专利摘要:
lift door assembly the present invention provides an acoustic flow meter assembly for open tubes or channels. said set including a structure with a predetermined geometry. the structure having at least one user-accessible port adapted to receive a replaceable cartridge, containing at least one acoustic transducer, to measure the fluid velocity through said structure. the present invention also relates to hinged lift gate assemblies for measuring fluid flow, and a method for measuring fluid velocity in open tubes and channels, characterized by the use of a delay circuit, which uses redundant pairs of transducers, and a method for synchronizing two transducers in an apparatus to measure flow in an open channel.
公开号:BR112012003537B1
申请号:R112012003537-1
申请日:2010-08-18
公开日:2020-02-18
发明作者:David John Aughton;Damien Vernon Pearson
申请人:Rubicon Research Pty Ltd;
IPC主号:
专利说明:

“LIFT DOOR ASSEMBLY
Field of the Invention [0001] The present invention relates to an acoustic flow meter set for open tubes and channels, and particularly, though not exclusively, to an acoustic flow meter set for monitoring water flow. The present invention also relates to an undershot door leaf assembly, which can be used with the acoustic flow meter assembly.
History of the Invention [0002] Flow meters are commonly used to measure the flow rate in underground tubes and galleries or open channels. Travel time acoustic flow meters use well-established measurement technology. When flow meters are installed in underground pipes, maintenance requirements require that they be installed in measuring wells, typically concrete boxes. The well must be easily accessible to allow access to the flow meter components.
[0003] When ultrasonic flow meters (transit time) are installed in open channels and tubes, they are installed as a collection of subcomponents, which must be assembled and calibrated. Adjustment of measurement systems requires accurate measurement of the distance between the transducers, angle of the measurement path in relation to the flow direction, water level transducer data, and other meter configuration parameters. Other products available on the market for acoustic flow measurement are mounted on site, fixing the acoustic transducers around the internal diameter or
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2/39 outer diameter of the tube, where the flow passes. In open duct applications, the transducers are screwed to opposite duct walls. The transducers must be precisely installed and calibrated in the field. For an installation in which the transducers are installed on the inside diameter of a pipe, the pipe must be of sufficient diameter to allow safe access to be installed. For installations where the transducers are installed on the outside diameter of the pipe, the pipe must be above the ground or in a concrete pit, which must be built around the pipe to allow safe access to the outside diameter of the pipe to allow fixation and maintenance of the sensors.
[0004] In open channel applications, the accuracy of flow meters can be affected by conditions provided by the flow meter neighborhood. The geometry of the channel upstream and downstream of the flow meter affects the distribution of the speed with which the fluid passes through the flow meter. The speed distribution is measurable at all points on the flow meter, except on the surface. The fluid speed on the floor and walls of the flow meter is zero. The speed at certain elevations on the flow meter can be measured, and the speed between these measurements can be interpolated from the measured speeds. However, generally, the surface velocity of the flow is not measured, and the velocity distribution at the upper levels must be extrapolated, implying a potentially high degree of uncertainty. To minimize the uncertainty in the calculation of the surface velocity of the flow, the variation in the surface velocity behavior must be minimized.
Purpose of the Invention
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3/39 [0005] It is an objective of the present invention to reduce the infrastructure costs of an installation for an acoustic flow meter, to allow the installation of a larger number of flow meters to provide more data to determine and locate the losses in a distribution system.
[0006] An additional objective of the present invention is to provide a flow meter, which completely defines its own geometry, and does not require calibration of the installation or its surroundings.
[0007] Another objective of the present invention is to provide a lower flow port of travel below that affects the flow profile, and creates a laminar and repeatable non-turbulent flow behavior.
[0008] Yet another objective of the present invention is to provide a flow meter for closed ducts, including a gate valve or equivalent, but without a cap (bonnet), which is an integrated component of a traditional gate valve.
Summary of the Invention [0009] For these purposes, the invention provides an acoustic flow meter assembly for open tubes or channels. The aforementioned set includes a structure of a certain geometry. The said structure includes at least one user-accessible port adapted to receive a replaceable cartridge, having at least one acoustic transducer, for measuring the fluid velocity through said structure.
[0010] Preferably, the acoustic flow meter assembly includes a plurality of user-accessible ports with the respective cartridge. The accessible door to
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4/39 user can be located in the corners of a square or rectangle in the aforementioned structure. Preferably, two cartridges are arranged diagonally opposite.
[0011] In a preferred configuration, each cartridge includes a plurality of acoustic transducers to measure the flow at predetermined depths. The acoustic flow meter assembly may additionally include a hollow tube for coupling, at either end, a pipe to determine the speed with which the fluid passes through said pipe. In a practical configuration, each transducer is placed at one end of the respective sound transmitting tube, while the other end opens up to the said hollow tube. The sound transmitting tubes can be associated with the respective cartridges and angled towards the associated sound transmitting tube. The sound transmitting tubes may contain a fluid coming from the said hollow tube. The sound transmitting tubes may contain a fluid stopped outside the flow path.
[0012] In an additional configuration, the sound transmitting tubes are filled with a sound-conducting material. The acoustic flow meter assembly may additionally include an interface between the fluid in said sound transmitting tube and the current fluid. the aforementioned interface is made of a material having suitable acoustic properties for prompt transmission of the acoustic signal. The fluid in the acoustic transmitter tubes can also be contained in a sealed well, so that the fluid attaches the transducers to the inner face of the sound transmitter tubes.
[0013] The present invention can also provide an articulating lift door assembly including a door member
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5/39 that can be raised / lowered from a vertically closed position to a substantially horizontal arrangement. Said door member is pivotally mounted, by the top end, to a mechanism, for pulling said door member from the vertically closed position to the substantially horizontal position, and at least one extension extending from said door member with a point pivot at said end of said at least one extension. The said pivot point cooperating with a guide means angled downwards, whereby the movement of said door member does not cross said guide means angled downwards.
[0014] It is preferable that one the extensions (pair) are on each side of the said door member, which cooperates with the respective guide means angled downwards. The hinged lift door assembly can be in the open fluid channel, and the aforementioned at least one extension is positioned substantially two thirds of the fluid depth.
[0015] The present invention can also provide a system for measuring the velocity of open channel fluid. Said system includes an open channel with said current fluid, an acoustic flow meter set, as described above, and a hinged lift door set, as described above, downstream of said acoustic flow meter set, and said member effect affecting the surface speed of said fluid.
