn, a rear end of the output pin comprises a hollow transverse disc which disc is connected to the rear end of the axial stem by means of equally spaced angular radial arms.
The nozzle structure described up to this point is known from EP3395449. However, the nozzle of the present invention differs from that in the way that a rotating component is achieved to be imparted to the emitted conical flow. In the nozzle of document EP3395449, pressurized air was introduced into the second cavity through tangential channels in the cylindrical block. The present invention achieves a similar effect by replacing these difficult-to-manufacture tangential channels with much more easily manufactured axial channels.
In fact, in the nozzle of the present invention, the cylindrical block comprises axial holes that join the first cavity with the second cavity for the passage of pressurized gas. These axial holes are radially spaced from the central axis of the cylindrical block and angularly equally spaced. Also, the number of axial holes of the cylindrical block is the same as the number of radial arms of the output pin. Thus, the cylindrical block and the output pin are configured in such a way that the mixture of liquid and gas driven by the pressurized gas injected through the axial holes of the cylindrical block is deflected asymmetrically by the respective radial arms, causing the appearance of a rotating tangential component in the conical flow of fog emitted by the nozzle.
In this way, it is possible to generate a tangential component in the conical flow of fog emitted without the need for moving parts or parts with intricate shapes that are difficult to manufacture. In principle, this effect can be achieved in different ways, although two particularly preferred embodiments are described in this document. In a first preferred embodiment, the tangential effect on the outflow is achieved by a misalignment between the axial holes of the cylindrical block and the radial arms. In a second preferred embodiment, alternative to the first preferred embodiment, the tangential effect is achieved by means of a suitable shape of the portion of the arms where the flow discharging from the second cavity impacts on. Each of these preferred embodiments is described in more detail below.
According to a first embodiment of the nozzle, the cylindrical block and the output pin are angularly misaligned relative to the position of said axial holes and said radial arms. In other words, the flow of pressurized gas injected through the axial holes of the cylindrical block, which carries liquid particles with it, does not hit the center of the respective radial arms, but does so in a laterally offset position relative to the main direction of each arm. This means that the flow of gas and liquid particles is not deflected symmetrically on both sides of each arm, but rather that a larger portion of the flow passes through one side of the arm than the other. As a consequence, a tangential component is generated in the direction of the resulting flow downstream of the arms.
This configuration makes it possible to modify the magnitude of the tangential component of the conical outlet flow of the nozzle by means of a suitable selection of the angular misalignment between the cylindrical block and the outlet pin during assembly of the nozzle. This angle can in principle be freely selected, since both elements have an essentially cylindrical shape that can be mounted inside the nozzle body in any orientation. The greater the misalignment, the greater the tangential component of the outflow. More specifically, in preferred embodiments of the invention, the misalignment angle can be between 0° and 60°, preferably between 5° and 45°, and even more preferably between 5° and 13°. In particular, the inventors of the application have found that a particularly advantageous value of the angle of misalignment is approximately 9°.
In principle, the shape of the portion of the arms where the flow of gas and liquid particles impacts can have different shapes, including a flat shape contained in a plane transverse to the main axis of the nozzle. However, preferably the cross section of the portion of the radial arms impacted by the flow of liquid and gas driven by the pressurized gas injected through the axial holes of the cylindrical block comprises a central peak that separates two essentially equal descending curved sections. These two curved sections can have a suitably calculated shape to minimize the speed or pressure losses of the outlet flow and, at the same time, print the desired characteristics to its tangential component.
Thus, when the axial holes and radial arms are aligned, each radial arm divides the flow of liquid and gas into two essentially equal portions. In this case, no component is printed tangential to the conical flow exiting the nozzle, which is therefore not rotating. In contrast, when the axial holes and radial arms are misaligned, each radial arm directs most of the liquid and gas flow to one side of the radial arms. In this case, a component tangential to the conical flow exiting the nozzle is printed in an optimized manner.
According to a second embodiment of the nozzle, the cross section of the portion of the radial arms impacted by the mixture of liquid and gas propelled by the pressurized gas injected through the axial holes of the cylindrical block has a lateral peak which, when the axial holes and radial arms are aligned, directs most of the liquid and gas flow to one side of the radial arms.
That is, the cylindrical block and the output pin in this case are mounted in such a way that axial holes and cylindrical holes are aligned, and the very shape of the portion of the arms on which the air and gas flow impacts causes the appearance of the tangential component. This shape can be suitably selected to obtain tangential components of different magnitudes and characteristics.
Thus, this new nozzle configuration makes it possible to obtain a rotating cone of fog at the outlet in a simpler way than the nozzle of the prior art.
As for the liquid and gas feed pressures, they should preferably be of the same order to achieve the appropriate droplet size distribution, the gas pressure being preferably between 8 and 12 bar and the liquid pressure preferably between 6 and 12 bar.
In principle, this nozzle can be implemented in different ways and using parts of different shapes and in different numbers. For example, in a particularly preferred embodiment of the invention, the body is divided along an axial plane into a first body portion and a second body portion engageable with each other by screwing along respective flat axial faces. In this case, the periphery of a flat axial face of the first body portion may comprise a channel for receiving a seal that leaves two gaps close to the axial duct unsealed. As will be described later in more detail, this configuration is particularly advantageous because it increases the gradient imprinted on the injected fog cone, thus improving its effectiveness.
In short, the nozzle of the described invention provides a tangential component in the output flow using simpler parts and fewer than the nozzle described in document EP3395449.
