MONITORING OF A FLUIDIC FREE JET

Abstract

A system and method for monitoring a dispensed fluid jet with an oscillation nozzle, comprising a main channel and at least one secondary channel surrounding the main channel, wherein the nozzle has an inlet and an outlet for an air flow defining a flow axis running centrally through the main channel, characterized in that the secondary channel comprises a drill hole.

Claims

1. An oscillation nozzle, comprising a main channel and at least one secondary channel surrounding the main channel, wherein the nozzle has an inlet and an outlet for an air flow defining a flow axis running centrally through the main channel, characterized in that the secondary channel comprises a drill hole.

2. The nozzle according to claim 1, wherein the outlet comprises a sensor for measuring the oscillation of the air flow.

3. The nozzle according to claim 2, wherein the sensor is a pressure sensor.

4. The nozzle according to claim 1, further comprising a second secondary channel which surrounds the main channel opposite of a first secondary channel.

5. A system comprising: an oscillation nozzle, comprising a main channel and at least one secondary channel surrounding the main channel, wherein the nozzle has an inlet and an outlet for a fluid defining a flow axis running centrally through the main channel, characterized in that the secondary channel comprises a drill hole; and a sensor for sensing the oscillation frequency.

6. The system according to claim 5, wherein the sensor is arranged within the outlet of the nozzle.

7. The system according to claim 5, wherein the sensor is a pressure sensor.

8. The system according to claim 5, comprising a control member connected to the pressure sensor for monitoring the oscillation frequency to a predefined intended frequency.

9. The system according to claim 5, wherein the outlet of the nozzle comprises a sensor for measuring the oscillation of the air.

10. The system according to claim 5, wherein the nozzle comprises a second secondary channel which surrounds the main channel opposite of a first secondary channel.

11. A method for monitoring a dispensed fluid jet, comprising the steps of: a. providing an oscillating flow by injecting a constant air flow in an oscillation nozzle comprising a main channel and at least one secondary channel surrounding the main channel, wherein the nozzle has an inlet and an outlet for an air flow defining a flow axis running centrally through the main channel, wherein the secondary channel comprises a drill hole; b. determining an oscillation frequency of the air flow; c. injecting a fluid jet and in parallel monitoring frequency, amplitude and phase of the air flow; d. determining the time of the fluid jet for passing the oscillation nozzle; and e. calculating the fluid volume from the determined passing time and known fluid flow rates.

12. The method according to claim 11, wherein the dispensed fluid has a volume of maximum 50 l.

Description

BRIEF DESCRIPTION OF THE FIGURES

[0033] The invention will be described based on figures. It will be understood that the embodiments and aspects of the invention described in the figures are only examples and do not limit the protective scope of the claims in any way. The invention is defined by the claims and their equivalents. It will be understood that features of one aspect or embodiment of the invention can be combined with a feature of a different aspect or aspects of other embodiments of the invention, in which:

[0034] FIGS. 1A-1D show pneumatic sensors of the state of the art. FIG. 1A shows a stagnation pressure sensor, FIG. 1B shows a ring barrier sensor, FIG. 1C shoes a counter barrier sensor, FIG. 1D shows a barrier sensor.

[0035] FIGS. 2A-2F illustrate an oscillation nozzle.

[0036] FIG. 3 shows an oscillation nozzle with a drill hole in a secondary channel.

DETAILED DESCRIPTION OF THE INVENTION

[0037] The technical problem is solved by the independent claims. The dependent claims cover further specific embodiments of the invention.

[0038] The present invention is based on an oscillation nozzle, which is available in the market in different embodiments. The oscillation nozzle is supplied with a fluid flow which is set in oscillation by the geometry of the nozzle itself. This results in an oscillation jet at the outlet of the nozzle.

[0039] FIG. 2A-F shows an oscillation nozzle 1. The air flow starts with a main air flow (bold arrows) passing through the middle of the main channel 15 and leaving the outlet 30 of the nozzle without oscillation (FIG. 2A). Because of asymmetries and turbulences, the air flow splits into main air flow and a first secondary side flow (dotted arrows). Said first secondary air flow goes through the upper secondary channel 10 (FIG. 2B) and deflects the main air flow so that it adheres to one side of the main channel 15 (FIG. 2C), due to the so called Coanda-effect. The deflected main air flow leaves the oscillation nozzle with an angle and splits in the main channel again so that a second secondary air flow goes through the lower secondary channel 11 at the opposite side (FIG. 2D). In parallel the first secondary air flow weakens and changes its direction in the upper secondary channel (FIG. 2D). The main air flow separates as a consequence from the wall of main channel 15 to which it adhered so far and adheres to the opposite side of the main channel 15 so that the angle with which it leaves the oscillation nozzle changes too (FIG. 2E). The described process will repeat itself iteratively and as a result (FIG. 2F), the jet leaves the nozzle outlet with changing angles having different directions. Depending on the specific geometry and the volume flow, the oscillation frequencies of the nozzle may vary. It is to be noted that the terms upper and lower are only used regarding the description of FIGS. 2A-F and shall not be understood as limiting regarding the orientation of secondary channels or secondary air flows.