[0016] The present invention can also provide a system for measuring the velocity of fluid in an open channel. Said system includes an open channel containing said fluid, and an acoustic flow meter assembly, as described above, and
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6/39 an underpass port downstream of said acoustic flow meter assembly, said underpass port allowing the fluid level in front of said port to recede to provide a uniform depth of fluid across said acoustic flow meter set. [0017] The present invention also provides a method for measuring the velocity of fluid in an open tube or channel, including the steps of: providing a timing circuit, including a first circuit, having at least one acoustic transducer upstream, and one second circuit having at least one acoustic transducer downstream; measuring the time delay when detecting an acoustic signal from said at least one acoustic transducer upstream to said acoustic transducer downstream, from said first circuit; measuring the time delay when detecting the acoustic signal from said at least one acoustic transducer downstream to said at least one acoustic transducer upstream, from said second circuit; measure the time delay in said first circuit, when said at least one acoustic transducer upstream is passed through in said first circuit; measure the time delay in said second circuit when said at least one downstream acoustic transducer is passed through in said second circuit; and calculate the fluid velocity from these measurements.
[0018] In yet another aspect of the present invention, an acoustic flow meter assembly for tubes is provided, including at least three pairs of acoustic transducers, the pairs of said transducers located on opposite sides of said tube and displaced longitudinally along of the aforementioned
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7/39 tube, to provide upstream and downstream transducers, the acoustic transducer pairs have their acoustic trajectories intersecting at a point along the geometric axis of the aforementioned tube, to provide a certain degree of redundancy to allow measuring the flow through the mentioned tube, even when one of the mentioned acoustic transducers fails.
[0019] The present invention also provides a lift door assembly including a door member associated with a structure. This lift door assembly can be raised and / or lowered between open / closed positions. The aforementioned structure having upstream an apparatus for measuring the passage of the fluid. Said apparatus, in the form of a duct, having one or more opposite pairs of acoustic or similar transducers associated.
[0020] In another aspect of the present invention, a method is provided to measure travel times in an open channel or river, including the steps of: providing a first circuit having an acoustic transducer upstream on one side of said open channel or river, and a second circuit having at least one acoustic transducer downstream on the opposite side of said open channel or river. The aforementioned first and second circuits including the respective non-synchronized timing circuits, each of the circuits measuring the respective signal transmission and reception events. At least one of the aforementioned first and second circuits including RF or Laser, to provide synchronism signals between the aforementioned first and second circuits. An RF or Laser sync signal being transmitted between the aforementioned first and second circuits, before the acoustic signal is transmitted
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8/39 of one of the aforementioned acoustic transducers between the aforementioned first and second circuits, with which the aforementioned RF or Laser synchronization signal allows the synchronization between the respective synchronization circuits of the aforementioned first and second circuits of said acoustic signal. Brief Description of the Drawings [0021] For the present invention to be more readily intelligible and put into practice, reference is made to the accompanying drawings, in which:
[0022] Figure 1 is an exploded perspective view of a first configuration of an acoustic flow meter assembly for a tube according to the present invention;
[0023] Figure 2 is a diagonal cross-sectional view of the acoustic flow meter set shown in Figure 1 in the position buried in the ground;
[0024] Figure 3 is a front view of the acoustic flow meter set shown in figure 1;
[0025] Figure 4 is a plan view of the acoustic flow meter set shown in figure 1;
[0026] THE figure 5a it's a sight cross-section longitudinal in the direction of 5-5 arrows of the meter set in flow acoustic shown at figure 1, showing the flow in Water; [0027] THE figure 5b is an similar view of figure 5a, with
the full sound transmitting tubes;
[0028] The figure 6th is an View longitudinal flow in Water, showing the profile speed; [0029] The figure 6b is an View cross-section to long and in the direction of arrows A-A of figure 6a; [0030] The figure 7 is an View in perspective in an
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9/39 second configuration of an acoustic flow meter set for use in an open channel environment;
[0031] Figure 8 is a plan view of Figure 7;
[0032] Figure 9 is a cross-sectional view along and in the direction of the arrows A-A in figure 8;
[0033] Figure 10 is a view similar to that of figure
6A, but showing the configuration of the acoustic flow meter assembly of figure 7 used in combination with a vertically liftable door leaf underneath, to control the water flow;
[0034] Figure 11 is a view similar to that of figure 10, but having a folding door leaf from below;
[0035] Figure 12 is a perspective view of a configuration of the construction of the hinged door leaf assembly from below, shown in Figure 8 in the closed position;
[0036] Figure 13 is a view similar to that of figure 12 with the door leaf being raised;
[0037] A figure 14 is an similar view that of figure 13 with the leaf door on pos fully raised; [0038] A figure 15 is a view of section transversal longitudinal of the figure 12; [0039] A figure 16 is a view of section transversal longitudinal of the figure 13; [0040] A figure 17 is a view of section transversal longitudinal of the figure 14;
[0041] THE figure 18 is an View similar that gives figure 15, showing the flow in Water ; and [0042] THE figure 19 is an View similar that gives figure
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10/39
16, showing the flow of water;
[0043] Figure 20 is a flow schematic diagram, as typically used to control acoustic transducers in the acoustic flow meter assembly of figures 1 to 19 to measure the acoustic travel time between transducers;
[0044] Figure 21 is a partial view of the flow schematic diagram shown in figure 20, measuring the flow in a first direction;
[0045] Figure 22 is a partial view of a flow schematic diagram shown in figure 20 measuring the flow in a second direction, opposite to that shown in figure 21;
[0046] Figure 23 is a schematic diagram of a calibration circuit, used in connection with the flow schematic diagram of figure 20, to eliminate circuit circuit delays from figure 20;
[0047] Figure 24 is a partial view of the schematic flow diagram of figure 23, to calibrate delays in measuring the flow in the first direction shown in figure 21;
[0048] Figure 25 is a partial view of the schematic flow diagram shown in figure 23, to calibrate delays in measuring the flow in the second direction, opposite the direction shown in figure 21;
[0049] Figure 26 is a side view of a tube, showing an additional configuration of the present invention, for measuring the velocity of fluid in the tube;
[0050] Figure 27 is an end view of Figure 26;
[0051] Figure 28 is a top view of a flow port, including an apparatus for measuring travel time in accordance with the present invention;
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11/39 [0052] Figure 29 is a view similar to figure 28 of an alternative flow port arrangement and apparatus for measuring travel time;
[0053] Figure 30 is a front view of the arrangement in Figure 28;
[0054] Figure 31 is a cross-sectional view, taken along line A-A in figure 30 with the door closed;
[0055] Figure 32 is a cross-sectional view taken along line B-B in figure 30;
[0056] Figure 33 is a cross-sectional view taken along line B-B in figure 30;
[0057] THE figure 34 is detailed view taken in E in the figure 33 ; [0058] THE figure 35 is detailed view taken in D in the figure 32 ; [0059] THE figure 36 is detailed view taken in B in the figure 31 ; [0060] THE figure 37 is reduced view, similar that of the figure 28 , with a divider in the measuring device;[0061] THE figure 38 is view similar to that of figure 37, but with two dividers on measuring apparatus;[0062] THE figure 39 is a reduced view similar to that of figure 29, but with one divider on the measuring device;[0063] THE figure 40 is view similar to that of figure 39 but with two dividers on measuring apparatus;[0064] THE figure 41 is a top perspective of a door
flow similar to that of figure 28, but having an inclined control port;
[0065] Figure 42 is a reduced view similar to that
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12/39 of figure 41, but with a divider in the measuring device;
[0066] Figure 43 is a view similar to that of figure 42, but with two dividers in the measuring device;
[0067] Figure 44 is a plan view of an additional configuration to measure the acoustic travel time between transducers, using a radio transmitter;
[0068] Figure 45 is a plan view of a configuration similar to that shown in Figure 44, l to measure the acoustic travel time between transducers using Laser;
[0069] Figure 46 is a vertical cross section of the configuration shown in figure 44; and [0070] Figure 47 is a perspective view of a sealed cartridge having electronic components from figures 44 to 46.
