CN114459554A - Method for improving instantaneous flow metering precision of ultrasonic gas meter based on pressure data - Google Patents

Method for improving instantaneous flow metering precision of ultrasonic gas meter based on pressure data Download PDF

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CN114459554A
CN114459554A CN202210372274.8A CN202210372274A CN114459554A CN 114459554 A CN114459554 A CN 114459554A CN 202210372274 A CN202210372274 A CN 202210372274A CN 114459554 A CN114459554 A CN 114459554A
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ultrasonic
flow
propagation time
pressure difference
gas meter
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CN114459554B (en
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石爱国
宋莎莎
张金龙
徐伟
王颖嘉
杨庆珍
李腾
康惠海
曹国荣
管利军
蒋宇航
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Hangzhou Innover Technology Co ltd
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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
    • 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
    • G01F1/05Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow by using mechanical effects
    • G01F1/34Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow by using mechanical effects by measuring pressure or differential pressure
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01FMEASURING VOLUME, VOLUME FLOW, MASS FLOW OR LIQUID LEVEL; METERING BY VOLUME
    • G01F15/00Details of, or accessories for, apparatus of groups G01F1/00 - G01F13/00 insofar as such details or appliances are not adapted to particular types of such apparatus
    • G01F15/02Compensating or correcting for variations in pressure, density or temperature
    • G01F15/04Compensating or correcting for variations in pressure, density or temperature of gases to be measured

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

Abstract

The invention relates to a method for improving the instantaneous flow metering precision of an ultrasonic gas meter based on pressure data. The method is characterized in that: installing a differential pressure sensor in the ultrasonic gas meter, wherein two gas pressure acquisition ports of the differential pressure sensor are respectively installed in a flow channel and outside the flow channel, so that the pressure difference between the inside and outside of the flow channel of the ultrasonic gas meter is detected, the downstream propagation time and the upstream propagation time of the ultrasonic wave in the gas at the current moment are measured by adopting a time difference method, and the instantaneous flow is calculated by utilizing the downstream propagation time and the upstream propagation time of the ultrasonic wave in a gas medium; and judging whether the wave jump problem exists or not according to the measured pressure difference and the instantaneous flow, and correcting the downstream propagation time and the upstream propagation time at the current moment by using pressure difference data when the wave jump phenomenon occurs, so that the accurate instantaneous flow at the current moment is obtained, and the metering precision of the instantaneous flow of the ultrasonic gas meter is improved.

Description

Method for improving instantaneous flow metering precision of ultrasonic gas meter based on pressure data
Technical Field
The invention relates to a method for improving the instantaneous flow metering precision of an ultrasonic gas meter based on pressure data.
Background
The ultrasonic gas meter has the advantages of non-contact measurement, no movable part, no pressure loss, extremely high measurement precision and the like, and is a research hotspot in the field of gas measurement. The ultrasonic gas meter widely used in the market is generally based on a time difference method, and instantaneous flow is estimated by measuring forward flow propagation time and backward flow propagation time of ultrasonic waves in a gas medium, so that the forward flow propagation time and the backward flow propagation time of the ultrasonic waves in the gas medium are key measurement values of instantaneous flow measurement of the ultrasonic gas meter, and the measurement precision is directly influenced. In the existing scheme, a threshold value method is adopted to detect the propagation time of an ultrasonic signal in a gas medium, but the amplitude change or deformation of the received ultrasonic signal can be caused by the change of the working temperature of an ultrasonic gas meter, the instability of a gas flow field or the change of gas components, so that the threshold value is easily triggered on different rising edges of the ultrasonic signal instead of being always triggered on the same rising edge, and the measured downstream propagation time and the measured upstream propagation time generate time errors of one or more ultrasonic transducer excitation signal periods, namely, a wave jumping phenomenon, thereby causing the calculation of instantaneous flow and larger deviation of an actual value. In the prior art, a plurality of groups of data are collected, and the problem of wave hopping is processed by using a software averaging algorithm, but the method can influence the timeliness and accuracy of metering readings.
Disclosure of Invention
Aiming at the problems in the prior art, the invention aims to provide a technical scheme of a method for improving the instantaneous flow metering precision of an ultrasonic gas meter based on pressure data.
The method for improving the instantaneous flow metering precision of the ultrasonic gas meter based on the pressure data is characterized by comprising the following steps of: installing a differential pressure sensor in the ultrasonic gas meter, wherein two gas pressure acquisition ports of the differential pressure sensor are respectively installed in a flow channel and outside the flow channel, so that the pressure difference between the inside and outside of the flow channel of the ultrasonic gas meter is detected, the downstream propagation time and the upstream propagation time of the ultrasonic wave in the gas at the current moment are measured by adopting a time difference method, and the instantaneous flow is calculated by utilizing the downstream propagation time and the upstream propagation time of the ultrasonic wave in a gas medium; and judging whether the wave jump problem exists according to the measured pressure difference and the instantaneous flow, and correcting the downstream propagation time and the upstream propagation time at the current moment by using pressure difference data when the wave jump phenomenon occurs, so as to obtain the accurate instantaneous flow at the current moment.