[0040] Oscillation nozzles are mostly used for cooling, distribution or mixing of fluids or for cleaning purposes. The amount of the supplied volume flow is proportional to the oscillation frequency of the nozzle.

[0041] The application of an oscillation nozzle ensures the measurement of a robust periodic signal at the pressure sensor. The present invention uses the secondary air flow, which is not strong enough to deflect the fluid jet but is sufficient to change the direction of the main air flow of the oscillation nozzle. When the fluid jet interacts with the air flow of the nozzle, the secondary air flow is reduced and therefore the oscillation frequency and the amplitude of the primary air flow is changed. It is therefore possible to detect the fluid jet by the change of the oscillation frequency and amplitude with the pressure sensor. Using this method of the present invention, it will possible to measure the exact time that the fluid needs to pass the nozzle, and therefore to determine the total amount of fluid. Contamination by droplets or other substances does not lead to a negative impact on the system, as it is permanently traversed by air and cleans itself. If there is a drop in the nozzle geometry, this will be blown out by the volume flow, which constantly changes its direction.

[0042] The effect of external disturbances or the total failure of the system can be evaluated by a change in the oscillation in combination with the amplitude signal, so that a robust measurement is guaranteed.

[0043] The present invention uses a drill hole 5 in a secondary channel 10 of the oscillation nozzle 1 to influence the frequency of the system and the amplitude of the measured signal (FIG. 3 left part). Due to the fluid-gas interaction, the secondary air flow is reduced by the fluid jet 12, which causes the amplitude as well as the frequency of the signal to drop (FIG. 3 right part). This difference is then measured by a pressure sensor 20. The drill hole 5 in the secondary channel 10 also provides an asymmetry of the system, which ensures reproducible starting conditions for the oscillation.

[0044] The advantages of the invention can be summarized as follows: [0045] f. Negligible beam deflection: Due to the low air flow in the secondary channel, the free fluid is only slightly deflected due to the low air flow. This small deflection additionally is compensated by a constant change of direction in the secondary channel (compared to FIG. 2). [0046] g. Flexibility: Detection of gases, liquids (regardless of diameter, amount, drops, bubbles, foam) and solids is possible, regardless of the optical properties. [0047] h. Self-Cleaning: A self-cleaning regarding small drops, dirt particles etc. is ensured by a permanent flow through the nozzle with air. [0048] i. Periodic Signal: The Oscillation itself and the change of the oscillation frequency and the amplitude of the measured signal ensures a very robust measurement/system. Slammed doors for example will only change the amplitude but not the frequency of the signal. Additionally, the frequency of a disturbance will be different in comparison to the system frequency and can be blocked by a suitable filter. The oscillation also allows a self-test of the system, as the signal can be measured without an interruption of the air flow by the fluid jet.

[0049] It is possible to guide the fluidic free jet not through the control channel of the oscillation nozzle, but at any other point through or behind the nozzle, which changes the oscillation behavior. The positioning of the pressure sensor can be changed. For example, the oscillation of the nozzle at a laterally offset position may be determined by one or more sensors. This also applies to the angle at which the oscillating beam hits the sensor. The task of the sensor is to measure the oscillation of the air flow at the outlet 30 of the nozzle. This can be done by various methods, like a pressure sensor, a microphone or thermal measurement.

[0050] In order to improve the pressure signal, the geometry of the oscillation nozzle 1 can be further optimized. Through an adjustment of specific geometry parameters like the nozzle length, meaning the distance between in- and outlet of the nozzle, it is possible to vary frequency of the oscillation air flow, as well as by changing the angle and diameter at the outlet.

[0051] The foregoing description of the preferred embodiment of the invention has been presented for purposes of illustration and description. It is not intended to be exhaustive or to limit the invention to the precise form disclosed, and modifications and variations are possible in light of the above teachings or may be acquired from practice of the invention. The embodiment was chosen and described in order to explain the principles of the invention and its practical application to enable one skilled in the art to utilize the invention in various embodiments as are suited to the particular use contemplated. It is intended that the scope of the invention be defined by the claims appended hereto, and their equivalents. The entirety of each of the aforementioned documents is incorporated by reference herein.

REFERENCE NUMERALS

[0052] 1 oscillation nozzle [0053] 5 drill hole/detection hole [0054] 10 upper secondary channel [0055] 11 lower secondary channel [0056] 12 fluid jet [0057] 15 main channel [0058] 20 pressure sensor [0059] 30 outlet nozzle