Detailed Description of the Configurations [0071] Throughout the specification the same reference numbers will be used where appropriate to avoid repetition and duplication in the different configurations, and equally applicable to the description of the construction and operation.
[0072] In figures 1 to 6 there is shown an acoustic flow meter set 20 adapted for a pipe (not shown), where a fluid passes, preferably, in this configuration, water, but it can also be other liquids. Preferred configurations are particularly useful for measuring water consumption in irrigation canals and measuring water supply in cities. The flow meter assembly 20 is buried in the ground 22 (figure 2) and includes a frame 24, which supports the tube section 26. The tube section 26 is adapted to be attached to any end of the
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13/39 piping, through which the flow velocity must be determined. The structure 24, in this square shape configuration, has two end members 28, 30, and two side members 32, 34. The shape and construction of the structure 24 varies to suit the requirements of the particular meter set. Four hollow legs 36, 38, 40, 42 are part of the structure 24 and receive cartridges 44 slidably. The number and position of the cartridges 44 vary, depending on where the flow speed is to be determined In this configuration, each cartridge includes four acoustic transducers 46. The number and position of the acoustic transducers 46 also vary depending on the configuration. Acoustic transducers 46 are integrated with circuitry (not shown) included in cartridge 44 and frame 24. Components that must be serviced, including acoustic transducers 46 and electronic processing components, are contained in replaceable sealed cartridges 44. Typically, cartridges 44 can provide measurements, via cables or wirelessly, to a remote device.
[0073] The tube section 26 has a number of horizontally mounted sound transmitting tubes 48, as shown in figures 2 and 3. Sound transmitting tubes 48 typically have a cylindrical shape and are made of a sound-conducting material that couples the acoustic transducers 46 to the inner hole of the tube section 26. Sound transmitting tubes 48 are arranged to intersect the tube section 26 at an angle θ (figure 5a) with respect to the direction of the fluid flow 50. The preferred intersection angle θ is 45 o , however, other implementations can be used with an angle of intersection θ in the range between 0 o and 90 o , for
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14/39 adapt to geometry requirements for various uses. The sound transmitting tubes 48 provide an acoustic path for the acoustic transducers 46 located inside the flow meter cartridge 44. In figure 5a, the sound transmitting tubes 48 are hollow, and contain the fluid in the tube section 26, and the sound propagates through this fluid. The sound transmitting tubes 48 contain standing water and out of the water flow path.
[0074] Alternatively, as shown in figure 5b, the sound transmitting tubes 48 can be filled with solid material, with appropriate acoustic behavior, completely sealing the tube section 26, and allowing the recovery of the cartridges 44 while the tube is in operation with negative or positive pressure, without having to seal the access doors 52 against this pressure. Sound transmitting tubes 48 can also be filled with water, providing an interface (not shown) between standing water 48 and running water. This interface can be made of a material with appropriate acoustic properties, to allow an immediate transmission of acoustic signals. An advantage of this configuration, which closes the sound transmitting tubes 48, is the fact that the inner hole of the tube section 26 is smooth, preventing possible blocking in the tube section 26 or sound transmitting tubes 48. In this arrangement, we obtain a good acoustic coupling between the acoustic transducers 46 in the cartridges 44 and the end faces of the sound transmitting tubes 48, employing a cam mechanism in the access ports 54 that engages the acoustic transducers 46 in the faces of the sound transmitting tubes 48.
[0075] Alternatively, a simple mechanism of
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15/39 coupling can be achieved by filling the access ducts 52 with water or another fluid, acoustically coupling the acoustic transducers 46 contained in the cartridges 44 to the end faces of the sound transmitting tubes 48. In this implementation, the access ducts 52 form a sealed well containing a fluid that couples the transducers 46 to the inner face of the sound transmitting tubes 48. The access doors are typically vertically aligned and accessed by covers 54 at ground level. In some applications, access ducts 52 can be aligned horizontally and accessed by covers mounted on the walls. The access ducts can be installed at any angle that meets the installation.
[0076] In a horizontal plane of the acoustic flow meter set 20, it has four acoustic transducers 46, which are arranged to provide acoustic trajectories 58, 60 in the horizontal planes (figures 5a, 5b). If there are four transducers on cartridge 44, then there should be four horizontal planes 62, 64, 66, 68 (figures 6a, 6b). These acoustic trajectories form right angles, and such an arrangement eliminates cross flow errors, as discussed in Section 13.13 of ASTM D5389-93 (2007) - Standard Test “Method for OpenChannel Fluido Measurement by Acoustic Velocity Meter Systems.
[0077] The acoustic transducers 46 transmit a high frequency sound pulse (in the kilohertz to megahertz range) through the tube section 26. The travel time of other acoustic signals is measured in the upstream and downstream direction of the flow 50 , as in figures 5a, 5b. The speed of the flow creates a difference in the travel time of sound waves in
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16/39 upstream and downstream directions. The travel time difference is recorded and used to determine the average speed of the fluid along the acoustic trajectory line. The four measurement paths provide the average fluid velocity in four different planes 62-68, as shown in figure 6a. The velocity distribution in the pipe section 26, then, is calculated from the velocities in each of the four planes 62, 68, using a calibrated mathematical relationship.
[0078] A level sensor, preferably an acoustic water level sensor 45, is associated with cartridges 44. In the preferred configuration of figures 1 to 10, for example, each cartridge 44 includes a duct generally designated with number 47, to receive and reliably attach an acoustic water level sensor 45. It should be understood, however, that it is not essential that the water level sensor is physically integrated into the associated cartridge 45, since the water level sensor is located in the cartridges 44 (or close to them).
[0079] The water level sensors 45 provide an accurate measurement of the profile of the water surface in or near the flow meter assembly. Once the average velocity of the water flow has been taken, then to accurately compute the volumetric flow rate, precise measurement of the flow cross-sectional area is required at the location of the acoustic flow meter assembly.