The method for improving the instantaneous flow metering precision of the ultrasonic gas meter based on the pressure data is characterized in that the instantaneous flow calculation comprises the following steps:
(1) measuring the relation between the pressure difference and the instantaneous flow, (2) measuring the instantaneous flow by using a time difference method, and (3) judging whether the wave is jumped or not, and adjusting the forward flow propagation time and the reverse flow propagation time of the ultrasonic wave in the gas medium.
The method for improving the instantaneous flow metering precision of the ultrasonic gas meter based on the pressure data is characterized in that the method for measuring the relation between the pressure difference and the instantaneous flow in the step (1) is as follows:
installing a differential pressure sensor in the flow channel of the ultrasonic gas meter, and detecting the pressure difference inside and outside the flow channel of the ultrasonic gas meter through the differential pressure sensor; according to the Bernoulli equation, the pressure inside and outside the flow channel of the ultrasonic gas meter meets the following formula:
Figure DEST_PATH_IMAGE001
(1)
wherein the content of the first and second substances,
Figure 121548DEST_PATH_IMAGE002
is the pressure in the cavity of the ultrasonic gas meter,
Figure DEST_PATH_IMAGE003
is the pressure in the flow channel of the ultrasonic gas meter,
Figure 117317DEST_PATH_IMAGE004
is the average flow velocity of the gas medium in the cavity of the ultrasonic gas meter,
Figure DEST_PATH_IMAGE005
is the average flow velocity of the gas medium in the flow passage of the ultrasonic gas meter,
Figure 756109DEST_PATH_IMAGE006
is the gas density;
from conservation of mass, we obtain:
Figure DEST_PATH_IMAGE007
(2)
wherein the content of the first and second substances,
Figure 197323DEST_PATH_IMAGE008
is the sectional area in the cavity of the ultrasonic gas meter,
Figure DEST_PATH_IMAGE009
the cross section area in the flow channel of the ultrasonic gas meter;
the pressure difference between the inside and the outside of the flow passage of the ultrasonic gas meter is obtained by the formulas (1) and (2)
Figure 621482DEST_PATH_IMAGE010
Figure DEST_PATH_IMAGE011
(3)
According to the formula (3), the pressure difference between the inside and the outside of the flow channel of the ultrasonic gas meter measured by the differential pressure sensor is related to the average flow velocity of the gas medium in the flow channel, and the instantaneous flow is the product of the average flow velocity of the gas medium in the flow channel and the cross section area of the flow channel, so that the pressure difference between the inside and the outside of the flow channel of the ultrasonic gas meter is related to the instantaneous flow of the ultrasonic gas meter;
and (3) sequentially introducing flow to obtain pressure difference data under different instantaneous flows, and performing data fitting on the pressure difference data and the instantaneous flows by using a function model:
Figure 240682DEST_PATH_IMAGE012
wherein, in the step (A),
Figure DEST_PATH_IMAGE013
which is indicative of a pressure difference,
Figure 610179DEST_PATH_IMAGE014
which is indicative of the instantaneous flow rate of the fluid,
Figure DEST_PATH_IMAGE015
is a functional model fitted to the pressure difference and instantaneous flow.
The method for improving the instantaneous flow metering precision of the ultrasonic gas meter based on the pressure data is characterized in that the step (2) of measuring the instantaneous flow by using a time difference method comprises the following steps:
Figure 605816DEST_PATH_IMAGE016
(4)
Figure DEST_PATH_IMAGE017
(5)
in the above formulas (4) and (5),
Figure 884482DEST_PATH_IMAGE018
is the cross section area of the flow passage of the ultrasonic gas meter,
Figure DEST_PATH_IMAGE019
is the gas in the flow passage of the ultrasonic gas meterThe average velocity of the bulk medium is,
Figure 455010DEST_PATH_IMAGE020
is the length of the sound path,
Figure DEST_PATH_IMAGE021
is the angle of the sound track,
Figure 553547DEST_PATH_IMAGE022
is the downstream propagation time of the ultrasonic wave in the gas medium,
Figure DEST_PATH_IMAGE023
is the countercurrent propagation time of ultrasonic waves in a gas medium; wherein, the cross section area of the flow passage
Figure 149613DEST_PATH_IMAGE018
Length of sound path
Figure 453424DEST_PATH_IMAGE020
Angle of sound channel
Figure 148848DEST_PATH_IMAGE021
Is a constant value, and the instantaneous flow can be calculated according to the downstream propagation time and the upstream propagation time of the ultrasonic wave in the gas medium
Figure 921632DEST_PATH_IMAGE024
The method for improving the instantaneous flow metering precision of the ultrasonic gas meter based on the pressure data is characterized in that the step (3) is used for judging whether the wave is jumped or not, and the steps of adjusting the forward flow propagation time and the reverse flow propagation time of the ultrasonic wave in the gas medium are as follows:
