WO2011055532A1 - Ultrasonic flowmeter - Google Patents

Ultrasonic flowmeter Download PDF

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Publication number
WO2011055532A1
WO2011055532A1 PCT/JP2010/006459 JP2010006459W WO2011055532A1 WO 2011055532 A1 WO2011055532 A1 WO 2011055532A1 JP 2010006459 W JP2010006459 W JP 2010006459W WO 2011055532 A1 WO2011055532 A1 WO 2011055532A1
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WIPO (PCT)
Prior art keywords
ultrasonic
measured
propagation time
wave
amplitude
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PCT/JP2010/006459
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French (fr)
Japanese (ja)
Inventor
裕史 藤井
尋一 後藤
葵 渡辺
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パナソニック株式会社
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Publication of WO2011055532A1 publication Critical patent/WO2011055532A1/en

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    • GPHYSICS
    • G01MEASURING; TESTING
    • G01FMEASURING VOLUME, VOLUME FLOW, MASS FLOW OR LIQUID LEVEL; METERING BY VOLUME
    • G01F1/00Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow
    • G01F1/66Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow by measuring frequency, phase shift or propagation time of electromagnetic or other waves, e.g. using ultrasonic flowmeters
    • G01F1/667Arrangements of transducers for ultrasonic flowmeters; Circuits for operating ultrasonic flowmeters
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01FMEASURING VOLUME, VOLUME FLOW, MASS FLOW OR LIQUID LEVEL; METERING BY VOLUME
    • G01F25/00Testing or calibration of apparatus for measuring volume, volume flow or liquid level or for metering by volume
    • G01F25/10Testing or calibration of apparatus for measuring volume, volume flow or liquid level or for metering by volume of flowmeters

Definitions

  • the present invention relates to an ultrasonic flowmeter that measures the propagation time of ultrasonic waves using a pair of ultrasonic transducers capable of transmitting and receiving and measures the flow rate of a fluid to be measured.
  • the ultrasonic propagation time measurement method used in conventional ultrasonic flowmeters is a method in which a pair of ultrasonic transducers capable of transmitting and receiving are arranged facing each other and one ultrasonic transducer is driven by a burst signal. The ultrasonic wave was transmitted and received and measured by the other ultrasonic transducer.
  • Fig. 6 shows a transmission / reception waveform diagram of the ultrasonic flowmeter.
  • the horizontal axis indicates time, and the vertical axis indicates voltage.
  • the upper side of FIG. 6 shows the driving waveform A of the transmitting-side ultrasonic transducer
  • the lower side of FIG. 6 shows the received waveform B received by the receiving-side ultrasonic transducer.
  • T0 indicates the start point of the drive waveform A
  • T1 indicates the end point of the third wave after the start of drive
  • R0 indicates the reception start time
  • R1 indicates the end time of the third wave after the start of reception.
  • the m-th wave of driving waveform A (m is an integer, in the ultrasonic transducer on the transmission side, an example shown in FIG.
  • the flow measuring device measures the time Tp between the starting point T1 and the end point R1 as the propagation time of the ultrasonic wave, measures the flow velocity of the fluid to be measured using the propagation time, and calculates the flow rate. It was.
  • FIG. 7 shows the configuration of the fluid flow measuring device disclosed in Patent Document 1.
  • This flow measurement apparatus includes an ultrasonic transducer 2 installed in a measurement flow path 1 through which a fluid flows, a drive circuit 3 that drives the ultrasonic transducer 2, a control unit 26 that outputs a start signal to the drive circuit 3, A propagation time measuring unit 5 that measures the propagation time of the ultrasonic wave, an ultrasonic vibrator 7 that receives the ultrasonic wave transmitted from the ultrasonic vibrator 2, an amplifier 6 that amplifies the output of the ultrasonic vibrator 7, and an amplifier 6 And a reception detection circuit 8 that stops the propagation time measurement unit 5 when the magnitude relationship is inverted by comparing the output of the signal and the reference voltage.
  • the changeover switch 10 is generally provided.
  • the changeover switch 10 is used to measure the propagation time of the ultrasonic wave from the upstream side to the downstream side of the measurement flow channel 1 and the propagation time from the downstream side to the upstream side.
  • the reference voltage 25 is set in advance between the amplitudes of the second and third waves.
  • the next zero cross when the received signal exceeds the reference voltage 25 is set to be the third wave.
  • the flow measuring device includes a received waveform amplitude measuring unit 9 for automatically adjusting the reference voltage 25 when the flow measuring device is initially set. In the reception waveform amplitude measuring unit 9, by increasing the reference voltage 25 for detecting reception little by little from a low voltage, a voltage whose propagation time changes can be stored as each amplitude of the reception wave.
  • the propagation time remains Ta because the reference voltage 25 is within the amplitude range of the first wave.
  • the reference voltage 25 is changed from V1 to V3
  • the reference voltage 25 is in a range larger than the amplitude (V2) of the first wave and smaller than the amplitude (V3) of the second wave. Therefore, the propagation time is Tb. Therefore, it can be seen that the voltage at which the propagation time is switched from Ta to Tb, in this example, V2, is the amplitude of the first wave of the received wave.
  • the amplitude (voltage) of each wave from the first wave of the received wave to the peak wave (the wave having the maximum amplitude among the waves constituting the series of received waveforms B) by switching the propagation time. Can be measured.
  • the amplitude of the second and third waves is selected from the measured amplitudes up to the peak wave, and is normally measured between the voltage that is the amplitude of the second wave and the voltage that is the amplitude of the third wave.
  • the hourly reference voltage 25 can be set.
  • the present invention has been made to solve such a problem. In the manufacturing stage, it is not necessary to flow the measured fluid at an actual flow rate to correct the difference in the dimensions of the measurement flow path.
  • An object of the present invention is to provide an ultrasonic flowmeter that can be manufactured at a lower cost.
  • an ultrasonic flowmeter includes a measurement channel for flowing a fluid to be measured for measuring a flow rate, and a pair of ultrasonic channels arranged in the measurement channel and capable of transmitting and receiving ultrasonic signals.
  • a control unit that calculates the flow rate of the fluid to be measured that satisfies the space between the ultrasonic transducers from the propagation time, and a received waveform amplitude measuring unit that measures the amplitude of the mth wave of the received waveform received by the ultrasonic transducer And the difference between the amplitude of each measured waveform of the received waveform and the amplitude of the m-th wave of the normal received waveform, the dimensional difference between the actual measurement channel and the measurement channel preset for flow rate calculation is estimated.
  • the control unit A measurement channel dimension correction unit for correcting the size of the measurement flow path is configured for flow calculation is Configurations which comprises a.
  • the measurement flow path dimension correction unit is configured to determine an actual measurement flow path from a difference between the amplitude of each wave of the measured reception waveform and the amplitude of each wave of the normal reception waveform. And a dimensional difference between the measurement channel set in advance for flow rate calculation may be used.
  • the ultrasonic flowmeter provides a predetermined temperature between the measurement flow path, the ultrasonic transducer, the propagation time measurement unit, the control unit, and the pair of ultrasonic transducers. It is filled with the set fluid to be measured, and the ultrasonic propagation time between the ultrasonic transducers is measured and compared with the normal propagation time set in advance in the control unit. Estimate the difference between the distance between the actual ultrasonic transducers and the distance between the ultrasonic transducers set for flow rate calculation from the difference in propagation time, and set the flow rate calculation in the control unit based on the estimation result And an ultrasonic transducer distance correcting unit that corrects the distance between the ultrasonic transducers that are arranged.
  • the manufacturing stage it is not necessary to flow the measured fluid at the actual flow rate to correct the difference in the dimensions of the measurement flow path, and the manufacturing can be performed at a lower cost than in the past. There is an effect that a possible ultrasonic flowmeter can be provided.
  • FIG. 1 It is a block diagram which shows schematic structure of the ultrasonic flowmeter which concerns on Embodiment 1 of this invention.
  • A is a schematic diagram which shows the propagation path of the ultrasonic wave in the said measurement flow path in case the height dimension of a measurement flow path is a reference value
  • (b) is the propagation path shown to (a).
  • A) is a schematic diagram which shows the propagation path of the ultrasonic wave in the said measurement flow path in case the height dimension of a measurement flow path is higher than a reference value
  • (b) is shown to (a).
  • the present invention includes a measurement flow channel for flowing a fluid to be measured for measuring a flow rate, a pair of ultrasonic transducers arranged in the measurement flow channel and capable of transmitting and receiving ultrasonic signals, A propagation time measuring unit for measuring a propagation time transmitted from one of the ultrasonic transducers until the other ultrasonic transducer receives an ultrasonic signal propagated through the fluid to be measured; A control unit for obtaining a flow rate of the fluid to be measured that fills between the ultrasonic transducers, a received waveform amplitude measuring unit that measures the amplitude of the mth wave of the received waveform received by the ultrasonic transducer, and the measured received waveform Based on the difference between the amplitude of each wave and the amplitude of the m-th wave of the regular received waveform, the dimensional difference between the actual measurement channel and the measurement channel preset for flow rate calculation is estimated.
  • an ultrasonic flowmeter structure comprises
  • the measurement flow channel set as the actual measurement flow channel can be obtained without flowing the measured fluid at the actual flow rate and checking the measurement value error at the manufacturing stage of the ultrasonic flow meter. And the difference in dimensions can be corrected. Therefore, the deviation of the flow rate value due to the dimensional deviation of the measurement flow path can be suitably corrected. Therefore, an expensive flow rate generator is not required in the manufacturing process, and the time required for dimensional correction can be shortened. Therefore, it is possible to manufacture an ultrasonic flowmeter at a lower cost than in the past.
  • the m-th wave measured by the received waveform amplitude measuring unit may be a peak wave.
  • the accuracy of dimensional correction can be improved.
  • the present invention also provides a measurement channel for flowing a fluid to be measured for measuring a flow rate, a pair of ultrasonic transducers arranged in the measurement channel and capable of transmitting and receiving ultrasonic signals, and one of the ultrasonic vibrations
  • a propagation time measuring unit that measures a propagation time until the other ultrasonic transducer receives an ultrasonic signal transmitted from the child and propagated through the fluid to be measured, and between the ultrasonic transducers by calculation from the propagation time.
  • a control unit for obtaining a flow rate of the fluid to be measured to be satisfied a received waveform amplitude measuring unit for measuring the amplitudes of a plurality of received waveforms received by the ultrasonic transducer, and the amplitude and normality of each wave of the measured received waveform Estimate the dimensional difference between the actual measurement flow path and the measurement flow path set in advance for flow rate calculation from the difference between the amplitude of each wave of the received waveform, and based on this estimation result, calculate the flow rate in the control unit.
  • Set the measurement channel dimensions A measurement channel dimension correction unit positive for, may be an ultrasonic flowmeter structure comprises a.
  • the present invention may be configured such that at least one of the plurality of waves measured by the received waveform amplitude measuring unit is a peak wave.
  • the accuracy of dimensional correction can be improved.
  • the present invention also provides a measurement channel for flowing a fluid to be measured for measuring a flow rate, a pair of ultrasonic transducers arranged in the measurement channel and capable of transmitting and receiving ultrasonic signals, and one of the ultrasonic vibrations
  • a propagation time measuring unit that measures a propagation time until the other ultrasonic transducer receives an ultrasonic signal transmitted from the child and propagated through the fluid to be measured, and between the ultrasonic transducers by calculation from the propagation time.
  • the ultrasonic wave set for calculating the distance between the actual ultrasonic transducers and the flow rate from the difference between the measured propagation time and the normal propagation time may be configured to include an ultrasonic transducer distance correction unit that corrects a distance between ultrasonic transducers set for flow rate calculation in the control unit based on the result. .
  • the ultrasonic wave propagation between ultrasonic transducers may be achieved by filling the predetermined fluid to be measured with a predetermined temperature between the pair of ultrasonic transducers.
  • the time is measured, compared with the normal propagation time set in advance in the control unit, and the distance between the actual ultrasonic transducers and the flow rate calculation are set based on the difference between the measured propagation time and the normal propagation time.
  • a distance correction unit between the ultrasonic transducers that estimates a difference in distance between the ultrasonic transducers and corrects a distance between the ultrasonic transducers set for flow rate calculation in the control unit based on the estimation result.