[0080] The preferred arrangements, illustrated and described, with a water level sensor 45 associated with each of the four cartridges 44, guarantee the precise determination of the volumetric flow of water, even when the water surface is disturbed or irregular, such as, for example, in
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17/39 a turbulent flow situation or, alternatively, on a sloping surface.
[0081] Other configurations may include any number of combinations of acoustic transducers 46, as required for other signal path configurations. The use of signal reflectors to replace some of the transducers in each measurement plane, can also be considered. It is not necessary to have four planes 62-68 passing through the acoustic flow meter set 20, and any number of planes can be used, for example, one or several planes, and furthermore, the planes need not be horizontal, as in this configuration.
[0082] Figures 7 to 9 show the use of an acoustic flow meter set 20 for open channels, typically used for water irrigation. A U 70 shaped channel with base 72 and side walls 74, 76 is used to control water irrigation. The flow meter assembly 20 of figure 1 can be used, but does not require access ducts 52 when the installation is not underground. Tube section 26 is not required. This configuration is similar to the construction of the previous configuration, with respect to the fact that four replaceable cartridges 44 are provided. However, the system can be designed with two, three, or more replaceable cartridges 44, as in the previous configuration. The acoustic flow meter assembly 20 is manufactured with a tight tolerance and completely defines the geometry, through which the fluid must pass. This acoustic flow meter set 20 ensures that the fluid always passes through the same geometry through the body of the acoustic flow meter set 20, regardless of the geometry of the channel 70 in which it is installed. Cartridges 44
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18/39 can slide and can be replaced without changing the geometry of the flowmeter assembly 20. Cartridges 44 are individually calibrated with respect to their mounting points on the four hollow legs 36, 38, 40, 42, allowing the cartridges to be interchangeable, without affecting the calibration of the flow meter set 20. The behavior of the acoustic transducer and the geometry requirements are similar to those described in the previous configuration.
[0083] In figure 10, the acoustic flow meter set 20 in figures 7 to 9 includes a control door downstream 80. In this configuration, control door 80 is a guillotine door that can be raised and lowered vertically, to close seal 82. Control port 80 can be separated from flow meter assembly 20, as shown, or integrated into a combined assembly. The control port 80 provides an underpass port, which affects the surface speed of the fluid 84 passing through the flow meter assembly 20, and reduces the influence of the surrounding environment on the flow profile, which passes through the flow meter assembly. flow 20. As described above, the speed is measured at each elevation and adjusted to a ratio used to interpolate the speed at heights between the sampled elevations.
[0084] The surface velocity of fluid 84 is typically not measured, because the elevation of the surface varies in operation and thus it is generally not possible to locate a plane of the acoustic transducer on the surface 86 of the fluid. The fluid velocity is always zero, and the velocity at all elevations under the top transducer plane 62 can be interpolated from values measured in the over / under planes
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19/39 the desired elevation. Unknown surface velocity means that the elevation velocity over the top transducer plane 62 must be extrapolated based on the shape of the velocity profile. This top section of the flow is typically located where the greatest uncertainty in the velocity profile occurs due to the lack of any information regarding velocity on the surface. In the worst case, the speed would be too high or even in the reverse direction to the flow, due to other influences, such as the wind. By locating control port 80 downstream of flow meter assembly 20 and ensuring that the lower end 88 of control port 80 is always submerged, control port 80 maintains a laminar flow profile without turbulence. The fluid speed is zero in front of the control port 80. This low profile is repeatable, and characterized by a flow model, using measurements of the port position and fluid speeds measured by the acoustic transducer system. The repeatability of the flow profile that passes under control port 80 is combined with the flow velocities measured at the sensor plane elevations 62, 64, 66, 68, and used to reduce uncertainty in estimating the surface velocity of the passing fluid by the body of the acoustic flow meter assembly 20.
[0085] The influence of the lower control port 80 reduces the potential variation in the flow pattern through the acoustic flow meter set 20.
[0086] In figure 11, the guillotine control door 80 of figure 10 is replaced by an articulated lift door 90. The control door 90 can be separated from the acoustic flow meter assembly 20, as shown, or integrated into
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20/39 a combined set. Door 90 allows installation in the vertical position, if closed on seal 82, and tilted or horizontal in the open position. Port 90 is held between a frame 92, which includes a horizontal track 94 and vertical track 96. Pins or rollers 98, 100 are located in the corners of port 90 and run on tracks 94, 96. Pins or rollers 98, 100 are move along the respective tracks, to allow opening or closing of door 90. The movement of door 90 is controlled by a motor or hydraulic arm (not shown) coupled to the top 102 of door 90. Raising or lowering door 90, makes it acts as a passage door from below.
[0087] The lift door 90 allows a repeatable laminar flow for a given port position, and keeps the fluid speed on the surface to a minimum, ensuring a
minimal error at computation of flow for the segment between sensors 40 at elevation in plan top sensor 62 and surface gives water 84. THE door in passing by low
downstream 90 creates a surface velocity distribution across the body of the acoustic flow meter assembly 20, providing a more repeatable and predictable measurement than it would be without it. The underpass port 90 provides a non-turbulent or laminar flow. The underpass door 90 allows to create a flow computation algorithm, which is a function of the door position and the speeds measured by the acoustic transducers 46.
[0088] The open channel and closed duct implementations of the acoustic flow meter set 20 are supplied as a single set, completely defining their own geometry, not requiring determination in the field of
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21/39 meter geometry parameters.
[0089] Figures 12 to 17 show an additional variation of the hinged lift door 90 of figure 11. In this configuration, door 120 does not include pins or rollers 89, 100 at both ends of door 90 in figure 11. The control door 120 it can be separated from the acoustic flow meter assembly 20 or integrated into a combined assembly, as shown. The integration of the control door 120 with the acoustic flow meter assembly 20 allows entering the calibrated solution. The top 122 of the door 120 is pivotally mounted on supports 124 and shaft 126. The shaft 126 runs on the guide tracks 128. Horizontal arm members 130 are pivotally mounted on the shaft 126, and allow the door 120 to move through an electric motor or hydraulic means, depending on the requirements. In this configuration, the arm members 130 consist of cables driven by spools 132 that are coupled to the electric motor 134. A gear box 136 drives the spools 132. The cables of the spools 132 are attached to the arm members 130 or shaft 126.
[0090] The position of the door 120 is controlled by an extension arm 138 affixed to the underside 140 of the door 120. The extension arm 138 has a pivot point 142 at its free end. The pivot point 142 is in a position that produces a minimum force (actuation force) on the open door 120. This results in a low cost actuation and a 132-136 drive train system. The preferred location of the pivot point is on the line of the resulting force, with the door in the closed position, typically 2/3 of the depth of the water, under the level of the water surface. The strength of port 120 is due to the water pressure which is equal to:
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22/39 ρ * g * h, at a given depth h under the water surface. Where:
ρ is the fluid's specific weight, and g is the acceleration due to gravity.