calculating the instantaneous flow at the current moment according to the time difference method measuring principle in the step (2)
Figure DEST_PATH_IMAGE025
And (2) the function relation between the pressure difference and the instantaneous flow obtained in the step (1) can be used for deducing the theoretical pressure difference at the current moment
Figure 806542DEST_PATH_IMAGE026
(ii) a Differential pressure sensor for detecting pressure difference inside and outside flow channel of ultrasonic gas meter in real time
Figure DEST_PATH_IMAGE027
When the difference between the measured pressure difference and the theoretical pressure difference
Figure 246751DEST_PATH_IMAGE028
Figure DEST_PATH_IMAGE029
The maximum range of the allowable difference between the actually measured pressure difference and the theoretical pressure difference indicates that no wave jump phenomenon exists at the moment; when the difference between the measured pressure difference and the theoretical pressure difference
Figure 893502DEST_PATH_IMAGE030
When the instantaneous flow is calculated incorrectly, the ultrasonic waves have the existence of bouncing waves in the time measurement of the downstream propagation time and the upstream propagation time in the gas medium, so that the downstream propagation time and the upstream propagation time of the ultrasonic waves in the gas medium need to be adjusted;
from measured pressure differences
Figure DEST_PATH_IMAGE031
And the functional relation between the pressure difference and the instantaneous flow rate to deduce the theoretical instantaneous flow rate
Figure 966631DEST_PATH_IMAGE032
Figure DEST_PATH_IMAGE033
The theoretical forward flow propagation time and the theoretical reverse flow propagation time of the ultrasonic wave in the gas medium approximately satisfy the following relations:
Figure 904500DEST_PATH_IMAGE034
(6)
Figure DEST_PATH_IMAGE035
(7)
in the formulae (6) and (7),
Figure 454342DEST_PATH_IMAGE036
is the theoretical downstream propagation time of the ultrasonic wave in the gas medium,
Figure DEST_PATH_IMAGE037
is the theoretical countercurrent propagation time of ultrasonic waves in a gas medium,
Figure 570197DEST_PATH_IMAGE038
is the propagation velocity of sound waves in a gaseous medium; in addition, when the wave jumping phenomenon occurs, the forward flow propagation time of the ultrasonic wave in the gas medium is actually measured
Figure DEST_PATH_IMAGE039
And the theoretical downstream propagation time of ultrasonic waves in a gas medium
Figure 583152DEST_PATH_IMAGE040
Approximately differing by an integer number of ultrasonic transducer excitation signal periods, and actually measuring the counter-current propagation time of ultrasonic waves in a gas medium
Figure DEST_PATH_IMAGE041
Theoretical counter-current propagation time with ultrasonic wave in gas medium
Figure 308401DEST_PATH_IMAGE042
Approximately differing by an integer number of ultrasonic transducer excitation signal periods, the approximate relationship is as follows:
Figure DEST_PATH_IMAGE043
(8)
Figure 270672DEST_PATH_IMAGE044
(9)
in the formulas (8) and (9),
Figure DEST_PATH_IMAGE045
is the period of the excitation signal of the ultrasonic transducer,
Figure 9957DEST_PATH_IMAGE046
Figure 979050DEST_PATH_IMAGE047
represents the wave number; the passing formula (6) -9 can adjust the actual measurement forward flow propagation time and the actual measurement reverse flow propagation time of the ultrasonic wave in the gas medium, thereby obtaining the instantaneous flow at the current moment
Figure 100002_DEST_PATH_IMAGE048
The following formula:
Figure 507990DEST_PATH_IMAGE049
(10) 。
the invention installs a differential pressure sensor in the ultrasonic gas meter, the differential pressure sensor detects the pressure difference inside and outside the flow channel of the ultrasonic gas meter, obtains the data corresponding to the pressure difference and the instantaneous flow, and fits the data, and establishes the functional relation between the pressure difference and the instantaneous flow; when the ultrasonic gas meter is used, the theoretical pressure difference at the current moment is obtained according to the current moment instantaneous flow and the function relation between the pressure difference and the instantaneous flow, and the theoretical pressure difference is compared with the pressure difference actually measured by the differential pressure sensor, so that whether the wave jumping phenomenon exists or not is judged; when the wave hopping phenomenon occurs, the actually measured downstream propagation time and the actually measured upstream propagation time of the ultrasonic wave in the gas medium are corrected by using the pressure difference data, so that the accurate instantaneous flow is obtained, and the measurement precision of the instantaneous flow of the ultrasonic gas meter is improved.
