A METHOD AND A DEVICE FOR DETERMINING THE FLOW RATE OF A FLOWING MEDIUM

Abstract: In a method for determining the flow rate of a fluid flowing in a channel (2), the fluid being constituted by a liquid or a gas, two pulse shaped, oscillating signals are sent through the medium with one signal directed against (14) and the other signal directed with (12) the flow direction (4) of the fluid. The transmitted signals are received and the flow rate is determined by means of the phase shift between the received, pulse shaped signals caused by the flow of the fluid. The phase shift (20) between the signals is determined while compensating for the dwell time of the pulse shaped oscillating signals in the fluid.

Description: A method and a device for determining the flow rate of a flowing medium The present invention relates to a method and a device for determining the flow rate of a fluid flowing in a channel, the fluid being constituted by a liquid or a gas. It is previously known to determine the flow rate of a fluid flowing in a channel by sending two pulse shaped, oscillating signals through the fluid, one of the signals being directed against and the other signal being directed with the flow of the fluid, whereupon the signals are received and the flow rate is determined by means of the phase shift between the received, pulse shaped signals, caused by the fluid flow. The signal sent with the fluid flow will more rapidly reach the signal receiver than the signal sent against the fluid flow, and this provides for a phase shift between the two signals by means of which it is possible to determine the flow rate. It is when using this method for determining the flow rate known to use a device consisting of two signal generators positioned at a distance from each other in the direction of the fluid flow, the signals being sent from each of the signal generators against the other signal generator, the signal generators being switched over to signal receivers before the transmitted pulse shaped signals arrive to the signal generators. As the speeds of the signals in the fluid are different at different fluids and also in one and the same fluid if this has different pressures and temperatures the dwell time of the pulse shaped oscillating signals in the fluid will be different which causes that the phase shift between the signals is different even if the flow rates of the fluids are the same. This is of course a great disadvantage of the previously known method for determining the fluid rate as the determination is thereby less exact. In another previously known method for determining the flow rate of a fluid flowing in a channel there is sent a pulse shaped, oscillating signal from a first point to a second point which points are positioned at a distance from each other in the direction of flow, whereupon the signal arriving to the second point is digitized and the digitized representation of the signal is registered in an electronic memory. Thereupon a pulse shaped, oscillating signal is sent in the opposite direction, i.e. from the second to the first point, whereupon the signal is in the same way digitized and registered in the electronic memory. Because of the fact that one signal moves with the flow and the other signal moves against the flow in the fluid there is provided a phase shift between the signals, and this phase shift is used for determining the flow rate. In this previously known method it is a drawback that the signals are not sent and received at the same time which provides that a temporary variation in the flow rate will have an influence on the determination of the flow rate. A further drawback is that extremely expensive circuits are required for conducting this method. The object of the invention is to provide a method and a device for determining the flow rate of a fluid flowing in a channel, which obviates the lacking exactness in the methods described above and makes it possible to use less expensive circuits for conducting the different functions. In order to comply with this object the method according to the invention is characterized in that the determination of the phase shift between the signals is conducted while compensating for the dwell time of the pulse shaped oscillating signals in the fluid. Thus, the phase shift between the signals is corrected with regard to the speed of the signals in the fluid so that the phase shift which is utilized for the determination of the fluid rate is constituted by the phase shift between the signals present at one and the same dwell time for the signals in the fluid. It is in the method according to the invention preferred that the two pulse shaped oscillating signals are concurrently sent from one signal generator each, the signal generators being positioned at a distance from each other in the direction of flow of the fluid, towards one signal receiver each, wherein it is suitable to use signal generators which can be switched over to signal receivers. Thereby, the two pulse shaped oscillating signals are sent from each of the signal generators towards the other signal generator and the signal generators are switched over to signal receivers before the transmitted pulse shaped signals arrive thereto. In the method according to the invention it is preferred that the signals are sent and received at different sides of the channel and that the determination of the phase shift between the signals is conducted under compensation also for the angle between the direction of movement of the signals and the direction of flow of the fluid. It is suitable that each of the signal generators is supplied with a sinusoidal, pulse shaped