[0091] The pivot point is displaced perpendicularly from the bottom side 140 of door 120. The pivot point 142 is restricted to move along a groove or rail 144 at an angle downward towards door 120. The displacement helps to provide a downward force when the door is closed from a fully substantially horizontal position. The offset also ensures that side door seals (not shown) do not cross the rail or groove 144, to prevent leakage around the seals. The angle of the rail or groove 144 also helps with the downward force when the door 120 closes from the substantially horizontally open position.
[0092] To minimize any leakage, a seal 146 is provided on the edge of the free end and sides of port 120. The seal (a bulb seal) engages a slightly raised face 148 on the base 72 and sides 74, 76 and U channel when door 120 is in the vertical position, ie closed. Seal 146 undergoes minimal compression in contact with the U channel.
[0093] Figure 18 shows the situation of the downstream door 120 supporting the water level 84 in the body of the acoustic flow meter under the same flow conditions and depth of figure 19 without obstruction downstream. It can be seen that port 120 maintains a deeper flow through the meter body, so that all transducers are submerged in the water. In figure 19, the water surface lowers as the flow velocity increases through the body of the
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23/39 acoustic flow meter, so that several transducers 48 are not submerged in the water surface. This advantage, discovered by dynamic flow simulations, makes the water withstand situations where there is no water tail downstream. The depth profile is problematic, as many sensor paths are above water, and cannot be used in measurement. A partially open door downstream of the meter supports the water, so that water flows through the meter body at an approximately constant depth, allowing for a greater number of measurements. This allows the flow meter to be used in hydraulic conditions, which would otherwise be incompatible with the measurement with this solution.
[0094] A number of variations to the settings can be introduced to adjust them to the various conditions or requirements of designs or environment. The angular position of the sensor pairs 48 is not restricted to the horizontal planes, it is preferable that it forms an angle of 45 o with the center line. The sensor pairs 48 can form in an angular orientation. Sensor 48 is not limited to a send and receive device to a corresponding pair. Many sensors can receive signals from the transmit sensor.
[0095] In figures 1 to 6, the present invention can be incorporated in situ to an existing pipe. Tubes of sound transmitters 48 can be coupled and welded to an existing pipe, instead of providing a separate acoustic flow meter assembly 20 inserted in the pipe. The set includes 44 cartridges in a modified structure.
[0096] In figures 1 to 19, the acoustic transducers 46 have been described in connection with their operation. The transducers
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Acoustic 24/39 46 preferably work in opposite pairs. The acoustic flow meter assembly 20 measures the acoustic signal travel time in an upstream direction 58B, 60B to the flow direction 50, and also downstream direction 58a, 60a to the flow direction 50, as seen in figures 58a, 58b. The speed of the flow creates a difference in the time of the sound wave path in the upstream and downstream directions. This travel time is recorded and used to determine the average speed of the water along the line of the acoustic trajectory.
[0097] The time difference is recorded using transducers and circuitry that together have intrinsic time delays that add to the actual travel time of the acoustic signal. These circuit time delays and transducers 46 must be subtracted from the recorded acoustic signal travel time, to allow the actual acoustic signal travel time to be determined.
[0098] Circuit and transducer time delays 46 are typically measured in the calibration of the acoustic flow meter set 20 and characterized as a numerical constant that must be subtracted from the measured acoustic signal travel time to calculate the best estimate of the acoustic time. actual acoustic signal path.
[0099] Two constants can be determined by calibrating the acoustic signal travel time measurements in both upstream and downstream directions. However, this will not be necessary as the acoustic signal travel time in the upstream direction is subtracted from the acoustic signal travel time in the downstream direction, so a single calibrated time delay constant is sufficient to
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25/39 calibrate the required time measurement. Under zero flow conditions, the upstream signal travel time is precisely equal to the downstream signal travel time. However, due to the different transducer and delay time characteristics that are used to measure the travel time in the upstream and downstream directions, the measured travel times will not be identical. The difference in the measured travel times reflects the different time delay characteristics in the circuit, which are used to measure the travel times upstream and downstream, and can be determined as a single numerical value in an instant of time, calibrating the measuring system under zero flow conditions of standing water.
[0100] Unfortunately, however, the time delays provided by transducers 46 and measurement circuitry upstream and downstream are not constant, but otherwise, due to environmental influences, such as temperature and pressure, and electronic circuit conditions , such as voltage and temperature. Changes in time delays result from changes in temperature, pressure, operating voltages, and other environmental disturbances. These changes result in a change in the measurement of the differences in the acoustic signal travel times, producing errors in the flow velocity measurement, which are particularly significant for low speed measurements.
[0101] To compensate for changes in time delays in the upstream and downstream circuits, a self-calibrating measurement system capable of calibrating with a reference standard in each flow rate measurement has been proposed, thereby avoiding errors in the measurement of signal travel times
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26/39 acoustic. Although the configuration will be described with
reference to operation in systems in irrigation, the invention it is not limited to this.[0102] Referring to at figures 20 to 25, one system of measurement 200 is represented, as one timer 202, having a
start input 204 and a stop insert 206 along several signal paths through which electrical information is transmitted. The drawings show only two transducers shown in measurement system 200, specifically transducer 46A and transducer 46B from figures 5a and 5b, for clarity. All transducers in pairs 46 of figures 1 to 20 will be connected in the same way.
[0103] As in figure 20, electronic system time delays occur in measurement system 200:
- 5TA is the delay between a starting signal 208 inserted in timer 202 and the corresponding electrical signal received by transducer 46A;
- 5RB is the delay between the acoustic signal received by transducer 46B and the corresponding electrical signal inserted at stop insert 206 of timer 202;
- 5TB is the delay between the starting signal 208 inserted in timer 202 and the corresponding electrical signal received by transducer 46B;
- 5RA is a delay between the acoustic signal received by transducer 46A and the corresponding electrical signal inserted for the insertion of stop 206 of timer 202.
[0104] The acoustic signal travel time from transducer 46A to transducer 46B along path 58A is represented by TFLUIDO A-> B and the signal travel time
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27/39 acoustic from transducer 46B to transducer 46A along path 58B is represented as T FLUID B- > A.