Detailed Description
The invention relates to a method for improving the instantaneous flow metering precision of an ultrasonic gas meter based on pressure data, wherein a differential pressure sensor is arranged in a flow passage of the ultrasonic gas meter, the differential pressure sensor is used for detecting the pressure difference between the inside and the outside of the flow passage of the ultrasonic gas meter, obtaining the data corresponding to the pressure difference and the instantaneous flow, and fitting the data to establish the functional relation between the pressure difference and the instantaneous flow; when the ultrasonic gas meter is used, the theoretical pressure difference at the current moment is obtained according to the current moment instantaneous flow and the function relation between the pressure difference and the instantaneous flow, and the theoretical pressure difference is compared with the pressure difference actually measured by the differential pressure sensor, so that whether the wave jumping phenomenon exists or not is judged; when the wave jump phenomenon occurs, the pressure difference is used for correcting the measured forward flow propagation time and the measured backward flow propagation time of the ultrasonic wave in the gas medium.
The calculation of the instantaneous flow rate comprises the following steps:
(1) measuring pressure differential versus instantaneous flow
A differential pressure sensor is arranged in a flow channel of the ultrasonic gas meter, and two gas pressure acquisition ports of the differential pressure sensor are respectively arranged in the flow channel and outside the flow channel, so that the pressure difference between the inside and the outside of the flow channel of the ultrasonic gas meter is detected. According to the Bernoulli equation, the pressure inside and outside the flow channel of the ultrasonic gas meter meets the following formula:
Figure 100002_DEST_PATH_IMAGE050
(1)
wherein the content of the first and second substances,
Figure 528029DEST_PATH_IMAGE002
is the pressure in the cavity of the ultrasonic gas meter,
Figure 969375DEST_PATH_IMAGE003
is the pressure in the flow channel of the ultrasonic gas meter,
Figure 425764DEST_PATH_IMAGE004
is the average flow velocity of the gas medium in the cavity of the ultrasonic gas meter,
Figure 164919DEST_PATH_IMAGE005
is the average flow velocity of the gas medium in the flow passage of the ultrasonic gas meter,
Figure 554312DEST_PATH_IMAGE006
is the gas density;
from conservation of mass, we obtain:
Figure 369821DEST_PATH_IMAGE051
(2)
wherein the content of the first and second substances,
Figure 798660DEST_PATH_IMAGE008
is the sectional area in the cavity of the ultrasonic gas meter,
Figure 357817DEST_PATH_IMAGE009
the cross section area in the flow channel of the ultrasonic gas meter;
the pressure difference between the inside and the outside of the flow passage of the ultrasonic gas meter is obtained by the formulas (1) and (2)
Figure 70558DEST_PATH_IMAGE010
Figure 667473DEST_PATH_IMAGE011
(3)
According to the formula (3), the pressure difference between the inside and the outside of the flow channel of the ultrasonic gas meter measured by the differential pressure sensor has a certain relation with the average flow velocity of the gas medium in the flow channel, and the instantaneous flow is the product of the average flow velocity of the gas medium in the flow channel and the cross section area of the flow channel, so that the pressure difference between the inside and the outside of the flow channel of the ultrasonic gas meter has a certain relation with the instantaneous flow of the ultrasonic gas meter. And (3) sequentially introducing flow to obtain pressure difference data under different instantaneous flows, and performing data fitting on the pressure difference data and the instantaneous flows by using a function model:
Figure 100002_DEST_PATH_IMAGE052
wherein, in the step (A),
Figure 364033DEST_PATH_IMAGE053
which is indicative of a pressure difference,
Figure 8772DEST_PATH_IMAGE014
which is indicative of the instantaneous flow rate of the fluid,
Figure 841599DEST_PATH_IMAGE015
is a functional model fitted to the pressure difference and instantaneous flow. With reference to equation (3), function
Figure 100002_DEST_PATH_IMAGE054
Can be
Figure 44916DEST_PATH_IMAGE055
Figure 100002_DEST_PATH_IMAGE056
Figure 25511DEST_PATH_IMAGE057
Figure 100002_DEST_PATH_IMAGE058
Is the pressure difference data and instantaneous flow rate according to
Figure 942782DEST_PATH_IMAGE059
And (5) carrying out coefficient obtained by data fitting. Therefore, according to the functional relation between the pressure difference and the instantaneous flow, the theoretical pressure difference at the current moment can be deduced from the instantaneous flow at the current moment; the theoretical instantaneous flow at the current moment can be deduced from the actually measured pressure difference at the current moment.
In practical application, the structures of the flow channel and the cavity of the ultrasonic gas meters in different types can be different, so that the relation between the pressure difference and the flow needs to be measured through the device firstly. In this embodiment, a G6 ultrasonic gas meter is selected, a critical flow venturi nozzle method gas flow standard device is adopted, two gas pressure acquisition ports of a differential pressure sensor are respectively installed inside and outside a flow channel, a gas medium is air, and a relationship between a pressure difference and a flow rate is shown in the following table under the temperature of 20 ℃ in the experimental environment.