voltage which by means of the signal generators is converted into an ultra- sonic signal which is through the flowing fluid supplied to the signal receiver and is thereby converted into a sinusoidal pulse shaped voltage. The sinusoidal, pulse shaped voltages from the signal receivers are supplied to an analogue phase detector for determining the phase shift between the sinusoidal pulse shaped voltages. Thereby the channel for the flowing fluid can be constituted by a pipe which consists of a material allowing the ultrasonics to pass without too much damping or abduction. However, the pipe walls should consist of a relatively homogenous material which provides for better and cleaner signals. I order to avoid the problems which can appear when the ultrasonic passes the pipe walls it is possible also to position the signal generators inside the pipe. The invention comprises also a device for conducting the method. The invention shall in the following be described with reference to the accompanying drawings. Fig. 1 is a schematic representation showing a device according to the invention illustrating the principles constituting the basic idea of the invention. Figs. 2, 3 and 4 are schematic representations of alternative devices according to the invention. Fig. 5 shows the method and the device according to the invention in the form of a logic circuit. Fig. 6 illustrates in the form of a block diagram the electronic circuit included in the device according to the invention. The device schematically shown in Fig. 1 is intended for determining the flow rate of a fluid, for example a liquid, flowing through a pipe 2 in the direction of the arrows 4. The device comprises two sensor units 6 and 8 connected with the pipe 2 and an electronic computer unit 10. The sensor units 6 and 8 are constituted by switchable transmitters/receivers for ultrasonics and are positioned at opposite sides of the pipe 2 at a distance from each other in the longitudinal direction of the pipe and adjusted so that ultrasonics transmitted from one of the sensor units 6 or 8 hit the other sen- sor unit 8 or 6. The sensor units 6 and 8 are during a predetermining time and con- currently supplied with a sinusoidal voltage pulse. The voltage pulses are in the sensor units transformed into one ultrasonic pulse by means of piezo-electric elements positioned in the sensor units. The ultrasonic pulse created in the sensor unit 6 leaves the sensor unit in the direction shown by means of the arrow 14 towards the sensor unit 8, at the same time as the ultrasonic pulse created by the sensor unit 8 leaves the sensor unit 8 in the direction shown by means of the arrow 14 towards the sensor unit 6. When the ultrasonic pulses have left the sensor units 6 and 8 these are switched over to receiving positions so that the sensor unit 6 can receive the ultrasonic pulse from the sensor unit 8 and the sensor unit 8 can receive the ultrasonic pulse from the sensor unit 6, when the ultrasonic pulses arrive to the sensor units 6 and 8, respectively. When the ultrasonic pulses arrive to the sensor units 6 and 8 they are transformed to sinusoidal voltage pulses by means of the piezo-electric elements arranged in the sensor units, and these voltage pulses are transferred to the electronic unit 10. It is realized that the two ultrasonic pulses which are transmitted through the fluid flowing through the pipe 2 move with the same speed in relation to the flowing fluid. This speed is defined by the speed at which said fluid transmits sound at existing conditions with regard to temperature and pressure. It is realized also that the ultra- sonic pulses will be transmitted with different speeds in relation to the sensor units 6 and 8, as the ultrasonic pulses from the sensor unit 6 move with the flow direction of the fluid while the ultrasonic pulses from the sensor unit 8 move against the flow direction of the fluid. This difference in the speeds of the ultrasonic pulses in relation to the sensor units provides that the ultrasonic pulse leaving the sensor unit 6 will reach the sensor unit 8 before the ultrasonic pulse leaving the sensor unit 8 will reach the sensor unit 6. This time difference is determined by the flow rate of the flowing medium but also by the speed of the ultrasonic pulse in the fluid and the angle of the ultrasonic pulses in relation to the flow direction of the fluid. The time difference at which the ultrasonic pulses arrive to the sensor units 6 and 8 provides for a phase shift between the two sinusoidal voltage pulses created by the piezo-electric crystals in the sensor units 6 and 8. Thus, the sinusoidal voltage pulses 16 and 18 which are schematically shown in Fig. 1 will present a phase shift 20, which as mentioned above is mainly determined by the flow rate of the fluid in the pipe 2 but it is also influenced by the speed of the ultrasonic pulses in the medium and the direction of movement of the ultrasonic pulses in relation to the flow direction of the flowing fluid. The electronic unit 10 records the time which it takes for the ultrasonic pulse to move from the sensor unit 6 to the sensor unit 8, the phase shift 20 being in the electronic unit 10 corrected with regard to different ultrasonic speeds in the medium flowing through the pipe 2. Subsequently to the correction the sinusoidal voltage pulses are transmitted to an analogous phase detector in which the phase shift between the pulses is determined. It is thereby also considered what frequency has been used, and the result is used for defining with high accuracy the time difference between the voltage pulses and thereby the flow rate of the fluid in the pipe 2. When defining