  • the structure provided may be sufficient.
  • FIG. 1 is a block diagram showing an example of the configuration of the ultrasonic flowmeter according to Embodiment 1 of the present invention.
  • the ultrasonic flowmeter includes a pair of ultrasonic transducers 2 and 7, a drive circuit 3, a control unit 4, a propagation time measuring unit 5, an amplifier 6, A reception detection circuit 8, a changeover switch 10, a reception waveform amplitude measurement unit 9, and a measurement flow path dimension correction unit 11 are provided.
  • the ultrasonic vibrators 2 and 7 are installed in the measurement channel 1 through which the fluid to be measured flows, and the ultrasonic vibrators 2 and 7 are driven by the drive circuit 3. Transmission / reception between the upstream ultrasonic transducer 7 and the downstream ultrasonic transducer 2 is switched by a changeover switch 10.
  • the amplifier 6 amplifies the outputs (particularly ultrasonic reception waves) of the ultrasonic transducers 2 and 7 and outputs them to the reception detection circuit 8.
  • the reception detection circuit 8 compares the output of the amplifier 6 with the reference voltage, and stops the propagation time measurement unit 5 when the magnitude relationship is reversed.
  • the control unit 4 controls the ultrasonic flowmeter shown in FIG. Specifically, a start signal can be output to the drive circuit 3 and, as will be described later, an ultrasonic signal transmitted and received between the ultrasonic transducers 2 and 7 by controlling the propagation time measurement unit 5. Calculation of the flow rate of the fluid to be measured that fills the space between the ultrasonic transducers 2 and 7 from the propagation time, and control of the changeover switch 10, the received waveform amplitude measuring unit 9 and the measurement channel size correcting unit 11. The set value is corrected from the output of.
  • the propagation time measuring unit 5 measures the propagation time of the ultrasonic wave between the ultrasonic transducers 2 and 7 used for the calculation under the control of the control unit 4, and also converts the received waveform of the ultrasonic wave into the received waveform amplitude. Output to the measurement unit 9.
  • the received waveform amplitude measuring unit 9 measures the amplitude from the first wave to the peak wave of the received waveform of the ultrasonic wave, and outputs it to the control unit 4 and the measurement flow path dimension correcting unit 11.
  • the measurement flow path dimension correction unit 11 corrects the measurement flow path dimension from the difference between the amplitude of each wave of the received waveform and the amplitude of the reference reception waveform set in advance (details of the correction process will be described later).
  • the control switch 4 sets the ultrasonic transducer 2 to the reception side and the ultrasonic transducer 7 to the transmission side under the control of the control unit 4.
  • the ultrasonic vibrator 2 is driven by the drive circuit 3 and the ultrasonic wave propagated through the fluid to be measured is received by the ultrasonic vibrator 2.
  • the received ultrasonic wave (received wave) is input to the propagation time measurement unit 5 via the amplifier 6 and the reception detection circuit 8, and the propagation time of the ultrasonic wave is measured.
  • the control unit 4 performs an operation for obtaining the flow rate of the fluid to be measured, the control unit 4 acquires the propagation time indirectly from the propagation time measurement unit 5, or the propagation time through a signal transmission path (not shown).
  • the propagation time may be acquired directly from the measurement unit 5.
  • the ultrasonic transducer 2 As the ultrasonic transducer 2, the ultrasonic transducer 7, the drive circuit 3, the amplifier 6, the reception detection circuit 8, and the changeover switch 10, those known in the field of ultrasonic flowmeters are preferably used.
  • control unit 4 is configured by, for example, a microcomputer, and the microcomputer is configured by, for example, a calculation unit and a storage unit, although not illustrated in FIG.
  • the arithmetic unit is composed of a CPU of a microcomputer
  • the storage unit is composed of an internal memory.
  • Various programs are stored in the storage unit, and various set values such as the dimensions of the measurement flow path set in advance for flow rate calculation are stored.
  • the calculation unit executes the above-described calculation for determining the flow rate using the program stored in the storage unit, and corrects the setting value stored in the storage unit as necessary.
  • the storage unit is not limited to the internal memory, and may be configured as an independent memory or may be configured from a plurality of storage devices.
  • the propagation time measurement unit 5, the received waveform amplitude measurement unit 9, and the measurement flow path dimension correction unit 11 may be configured as a logic circuit or the like using a known switching element, subtractor, comparator, or the like. May be a configuration realized by operating according to a program stored in the storage unit, that is, a functional configuration of the control unit 4.
  • the ultrasonic flowmeter is the m-th drive waveform (m is an integer, and is shown in FIG. 6.
  • m is an integer, and is shown in FIG. 6.
  • the reference voltage 25 is set in advance between the amplitudes of the second and third waves, and the received signal (received wave) exceeds the reference voltage 25.
  • the next zero cross is set to be the zero cross at the end of the third wave.
  • the reference voltage 25 is a voltage for detecting reception of a received wave, and the reception waveform amplitude measuring unit 9 adjusts the reference voltage 25 slightly from a low voltage in order to automatically adjust the reference voltage 25 at the initial setting. By increasing the voltage one by one, the voltage whose propagation time changes is stored as the amplitude of each received wave.
  • the propagation time remains Ta because the reference voltage 25 is within the amplitude range of the first wave.
  • the reference voltage 25 is changed from V1 to V3
  • the reference voltage 25 is in a range larger than the amplitude (V2) of the first wave and smaller than the amplitude (V3) of the second wave. Therefore, the propagation time is Tb. Therefore, it can be seen that the voltage at which the propagation time is switched from Ta to Tb, in this example, V2, is the amplitude of the first wave of the received wave.
  • the amplitude (voltage) of each wave from the first wave of the received wave to the peak wave (the wave having the maximum amplitude among the waves constituting the series of received waveforms B) by switching the propagation time. Can be measured.
  • the amplitude of the second and third waves is selected from the measured amplitudes up to the peak wave, and is normally measured between the voltage that is the amplitude of the second wave and the voltage that is the amplitude of the third wave.
  • the hourly reference voltage 25 can be set.
  • the measurement channel size correction unit 11 is configured to control the actual height of the measurement channel 1 (the channel diameter of the measurement channel 1) and the flow rate value in advance. 4 is corrected based on the difference from the reference height dimension stored in the storage section 4 that constitutes 4.
  • ultrasonic waves are transmitted and received in the state where no flow rate is generated in the measurement flow channel 1 during the manufacture of the ultrasonic flowmeter, and the first to nth waves (n is the peak wave) of the received waveform.
  • the received waveform amplitude measuring unit 9 measures the amplitude of each wave up to an arbitrary integer).
  • FIG. 2A shows an ultrasonic wave propagation path when the dimension of the measurement channel 1 is the same as that of the reference
  • FIG. 2B shows an ultrasonic wave reception waveform in this propagation path
  • FIG. 3A shows an ultrasonic wave propagation path when the height dimension of the measurement channel 1 is higher than the reference
  • FIG. 3B shows an ultrasonic reception waveform in the propagation path.
  • the received waveform of the ultrasonic wave passes through the path 12 that goes straight between the ultrasonic transducers 2 and 7.
  • the waveform of the ultrasonic wave and the waveform of the ultrasonic wave that has passed through the path 13 reflected by the inner surface of the measurement channel 1 are combined. Therefore, the received wave received by the ultrasonic transducer 2 is, as shown in FIG. 2B, the received waveform 15 of the ultrasonic wave passing through the path 12 and the received waveform of the ultrasonic wave passing through the path 13.
  • the amplitude 18 a and the amplitude 18 b of each wave are both larger than the amplitude of the reception waveform 15 or the reception waveform 16.
  • the received wave received by the ultrasonic transducer 2 is a combined waveform 20 of the received waveform 15 and the received waveform 19 as shown in FIG.
  • the measurement flow channel 1 can be obtained by comparing the synthetic waveform 20 with the normal waveform (synthetic waveform 17).
  • the difference between the height dimension H and the dimension H ′ can be estimated. That is, as shown in FIG. 3B, the amplitude 21a and the amplitude 21b of each wave (the first wave and the second wave) in the synthesized waveform 20 are the amplitude 18a and the amplitude of the synthesized waveform 17 which is a normal waveform. Since it is smaller than 18b, the actually measured amplitude 21a and amplitude 21b will deviate from the reference amplitude 18a and amplitude 18b. This deviation corresponds to the difference between the height dimensions H and H ′ (dimension deviation).
  • the control unit 4 based on the above principle, the relationship between the amplitude of the combined wave formed when an amplitude shift occurs in each wave of the received waveform and the height dimension of the measurement channel 1,
  • the correction amount is set and stored in advance in the storage unit.
  • the measurement channel dimension correction unit 11 calculates the measurement channel 1 by a preset correction amount based on the difference between the measured amplitude of each wave and the amplitude set and stored in the storage unit in advance. Correct the height dimension above. Thereby, the deviation of the measured value caused by the actual deviation of the dimension of the measurement channel 1 can be corrected.
  • the correction amount may not be stored in the storage unit in advance, but may be calculated and acquired by the calculation unit.
  • the measurement flow path dimension correction unit 11 is provided so that the measured fluid does not flow through the measurement flow path 1 at the actual flow rate when the ultrasonic flowmeter is manufactured.
  • the deviation of the flow rate value due to the dimensional deviation of the measurement channel 1 can be suitably corrected.
  • the correction amount set in the storage unit is based on the measurement result using the predetermined fluid to be measured, and the measurement for performing the correction is also performed using the same predetermined fluid to be measured. .
  • the number of waves whose amplitude is to be measured is described as 2 (first wave and second wave).
  • an arbitrary number of waves from the first wave to the peak wave are measured and compared. It is also possible to do.
  • the peak wave has the largest amplitude in the received waveform. Therefore, if the dimension of the measurement channel 1 is shifted, the difference from the amplitude in the reference case is relative. Become bigger. Therefore, the accuracy of dimensional correction (as well as the accuracy of deviation in flow rate value) can be improved.
  • the accuracy of dimensional correction can be further improved.
  • the number of waves whose amplitude is measured need not be plural.
  • the amplitude may be compared for one wave of the m-th wave (any wave from the first wave to the n-th wave).
  • the reference configuration (particularly, the position where the ultrasonic transducers 2 and 7 are disposed with respect to the measurement flow path 1) employed when determining the correction amount stored in the storage unit is a correction target. It is preferable that the measurement channel 1 is also shared. In other words, it is preferable that the reference configuration is always set to have a predetermined positional relationship. For example, the point where the ultrasonic transducers 2 and 7 are arranged at the center of the cross section of the measurement flow channel 1 is set so as to have a common configuration. Thereby, the correction accuracy can be further improved.
  • FIG. 4 is a block diagram illustrating an example of the configuration of the ultrasonic flowmeter according to the second embodiment.
  • the ultrasonic flowmeter according to the present embodiment has the same basic structure as that of the ultrasonic flowmeter according to the first embodiment, but the measurement flow path dimensions. The difference is that the correction unit 11 is not provided and the ultrasonic transducer distance correction unit 22 is provided.
  • the control unit 23 includes, for example, a calculation unit and a storage unit, similarly to the control unit 4 in the first embodiment.
  • a propagation time (set value) measured using a predetermined fluid to be measured set to a predetermined temperature is set in advance, and the ultrasonic transducers 2 and 7 For the inter-vibrator distance, which is the distance between them, a calculated value (a set value used when calculating the flow rate) is preset.
  • set value a propagation time measured using a predetermined fluid to be measured set to a predetermined temperature
  • a calculated value a set value used when calculating the flow rate
  • other set values may be stored.
  • the ultrasonic transducer distance correction unit 22 may be configured as a logic circuit or the like using a known switching element, subtractor, comparator, or the like, or realized by the arithmetic unit operating according to a program stored in the storage unit. That is, the functional configuration of the control unit 23 may be used.
  • the description thereof will be omitted, and the operation of the ultrasonic transducer distance correction unit 22 will be omitted. explain.