Figure 100002_DEST_PATH_IMAGE060
As can be seen from the above table, when the flow rate is 2.5m3The pressure difference is 21.29Pa, and the flow range is (4-5) m3At the time of/h, the pressure difference is (40-60) Pa. In this embodiment, the selection is made
Figure 941700DEST_PATH_IMAGE059
The function model performs data fitting on the pressure difference data and the instantaneous flow. Wherein the density of the gas
Figure 269913DEST_PATH_IMAGE006
1.208kg/m are taken3(temperature 20 ℃ C., pressure 101.6 kPa),
Figure 144328DEST_PATH_IMAGE061
Figure 100002_DEST_PATH_IMAGE062
Figure 927608DEST_PATH_IMAGE063
is a fitting coefficient to be solved, and obtains the following functional relation:
Figure 203868DEST_PATH_IMAGE064
(11)
the density of the gas is affected by the temperature, known as the absolute temperature
Figure 100002_DEST_PATH_IMAGE065
Lower gas density
Figure 14567DEST_PATH_IMAGE066
(the present embodiment)
Figure 100002_DEST_PATH_IMAGE067
Is a light-emitting diode of 293.15K,
Figure 720486DEST_PATH_IMAGE068
is 1.208 kg/L) at absolute temperature by the ideal gas equation
Figure 100002_DEST_PATH_IMAGE069
Lower density
Figure 228828DEST_PATH_IMAGE070
Figure 100002_DEST_PATH_IMAGE071
(12)
That is, the pressure difference versus flow becomes:
Figure 208197DEST_PATH_IMAGE072
(13)
(2) calculating instantaneous flow by using time difference method measurement principle
Figure 612634DEST_PATH_IMAGE014
Figure 727220DEST_PATH_IMAGE016
(4)
Figure 258827DEST_PATH_IMAGE017
(5)
In the above formulas (4) and (5),
Figure 100002_DEST_PATH_IMAGE073
is the cross section area of the flow passage of the ultrasonic gas meter,
Figure 837576DEST_PATH_IMAGE019
is the average velocity of the gas medium in the flow passage of the ultrasonic gas meter,
Figure 927760DEST_PATH_IMAGE074
is the length of the sound path,
Figure 529643DEST_PATH_IMAGE021
is the angle of the sound track,
Figure 910946DEST_PATH_IMAGE022
is the downstream propagation time of the ultrasonic wave in the gas medium,
Figure 32617DEST_PATH_IMAGE023
is the countercurrent propagation time of ultrasonic waves in a gas medium; wherein, the cross-sectional area of the flow passage
Figure 778856DEST_PATH_IMAGE073
Length of sound path
Figure 399193DEST_PATH_IMAGE074
Angle of sound channel
Figure 36716DEST_PATH_IMAGE021
Is a constant value, and the instantaneous flow can be calculated according to the downstream propagation time and the upstream propagation time of the ultrasonic wave in the gas medium
Figure 996582DEST_PATH_IMAGE024
. It can be seen that the forward flow propagation time and the backward flow propagation time of the ultrasonic wave in the gas medium are key measurement values of the instantaneous flow measurement of the ultrasonic gas meter, and the measurement precision is affected.
(3) Judging whether the wave is jumped or not, and adjusting the downstream propagation time and the upstream propagation time of the ultrasonic waves in the gas medium
Calculating the instantaneous flow at the current moment according to the time difference method measuring principle in the step (2)
Figure 179302DEST_PATH_IMAGE025
And (2) the function relation between the pressure difference and the instantaneous flow obtained in the step (1) can be used for deducing the theoretical pressure difference at the current moment
Figure 303247DEST_PATH_IMAGE026
Figure 100002_DEST_PATH_IMAGE075
(14)
Differential pressure sensor for detecting pressure difference inside and outside flow channel of ultrasonic gas meter in real time
Figure 760773DEST_PATH_IMAGE076
When the difference between the measured pressure difference and the theoretical pressure difference
Figure 100002_DEST_PATH_IMAGE077
Figure 355571DEST_PATH_IMAGE078
The maximum range of the allowable difference between the actually measured pressure difference and the theoretical pressure difference indicates that no wave jump phenomenon exists at the moment; when the difference between the measured pressure difference and the theoretical pressure difference
Figure 100002_DEST_PATH_IMAGE079
It is explained that the instantaneous flow rate is calculated with an error, and the forward propagation time and the backward propagation time of the ultrasonic wave in the gas medium need to be adjusted because a beat wave exists in the time measurement of the forward propagation time and the backward propagation time of the ultrasonic wave in the gas medium. According to the curve fitted in the present embodiment,
Figure 302667DEST_PATH_IMAGE080
is 3.2Pa, so the maximum range of the allowable difference between the measured pressure difference and the theoretical pressure difference at the current moment
Figure 100002_DEST_PATH_IMAGE081
5Pa may be taken.