the sound speed in the fluid the above time which it takes for the ultrasonic signals to pass between the sensor units 6 and 8 is related to the passed way, i.e. the size of the inner diameter of the pipe and the angle of the signal direction in relation to the flow direction of the flowing fluid. Thus, the calculations conducted in the electronic unit 10 are as follows: a) the speeds of the ultrasonic signals in the fluid are determined by relating the time taken for the ultrasonic signals to pass from the sensor unit 6 to the sensor unit 8 to the inner diameter of the pipe 2 and the angle of the signal direction in relation to the direction of movement of the fluid, b) the phase shifts of the signals are determined and are related to the frequency used so as to provide for the same output signal irrespectively of the frequency which has been used, and c) the determined phase shift is related to the existing sound speed so as to provide for the same output signal irrespectively of the speed of the sound in the fluid, whereupon the last mentioned output signal can be directly utilized for defining the flow rate of the fluid in the pipe 2. Example 1 When using the device according to Fig. 1 and at the following values of the inner diameter of the pipe, the angle between the transmission direction of the ultrasonic signals and the flow direction of the fluid, the frequency of the signals and the phase shift the following calculations give the value of the flow rate of the fluid. Inner diameter of the pipe: 200 Angle: 20° Frequency: 2 MHz Fluid: Water, sound velocity 1390 m/sec Time unit: Nanosec Digital resolution, phase shift: 1024 bites Digital resolution, time for the 200 ns (for calculating the sound velocity signal in the pipe: in the fluid) Measurement of phase shift: Comments: The digital reading of the analogous measurement of the phase shift means that the method gives by means of very simple means a time resolution of about a half nanosecond in this example. Measurement of the sound velocity in the fluid: (Minimal influence if up-stream or down-stream is selected therefor) Comments: The proportionately long time which it takes for the signal to pass the fluid in relation to the changes of this time caused by the influence from the flow means that it is in practice possible to disregard the influence of the flow at this measurement. In this example there is provided for an accuracy of 765 steps for a sound velocity in the fluid of 1390, i.e. a resolution of 1390/765 = 1.8 m/sec. 1.8 m/sec divided by the sound velocity 1390 gives a maximum error of 0.12%. Example 2 Preferences: Same as above but with a change of the sound velocity in the fluid (for example caused by a change of temperature). Fluid: Water, sound velocity 1430 m/sec. Measurement of phase shift: Measurement of the sound velocity in the fluid The digital values given in the two examples mentioned above can by being related to the used angle and the used frequency in a simple way be converted to the real values of time differences and sound velocities. This does in turn give the flow rate in the fluid irrespectively of the sound velocity existing in the fluid and the used frequency. In Figs. 2, 3 and 4 there are shown alternative ways of connecting sensor units to a pipe through which the fluid flows. In Fig. 2 there is shown a pipe 2a through which the fluid flows in the direction of the arrows 4a. Two sensor units 6a and 8a of the same kind as the sensor units 6 and 8 according to Fig. 1 are positioned at the same side of the pipe. The sensor units 6a and 8a create in the same way as the sensor units according to Fig. 1 ultrasonic pulses which are sent in the directions 12a and 14a. The ultrasonic pulses bounce against the wall of the pipe 2a opposite to the sensor units 6a and 8a in such a way that the ultrasonic pulse sent by the sensor unit 6a arrives to the sensor unit 8a and the ultrasonic pulse sent by the sensor unit 8a arrives to the sensor unit 6a. The sensor units 6a and 8a are in the same way as the sensor units according to Fig. 1 switchable between transmission and reception. The fluid flows through the pipe 2b shown in Fig. 3 in the direction of the arrows 4b and the pipe has a large, U-shaped portion 22. In this embodiment the sensor units 6b and 8b are arranged at the ends of the web portion of the U-shaped element 22 of the pipe 2b in such a way that the ultrasonic signals sent from the sensor units 6b and 8b have a direction which is shown by the arrows 12b and 14b and which is the same as the flow direction of the fluid. Thus, in this embodiment there is not required any compensation for angular deviations between the ultrasonic signals and the flow direction of the fluid. In the embodiment shown in Fig. 4 the fluid flows through the pipe 2c in the direction of the arrows 4c, and the sensor units 6c and 8c are centrally supported in the pipe by means of radially extending retainers 24. As in the embodiment according to Fig. 3 the ultrasonic signals are transmitted from the sensor units 6c and 8c in directions shown by means of the arrows 12c and 14c and parallel with the flow direction of the fluid. In this embodiment there is not either required any compensation for angular deviation between the direction of the ultrasonic signals and the flow direction of the fluid but only a compensation for the dwell time of the ultrasonic signals in the fluid, i.e. different sound velocities of the ultrasonics in the fluid. Fig. 5 illustrates the method and the device according to the invention in the form of a block diagram. The block 32 defines the non-variable quantities of the device according to the