The present invention is herein described with reference to
The nozzle (1) of the present invention is formed by a body (2) which is formed by two halves (21a, 21b) separated along a flat axial face. The two halves (21a, 21b) have two rows of three holes (22) arranged along the side walls of their respective flat axial face for fixing by means of screws (14). An additional piece (13) in the form of a transverse disc is fixed, also by means of screws (15), to the rear end of the body (2) of the nozzle (1). Furthermore, the peripheral walls of the flat axial face of the first half (21) are traversed by a channel (12) for receiving a seal (not shown). An adequate selection of the tightening force of the screws (14) causes that, during the use of the nozzle (1), a small part of air escapes through the slot closed by the sealing gasket. This small air leak causes an enhancing effect on the rotational properties of the emitted fog, as will be described in greater detail later in this document.
The transverse disc (13) that closes the rear end of the body (2) comprises, on its front face, an axial conduit (4) for liquid that runs through a first cylindrical cavity (3) of the nozzle (1) whose diameter is substantially greater than that of said axial duct (4). At its rear end, the axial liquid conduit (4) is connected to a pressurized liquid inlet port (5). The liquid inlet port (5) is formed on a rear side of the transverse disc (13) itself. At its front end, this axial liquid conduit (4) is joined to an axial conduit (81) of a cylindrical block (8) located inside a housing (16) adjacent to the front end of the first cavity (3). The gas inlet to the nozzle (1) takes place in a radial direction through a gas inlet port (6) connected to the first cavity (3) through a radial duct (7).
Therefore, the liquid introduced through the inlet port (5) runs through the axial conduit (4), passes through the axial conduit (81) of the cylindrical block (8) that covers the front side of the first cavity (3), and exits into a second cylindrical cavity (9) through the front end of said axial duct (81). The cylindrical block (8) also has three axial holes (82) radially separated from the central axis (E) and equally spaced angularly. These axial holes (82) join the first cavity (3) with a second cavity (9) located on the front side of the cylindrical block (8). In this way, the pressurized gas that is introduced into the first cavity (3) through the inlet port (6) passes, through said axial holes (82), to the second cavity (9). Therefore, in the second cavity (9) the interaction between the pressurized gas flow and the pressurized liquid flow takes place. In particular, the pressurized liquid flow emitted through the axial conduit (81) impacts against a rear end surface of an output pin (10), which is described later, fragmenting into small size particles. The pressurized gas injected through the axial holes (82) then entrains these particles through an axial outlet duct (11) of the nozzle (1) located on the front side of the second cavity (9).
The axial duct (11) takes the form of a nozzle whose section is decreasing in a first section, and increasing in the second section, thus connecting the second cavity (9) with the outside of the nozzle (1). Inside the axial duct (11) there is an outlet pin (10) that guides the fog flow to generate a rotating conical flow at the outlet of the nozzle. The output pin (10) is basically formed by an axial rod (101) located on its front side and connected to a hollow transverse disc (103) located on its rear side. The axial stem (101) has a first portion that narrows to run through the first section of the nozzle with a decreasing section of the axial duct (11) parallel to its walls. A second portion of the axial stem (101) is formed by a widening (102) that runs through the second section of the nozzle with an increasing section of the axial duct (11) also parallel to its walls. For its part, the hollow transverse disc (103) is connected to the rear end of the axial stem (101) through three radial arms (104) equally spaced angularly. As can be seen, the rear surface of the radial arms (104) has a flat cross-sectional shape. Furthermore, the distance between the axial holes (82) of the cylindrical block (8) and the main axis (E) of the nozzle (1) is selected such that the axial holes (82) are located opposite the area of the arms radials (104) of the hollow transverse disc (103).
Thus, when the cylindrical block (8) and output pin (10) are angularly aligned, the flow emitted through each axial hole (82) impacts the center of a respective radial arm (104). This situation is shown in greater detail in
In contrast,
In the previous figures, the rear surfaces of the radial arms (104) have been shown as flat. This causes high losses due to the impact of the flow emitted through the axial holes (82) against said flat surfaces perpendicular to the main direction of the flow. To avoid this, it is possible to provide the rear surfaces of the radial arms 104 with a specially designed shape to reduce losses. For example, as shown in
Thus, as shown in
In contrast,
Lastly,
In addition, as mentioned previously in this document, in any of the described configurations it is possible to increase the gradient effect printed on the fog cone at the nozzle (1) outlet thanks to a suitable selection of the sealing gasket and the tightening force of the screws (14) that join the two halves (21a, 21b) of the body (2) of the nozzle (1). Indeed, when the continuity of the sealing joint is interrupted near the outlet duct (11), two gaps are produced between the two parts of the assembly through which the fog can escape at high speed. As it occurs only at two angles, it increases the angular asymmetry and therefore the velocity gradients in the fluid-fog-that escapes, which makes it easier to attract surrounding air and trap suspended particles.
Number | Date | Country | Kind |
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P202030349 | Apr 2020 | ES | national |
This application is a continuation of International Application PCT/ES2021/070232, filed on Apr. 8, 2021, which claim priority to Spanish Application No. P202030349, filed Apr. 25, 2020. The entirety International Application PCT/ES2021/070232 is incorporated in its entirety into the present continuation application by reference.
Number | Date | Country | |
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Parent | PCT/ES2021/070232 | Apr 2021 | US |
Child | 17972951 | US |