From measured pressure differences
Figure 117171DEST_PATH_IMAGE031
And the functional relation between the pressure difference and the instantaneous flow rate to deduce the theoretical instantaneous flow rate
Figure 847229DEST_PATH_IMAGE032
Figure 821833DEST_PATH_IMAGE082
(15)
Theoretical instantaneous flow
Figure 100002_DEST_PATH_IMAGE083
The theoretical forward flow propagation time and the theoretical reverse flow propagation time of the ultrasonic wave in the gas medium approximately satisfy the following relations:
Figure 877514DEST_PATH_IMAGE084
(6)
Figure 163002DEST_PATH_IMAGE035
(7)
in the formulae (6) and (7),
Figure 100002_DEST_PATH_IMAGE085
is the theoretical downstream propagation time of the ultrasonic wave in the gas medium,
Figure 244221DEST_PATH_IMAGE086
is the theoretical countercurrent propagation time of ultrasonic waves in a gas medium,
Figure 100002_DEST_PATH_IMAGE087
is the propagation velocity of sound waves in a gaseous medium.
Figure 610350DEST_PATH_IMAGE067
Speed of sound in air at 293.15K
Figure 384402DEST_PATH_IMAGE087
Taking the value of 343.64m/s, the speed of sound is affected by temperature, at absolute temperature
Figure 688344DEST_PATH_IMAGE088
Speed of sound of lower
Figure 100002_DEST_PATH_IMAGE089
Figure 275052DEST_PATH_IMAGE090
(16)
Speed of sound in equation (16) when temperature changes
Figure 100002_DEST_PATH_IMAGE091
And (6) carrying out calculation by the formulas (6) and (7) to obtain the theoretical forward flow propagation time and the theoretical reverse flow propagation time of the ultrasonic wave in the gas medium.
In addition, when the wave jumping phenomenon occurs, the forward flow propagation time of the ultrasonic wave in the gas medium is actually measured
Figure 980840DEST_PATH_IMAGE092
And the theoretical downstream propagation time of ultrasonic waves in a gas medium
Figure 394635DEST_PATH_IMAGE036
Approximately differing by an integer number of ultrasonic transducer excitation signal periods, and actually measuring the counter-current propagation time of ultrasonic waves in a gas medium
Figure 654715DEST_PATH_IMAGE041
Theoretical counter-current propagation time with ultrasonic wave in gas medium
Figure 999109DEST_PATH_IMAGE042
Approximately differing by an integer number of ultrasonic transducer excitation signal periods, the approximate relationship is as follows:
Figure 74250DEST_PATH_IMAGE043
(8)
Figure 111476DEST_PATH_IMAGE044
(9)
in the formulas (8) and (9),
Figure 593273DEST_PATH_IMAGE045
is the period of the excitation signal of the ultrasonic transducer,
Figure 554407DEST_PATH_IMAGE046
Figure 438049DEST_PATH_IMAGE047
representing the wave number. The passing formula (6) -9 can adjust the actual measurement forward flow propagation time and the actual measurement reverse flow propagation time of the ultrasonic wave in the gas medium, thereby obtaining the instantaneous flow at the current moment
Figure 100002_DEST_PATH_IMAGE093
The following formula:
Figure 177335DEST_PATH_IMAGE049
(10)
sound path length of ultrasonic gas meter in this embodiment
Figure 401555DEST_PATH_IMAGE074
Is 0.0725m, vocal tract angle
Figure 353330DEST_PATH_IMAGE021
Is 45 ℃ and the cross-sectional area of the flow passage
Figure 153796DEST_PATH_IMAGE073
Is 0.0004m2Period of excitation signal of ultrasonic transducer
Figure 283557DEST_PATH_IMAGE094
Is 5 us. A set of experimental data was selected to further illustrate that when the instantaneous flow rate was 4.89m3H, function of pressure difference and instantaneous flowThe difference value between the theoretical pressure difference and the actually measured pressure difference at the current moment is 1.69Pa due to the number relation, and the difference value between the theoretical pressure difference and the actually measured pressure difference is less than 5Pa, so that the phenomenon of wave jumping is avoided. It can now be further verified that the theoretical instantaneous flow rate is 4.79m from the measured pressure difference of 56.07Pa and the instantaneous flow rate as a function of the pressure difference3Therefore, the wave number is 212.59us by the formulas (8) and (9) when the theoretical forward propagation time of the ultrasonic wave in the gas medium is 209.36us and the theoretical reverse propagation time of the ultrasonic wave in the gas medium is 212.62us, the actual forward propagation time of the ultrasonic wave in the gas medium is 210.3us, and the theoretical reverse propagation time of the ultrasonic wave in the gas medium is 212.59us
Figure 474367DEST_PATH_IMAGE046
Figure 229834DEST_PATH_IMAGE047
Is 0.