  • the ultrasonic transducer distance correction unit 22 measures the propagation time (measured value) in a state where the measurement flow path 1 is filled with a predetermined fluid to be measured set to a predetermined temperature when the ultrasonic flowmeter is manufactured. Thereafter, based on the difference between the preset propagation time setting value and the propagation time measurement value, the difference between the preset inter-vibrator distance setting value and the actual inter-vibrator distance is obtained. Then, the inter-vibrator distance stored in the storage unit is corrected from the obtained difference. Thereby, the deviation of the measured value can be corrected.
  • FIG. 5 is a block diagram illustrating an example of the configuration of the ultrasonic flowmeter according to the third embodiment.
  • the ultrasonic flowmeter according to the present embodiment has the same basic structure as that of the ultrasonic flowmeter according to the second embodiment. The difference is that a dimension correction unit 11 is provided.
  • the control unit 24 includes, for example, a calculation unit and a storage unit, similar to the control unit 4 in the first embodiment, and the above-described various setting values are set in the storage unit.
  • the basic operation of the ultrasonic flowmeter according to the present embodiment is the same as that of the ultrasonic flowmeter according to the first or second embodiment, it is omitted, and the measurement flow path dimension correction unit 11 and the ultrasonic wave are omitted.
  • the operation of the inter-vibrator distance correction unit 22 will be described.
  • the measurement channel size correction unit 11 stores in advance a measurement value of the amplitude of each wave included in the received wave and a storage unit in a state where the measurement channel 1 is filled with a predetermined fluid to be measured set to a predetermined temperature. Based on the difference from the set amplitude value, the calculated height dimension of the measurement channel 1 is corrected by a preset correction amount, and then the ultrasonic transducer distance correcting unit 22 is corrected. Thus, the deviation of the inter-vibrator distance is corrected.
  • the measurement channel dimension correction unit 11 corrects the dimension of the measurement channel 1 based on the difference between the measured value and the set value of the amplitude.
  • the measurement of the amplitude is almost affected by the deviation of the distance between the transducers. Absent.
  • the ultrasonic transducer distance correction unit 22 corrects the deviation of the inter-vibrator distance by measuring the propagation distance based on the dimension correction of the measurement channel 1. Therefore, the object (amplitude) measured by the measurement flow path dimension correction unit 11 and the object (propagation distance) measured by the ultrasonic transducer distance correction unit 22 are substantially independent measurement objects.
  • the correction accuracy of the deviation between the transducer distances in the ultrasonic transducer distance correction unit 22 can be further improved.
  • the fluid to be measured is placed in the measurement flow channel 1 when the ultrasonic flowmeter is manufactured. Even if the actual flow rate does not flow, it is possible to suitably correct the deviation of the flow rate value due to the deviation of the dimension of the measurement channel 1 and the distance between the ultrasonic transducers 2 and 7 (distance between the transducers). it can.
  • the ultrasonic flowmeter according to the present invention does not require an actual flow rate in the manufacturing stage to correct the difference in the dimensions of the measurement flow path, so that an expensive flow rate generator is not required in the manufacturing process.
  • the time required for correction can be shortened. Therefore, it is possible to manufacture ultrasonic flowmeters at a lower cost than conventional methods, so it is widely used in applications that measure the flow rate of fluids with ultrasonic waves, such as flow measurement standards, gas meters, or water meters. Can be applied.

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  • Physics & Mathematics (AREA)
  • Fluid Mechanics (AREA)
  • General Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Measuring Volume Flow (AREA)

Abstract

Disclosed is an ultrasonic flowmeter which automatically corrects, without actually having a fluid flow, the difference between the actual size of measurement flow channel (1) and a flow channel size for calculating the flow volume, said flow channel size being set in control unit (4). The ultrasonic flowmeter is provided with, for example: a pair of ultrasonic vibrators (2, 7) which can transmit and receive ultrasonic signals; propagation time measuring unit (5), which measures the propagation time required for ultrasonic vibrator (7) to receive the ultrasonic signals transmitted from ultrasonic vibrator (2); control unit (4), which obtains a flow volume from the propagation time; received waveform amplitude measuring unit (9), which measures the amplitude of the waveform received by ultrasonic vibrator (7); and measuring flow channel size correcting unit (11), which corrects the size of the measurement flow channel on the basis of the difference between the amplitude and the amplitude of the specified received waveform. Thus, the difference between the actual size of measurement flow channel (1), and the size set for measuring flow channel (1) in the control unit (4) for calculating the flow volume can be corrected.

Description

超音波流量計Ultrasonic flow meter
 本発明は、一対の送受信可能な超音波振動子を用いて超音波の伝搬時間を計測し、被測定流体の流量を計測する超音波流量計に関するものである。 The present invention relates to an ultrasonic flowmeter that measures the propagation time of ultrasonic waves using a pair of ultrasonic transducers capable of transmitting and receiving and measures the flow rate of a fluid to be measured.
 従来の超音波流量計に用いられている超音波伝搬時間の測定方法は、一対の送受信可能な超音波振動子を対向して配置し、一方の超音波振動子をバ-スト信号で駆動し、超音波を送信し、他方の超音波振動子で受信し測定していた。 The ultrasonic propagation time measurement method used in conventional ultrasonic flowmeters is a method in which a pair of ultrasonic transducers capable of transmitting and receiving are arranged facing each other and one ultrasonic transducer is driven by a burst signal. The ultrasonic wave was transmitted and received and measured by the other ultrasonic transducer.
 図6に超音波流量計の送受信波形図を示す。なお、図6においては、横軸が時間を示し、縦軸が電圧を示す。また、図6の上側には、送信側の超音波振動子の駆動波形Aを示し、図6の下側には、受信側の超音波振動子で受信した受信波形Bを示す。図中のT0は駆動波形Aの開始時点を、T1は駆動開始後の第3波の終了時点を示す。R0は受信開始時点を、R1は受信開始後の第3波の終了時点を示す。例えば、特許文献1に開示の流体の流れ測定装置(超音波流量計)では、送信側の超音波振動子において、駆動波形Aの第m波目(mは整数であり、図6に示す例ではm=3)のゼロクロス点T1を、伝搬時間の計測の起点とし、他方の超音波振動子で受信した受信波形Bの第m(m=3)波目を終点R1としている。そして、当該流れ測定装置は、前記起点T1と前記終点R1との間の時間Tpを超音波の伝搬時間として計測し、この伝搬時間を用いて被測定流体の流速を計測し、流量を演算していた。 Fig. 6 shows a transmission / reception waveform diagram of the ultrasonic flowmeter. In FIG. 6, the horizontal axis indicates time, and the vertical axis indicates voltage. Further, the upper side of FIG. 6 shows the driving waveform A of the transmitting-side ultrasonic transducer, and the lower side of FIG. 6 shows the received waveform B received by the receiving-side ultrasonic transducer. In the figure, T0 indicates the start point of the drive waveform A, and T1 indicates the end point of the third wave after the start of drive. R0 indicates the reception start time, and R1 indicates the end time of the third wave after the start of reception. For example, in the fluid flow measuring device (ultrasonic flowmeter) disclosed in Patent Document 1, the m-th wave of driving waveform A (m is an integer, in the ultrasonic transducer on the transmission side, an example shown in FIG. Then, the zero crossing point T1 of m = 3) is set as the starting point of propagation time measurement, and the mth (m = 3) wave of the received waveform B received by the other ultrasonic transducer is set as the end point R1. Then, the flow measuring device measures the time Tp between the starting point T1 and the end point R1 as the propagation time of the ultrasonic wave, measures the flow velocity of the fluid to be measured using the propagation time, and calculates the flow rate. It was.
 特許文献1に開示の流体の流れ測定装置の構成を図7に示す。この流れ測定装置は、流体の流れる測定流路1に設置した超音波振動子2と、超音波振動子2を駆動する駆動回路3と、駆動回路3にスタート信号を出力する制御部26と、超音波の伝搬時間を測定する伝搬時間測定部5と、超音波振動子2から送信した超音波を受ける超音波振動子7と、超音波振動子7の出力を増幅するアンプ6と、アンプ6の出力と基準電圧とを比較し大小関係が反転したときに伝搬時間測定部5を停止させる受信検知回路8と、から構成されている。 FIG. 7 shows the configuration of the fluid flow measuring device disclosed in Patent Document 1. This flow measurement apparatus includes an ultrasonic transducer 2 installed in a measurement flow path 1 through which a fluid flows, a drive circuit 3 that drives the ultrasonic transducer 2, a control unit 26 that outputs a start signal to the drive circuit 3, A propagation time measuring unit 5 that measures the propagation time of the ultrasonic wave, an ultrasonic vibrator 7 that receives the ultrasonic wave transmitted from the ultrasonic vibrator 2, an amplifier 6 that amplifies the output of the ultrasonic vibrator 7, and an amplifier 6 And a reception detection circuit 8 that stops the propagation time measurement unit 5 when the magnitude relationship is inverted by comparing the output of the signal and the reference voltage.
 また、この流れ測定装置では、音速に対する温度の影響を無視できるように伝搬時間逆数差法を用いるが、そのために、一般的には、切り替えスイッチ10を備えている。この切り替えスイッチ10は、測定流路1の上流側から下流側への超音波の伝搬時間と、下流側から上流側への伝搬時間と、を測定するために用いられる。 In addition, in this flow measuring device, the inverse propagation time difference method is used so that the influence of the temperature on the sound speed can be ignored. For this purpose, the changeover switch 10 is generally provided. The changeover switch 10 is used to measure the propagation time of the ultrasonic wave from the upstream side to the downstream side of the measurement flow channel 1 and the propagation time from the downstream side to the upstream side.
 また、この流れ測定装置では、第m(m=3)波目の終了時のゼロクロス点を判定するために、基準電圧25をあらかじめ2波目および3波目の振幅の間に設定しておき、受信信号が基準電圧25を超えた次のゼロクロスが3波目となるように設定されている。そして、この流れ測定装置は、基準電圧25を、当該流れ測定装置の初期設定時に自動で調整するために受信波形振幅測定部9を備えている。この受信波形振幅測定部9では、受信を検知する基準電圧25を、低い電圧から少しずつ高くすることによって、伝搬時間が変化する電圧を、受信波のそれぞれの振幅として記憶することができる。 Further, in this flow measuring apparatus, in order to determine the zero cross point at the end of the m-th (m = 3) wave, the reference voltage 25 is set in advance between the amplitudes of the second and third waves. The next zero cross when the received signal exceeds the reference voltage 25 is set to be the third wave. The flow measuring device includes a received waveform amplitude measuring unit 9 for automatically adjusting the reference voltage 25 when the flow measuring device is initially set. In the reception waveform amplitude measuring unit 9, by increasing the reference voltage 25 for detecting reception little by little from a low voltage, a voltage whose propagation time changes can be stored as each amplitude of the reception wave.
 例えば、図6に示すように、基準電圧25をV1からV2まで変化させても、当該基準電圧25は第1波目の振幅の範囲内であるため、伝搬時間はTaのままである。これに対して、基準電圧25をV1からV3まで変化させれば、当該基準電圧25は、第1波目の振幅(V2)より大きく第2波目の振幅(V3)よりも小さい範囲となるため、伝搬時間はTbとなる。よって、伝搬時間がTaからTbに切り替わるときの電圧、この例ではV2が、受信波の第1波目の振幅であることが判る。このようにして、伝搬時間の切り替りにより、受信波の第1波からピーク波(一連の受信波形Bを構成する各波のうち、最大振幅を有する波)までの各波の振幅(電圧)を測定することが可能となる。測定されたピーク波までの振幅から、第2波目と第3波目の振幅を選択し、第2波目の振幅である電圧と第3波目の振幅である電圧との中間に通常計測時の基準電圧25を設定することができる。 For example, as shown in FIG. 6, even if the reference voltage 25 is changed from V1 to V2, the propagation time remains Ta because the reference voltage 25 is within the amplitude range of the first wave. On the other hand, if the reference voltage 25 is changed from V1 to V3, the reference voltage 25 is in a range larger than the amplitude (V2) of the first wave and smaller than the amplitude (V3) of the second wave. Therefore, the propagation time is Tb. Therefore, it can be seen that the voltage at which the propagation time is switched from Ta to Tb, in this example, V2, is the amplitude of the first wave of the received wave. In this way, the amplitude (voltage) of each wave from the first wave of the received wave to the peak wave (the wave having the maximum amplitude among the waves constituting the series of received waveforms B) by switching the propagation time. Can be measured. The amplitude of the second and third waves is selected from the measured amplitudes up to the peak wave, and is normally measured between the voltage that is the amplitude of the second wave and the voltage that is the amplitude of the third wave. The hourly reference voltage 25 can be set.