[0105] Figure 21 shows the signal path in the measurement of the acoustic signal travel time from transducer 46A to transducer 46B. The travel time being determined by sending transmission signal 208 to transducer 46A. The transmission signal 208 has an initial signal characteristic, which defines the beginning of the transmission signal. This signal characteristic is inserted into timer 202, and defines the beginning of the time band. Transmission signal 208 is transmitted to transducer 46A which responds by transmitting an acoustic signal to transducer 46B. Transducer 46B converts this acoustic signal into an electrical signal, which is inserted into timer 202, and defines the end of time measurement. The time measured in the transmission of the acoustic signal from transducer 46A to transducer 46B is given by the equation:
T AB = [ ( δΤΑ + T FLUID A-> B + Õ RB)] [0106] This procedure is then repeated in the opposite direction, as shown in figure 22. The travel time of the beep signal from transducer 46B to the transducer 46A is determined by sending a transmission signal 208 to transducer 46B. Transmission signal 208 is an initial signal characteristic, which defines the beginning of the transmission signal. This signal characteristic is inserted into timer 202, and defines the start of the time measurement. Transmission signal 208 is transmitted to transducer 46B, which responds by transmitting an acoustic signal to transducer 46A. Transducer 46A converts the acoustic signal into an electrical signal, which is inserted in timer 202, and defines the end of the
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28/39 time measurement. The time measured in the transmission of an acoustic signal from transducer 46B to transducer 46A is given by the equation:
T BA = [ (ÕTB + T FLUID B-> A + ÕRA) ] [0107]
The difference in the sound wave path times in the upstream and downstream directions, then, is given by:
ΔΤ = T AB - T BA = [(ÕTa + Fluid a-> b + ÕRB)] - [(ÕTB + Fluid b-> a + ÕRA)]
- (Fluid a-> b-Fluid b-> a) + ((ÕTa + ÕRB) - (ÕTb + ÕRA))
- (T fluid a-> b - T fluid b-> a) + X where X is the calibration constant.
[0108] To calculate the calibration constant, the present invention provides additional measurements without using 46A, 46B transducers. This aspect is shown in figure 23. The present invention changes an alternative signal path that passes through the ultrasonic transducers 46A, 46B, to allow measurement of circuit time delays. If transducers 46a, 46B are removed from the circuit and a delay path is used when transducer 46A is used as a transmitting transducer, then the equation will apply:
T AB_calibrated [(ÕTA + õC + ÕRB)] [0109]
This system configuration is shown in the figure
24.
[0110] Similarly, if transducers 46A, 46B are removed from the circuit and the delay path ÕC is used, then when transducer 46B is used as a transmitting transducer, then the equation will apply:
Calibrated T BA [(ÕTB + ÕC + ÕRA) [0111]
This system configuration is shown in the figure
25.
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29/39 [0112] These calibration measurements can then be used in connection with the acoustic signal travel time measurements to eliminate 5TA, 5TB, 5RA, 5RB circuit delay from the acoustic signal time estimates , so that travel times are precisely determined.
1 - The system measurement 200 is first configured, in according to figure 21, to measure FLUID T A—>B;2- The system measurement 200, so is configured, in according to figure 22, to measure T FLUID B—>A;3— The system measurement 200, so is configured, in according to figure 24, to measure T BA_calibration;4— The system measurement 200, so is configured, in according to figure 25, to measure T AB_calibration;
[0113] The four system measurements are then combined to determine the result (T FLUID A— > B * T FLUID B > A) · [0114] If the calibration times are subtracted from the flow measurement times, results:
Tab - Tab_ .calibrated
[(5TA + T FLUID A—> B + 5RB)] - [(5TA + 5C + 5RB) = [ FLUID T A—> B 5C] T BA T BA_calibrated [(5TB + T FLUID B—> A + 5RA)] - [(5TB + 5C + 5RA) = [ FLUID T B—> A - 5C] [0115] The difference in time in transmission then can
determined as follows:
(T AB T AB_calibrated) (T BA T BA_calibrated) [T FLUID A—> B - SC ] - [T FLUID B—> A - 5C] = [T FLUID A—> B —T FLUID B—> A ] [ 0116] As can be seen in the formula above, the electronic circuit delay times have been removed from the
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30/39 acoustic signal travel time, and the difference in signal travel time measurements accurately determined. Using high-speed computing technology, calibration can be done in real time or monitored at predetermined intervals.
[0117] The present invention, in another aspect, provides an additional method of measuring the speed of the fluid passing through the tubes. In the conventional application of acoustic travel time technology to measure the flow rate in the tubes, it is common to use either a single or transverse path technology. These applications are based on whether the tube is fully filled or pressurized. The single path technique assumes a symmetrical velocity distribution around the center line of the tube with opposite and displaced acoustic base and top transducers. The transverse path technique is used where the velocity distribution is not symmetrical around the center line of the pipe. In this transverse trajectory technique, two pairs of acoustic transducers, base and top, displaced and opposite, are used, and their acoustic trajectories are transversal to the center line. Many flow meter applications not only require the condition of detecting a real-time flow meter failure, but also the condition of recording the flow measurement, without loss of data continuity. In particular, this is a requirement for meters for charging water use that require a very high level of quality, and it also applies to remote meters, which require some time to be achieved. Consequently, the failure of an acoustic transducer in the asymmetric velocity distribution produces inaccurate readings depending on
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31/39 of the single trajectory technique, which only provides accurate readings in a symmetric velocity distribution.
[0118] In figures 26 and 27 a tube 250 is shown where a fluid passes in the direction 251. Six pairs of acoustic transducers 252 and 254; 256 and 258; 260 and 262; and 264 and 266, with two pairs of acoustic transducers hidden by their alignment with transducers 260-266, are equally spaced around the tube 250. The position of the acoustic transducers is not restricted to an equally spaced arrangement, but can be placed in other positions to meet other requirements. The number of acoustic transducer pairs may vary, but at least three pairs must be provided. The acoustic trajectories upstream and downstream 270-276, and the hidden trajectories, cross a central point 278 along the central geometric axis 280 of the tube 250. Therefore, measurements along the six trajectories 270-276, and the hidden trajectories , can be made to increase accuracy. If one of the acoustic transducers 252-266 fails, or the transducers are hidden, the measurement can still be made with the remaining acoustic transducers. The failure can be detected and the defective acoustic transducer replaced at a more convenient time.
[0119] This aspect of the present invention provides at least three unique or transverse paths located around the center line 280 of the tube 250. This solution provides at least three independent flow meters, formed by pairs of acoustic transducers in the tube 250. The result allows real-time detection of the failure of any of the independent flow meters, and is also able to maintain
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32/39 flow measurements until the fault is corrected. To achieve this effect using other measurement technologies, for example, magnetic flow meters, three meters installed in series in a pipe section would be needed.
[0120] It is evident to those skilled in the art, that the configuration of figures 26 and 27 can be readily incorporated into the configuration shown in figures 1 to 6.
[0121] In accordance with an additionally preferred aspect of the present invention, and with respect to figures 28 to 35, including the drawings, and hereinafter called “apparatus for measuring travel time located immediately upstream of a control door 500, which may be of type constant in Australian Patent No. 2001/1283691 of this applicant and described earlier in this specification.
[0122] As shown in figures 28 and 29, preferably the apparatus for measuring travel time should be in the form of duct 600, having a cross section of any shape, but, more particularly, circular, as in figure 29, or paralepipedal, as in figure 28, with which cross section the duct 600 will be fixedly or removably associated with the structure of a control or flow port 500.