invention, viz. the inner diameter of the pipe through which the fluid flows and the an- gle between the ultrasonic signals and the flow direction of the fluid. Block 34 defines the start of the device including the adjustment of the frequency of the sinusoidal voltage pulses transmitted to the sensor units. The sensor units transmit as a consequence thereof their ultrasonic pulses in the fluid whereupon the sensor units are switched to the receiving function. If the signals are received which is determined by the block 38 the information is further transmitted to the block 40. If the signals are not received by the sensor units the block 30 orders through the block 32 and adjustment of the frequency of the sinusoidal voltage pulses supplied to the sensor units until a correct reception takes place. In the block 40 is decided whether the amplitude of the ultrasonic signals is positioned above a lower limit value. If this is not the case there is provided for a feed back to the block 42 for providing a new adjustment of the frequency of the sinusoidal voltage pulses. If the value of the amplitude is above the lower limit value the blocks 44 and 46 are ordered to determine the dwell time of the ultrasonic pulses in the fluid and the phase shift between the sinus-shaped voltage pulses created by the ultrasonic pulses in the sensor units which have been switched to reception. The information from the blocks 44 and 46 is supplied to the block 48 which by means of received information, i.e. 1. the inner diameter of the pipe 2. the angle between the ultrasonic signals and the flow direction of the fluid 3. the frequency 4. the dwell time of the ultrasonic signals in the fluid (the velocity of the ultrasonic signals in the fluid) 5. the phase shift calculates the flow rate of the fluid in the pipe. The result given from the device is designated with the block 50. The electronic circuits included in the device according to the invention appears from Fig. 6. The invention can be modified within the scope of the following claims.

Claims: CLAIMS 1. A method for determining the flow rate of a fluid flowing in a channel, the fluid being constituted by a liquid or a gas, wherein two pulse shaped, oscillating signals are sent through the fluid with one signal directed against and the other signal directed with the flow direction of the fluid, the signals are received and the flow rate is determined by means of the phase shift between the received, pulse shaped signals caused by the flow of the fluid, characterized in that the phase shift between the signals is determined while compensating for the dwell time of the pulse shaped oscillating signals in the fluid. 2. A method as claimed in claim 1 , characterized in that the two pulse shaped, oscillating signals are sent through the fluid at the same time. 3. A method as claimed in claim 1 or2, characterized in that the signals are sent and received at opposite sides of the channel and that the determination of the phase shift between the signals takes place under compensation also for the angle between the direction of movement of the signals and the flow direction of the fluid. 4. A method as claimed in any of the preceding claims, characterized in that the pulse shaped signals are sent from signal generators positioned at a distance from each other in the flow direction of the fluid towards one signal receiver each. 5. A method as claimed in claim 4, characterized in that the two pulse shaped oscillating signals are sent from each of the signal generators and against the other signal generator and that the signal generators are switched to signal receivers before the transmitted pulse shaped signals are received by the signal gen- erators. 6. A method as claimed in claim 4 or 5, characterized in that each of the signal generators is supplied with a sinusoidal pulse shaped voltage which is transferred into an ultrasonic signal which is supplied to the signal receiver through the flowing fluid and is by the signal receiver transferred into a sinusoidal, pulse shaped voltage. 7. A method as claimed in claim 6, characterized in that the sinusoidal, pulse shaped voltages from the signal receivers are transferred to an analogue phase detector for determining the phase shift between the sinusoidal voltages. 8. A method as claimed in claim 7, characterized in that the phase shift determined by the phase detector is adjusted with regard to the utilized frequency of the sinusoidal voltages so as to provide the same output signal at one and the same flow rate independently of the used frequency. 9. A method as claimed in claim 8, characterized in that the established output signal is adjusted with regard to the signal velocity present in the fluid for pro- viding the same output signal at one and the same flow rate independently of this signal velocity. 10. A device for determining according to the method of claim 1 the flow rate of a fluid flowing in a channel, comprising two signal generators (6, 8) for transmitting each of two pulse shaped, oscillating signals through the medium, one of the signals being directed against and the other signal being directed with the flow direction of the fluid, two signal receivers (8, 6) and means for defining the phase shift between the received, pulse shaped signals caused by the flow of the fluid, characterized in that the device comprises means for compensating for the dwell time of the pulse shaped, oscillating signals in the fluid when the phase shift is determined.

Inventors: LINDAHL JOERGEN, LINDAHL, JOERGEN
Applicants: LINDAHL JOERGEN, LINDAHL, JOERGEN
Application year: 1999
Main classification: G01F1
IPC codes: G01F1