特開2006-308449号公報JP 2006-308449 A
 しかしながら、前記従来の技術では、測定流路の実際の寸法と制御部4に設定されている流量計算用の流路寸法との間に差があると、計測結果に誤差が生じる。そのため、超音波流量計の製造段階で、実際に所定の流量を流して、計測値を補正する必要があるという課題があった。 However, in the conventional technique, if there is a difference between the actual dimension of the measurement channel and the channel size for flow rate calculation set in the control unit 4, an error occurs in the measurement result. Therefore, there has been a problem that it is necessary to correct a measured value by actually flowing a predetermined flow rate at the manufacturing stage of the ultrasonic flowmeter.
 本発明はこのような課題を解決するためになされたものであって、製造段階において、被測定流体を実際の流量で流して測定流路の寸法の差を補正する必要がなく、従来に比べてより安価な費用で製造することが可能な超音波流量計を提供することを目的とする。 The present invention has been made to solve such a problem. In the manufacturing stage, it is not necessary to flow the measured fluid at an actual flow rate to correct the difference in the dimensions of the measurement flow path. An object of the present invention is to provide an ultrasonic flowmeter that can be manufactured at a lower cost.
 本発明に係る超音波流量計は、前記の課題を解決するために、流量を測定するための被測定流体を流す測定流路と、前記測定流路に配置され超音波信号を送受信可能な一対の超音波振動子と、一方の前記超音波振動子から送信され、被測定流体を伝搬した超音波信号を他方の超音波振動子が受信するまでの伝搬時間を計測する伝搬時間測定部と、前記伝搬時間から演算によって前記超音波振動子間を満たす被測定流体の流量を求める制御部と、前記超音波振動子で受信した受信波形の第m波目の振幅を測定する受信波形振幅測定部と、測定した受信波形の各波の振幅と正規の受信波形の第m波目の振幅との差から実際の測定流路と流量計算用にあらかじめ設定された測定流路との寸法差を推定し、この推定結果に基づいて前記制御部において流量計算用に設定されている測定流路の寸法を補正する測定流路寸法補正部と、を備えている構成である。 In order to solve the above-described problem, an ultrasonic flowmeter according to the present invention includes a measurement channel for flowing a fluid to be measured for measuring a flow rate, and a pair of ultrasonic channels arranged in the measurement channel and capable of transmitting and receiving ultrasonic signals. An ultrasonic transducer, and a propagation time measuring unit that measures a propagation time until the other ultrasonic transducer receives an ultrasonic signal transmitted from one ultrasonic transducer and propagated through the fluid to be measured, A control unit that calculates the flow rate of the fluid to be measured that satisfies the space between the ultrasonic transducers from the propagation time, and a received waveform amplitude measuring unit that measures the amplitude of the mth wave of the received waveform received by the ultrasonic transducer And the difference between the amplitude of each measured waveform of the received waveform and the amplitude of the m-th wave of the normal received waveform, the dimensional difference between the actual measurement channel and the measurement channel preset for flow rate calculation is estimated. Based on the estimation result, the control unit A measurement channel dimension correction unit for correcting the size of the measurement flow path is configured for flow calculation is Configurations which comprises a.
 また、本発明に係る超音波流量計においては、前記測定流路寸法補正部は、測定した受信波形の各波の振幅と正規の受信波形の各波の振幅との差から実際の測定流路と流量計算用にあらかじめ設定された測定流路との寸法差を推定する構成であってもよい。 Further, in the ultrasonic flowmeter according to the present invention, the measurement flow path dimension correction unit is configured to determine an actual measurement flow path from a difference between the amplitude of each wave of the measured reception waveform and the amplitude of each wave of the normal reception waveform. And a dimensional difference between the measurement channel set in advance for flow rate calculation may be used.
 さらに、本発明に係る超音波流量計は、前記測定流路と、前記超音波振動子と、前記伝搬時間測定部と、前記制御部と、前記一対の超音波振動子間を所定の温度に設定した所定の被測定流体で充満して、超音波振動子間の超音波の伝搬時間を計測し、あらかじめ前記制御部に設定された正規の伝搬時間と比較し、測定した伝搬時間と正規の伝搬時間の差から実際の超音波振動子間の距離と流量計算用に設定されている超音波振動子間の距離の差を推定し、前記推定結果に基づいて制御部に流量計算用に設定されている超音波振動子間の距離を補正する超音波振動子間距離補正部と、を備える構成であってもよい。 Furthermore, the ultrasonic flowmeter according to the present invention provides a predetermined temperature between the measurement flow path, the ultrasonic transducer, the propagation time measurement unit, the control unit, and the pair of ultrasonic transducers. It is filled with the set fluid to be measured, and the ultrasonic propagation time between the ultrasonic transducers is measured and compared with the normal propagation time set in advance in the control unit. Estimate the difference between the distance between the actual ultrasonic transducers and the distance between the ultrasonic transducers set for flow rate calculation from the difference in propagation time, and set the flow rate calculation in the control unit based on the estimation result And an ultrasonic transducer distance correcting unit that corrects the distance between the ultrasonic transducers that are arranged.
 本発明の上記目的、他の目的、特徴、及び利点は、添付図面参照の下、以下の好適な実施態様の詳細な説明から明らかにされる。 The above object, other objects, features, and advantages of the present invention will become apparent from the following detailed description of preferred embodiments with reference to the accompanying drawings.
 以上のように、本発明では、製造段階において、被測定流体を実際の流量で流して測定流路の寸法の差を補正する必要がなく、従来に比べてより安価な費用で製造することが可能な超音波流量計を提供することができる、という効果を奏する。 As described above, in the present invention, in the manufacturing stage, it is not necessary to flow the measured fluid at the actual flow rate to correct the difference in the dimensions of the measurement flow path, and the manufacturing can be performed at a lower cost than in the past. There is an effect that a possible ultrasonic flowmeter can be provided.
本発明の実施の形態1に係る超音波流量計の概略構成を示すブロック図である。It is a block diagram which shows schematic structure of the ultrasonic flowmeter which concerns on Embodiment 1 of this invention. (a)は、測定流路の高さ寸法が基準値の場合における、当該測定流路内での超音波の伝搬経路を示す模式図であり、(b)は、(a)に示す伝搬経路における、超音波の受信波形を示す波形図である。(A) is a schematic diagram which shows the propagation path of the ultrasonic wave in the said measurement flow path in case the height dimension of a measurement flow path is a reference value, (b) is the propagation path shown to (a). It is a wave form diagram which shows the received waveform of an ultrasonic wave. (a)は、測定流路の高さ寸法が基準値より高めの場合における、当該測定流路内での超音波の伝搬経路を示す模式図であり、(b)は、(a)に示す伝搬経路における、超音波の受信波形を示す波形図である。(A) is a schematic diagram which shows the propagation path of the ultrasonic wave in the said measurement flow path in case the height dimension of a measurement flow path is higher than a reference value, (b) is shown to (a). It is a wave form diagram which shows the received waveform of the ultrasonic wave in a propagation path. 本発明の実施の形態2に係る超音波流量計の概略構成を示すブロック図である。It is a block diagram which shows schematic structure of the ultrasonic flowmeter which concerns on Embodiment 2 of this invention. 本発明の実施の形態3に係る超音波流量計の概略構成を示すブロック図である。It is a block diagram which shows schematic structure of the ultrasonic flowmeter which concerns on Embodiment 3 of this invention. 一般的な超音波流量計における典型的な送信波および受信波の一例を示す波形図である。It is a wave form diagram which shows an example of the typical transmission wave and reception wave in a general ultrasonic flowmeter. 従来の超音波流量計である流体の流れ計測装置の概略構成を示すブロック図である。It is a block diagram which shows schematic structure of the fluid flow measuring apparatus which is the conventional ultrasonic flowmeter.
 1 測定流路
 2、7 超音波振動子
 3 駆動回路
 4、23、24 制御部
 5 伝搬時間測定部
 8 受信検知回路
 9 受信波形振幅測定部
 10 切り替えスイッチ
 11 測定流路寸法補正部
 22 超音波振動子間距離補正部
DESCRIPTION OF SYMBOLS 1 Measurement flow path 2, 7 Ultrasonic vibrator 3 Drive circuit 4, 23, 24 Control part 5 Propagation time measurement part 8 Reception detection circuit 9 Received waveform amplitude measurement part 10 Changeover switch 11 Measurement flow path dimension correction | amendment part 22 Ultrasonic vibration Inter-child distance correction unit
 まず、本発明について説明すると、本発明は、流量を測定するための被測定流体を流す測定流路と、前記測定流路に配置され超音波信号を送受信可能な一対の超音波振動子と、一方の前記超音波振動子から送信され、被測定流体を伝搬した超音波信号を他方の超音波振動子が受信するまでの伝搬時間を計測する伝搬時間測定部と、前記伝搬時間から演算によって前記超音波振動子間を満たす被測定流体の流量を求める制御部と、前記超音波振動子で受信した受信波形の第m波目の振幅を測定する受信波形振幅測定部と、測定した受信波形の各波の振幅と正規の受信波形の第m波目の振幅との差から実際の測定流路と流量計算用にあらかじめ設定された測定流路との寸法差を推定し、この推定結果に基づいて前記制御部において流量計算用に設定されている測定流路の寸法を補正する測定流路寸法補正部と、を備えている構成の超音波流量計である。 First, the present invention will be described. The present invention includes a measurement flow channel for flowing a fluid to be measured for measuring a flow rate, a pair of ultrasonic transducers arranged in the measurement flow channel and capable of transmitting and receiving ultrasonic signals, A propagation time measuring unit for measuring a propagation time transmitted from one of the ultrasonic transducers until the other ultrasonic transducer receives an ultrasonic signal propagated through the fluid to be measured; A control unit for obtaining a flow rate of the fluid to be measured that fills between the ultrasonic transducers, a received waveform amplitude measuring unit that measures the amplitude of the mth wave of the received waveform received by the ultrasonic transducer, and the measured received waveform Based on the difference between the amplitude of each wave and the amplitude of the m-th wave of the regular received waveform, the dimensional difference between the actual measurement channel and the measurement channel preset for flow rate calculation is estimated. For the flow rate calculation in the control unit Is an ultrasonic flowmeter structure comprises a measuring channel dimension correction unit for correcting the size of the measurement flow path is constant, a.
 前記構成によれば、前記超音波流量計の製造段階で、被測定流体を実際の流量で流して計測値の誤差を確認しなくても、実際の測定流路と設定されている測定流路との寸法の差を補正することができる。それゆえ、測定流路の寸法ずれによる流量値のずれも好適に補正することができる。したがって、製造工程に高価な流量発生装置が必要なく、寸法補正に要する時間も短くて済むため、従来に比べてより安価な費用で超音波流量計を製造することが可能となる。 According to the above configuration, the measurement flow channel set as the actual measurement flow channel can be obtained without flowing the measured fluid at the actual flow rate and checking the measurement value error at the manufacturing stage of the ultrasonic flow meter. And the difference in dimensions can be corrected. Therefore, the deviation of the flow rate value due to the dimensional deviation of the measurement flow path can be suitably corrected. Therefore, an expensive flow rate generator is not required in the manufacturing process, and the time required for dimensional correction can be shortened. Therefore, it is possible to manufacture an ultrasonic flowmeter at a lower cost than in the past.
 また、本発明は、前記構成の超音波流量計において、前記受信波形振幅測定部が測定する第m波目が、ピーク波である構成であってもよい。第m波目をピーク波とすることで、寸法補正の精度を向上することができる。 In the ultrasonic flowmeter having the above-described configuration, the m-th wave measured by the received waveform amplitude measuring unit may be a peak wave. By setting the m-th wave as a peak wave, the accuracy of dimensional correction can be improved.