[0123] In figures 28 The 36, is shown an door in control 500 located in one duct, for example, a channel in irrigation (not shown), The occupation from the door of control is provide a controlled flow in water through channel . The door
Control panel 500 includes a sliding door leaf 501 in a frame 502, having an external door member permanently attached to the floor and sides of the channel or duct.
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33/39 irrigation and an internal sliding frame member on the external frame member. The internal frame member can be connected and separated from the external frame member without having to undergo any civil work on the floor and sides of the channel. This type of inner and outer engine structure can be seen in detail in International Patent Application Specification (PCT) No. PCT AU 2001/00136, the contents of which is included by this reference. The gate panel 501 can be raised or lowered by a lift mechanism 503, such as the mechanism illustrated and described in International Patent Application No. PCT / AU / 2010/000115 of this applicant. However, it should be understood that the present invention is not limited to just one control or flow port.
[0124] A typical installation comprises a control or flow port (of any type) with the measuring device 600 and using any known means at the entrance upstream of a duct or tube located, for example, in a channel, reservoir, or water course. In an alternative installation, a duct connection means can be provided at both ends downstream and upstream of the flow meter assembly, as mentioned earlier in the specification.
[0125] Duct 500 comprises 46 acoustic transducers associated with the generation of acoustic beams, which cross the flow that passes through duct 500.
[0126] It should be understood that the traditional time flow measuring device has for its operation conditions prescribed for both downstream and upstream of the measuring device to ensure minimal disturbance of the flow. These prescribed conditions were established in
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34/39 details, for example, in Australian Standard AS747.
[0127] The arrangement, according to the present invention, is based, for this operation, on a relationship between the flow through the duct and the travel time measurements of acoustic beams that cross the fluid. The relationship, moreover, is based on insertions of the water level values (determined by sensors) and the position of the door. In this regard, reference is made to the International Patent Application PCT / AU 2002/000230 of the applicant.
[0128] In practice, the number of acoustic beams that cross the flow may be a single beam or many beams, and may have different orientations. The preferred arrangement, as in the drawings, includes three pairs of acoustic transducers 46 for the duct 600 of figure 28 and a pair for circular duct 600 of figure 29.
[0129] The relationship between the travel time flow, door opening, and water level can be obtained using data flow experiments, as explained in detail in the applicant's PCT / AU Patent Application 20002/0000230, entitled “Fluid Regulation.
[0130] The arrangement is made in such a way that the duct 600 is substantially fixed in the channel, while the control door leaf 501 remains substantially vertically movable in the channel, allowing the variation of flow through the duct 600. The arrangement uses a seal double 601, as in figures 33 to 36, which runs the entire circumference of port 500. The double seal 601 guarantees the complete sealing of duct 600 upstream and downstream, and also external to it. The door 500 employs a flat face on both sides upstream and downstream of the sheet 501 to guarantee the positioning of the seal along the entire
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35/39 port 500 stroke.
[0131] In the conventional / traditional design of a gate valve, a cap (bonnet) is included in the set to close the duct, to protect against leakage. With an arrangement, according to the present invention, a double seal of the type mentioned above, does not require a lid or equivalent.
[0132] In the configurations of figures 37 and 38, a variation of the configuration of figure 28 with dividers 602 is shown. Figure 37 comprises a single divider 602, while figure 38 comprises a pair of dividers 602. Dividers 602 comprise a plurality of transducers 46 affixed to either side, which cooperate with the acoustic transducers 46 on the opposite walls of duct 600. As can be seen in figure 33, the lengths of the acoustic path (figure 28) are reduced when the acoustic transducers of the configuration of the 37 are located between divider 602 and the internal walls of duct 600 on either side. Similarly, for the configuration in figure 38, the acoustic trajectory extensions will be further reduced because the acoustic trajectory extensions are between the divider 602 and the internal walls of the duct 600, on either side, and between the dividers 602 in the middle part of the duct 600. The reduced length of acoustic trajectory reduces the length of duct 600. In addition, it would still be possible to provide a greater number of 602 dividers, but at a high and unjustifiable cost.
[0133] In the configurations of figures 39 and 40, a variation of the configuration of figure 29 is shown with dividers 602. dividers 602 operate in the same way as for figures 37 and 38. Again, the resulting reduction in the extension of the acoustic trajectory allows a reduction in the length of the duct
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36/39
600.
[0134] The configuration in figure 41 is similar to the configuration in figure 28, but different with respect to the inclination of the control door or drawer 500. The rear angle of the control door or drawer 500 reduces the head space required for its installation . Figures 42 and 43 relate to the use of dividers 602 for the configuration of figure 41 and operate as in the configurations of figures 37 and 38, discussed above.
[0135] Figures 44 to 46 show a schematic drawing of a measurement system in the form of an acoustic travel time flow meter designed to measure fluid flow 700, which does not require any wiring to connect acoustic transducers 46 to a central position. The measurement system 200 described in figures 20 to 25 requires cabling crossing opposite sides of the open channel. The system shows the left bank 702 and the right bank 701. Conventionally, cabling may be required to cross the river 706 from bank 702 to bank 704. As it may be impossible to excavate the channel bed 706 to install the cables, this configuration does not require the use of cabling or, at least, limit its use along the right and left margins 702, 704.
[0136] Acoustic transducers 46 are schematically shown affixed to the right and left banks 702, 704 of the river to facilitate description, but it should be understood that they can also be contained in 44A cartridges, as previously described, and inserted in a flow meter assembly acoustic 20 on the river or canal.
[0137] To be self-contained, 44A cartridges can
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37/39 contain acoustic transducers 46, as previously described. The cartridge 44A contains the required electronic components and the processing circuit can be powered by a solar panel 708. The telemetry radio 712 allows the generation of RF signals, which can be sent and received through a radio antenna 710. The data can be sent to a central location for storage and further processing.
[0138] Figure 44 shows the use of the travel time flow meter, where the travel time flow meter measures the flow by the standard travel time method. The flow meter consists of two or more cartridges 44 that supply their own power to a radio communication link, shared acoustic transducers 46 and synchronization radio signal, used to synchronize the signal by sampling the system clock on each cartridge 44A.
[0139] At a minimum, two 44A cartridges are installed, one on either side of the 702, 704 margins. Four 44A cartridges can also be installed as shown in figure 44 - two per side - to provide the standard cross-path measurement arrangement. Additional pairs of cartridges can be used to provide additional velocity information in the flow channel.