In summary, the invention installs the differential pressure sensor in the ultrasonic gas meter, detects the pressure difference inside and outside the flow channel of the ultrasonic gas meter through the differential pressure sensor, establishes the functional relationship between the pressure difference and the flow, and judges whether the wave jump problem exists in the downstream propagation time and the upstream propagation time of the ultrasonic wave in the gas medium measured in the time difference method, thereby preventing the occurrence of wrong measurement data. When the wave jumping phenomenon occurs, the pressure difference is used for correcting the forward flow propagation time and the reverse flow propagation time of the ultrasonic wave in the gas medium at the current moment, so that the instantaneous flow is adjusted, and the reliability and the accuracy of gas metering are improved.

Claims (5)

1. The method for improving the instantaneous flow metering precision of the ultrasonic gas meter based on the pressure data is characterized by comprising the following steps of: installing a differential pressure sensor in the ultrasonic gas meter, wherein two gas pressure acquisition ports of the differential pressure sensor are respectively installed in a flow channel and outside the flow channel, so that the pressure difference between the inside and outside of the flow channel of the ultrasonic gas meter is detected, the downstream propagation time and the upstream propagation time of the ultrasonic wave in the gas at the current moment are measured by adopting a time difference method, and the instantaneous flow is calculated by utilizing the downstream propagation time and the upstream propagation time of the ultrasonic wave in a gas medium; and judging whether the wave jump problem exists according to the measured pressure difference and the instantaneous flow, and correcting the downstream propagation time and the upstream propagation time at the current moment by using pressure difference data when the wave jump phenomenon occurs, so as to obtain the accurate instantaneous flow at the current moment.
2. The method for improving the instantaneous flow metering accuracy of the ultrasonic gas meter based on the pressure data as claimed in claim 1, wherein the calculation of the instantaneous flow comprises the following steps:
(1) measuring the relation between the pressure difference and the instantaneous flow, (2) measuring the instantaneous flow by using a time difference method, and (3) judging whether the wave is jumped or not, and adjusting the forward flow propagation time and the reverse flow propagation time of the ultrasonic wave in the gas medium.
3. The method for improving the instantaneous flow metering accuracy of the ultrasonic gas meter based on the pressure data as claimed in claim 2, wherein the method for measuring the relation between the pressure difference and the instantaneous flow in the step (1) is as follows:
installing a differential pressure sensor in the flow channel of the ultrasonic gas meter, and detecting the pressure difference inside and outside the flow channel of the ultrasonic gas meter through the differential pressure sensor; according to the Bernoulli equation, the pressure inside and outside the flow channel of the ultrasonic gas meter meets the following formula:
Figure DEST_PATH_IMAGE002
(1)
wherein the content of the first and second substances,
Figure DEST_PATH_IMAGE004
is the pressure in the cavity of the ultrasonic gas meter,
Figure DEST_PATH_IMAGE006
is the pressure in the flow channel of the ultrasonic gas meter,
Figure DEST_PATH_IMAGE008
is average flow of gas medium in the cavity of the ultrasonic gas meterAt the speed of the operation of the device,
Figure DEST_PATH_IMAGE010
is the average flow velocity of the gas medium in the flow passage of the ultrasonic gas meter,
Figure DEST_PATH_IMAGE012
is the gas density;
from conservation of mass, we obtain:
Figure DEST_PATH_IMAGE014
(2)
wherein, the first and the second end of the pipe are connected with each other,
Figure DEST_PATH_IMAGE016
is the sectional area in the cavity of the ultrasonic gas meter,
Figure DEST_PATH_IMAGE018
the cross section area in the flow channel of the ultrasonic gas meter;
the pressure difference between the inside and the outside of the flow passage of the ultrasonic gas meter is obtained by the formulas (1) and (2)
Figure DEST_PATH_IMAGE020
Figure DEST_PATH_IMAGE022
(3)
According to the formula (3), the pressure difference between the inside and the outside of the flow channel of the ultrasonic gas meter measured by the differential pressure sensor is related to the average flow velocity of the gas medium in the flow channel, and the instantaneous flow is the product of the average flow velocity of the gas medium in the flow channel and the cross section area of the flow channel, so that the pressure difference between the inside and the outside of the flow channel of the ultrasonic gas meter is related to the instantaneous flow of the ultrasonic gas meter;
sequentially introducing flow to obtain pressure difference data under different instantaneous flows, and performing data processing on the pressure difference data and the instantaneous flows by using a function modelFitting:
Figure DEST_PATH_IMAGE024
wherein, in the step (A),
Figure DEST_PATH_IMAGE026
which is indicative of a pressure difference,
Figure DEST_PATH_IMAGE028
which is indicative of the instantaneous flow rate of the fluid,
Figure DEST_PATH_IMAGE030
is a functional model fitted to the pressure difference and instantaneous flow.