 また、本発明は、流量を測定するための被測定流体を流す測定流路と、前記測定流路に配置され超音波信号を送受信可能な一対の超音波振動子と、一方の前記超音波振動子から送信され、被測定流体を伝搬した超音波信号を他方の超音波振動子が受信するまでの伝搬時間を計測する伝搬時間測定部と、前記伝搬時間から演算によって前記超音波振動子間を満たす被測定流体の流量を求める制御部と、前記超音波振動子で受信した受信波形の複数の波の振幅を測定する受信波形振幅測定部と、測定した受信波形の各波の振幅と正規の受信波形の各波の振幅との差から実際の測定流路と流量計算用にあらかじめ設定された測定流路との寸法差を推定し、この推定結果に基づいて前記制御部において流量計算用に設定されている測定流路の寸法を補正する測定流路寸法補正部と、を備えている構成の超音波流量計であってもよい。 The present invention also provides a measurement channel for flowing a fluid to be measured for measuring a flow rate, a pair of ultrasonic transducers arranged in the measurement channel and capable of transmitting and receiving ultrasonic signals, and one of the ultrasonic vibrations A propagation time measuring unit that measures a propagation time until the other ultrasonic transducer receives an ultrasonic signal transmitted from the child and propagated through the fluid to be measured, and between the ultrasonic transducers by calculation from the propagation time. A control unit for obtaining a flow rate of the fluid to be measured to be satisfied, a received waveform amplitude measuring unit for measuring the amplitudes of a plurality of received waveforms received by the ultrasonic transducer, and the amplitude and normality of each wave of the measured received waveform Estimate the dimensional difference between the actual measurement flow path and the measurement flow path set in advance for flow rate calculation from the difference between the amplitude of each wave of the received waveform, and based on this estimation result, calculate the flow rate in the control unit. Set the measurement channel dimensions A measurement channel dimension correction unit positive for, may be an ultrasonic flowmeter structure comprises a.
 前記構成によっても、製造段階で、被測定流体を実際の流量で流して計測値の誤差を確認しなくても、測定流路の寸法差を補正することができる。それゆえ、従来に比べてより安価な費用で超音波流量計を製造することが可能となる。 Even with the above-described configuration, it is possible to correct the dimensional difference of the measurement flow path without flowing the measured fluid at the actual flow rate and checking the measurement value error at the manufacturing stage. Therefore, it is possible to manufacture an ultrasonic flowmeter at a lower cost than in the past.
 また、本発明は、前記構成の超音波流量計において、前記受信波形振幅測定部が測定する複数の波の少なくとも1つを、ピーク波とした構成であってもよい。測定する複数の波にピーク波を含めることで、寸法補正の精度を向上することができる。 In the ultrasonic flowmeter having the above-described configuration, the present invention may be configured such that at least one of the plurality of waves measured by the received waveform amplitude measuring unit is a peak wave. By including peak waves in the plurality of waves to be measured, the accuracy of dimensional correction can be improved.
 また、本発明は、流量を測定するための被測定流体を流す測定流路と、前記測定流路に配置され超音波信号を送受信可能な一対の超音波振動子と、一方の前記超音波振動子から送信され、被測定流体を伝搬した超音波信号を他方の超音波振動子が受信するまでの伝搬時間を計測する伝搬時間測定部と、前記伝搬時間から演算によって前記超音波振動子間を満たす被測定流体の流量を求める制御部と、前記一対の超音波振動子間を所定の温度に設定した所定の被測定流体で充満して、超音波振動子間の超音波の伝搬時間を計測し、あらかじめ前記制御部に設定された正規の伝搬時間と比較し、測定した伝搬時間と正規の伝搬時間の差から実際の超音波振動子間の距離と流量計算用に設定されている超音波振動子間の距離の差を推定し、前記推定結果に基づいて制御部に流量計算用に設定されている超音波振動子間の距離を補正する超音波振動子間距離補正部と、を備えている構成の超音波流量計であってもよい。 The present invention also provides a measurement channel for flowing a fluid to be measured for measuring a flow rate, a pair of ultrasonic transducers arranged in the measurement channel and capable of transmitting and receiving ultrasonic signals, and one of the ultrasonic vibrations A propagation time measuring unit that measures a propagation time until the other ultrasonic transducer receives an ultrasonic signal transmitted from the child and propagated through the fluid to be measured, and between the ultrasonic transducers by calculation from the propagation time. A control unit for obtaining the flow rate of the fluid to be measured to be filled, and a predetermined fluid to be measured with a predetermined temperature set between the pair of ultrasonic transducers, and the propagation time of the ultrasonic wave between the ultrasonic transducers is measured. Compared with the normal propagation time previously set in the control unit, the ultrasonic wave set for calculating the distance between the actual ultrasonic transducers and the flow rate from the difference between the measured propagation time and the normal propagation time. Estimate the distance difference between the transducers and The ultrasonic flowmeter may be configured to include an ultrasonic transducer distance correction unit that corrects a distance between ultrasonic transducers set for flow rate calculation in the control unit based on the result. .
 前記構成によれば、超音波振動子間の距離の差を自動で補正できるため、被測定流体を実際の流量で流すことなく、より高精度な寸法補正が可能となる。 According to the above configuration, since the difference in distance between the ultrasonic transducers can be automatically corrected, more accurate dimensional correction can be performed without causing the fluid to be measured to flow at an actual flow rate.
 また、本発明は、前記構成の超音波流量計において、前記一対の超音波振動子間を所定の温度に設定した所定の被測定流体で充満して、超音波振動子間の超音波の伝搬時間を計測し、あらかじめ前記制御部に設定された正規の伝搬時間と比較し、測定した伝搬時間と正規の伝搬時間の差から実際の超音波振動子間の距離と流量計算用に設定されている超音波振動子間の距離の差を推定し、前記推定結果に基づいて制御部に流量計算用に設定されている超音波振動子間の距離を補正する超音波振動子間距離補正部を備えている構成であってもよい。 In the ultrasonic flowmeter having the above-described configuration, the ultrasonic wave propagation between ultrasonic transducers may be achieved by filling the predetermined fluid to be measured with a predetermined temperature between the pair of ultrasonic transducers. The time is measured, compared with the normal propagation time set in advance in the control unit, and the distance between the actual ultrasonic transducers and the flow rate calculation are set based on the difference between the measured propagation time and the normal propagation time. A distance correction unit between the ultrasonic transducers that estimates a difference in distance between the ultrasonic transducers and corrects a distance between the ultrasonic transducers set for flow rate calculation in the control unit based on the estimation result. The structure provided may be sufficient.
 前記構成によれば、測定流路だけでなく、超音波振動子間の距離の差も自動で補正することができるため、被測定流体を実際の流量で流すことなく、より高精度な寸法補正および距離補正が可能となる。 According to the above configuration, not only the measurement flow path but also the difference in distance between the ultrasonic transducers can be automatically corrected, so that more accurate dimensional correction can be made without flowing the measured fluid at the actual flow rate. And distance correction becomes possible.
 以下、本発明の好ましい実施の形態を、図面を参照しながら説明する。なお、以下では全ての図を通じて同一又は相当する要素には同一の参照符号を付して、その重複する説明を省略する。 Hereinafter, preferred embodiments of the present invention will be described with reference to the drawings. In the following description, the same or corresponding elements are denoted by the same reference symbols throughout the drawings, and redundant description thereof is omitted.
 (実施の形態1)
 図1は、本発明の実施の形態1に係る超音波流量計の構成の一例を示すブロック図である。
(Embodiment 1)
FIG. 1 is a block diagram showing an example of the configuration of the ultrasonic flowmeter according to Embodiment 1 of the present invention.
 図1に示すように、本実施の形態に係る超音波流量計は、一対の超音波振動子2および超音波振動子7、駆動回路3、制御部4、伝搬時間測定部5、アンプ6、受信検知回路8、切り替えスイッチ10、受信波形振幅測定部9、および測定流路寸法補正部11を備えている。 As shown in FIG. 1, the ultrasonic flowmeter according to the present embodiment includes a pair of ultrasonic transducers 2 and 7, a drive circuit 3, a control unit 4, a propagation time measuring unit 5, an amplifier 6, A reception detection circuit 8, a changeover switch 10, a reception waveform amplitude measurement unit 9, and a measurement flow path dimension correction unit 11 are provided.
 超音波振動子2、7は、被測定流体の流れる測定流路1に設置されており、駆動回路3により超音波振動子2、7が駆動される。上流側の超音波振動子7と下流側の超音波振動子2との送受信は切り替えスイッチ10により切り替えられる。アンプ6は、超音波振動子2、7の出力(特に超音波の受信波)を増幅し、受信検知回路8に出力する。受信検知回路8は、アンプ6の出力と基準電圧とを比較し大小関係が反転したときに伝搬時間測定部5を停止させる。 The ultrasonic vibrators 2 and 7 are installed in the measurement channel 1 through which the fluid to be measured flows, and the ultrasonic vibrators 2 and 7 are driven by the drive circuit 3. Transmission / reception between the upstream ultrasonic transducer 7 and the downstream ultrasonic transducer 2 is switched by a changeover switch 10. The amplifier 6 amplifies the outputs (particularly ultrasonic reception waves) of the ultrasonic transducers 2 and 7 and outputs them to the reception detection circuit 8. The reception detection circuit 8 compares the output of the amplifier 6 with the reference voltage, and stops the propagation time measurement unit 5 when the magnitude relationship is reversed.
 制御部4は、図1に示す超音波流量計の制御を行うものである。具体的には、駆動回路3にスタート信号を出力可能となっており、また、後述するように、伝搬時間測定部5を制御し、超音波振動子2、7間で送受信される超音波信号の伝搬時間から、これら超音波振動子2、7の間を満たす被測定流体の流量を求める演算を行い、切り替えスイッチ10の制御を行い、受信波形振幅測定部9および測定流路寸法補正部11の出力から、設定値の補正を行う。 The control unit 4 controls the ultrasonic flowmeter shown in FIG. Specifically, a start signal can be output to the drive circuit 3 and, as will be described later, an ultrasonic signal transmitted and received between the ultrasonic transducers 2 and 7 by controlling the propagation time measurement unit 5. Calculation of the flow rate of the fluid to be measured that fills the space between the ultrasonic transducers 2 and 7 from the propagation time, and control of the changeover switch 10, the received waveform amplitude measuring unit 9 and the measurement channel size correcting unit 11. The set value is corrected from the output of.
 伝搬時間測定部5は、前記のとおり、制御部4の制御によって演算に用いられる超音波振動子2、7間の超音波の伝搬時間を測定し、また、超音波の受信波形を受信波形振幅測定部9に出力する。受信波形振幅測定部9は、超音波の受信波形の第1波目からピーク波までの振幅を測定し、制御部4および測定流路寸法補正部11に出力する。測定流路寸法補正部11は、受信波形のそれぞれの波の振幅とあらかじめ設定された基準の受信波形の振幅との差から測定流路寸法を補正する(補正処理の詳細は後述する)。 As described above, the propagation time measuring unit 5 measures the propagation time of the ultrasonic wave between the ultrasonic transducers 2 and 7 used for the calculation under the control of the control unit 4, and also converts the received waveform of the ultrasonic wave into the received waveform amplitude. Output to the measurement unit 9. The received waveform amplitude measuring unit 9 measures the amplitude from the first wave to the peak wave of the received waveform of the ultrasonic wave, and outputs it to the control unit 4 and the measurement flow path dimension correcting unit 11. The measurement flow path dimension correction unit 11 corrects the measurement flow path dimension from the difference between the amplitude of each wave of the received waveform and the amplitude of the reference reception waveform set in advance (details of the correction process will be described later).