[0140] The 44A cartridge pairs act alternately as an acoustic transmitter and receiver. For example, cartridge 714 acts as a transmitter and cartridge 716 as a receiver, receiving acoustic signal 718, transmitted by cartridge 714. Cartridge 714 records the time of the triggering event in its high resolution timing circuitry and cartridge 716 records the reception event time in your circuit
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38/39 high resolution timing. The timing circuit of each cartridge is a high-speed binary counter, initialized to zero, and following the count. Each count in these counters is updated every 10 picoseconds, and a single count increment represents a time of 10 picoseconds. The transmission event is captured by the circuitry in the cartridge 714 and the timing count value, at this moment, is stored in a register in the cartridge 714. The reception event is captured by the circuitry in the cartridge 716 and the value of the time count, at this point, stored in the register on cartridge 716. However, the counter on cartridge 714 is not synchronized with the counter on cartridge 716 and, therefore, the time difference between the register value stored in cartridge 716 and the value stored in cartridge 714, is indeterminate. To synchronize the time stamp value on the cartridges, an RF synchronization pulse is transmitted from cartridge 714 to cartridge 716, before the clock. The clock runs between the two cartridges 714, 716 at the speed of light (3 * 10 6 m / s), that is, the time elapsed for a spacing between cartridges of 100 meters is 333 nanoseconds. This RF pulse is captured by both timing systems in cartridges 714, 716 and provides a common time value, called the trigger event and reception event in the two time circuits of the cartridges. The acoustic travel time is then calculated by subtracting the trigger event time from the reception event time. Cartridges 714, 716 then switch functions, so the transmitting cartridge becomes the receiving cartridge, and vice versa. The acoustic travel time in the reverse direction is then calculated, allowing
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39/39 a differential travel time, which will be recorded, and used to deduce the flow rate in the channel.
[0141] The present invention is to be understood as encompassing many additional modifications, as should be readily apparent to those skilled in the art, and will be determined within the extended scope of the invention, as established within the extended nature and specific configurations, by way of example.
权利要求:
Claims (12)
[1]
1. Lift door assembly, including a door member (501) slidable within a frame (502) and the aforementioned door member (501) which can be raised and / or lowered between respective closed and open configurations, characterized by the fact that said structure (502) is attached to, and upstream to, an apparatus (600) for measuring fluid passage times by means of acoustic signals, said apparatus (600) in the form of a duct (600), having one or more opposite confronting pairs of acoustic transducers (46).
[2]
2. Assembly according to claim 1, characterized in that the structure (502) includes a double seal (601) arranged around its entire periphery.
[3]
3. Assembly according to either of claims 1 or 2, characterized in that the said duct (600) has a circular or parallelepipedal cross section.
[4]
4. Set, according to claim 3, characterized by the fact that the aforementioned cross section is square or rectangular.
[5]
5. Assembly according to any one of claims 1 to 4, characterized in that said door member (501) and said structure (502) are substantially vertically oriented.
[6]
6. Assembly according to any one of claims 1 to 4, characterized in that said door member (501) and said structure (502) are angled or inclined in relation to said duct (600).
[7]
7. Assembly according to any one of claims 1 to 6, characterized by the fact that it additionally includes
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2/3 a divider (602) within said duct (600), said divider (602) having one or more opposite pairs of acoustic transducers (46) to cooperate with said one or more opposite pairs of acoustic transducers (46) in said pipeline (600).
[8]
8. Assembly according to any one of claims 1 to 6, characterized in that a plurality of dividers (602) is located in said duct (600), with each divider (602) having one or more opposite pairs of acoustic transducers (46) to cooperate with said one or more opposite pairs of acoustic transducers (46) in said duct (600) and / or acoustic transducers in opposite dividers (602).
[9]
9. Set, according to any of the claims of
1 to 6, characterized by the fact that it includes at least three pairs of acoustic transducers (252-266), with each pair of the mentioned acoustic transducers (252, 254) being located on opposite sides of the said duct (600), and longitudinally displaced along the aforementioned pipeline (600), to provide acoustic transducers upstream and downstream (252, 254), with each pair of acoustic transducers (252-266), in use, having their acoustic trajectories intersecting at one point ( 278) along the geometric axis of said duct (600) to provide redundancy in the flow measurement through said duct (600), if one of the said acoustic transducers (252-266) fails.
[10]
10. Lift door assembly, including a sliding door member (501) within a frame (502) and said door member (501) can be raised and / or lowered between respective closed and open configurations, characterized by the fact that said structure (502) is
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3/3 attached to, and upstream to, an apparatus (600) for measuring passage times of acoustic fluid signals, the said apparatus (600) being in the form of a duct (600) attached to the said structure (502) and said duct (600) having one or more opposite pairs of acoustic transducers (46).
[11]
11. Assembly, according to claim 2, characterized by the fact that the said double seal (601) guarantees the complete sealing of said duct (600) upstream and downstream, and also external to it to guarantee the sealing along the entire course of said door member (501).
[12]
12. Assembly according to claim 1, characterized in that one or more opposite acoustic transducers (252, 254) are diagonally directed towards each other.
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公开号 | 公开日
MX2012002121A|2012-06-19|
CL2012000414A1|2012-08-31|
BR112012003537A2|2016-03-08|
EP2467680A1|2012-06-27|
NZ705352A|2016-07-29|
CN102575950A|2012-07-11|
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EP2467680A4|2017-12-27|
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CN107356296A|2017-11-17|
US20150082911A1|2015-03-26|
AU2010283959A1|2012-03-22|
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ZA201201428B|2013-10-30|
MX341582B|2016-08-25|
US20140338466A1|2014-11-20|
MX346622B|2017-03-27|
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CN104075757A|2014-10-01|
US20130239698A1|2013-09-19|
WO2011020143A1|2011-02-24|
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NZ598472A|2014-07-25|
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MX364336B|2019-04-23|
CA2771310A1|2011-02-24|
MX344270B|2016-12-09|
CA2948307A1|2011-02-24|
ZA201305813B|2016-03-30|
CA2771310C|2017-12-19|
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法律状态:
2019-01-08| B06F| Objections, documents and/or translations needed after an examination request according [chapter 6.6 patent gazette]|
2019-07-09| B06T| Formal requirements before examination [chapter 6.20 patent gazette]|
2019-12-10| B09A| Decision: intention to grant [chapter 9.1 patent gazette]|
2020-02-18| B16A| Patent or certificate of addition of invention granted [chapter 16.1 patent gazette]|Free format text: PRAZO DE VALIDADE: 20 (VINTE) ANOS CONTADOS A PARTIR DE 18/08/2010, OBSERVADAS AS CONDICOES LEGAIS. |
优先权:
申请号 | 申请日 | 专利标题
AU2009903893A|AU2009903893A0|2009-08-18|Flow meter assembly|
AU2009903893|2009-08-18|
AU2009905149A|AU2009905149A0|2009-10-22|Flow meter assembly|
AU2009905149|2009-10-22|
AU2010902414|2010-06-02|
AU2010902414A|AU2010902414A0|2010-06-02|Flow meter assembly|
PCT/AU2010/001052|WO2011020143A1|2009-08-18|2010-08-18|Flow meter assembly, gate assemblies and methods of flow measurement|
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