4. The method for improving the instantaneous flow metering accuracy of the ultrasonic gas meter based on the pressure data as claimed in claim 3, wherein the step (2) of measuring the instantaneous flow by using the time difference method comprises the following steps:
Figure DEST_PATH_IMAGE032
(4)
Figure DEST_PATH_IMAGE034
(5)
in the above formulas (4) and (5),
Figure DEST_PATH_IMAGE036
is the cross section area of the flow passage of the ultrasonic gas meter,
Figure DEST_PATH_IMAGE038
is the average velocity of the gas medium in the flow passage of the ultrasonic gas meter,
Figure DEST_PATH_IMAGE040
is the length of the sound path,
Figure DEST_PATH_IMAGE042
is the angle of the sound track,
Figure DEST_PATH_IMAGE044
is the downstream propagation time of the ultrasonic wave in the gas medium,
Figure DEST_PATH_IMAGE046
is the countercurrent propagation time of ultrasonic waves in a gas medium; wherein, the cross-sectional area of the flow passage
Figure DEST_PATH_IMAGE036A
Length of sound path
Figure DEST_PATH_IMAGE047
Angle of sound channel
Figure DEST_PATH_IMAGE042A
Is a constant value, and the instantaneous flow can be calculated according to the downstream propagation time and the upstream propagation time of the ultrasonic wave in the gas medium
Figure DEST_PATH_IMAGE048
5. The method for improving the instantaneous flow metering accuracy of the ultrasonic gas meter based on the pressure data as claimed in claim 4, wherein the step (3) is to judge whether the wave is jumped or not, and the steps of adjusting the forward flow propagation time and the backward flow propagation time of the ultrasonic wave in the gas medium are as follows:
calculating the instantaneous flow at the current moment according to the time difference method measuring principle in the step (2)
Figure DEST_PATH_IMAGE050
And (2) the function relation between the pressure difference and the instantaneous flow obtained in the step (1) can be used for deducing the theoretical pressure difference at the current moment
Figure DEST_PATH_IMAGE052
(ii) a Differential pressure sensor for detecting pressure difference inside and outside flow channel of ultrasonic gas meter in real time
Figure DEST_PATH_IMAGE054
When the difference between the measured pressure difference and the theoretical pressure difference
Figure DEST_PATH_IMAGE056
Figure DEST_PATH_IMAGE058
The maximum range of the allowable difference between the actually measured pressure difference and the theoretical pressure difference indicates that no wave jump phenomenon exists at the moment; when the difference between the measured pressure difference and the theoretical pressure difference
Figure DEST_PATH_IMAGE060
When the instantaneous flow is calculated incorrectly, the ultrasonic waves have the existence of bouncing waves in the time measurement of the downstream propagation time and the upstream propagation time in the gas medium, so that the downstream propagation time and the upstream propagation time of the ultrasonic waves in the gas medium need to be adjusted;
from measured pressure differences
Figure DEST_PATH_IMAGE062
And the functional relation between the pressure difference and the instantaneous flow rate to deduce the theoretical instantaneous flow rate
Figure DEST_PATH_IMAGE064
Figure DEST_PATH_IMAGE065
The theoretical forward flow propagation time and the theoretical reverse flow propagation time of the ultrasonic wave in the gas medium approximately satisfy the following relations:
Figure DEST_PATH_IMAGE067
(6)
Figure DEST_PATH_IMAGE069
(7)
in the formulae (6) and (7),
Figure DEST_PATH_IMAGE071
is the theoretical downstream propagation time of the ultrasonic wave in the gas medium,
Figure DEST_PATH_IMAGE073
is the theoretical countercurrent propagation time of ultrasonic waves in a gas medium,
Figure DEST_PATH_IMAGE075
is the propagation velocity of sound waves in a gaseous medium; in addition, when the wave jumping phenomenon occurs, the forward flow propagation time of the ultrasonic wave in the gas medium is actually measured
Figure DEST_PATH_IMAGE077
And the theoretical downstream propagation time of ultrasonic waves in a gas medium
Figure DEST_PATH_IMAGE079
Approximately differing by an integer number of ultrasonic transducer excitation signal periods, and actually measuring the counter-current propagation time of ultrasonic waves in a gas medium
Figure DEST_PATH_IMAGE081
Theoretical counter-current propagation time with ultrasonic wave in gas medium
Figure DEST_PATH_IMAGE083
Approximately differing by an integer number of ultrasonic transducer excitation signal periods, the approximate relationship is as follows:
Figure DEST_PATH_IMAGE085
(8)
Figure DEST_PATH_IMAGE087
(9)
in the formulas (8) and (9),
Figure DEST_PATH_IMAGE089
is the period of the excitation signal of the ultrasonic transducer,
Figure DEST_PATH_IMAGE091
Figure DEST_PATH_IMAGE093
represents the wave number; the passing formula (6) -9 can adjust the actual measurement forward flow propagation time and the actual measurement reverse flow propagation time of the ultrasonic wave in the gas medium, thereby obtaining the instantaneous flow at the current moment
Figure DEST_PATH_IMAGE095
The following formula:
Figure DEST_PATH_IMAGE097
(10) 。
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