 制御部4の制御によって、切り替えスイッチ10は、超音波振動子2を受信側、超音波振動子7を送信側に設定する。この状態で、駆動回路3により超音波振動子2を駆動し、被測定流体を伝搬した超音波を超音波振動子2で受信する。受信された超音波(受信波)は、アンプ6、受信検知回路8を介して伝搬時間測定部5に入力され、超音波の伝搬時間が測定される。制御部4において被測定流体の流量を求める演算を行う場合には、制御部4は、伝搬時間測定部5から間接的に前記伝搬時間を取得し、あるいは、図示しない信号伝達経路を経て伝搬時間測定部5から直接的に伝搬時間を取得してもよい。 The control switch 4 sets the ultrasonic transducer 2 to the reception side and the ultrasonic transducer 7 to the transmission side under the control of the control unit 4. In this state, the ultrasonic vibrator 2 is driven by the drive circuit 3 and the ultrasonic wave propagated through the fluid to be measured is received by the ultrasonic vibrator 2. The received ultrasonic wave (received wave) is input to the propagation time measurement unit 5 via the amplifier 6 and the reception detection circuit 8, and the propagation time of the ultrasonic wave is measured. When the control unit 4 performs an operation for obtaining the flow rate of the fluid to be measured, the control unit 4 acquires the propagation time indirectly from the propagation time measurement unit 5, or the propagation time through a signal transmission path (not shown). The propagation time may be acquired directly from the measurement unit 5.
 超音波振動子2、超音波振動子7、駆動回路3、アンプ6、受信検知回路8、および切り替えスイッチ10としては、超音波流量計の分野で公知のものが好適に用いられる。 As the ultrasonic transducer 2, the ultrasonic transducer 7, the drive circuit 3, the amplifier 6, the reception detection circuit 8, and the changeover switch 10, those known in the field of ultrasonic flowmeters are preferably used.
 制御部4は、本実施の形態では、例えば、マイクロコンピュータにより構成され、当該マイクロコンピュータは、図1には図示しないが、例えば、演算部および記憶部等から構成される。演算部は、マイクロコンピュータのCPUで構成され、記憶部は内部メモリで構成される。記憶部には、種々のプログラムが記憶され、また、流量計算用にあらかじめ設定された測定流路等の寸法といった、種々の設定値が記憶されている。演算部は、記憶部に記憶されたプログラムを用いて、前述した流量を求める演算等を実行し、また、記憶部に記憶された設定値を必要に応じて補正する。なお、記憶部は内部メモリに限定されず、独立したメモリとして構成されてもよいし、複数の記憶装置から構成されてもよい。 In the present embodiment, the control unit 4 is configured by, for example, a microcomputer, and the microcomputer is configured by, for example, a calculation unit and a storage unit, although not illustrated in FIG. The arithmetic unit is composed of a CPU of a microcomputer, and the storage unit is composed of an internal memory. Various programs are stored in the storage unit, and various set values such as the dimensions of the measurement flow path set in advance for flow rate calculation are stored. The calculation unit executes the above-described calculation for determining the flow rate using the program stored in the storage unit, and corrects the setting value stored in the storage unit as necessary. The storage unit is not limited to the internal memory, and may be configured as an independent memory or may be configured from a plurality of storage devices.
 さらに、伝搬時間測定部5、受信波形振幅測定部9、および測定流路寸法補正部11は、公知のスイッチング素子、減算器、比較器等による論理回路等として構成されてもよいし、演算部が記憶部に格納されるプログラムに従って動作することにより実現される構成、すなわち、制御部4の機能構成であってもよい。 Further, the propagation time measurement unit 5, the received waveform amplitude measurement unit 9, and the measurement flow path dimension correction unit 11 may be configured as a logic circuit or the like using a known switching element, subtractor, comparator, or the like. May be a configuration realized by operating according to a program stored in the storage unit, that is, a functional configuration of the control unit 4.
 以上のように構成された超音波流量計について、以下その動作、作用を説明する。まず、基本的な流量測定動作等について、図6を参照して説明すると、本実施の形態に係る超音波流量計は、駆動波形の第m波目(mは整数であり、図6に示す例ではm=3)の終了時のゼロクロス点を判定するために、基準電圧25があらかじめ2波目および3波目の振幅の間に設定され、受信信号(受信波)が基準電圧25を超えた次のゼロクロスが、3波目終了時のゼロクロスとなるように設定されている。基準電圧25は、受信波の受信を検知するための電圧であり、受信波形振幅測定部9は、基準電圧25を初期設定時に自動で調整するために、当該基準電圧25を、低い電圧から少しずつ高くすることによって、伝搬時間が変化する電圧を、受信波のそれぞれの振幅として記憶する。 The operation and action of the ultrasonic flowmeter configured as described above will be described below. First, a basic flow measurement operation and the like will be described with reference to FIG. 6. The ultrasonic flowmeter according to the present embodiment is the m-th drive waveform (m is an integer, and is shown in FIG. 6. In the example, in order to determine the zero crossing point at the end of m = 3), the reference voltage 25 is set in advance between the amplitudes of the second and third waves, and the received signal (received wave) exceeds the reference voltage 25. The next zero cross is set to be the zero cross at the end of the third wave. The reference voltage 25 is a voltage for detecting reception of a received wave, and the reception waveform amplitude measuring unit 9 adjusts the reference voltage 25 slightly from a low voltage in order to automatically adjust the reference voltage 25 at the initial setting. By increasing the voltage one by one, the voltage whose propagation time changes is stored as the amplitude of each received wave.
 例えば、図6に示すように、基準電圧25をV1からV2まで変化させても、当該基準電圧25は第1波目の振幅の範囲内であるため、伝搬時間はTaのままである。これに対して、基準電圧25をV1からV3まで変化させれば、当該基準電圧25は、第1波目の振幅(V2)より大きく第2波目の振幅(V3)よりも小さい範囲となるため、伝搬時間はTbとなる。よって、伝搬時間がTaからTbに切り替わるときの電圧、この例ではV2が、受信波の第1波目の振幅であることが判る。このようにして、伝搬時間の切り替りにより、受信波の第1波からピーク波(一連の受信波形Bを構成する各波のうち、最大振幅を有する波)までの各波の振幅(電圧)を測定することが可能となる。測定されたピーク波までの振幅から、第2波目と第3波目の振幅を選択し、第2波目の振幅である電圧と第3波目の振幅である電圧との中間に通常計測時の基準電圧25を設定することができる。 For example, as shown in FIG. 6, even if the reference voltage 25 is changed from V1 to V2, the propagation time remains Ta because the reference voltage 25 is within the amplitude range of the first wave. On the other hand, if the reference voltage 25 is changed from V1 to V3, the reference voltage 25 is in a range larger than the amplitude (V2) of the first wave and smaller than the amplitude (V3) of the second wave. Therefore, the propagation time is Tb. Therefore, it can be seen that the voltage at which the propagation time is switched from Ta to Tb, in this example, V2, is the amplitude of the first wave of the received wave. In this way, the amplitude (voltage) of each wave from the first wave of the received wave to the peak wave (the wave having the maximum amplitude among the waves constituting the series of received waveforms B) by switching the propagation time. Can be measured. The amplitude of the second and third waves is selected from the measured amplitudes up to the peak wave, and is normally measured between the voltage that is the amplitude of the second wave and the voltage that is the amplitude of the third wave. The hourly reference voltage 25 can be set.
 送信側である超音波振動子2の駆動波形Aにおいては、前述のとおり、伝搬時間計測の起点は第m(m=3)波目のゼロクロス点T1に設定されている。それゆえ、受信側の超音波振動子7で受信した受信波形Bの第m(m=3)波目のゼロクロスを終点R1に設定すれば、伝搬時間測定部5は、起点T1と終点R1との間の時間Tpを超音波の伝搬時間として計測することができる。そして、制御部4は、この伝搬時間を用いて被測定流体の流速を計測し、当該被測定流体の流量を演算する。 In the drive waveform A of the ultrasonic transducer 2 on the transmission side, as described above, the starting point of the propagation time measurement is set to the zero-cross point T1 of the m-th (m = 3) wave. Therefore, if the zero cross of the m-th (m = 3) wave of the received waveform B received by the receiving-side ultrasonic transducer 7 is set as the end point R1, the propagation time measuring unit 5 determines the start point T1 and the end point R1. Can be measured as the propagation time of the ultrasonic wave. Then, the control unit 4 measures the flow velocity of the fluid under measurement using the propagation time, and calculates the flow rate of the fluid under measurement.
 さらに、本実施の形態においては、測定流路寸法補正部11では、実際の測定流路1の高さ寸法(測定流路1の流路径)と、あらかじめ流量値を計算するために、制御部4を構成する前記記憶部に記憶された基準となる高さ寸法との差から、当該記憶部に記憶された流量計算用の高さ寸法を補正する。補正する手段としては、超音波流量計の製造時に、測定流路1に流量が発生しない状態で、超音波を送受信し、受信波形の第1波目から第n波目(nはピーク波までの任意の整数)までの各波の振幅を受信波形振幅測定部9で測定する。 Furthermore, in the present embodiment, the measurement channel size correction unit 11 is configured to control the actual height of the measurement channel 1 (the channel diameter of the measurement channel 1) and the flow rate value in advance. 4 is corrected based on the difference from the reference height dimension stored in the storage section 4 that constitutes 4. As a means for correcting, ultrasonic waves are transmitted and received in the state where no flow rate is generated in the measurement flow channel 1 during the manufacture of the ultrasonic flowmeter, and the first to nth waves (n is the peak wave) of the received waveform. The received waveform amplitude measuring unit 9 measures the amplitude of each wave up to an arbitrary integer).
 ここで、測定流路1の高さ寸法が基準となる寸法からずれていた場合の現象をn=2として、図2(a)、(b)および図3(a)、(b)を参照して説明する。図2(a)は、測定流路1の寸法が基準どおりの場合における超音波の伝搬経路を示し、図2(b)は、この伝搬経路における超音波の受信波形を示している。図3(a)は、測定流路1の高さ寸法が基準より高めの場合における超音波の伝搬経路を示し、図3(b)は、この伝搬経路における超音波の受信波形を示している。 Here, assuming that the phenomenon when the height dimension of the measurement channel 1 is deviated from the reference dimension is n = 2, refer to FIGS. 2 (a), 2 (b) and FIGS. 3 (a), 3 (b). To explain. FIG. 2A shows an ultrasonic wave propagation path when the dimension of the measurement channel 1 is the same as that of the reference, and FIG. 2B shows an ultrasonic wave reception waveform in this propagation path. FIG. 3A shows an ultrasonic wave propagation path when the height dimension of the measurement channel 1 is higher than the reference, and FIG. 3B shows an ultrasonic reception waveform in the propagation path. .
 図2(a)に示すように、測定流路1の高さ寸法Hが基準どおりである場合、超音波の受信波形は、超音波振動子2、7の間を直進する経路12を通ってきた超音波の波形と、測定流路1の内側面に当たって反射する経路13を通ってきた超音波の波形との合成になる。それゆえ、超音波振動子2で受信される受信波は、図2(b)に示すように、経路12を通ってきた超音波の受信波形15と経路13を通ってきた超音波の受信波形16との合成波形17となり、各波(第1波目と第2波目)の振幅18aおよび振幅18bは、いずれも、受信波形15または受信波形16の振幅よりも大きくなる。 As shown in FIG. 2A, when the height dimension H of the measurement flow channel 1 is the same as the reference, the received waveform of the ultrasonic wave passes through the path 12 that goes straight between the ultrasonic transducers 2 and 7. The waveform of the ultrasonic wave and the waveform of the ultrasonic wave that has passed through the path 13 reflected by the inner surface of the measurement channel 1 are combined. Therefore, the received wave received by the ultrasonic transducer 2 is, as shown in FIG. 2B, the received waveform 15 of the ultrasonic wave passing through the path 12 and the received waveform of the ultrasonic wave passing through the path 13. 16, the amplitude 18 a and the amplitude 18 b of each wave (first wave and second wave) are both larger than the amplitude of the reception waveform 15 or the reception waveform 16.
 これに対して、図3(a)に示すように、測定流路1の高さ寸法H'が基準となる測定流路1の高さ寸法Hよりも高めになっている場合は、測定流路1の内側面に当たって反射する経路14が図2(a)に示す例より長くなり、超音波が受信側の超音波振動子2に到着するまでの時間が遅くなる。そのため、超音波振動子2で受信される受信波は、図3(b)に示すように、受信波形15と受信波形19との合成波形20となる。 On the other hand, as shown in FIG. 3A, when the height dimension H ′ of the measurement channel 1 is higher than the height dimension H of the reference measurement channel 1, The path 14 that is reflected by hitting the inner surface of the path 1 is longer than the example shown in FIG. 2A, and the time until the ultrasonic wave arrives at the ultrasonic transducer 2 on the receiving side is delayed. Therefore, the received wave received by the ultrasonic transducer 2 is a combined waveform 20 of the received waveform 15 and the received waveform 19 as shown in FIG.
 ここで、図2(b)に示す合成波形17を正規の波形(基準の波形)とすれば、当該合成波形20と正規の波形(合成波形17)とを比較することで、測定流路1の高さ寸法Hと寸法H’との差を推定することができる。つまり、図3(b)に示すように、合成波形20における各波(第1波目と第2波目)の振幅21aおよび振幅21bは、正規の波形である合成波形17の振幅18aおよび振幅18bよりも小さくなっているので、実際に測定された振幅21aおよび振幅21bは、基準の振幅18aおよび振幅18bからずれることになる。このずれが高さ寸法HおよびH’の差(寸法のずれ)に対応する。 Here, if the synthetic waveform 17 shown in FIG. 2B is a normal waveform (reference waveform), the measurement flow channel 1 can be obtained by comparing the synthetic waveform 20 with the normal waveform (synthetic waveform 17). The difference between the height dimension H and the dimension H ′ can be estimated. That is, as shown in FIG. 3B, the amplitude 21a and the amplitude 21b of each wave (the first wave and the second wave) in the synthesized waveform 20 are the amplitude 18a and the amplitude of the synthesized waveform 17 which is a normal waveform. Since it is smaller than 18b, the actually measured amplitude 21a and amplitude 21b will deviate from the reference amplitude 18a and amplitude 18b. This deviation corresponds to the difference between the height dimensions H and H ′ (dimension deviation).
 制御部4においては、以上の原理に基づいて、受信波形のそれぞれの波に振幅のずれが生じたときに形成される合成波の振幅と、測定流路1の高さ寸法との関係を、補正量として予め記憶部に設定記憶してある。そして、測定流路寸法補正部11は、測定した各波の振幅と、予め記憶部に設定記憶された振幅との差に基づいて、予め設定されている補正量だけ、測定流路1の計算上の高さ寸法を補正する。これによって、実際の測定流路1の寸法ずれにより生じる計測値のずれを補正することができる。なお、補正量を予め記憶部に記憶せず、演算部にて演算して取得するようにしてもよい。 In the control unit 4, based on the above principle, the relationship between the amplitude of the combined wave formed when an amplitude shift occurs in each wave of the received waveform and the height dimension of the measurement channel 1, The correction amount is set and stored in advance in the storage unit. Then, the measurement channel dimension correction unit 11 calculates the measurement channel 1 by a preset correction amount based on the difference between the measured amplitude of each wave and the amplitude set and stored in the storage unit in advance. Correct the height dimension above. Thereby, the deviation of the measured value caused by the actual deviation of the dimension of the measurement channel 1 can be corrected. Note that the correction amount may not be stored in the storage unit in advance, but may be calculated and acquired by the calculation unit.
 以上のように、本実施の形態においては測定流路寸法補正部11を備えることによって、超音波流量計の製造時に、測定流路1に被測定流体を実際の流量で流すことがなくても、測定流路1の寸法ずれによる流量値のずれを好適に補正することができる。 As described above, in the present embodiment, the measurement flow path dimension correction unit 11 is provided so that the measured fluid does not flow through the measurement flow path 1 at the actual flow rate when the ultrasonic flowmeter is manufactured. The deviation of the flow rate value due to the dimensional deviation of the measurement channel 1 can be suitably corrected.
 ここで、記憶部に設定される補正量は、所定の被測定流体を用いた測定結果に基づいたものであり、補正を行うための測定も、同じ所定の被測定流体を用いて行っている。 Here, the correction amount set in the storage unit is based on the measurement result using the predetermined fluid to be measured, and the measurement for performing the correction is also performed using the same predetermined fluid to be measured. .
 なお、本実施の形態では、振幅を測定する波の数を2(第1波および第2波)として説明したが、第1波目からピーク波までの任意の数の波を測定して比較することも可能である。特に、振幅を測定する波にピーク波を含めると、ピーク波は受信波形中で最も振幅が大きくなるので、測定流路1の寸法がずれていれば、基準の場合の振幅との差が相対的に大きくなる。それゆえ、寸法補正の精度(並びに流量値のずれの精度)を向上することができる。 In this embodiment, the number of waves whose amplitude is to be measured is described as 2 (first wave and second wave). However, an arbitrary number of waves from the first wave to the peak wave are measured and compared. It is also possible to do. In particular, if a peak wave is included in a wave whose amplitude is to be measured, the peak wave has the largest amplitude in the received waveform. Therefore, if the dimension of the measurement channel 1 is shifted, the difference from the amplitude in the reference case is relative. Become bigger. Therefore, the accuracy of dimensional correction (as well as the accuracy of deviation in flow rate value) can be improved.
 さらに、第1波目からピーク波までの全ての波について振幅を測定して、基準の場合の振幅と比較すれば、寸法補正の精度をより一層向上することができる。 Furthermore, if the amplitude is measured for all the waves from the first wave to the peak wave and compared with the amplitude in the case of the reference, the accuracy of dimensional correction can be further improved.
 また、本実施の形態では、振幅を測定する波の数が複数でなくてもよい。例えば、第m波目(第1波目から第n波目までの任意の波)の1つの波について、振幅を比較する構成であってもよい。この場合、第m波目をピーク波、すなわち、m=nとすれば、寸法補正の精度をさらに一層向上することができる。 Further, in the present embodiment, the number of waves whose amplitude is measured need not be plural. For example, the amplitude may be compared for one wave of the m-th wave (any wave from the first wave to the n-th wave). In this case, if the m-th wave is a peak wave, that is, m = n, the accuracy of dimensional correction can be further improved.
 また、上述したように記憶部に記憶する補正量を決定する際に採用する基準となる構成(特に、測定流路1に対する超音波振動子2,7の配設位置)は、補正対象である測定流路1においても共通化させておくことが好ましい。言い換えれば、上記基準となる構成は常に所定の位置関係となるように設定することが好ましい。例えば、超音波振動子2,7を測定流路1の流路断面の中心に配置する点を、両者の共通の構成となるように設定する。これにより、補正精度の更なる向上を図ることができる。 Further, as described above, the reference configuration (particularly, the position where the ultrasonic transducers 2 and 7 are disposed with respect to the measurement flow path 1) employed when determining the correction amount stored in the storage unit is a correction target. It is preferable that the measurement channel 1 is also shared. In other words, it is preferable that the reference configuration is always set to have a predetermined positional relationship. For example, the point where the ultrasonic transducers 2 and 7 are arranged at the center of the cross section of the measurement flow channel 1 is set so as to have a common configuration. Thereby, the correction accuracy can be further improved.
 (実施の形態2)
 次に、本発明の実施の形態2に係る超音波流量計について、図4を参照して説明する。図4は、実施の形態2に係る超音波流量計の構成の一例を示すブロック図である。本実施の形態に係る超音波流量計は、図4に示すように、基本的な構成は前記実施の形態1に係る超音波流量計と同様の構成を有しているが、測定流路寸法補正部11を備えておらず、超音波振動子間距離補正部22を備えている点で異なっている。
(Embodiment 2)
Next, an ultrasonic flowmeter according to Embodiment 2 of the present invention will be described with reference to FIG. FIG. 4 is a block diagram illustrating an example of the configuration of the ultrasonic flowmeter according to the second embodiment. As shown in FIG. 4, the ultrasonic flowmeter according to the present embodiment has the same basic structure as that of the ultrasonic flowmeter according to the first embodiment, but the measurement flow path dimensions. The difference is that the correction unit 11 is not provided and the ultrasonic transducer distance correction unit 22 is provided.
 制御部23は、前記実施の形態1における制御部4と同様に、例えば、演算部および記憶部で構成されている。当該記憶部には、前述したプログラムの他に、所定の温度に設定した所定の被測定流体を用いて測定した伝搬時間(設定値)が予め設定され、また、超音波振動子2、7の間の距離である振動子間距離について、その計算上の値(流量を算出する際に使用される設定値)が予め設定されている。もちろん他の設定値が記憶されてもよい。 The control unit 23 includes, for example, a calculation unit and a storage unit, similarly to the control unit 4 in the first embodiment. In the storage unit, in addition to the above-described program, a propagation time (set value) measured using a predetermined fluid to be measured set to a predetermined temperature is set in advance, and the ultrasonic transducers 2 and 7 For the inter-vibrator distance, which is the distance between them, a calculated value (a set value used when calculating the flow rate) is preset. Of course, other set values may be stored.
 超音波振動子間距離補正部22は、公知のスイッチング素子、減算器、比較器等による論理回路等として構成されてもよいし、演算部が記憶部に格納されるプログラムに従って動作することにより実現される構成、すなわち、制御部23の機能構成であってもよい。 The ultrasonic transducer distance correction unit 22 may be configured as a logic circuit or the like using a known switching element, subtractor, comparator, or the like, or realized by the arithmetic unit operating according to a program stored in the storage unit. That is, the functional configuration of the control unit 23 may be used.
 本実施の形態に係る超音波流量計の基本的な動作は、前記実施の形態1に係る超音波流量計の動作と同じであるため省略し、超音波振動子間距離補正部22の動作について説明する。 Since the basic operation of the ultrasonic flowmeter according to the present embodiment is the same as that of the ultrasonic flowmeter according to the first embodiment, the description thereof will be omitted, and the operation of the ultrasonic transducer distance correction unit 22 will be omitted. explain.
 超音波振動子間距離補正部22は、超音波流量計の製造時に、所定の温度に設定した所定の被測定流体で測定流路1を満たした状態で伝搬時間(測定値)を測定する。その後、予め設定されている伝搬時間の設定値と伝搬時間の測定値とのずれに基づいて、予め設定されている振動子間距離の設定値と実際の振動子間距離との差を求める。そして、求められた差から記憶部に記憶されている振動子間距離を補正する。これによって、計測値のずれを補正することができる。 The ultrasonic transducer distance correction unit 22 measures the propagation time (measured value) in a state where the measurement flow path 1 is filled with a predetermined fluid to be measured set to a predetermined temperature when the ultrasonic flowmeter is manufactured. Thereafter, based on the difference between the preset propagation time setting value and the propagation time measurement value, the difference between the preset inter-vibrator distance setting value and the actual inter-vibrator distance is obtained. Then, the inter-vibrator distance stored in the storage unit is corrected from the obtained difference. Thereby, the deviation of the measured value can be corrected.
 (実施の形態3)
 次に、本発明の実施の形態3に係る超音波流量計について、図5を参照して説明する。図5は、実施の形態3に係る超音波流量計の構成の一例を示すブロック図である。本実施の形態に係る超音波流量計は、図5に示すように、基本的な構成は前記実施の形態2に係る超音波流量計と同様の構成を有しているが、さらに測定流路寸法補正部11を備えている点で異なっている。
(Embodiment 3)
Next, an ultrasonic flowmeter according to Embodiment 3 of the present invention will be described with reference to FIG. FIG. 5 is a block diagram illustrating an example of the configuration of the ultrasonic flowmeter according to the third embodiment. As shown in FIG. 5, the ultrasonic flowmeter according to the present embodiment has the same basic structure as that of the ultrasonic flowmeter according to the second embodiment. The difference is that a dimension correction unit 11 is provided.
 制御部24は、前記実施の形態1における制御部4と同様に、例えば、演算部および記憶部で構成されており、当該記憶部には、前述した各種設定値が設定されている。 The control unit 24 includes, for example, a calculation unit and a storage unit, similar to the control unit 4 in the first embodiment, and the above-described various setting values are set in the storage unit.
 本実施の形態に係る超音波流量計の基本的な動作は、前記実施の形態1または2に係る超音波流量計の動作と同じであるため省略し、測定流路寸法補正部11および超音波振動子間距離補正部22の動作について説明する。 Since the basic operation of the ultrasonic flowmeter according to the present embodiment is the same as that of the ultrasonic flowmeter according to the first or second embodiment, it is omitted, and the measurement flow path dimension correction unit 11 and the ultrasonic wave are omitted. The operation of the inter-vibrator distance correction unit 22 will be described.
 測定流路寸法補正部11は、所定の温度に設定した所定の被測定流体で測定流路1を満たした状態で、受信波に含まれる各波の振幅の測定値と、記憶部に予め記憶されている振幅の設定値との差に基づいて、予め設定されている補正量だけ測定流路1の計算上の高さ寸法の補正を行い、次に、超音波振動子間距離補正部22により、前述した振動子間距離のずれを補正する。 The measurement channel size correction unit 11 stores in advance a measurement value of the amplitude of each wave included in the received wave and a storage unit in a state where the measurement channel 1 is filled with a predetermined fluid to be measured set to a predetermined temperature. Based on the difference from the set amplitude value, the calculated height dimension of the measurement channel 1 is corrected by a preset correction amount, and then the ultrasonic transducer distance correcting unit 22 is corrected. Thus, the deviation of the inter-vibrator distance is corrected.
 すなわち、測定流路寸法補正部11では、振幅の測定値および設定値の差から測定流路1の寸法補正を行うが、振幅の測定は、振動子間距離のずれの影響をほとんど受けることがない。そして、超音波振動子間距離補正部22は、測定流路1の寸法補正に基づいて、伝搬距離を測定することによって振動子間距離のずれを補正する。それゆえ、測定流路寸法補正部11で測定する対象(振幅)と、超音波振動子間距離補正部22で測定する対象(伝搬距離)とは、実質的に互いに独立した測定対象であるので、超音波振動子間距離補正部22における振動子間距離のずれの補正精度は、測定流路寸法補正部11による寸法補正の結果、さらに向上することが可能となる。 That is, the measurement channel dimension correction unit 11 corrects the dimension of the measurement channel 1 based on the difference between the measured value and the set value of the amplitude. However, the measurement of the amplitude is almost affected by the deviation of the distance between the transducers. Absent. Then, the ultrasonic transducer distance correction unit 22 corrects the deviation of the inter-vibrator distance by measuring the propagation distance based on the dimension correction of the measurement channel 1. Therefore, the object (amplitude) measured by the measurement flow path dimension correction unit 11 and the object (propagation distance) measured by the ultrasonic transducer distance correction unit 22 are substantially independent measurement objects. As a result of the dimensional correction by the measurement flow path dimension correction unit 11, the correction accuracy of the deviation between the transducer distances in the ultrasonic transducer distance correction unit 22 can be further improved.
 以上のように、本実施の形態においては、測定流路寸法補正部11および超音波振動子間距離補正部22を備えることによって、超音波流量計の製造時に、測定流路1に被測定流体を実際の流量で流すことがなくても、測定流路1の寸法及び超音波振動子2、7の間の距離(振動子間距離)のずれによる流量値のすれを好適に補正することができる。 As described above, in the present embodiment, by providing the measurement flow channel dimension correction unit 11 and the ultrasonic transducer distance correction unit 22, the fluid to be measured is placed in the measurement flow channel 1 when the ultrasonic flowmeter is manufactured. Even if the actual flow rate does not flow, it is possible to suitably correct the deviation of the flow rate value due to the deviation of the dimension of the measurement channel 1 and the distance between the ultrasonic transducers 2 and 7 (distance between the transducers). it can.
 上記説明から、当業者にとっては、本発明の多くの改良や他の実施形態が明らかである。従って、上記説明は、例示としてのみ解釈されるべきであり、本発明を実行する最良の態様を当業者に教示する目的で提供されたものである。本発明の精神を逸脱することなく、その構造及び/又は機能の詳細を実質的に変更できる。 From the above description, many modifications and other embodiments of the present invention are apparent to persons skilled in the art. Accordingly, the foregoing description should be construed as illustrative only and is provided for the purpose of teaching those skilled in the art the best mode of carrying out the invention. The details of the structure and / or function may be substantially changed without departing from the spirit of the invention.
 以上のように、本発明にかかる超音波流量計は、製造段階で実際の流量を流して測定流路の寸法の差を補正する必要がないため、製造工程に高価な流量発生装置が必要なく、補正に要する時間も短くて済む。それゆえ、従来に比べてより安価な費用で超音波流量計を製造することが可能となるので、流量測定基準器、ガスメーター、あるいは水道メーター等、流体の流量を超音波で測定する用途に広く適用することができる。 As described above, the ultrasonic flowmeter according to the present invention does not require an actual flow rate in the manufacturing stage to correct the difference in the dimensions of the measurement flow path, so that an expensive flow rate generator is not required in the manufacturing process. The time required for correction can be shortened. Therefore, it is possible to manufacture ultrasonic flowmeters at a lower cost than conventional methods, so it is widely used in applications that measure the flow rate of fluids with ultrasonic waves, such as flow measurement standards, gas meters, or water meters. Can be applied.

Claims (6)

  1.  流量を測定するための被測定流体を流す測定流路と、
     前記測定流路に配置され超音波信号を送受信可能な一対の超音波振動子と、
     一方の前記超音波振動子から送信され、被測定流体を伝搬した超音波信号を他方の超音波振動子が受信するまでの伝搬時間を計測する伝搬時間測定部と、
     前記伝搬時間から演算によって前記超音波振動子間を満たす被測定流体の流量を求める制御部と、
     前記超音波振動子で受信した受信波形の第m波目の振幅を測定する受信波形振幅測定部と、
     測定した受信波形の各波の振幅と正規の受信波形の第m波目の振幅との差から実際の測定流路と流量計算用にあらかじめ設定された測定流路との寸法差を推定し、この推定結果に基づいて前記制御部において流量計算用に設定されている測定流路の寸法を補正する測定流路寸法補正部を備えていることを特徴とする、超音波流量計。
    A measurement flow path for flowing a fluid to be measured for measuring a flow rate;
    A pair of ultrasonic transducers arranged in the measurement channel and capable of transmitting and receiving ultrasonic signals;
    A propagation time measuring unit that measures a propagation time transmitted from one ultrasonic transducer until the other ultrasonic transducer receives an ultrasonic signal propagated through the fluid to be measured;
    A control unit for obtaining a flow rate of a fluid to be measured that fills between the ultrasonic transducers by calculation from the propagation time;
    A received waveform amplitude measuring unit that measures the amplitude of the mth wave of the received waveform received by the ultrasonic transducer;
    From the difference between the amplitude of each measured waveform of the received waveform and the amplitude of the m-th wave of the regular received waveform, the dimensional difference between the actual measurement channel and the measurement channel preset for flow rate calculation is estimated, An ultrasonic flowmeter comprising: a measurement channel size correction unit that corrects a measurement channel size set for flow rate calculation in the control unit based on the estimation result.
  2.  前記受信波形振幅測定部が測定する第m波目が、ピーク波であることを特徴とする、請求項1に記載の超音波流量計。 The ultrasonic flowmeter according to claim 1, wherein the m-th wave measured by the received waveform amplitude measuring unit is a peak wave.
  3.  流量を測定するための被測定流体を流す測定流路と、
     前記測定流路に配置され超音波信号を送受信可能な一対の超音波振動子と、
     一方の前記超音波振動子から送信され、被測定流体を伝搬した超音波信号を他方の超音波振動子が受信するまでの伝搬時間を計測する伝搬時間測定部と、
     前記伝搬時間から演算によって前記超音波振動子間を満たす被測定流体の流量を求める制御部と、
     前記超音波振動子で受信した受信波形の複数の波の振幅を測定する受信波形振幅測定部と、
     測定した受信波形の各波の振幅と正規の受信波形の各波の振幅との差から実際の測定流路と流量計算用にあらかじめ設定された測定流路との寸法差を推定し、この推定結果に基づいて前記制御部において流量計算用に設定されている測定流路の寸法を補正する測定流路寸法補正部を備えていることを特徴とする、超音波流量計。
    A measurement flow path for flowing a fluid to be measured for measuring a flow rate;
    A pair of ultrasonic transducers arranged in the measurement channel and capable of transmitting and receiving ultrasonic signals;
    A propagation time measuring unit that measures a propagation time transmitted from one ultrasonic transducer until the other ultrasonic transducer receives an ultrasonic signal propagated through the fluid to be measured;
    A control unit for obtaining a flow rate of a fluid to be measured that fills between the ultrasonic transducers by calculation from the propagation time;
    A received waveform amplitude measuring unit that measures the amplitude of a plurality of received waveforms received by the ultrasonic transducer;
    Estimate the dimensional difference between the actual measurement channel and the measurement channel preset for flow rate calculation from the difference between the amplitude of each wave of the measured received waveform and the amplitude of each wave of the regular received waveform. An ultrasonic flowmeter, comprising: a measurement channel dimension correcting unit that corrects a dimension of a measurement channel set for flow rate calculation in the control unit based on a result.
  4.  前記受信波形振幅測定部が測定する複数の波の少なくとも1つを、ピーク波としたことを特徴とする、請求項3に記載の超音波流量計。 The ultrasonic flowmeter according to claim 3, wherein at least one of the plurality of waves measured by the received waveform amplitude measuring unit is a peak wave.
  5.  流量を測定するための被測定流体を流す測定流路と、
     前記測定流路に配置され超音波信号を送受信可能な一対の超音波振動子と、
     一方の前記超音波振動子から送信され、被測定流体を伝搬した超音波信号を他方の超音波振動子が受信するまでの伝搬時間を計測する伝搬時間測定部と、
     前記伝搬時間から演算によって前記超音波振動子間を満たす被測定流体の流量を求める制御部と、
     前記一対の超音波振動子間を所定の温度に設定した所定の被測定流体で充満して、超音波振動子間の超音波の伝搬時間を計測し、あらかじめ前記制御部に設定された正規の伝搬時間と比較し、測定した伝搬時間と正規の伝搬時間の差から実際の超音波振動子間の距離と流量計算用に設定されている超音波振動子間の距離の差を推定し、前記推定結果に基づいて制御部に流量計算用に設定されている超音波振動子間の距離を補正する超音波振動子間距離補正部を備えていることを特徴とする、超音波流量計。
    A measurement flow path for flowing a fluid to be measured for measuring a flow rate;
    A pair of ultrasonic transducers arranged in the measurement channel and capable of transmitting and receiving ultrasonic signals;
    A propagation time measuring unit that measures a propagation time transmitted from one ultrasonic transducer until the other ultrasonic transducer receives an ultrasonic signal propagated through the fluid to be measured;
    A control unit for obtaining a flow rate of a fluid to be measured that fills between the ultrasonic transducers by calculation from the propagation time;
    The pair of ultrasonic transducers is filled with a predetermined fluid to be measured which is set to a predetermined temperature, and the propagation time of ultrasonic waves between the ultrasonic transducers is measured. Compared with the propagation time, from the difference between the measured propagation time and the regular propagation time, estimate the difference between the distance between the actual ultrasonic transducers and the distance between the ultrasonic transducers set for flow rate calculation, An ultrasonic flowmeter comprising: an ultrasonic transducer distance correction unit that corrects a distance between ultrasonic transducers set for flow rate calculation in the control unit based on an estimation result.
  6.  前記一対の超音波振動子間を所定の温度に設定した所定の被測定流体で充満して、超音波振動子間の超音波の伝搬時間を計測し、あらかじめ前記制御部に設定された正規の伝搬時間と比較し、測定した伝搬時間と正規の伝搬時間の差から実際の超音波振動子間の距離と流量計算用に設定されている超音波振動子間の距離の差を推定し、前記推定結果に基づいて制御部に流量計算用に設定されている超音波振動子間の距離を補正する超音波振動子間距離補正部を備えていることを特徴とする、請求項3又は4に記載の超音波流量計。
     
     
    The pair of ultrasonic transducers is filled with a predetermined fluid to be measured which is set to a predetermined temperature, and the propagation time of ultrasonic waves between the ultrasonic transducers is measured. Compared with the propagation time, from the difference between the measured propagation time and the regular propagation time, estimate the difference between the distance between the actual ultrasonic transducers and the distance between the ultrasonic transducers set for flow rate calculation, 5. The ultrasonic transducer distance correcting unit that corrects the distance between ultrasonic transducers set for flow rate calculation in the control unit based on the estimation result, according to claim 3 or 4, The described ultrasonic flowmeter.

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