CN117109676A - Ultrasonic water meter flow field design with small pressure loss and strong fluid disturbance resistance - Google Patents

Ultrasonic water meter flow field design with small pressure loss and strong fluid disturbance resistance Download PDF

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Publication number
CN117109676A
CN117109676A CN202311376647.XA CN202311376647A CN117109676A CN 117109676 A CN117109676 A CN 117109676A CN 202311376647 A CN202311376647 A CN 202311376647A CN 117109676 A CN117109676 A CN 117109676A
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China
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area
water meter
flow
pressure loss
ultrasonic water
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CN202311376647.XA
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CN117109676B (en
Inventor
陈治国
沈华刚
宋冠锋
毕晨家
刘天扬
高鹏飞
范建华
王建华
陈维广
赵磊
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Qingdao Dingxin Communication Power Engineering Co ltd
Qingdao Topscomm Communication Co Ltd
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Qingdao Dingxin Communication Power Engineering Co ltd
Qingdao Topscomm Communication Co Ltd
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Priority to CN202410481642.1A priority Critical patent/CN118190095A/en
Priority to CN202311376647.XA priority patent/CN117109676B/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
    • G01F1/662Constructional details
    • 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

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

Abstract

The invention relates to the technical field of ultrasonic water meters, and discloses an ultrasonic water meter flow field design with small pressure loss and strong fluid disturbance resistance, which comprises a flow stable metering area, a rectifying transition area and a straight pipe area; two ends of the flow stabilizing and metering area are respectively connected with a rectification transition area; the other ends of the two rectification transition areas are respectively connected with a straight pipe area. The ultrasonic water meter flow channel is mainly divided into a flow stable metering area and a rectification transition area, smooth gradual reduction and curvature continuous transition between an uncontracted straight pipe section area and the flow stable metering area are realized by utilizing a Vitoxineski curve horizontal stretching curved surface, and 4 degrees of freedom including the length of the rectification transition area, the radial height of the section of the flow stable metering area, a streamline rectification blade and a diversion channel are introduced, so that the ultrasonic water meter has the advantages of small pressure loss and strong fluid disturbance resistance, and the low water delivery energy consumption and the accurate flow metering are realized.

Description

Ultrasonic water meter flow field design with small pressure loss and strong fluid disturbance resistance
Technical Field
The invention relates to the technical field of ultrasonic water meters, in particular to an ultrasonic water meter flow field design with small pressure loss and strong fluid disturbance resistance.
Background
The ultrasonic water meter utilizes an ultrasonic transit time method to obtain a forward and reverse flow time difference through ultrasonic signal processing by a metering algorithm, realizes accurate flow metering, and has the advantages of low starting flow, high range ratio, high metering precision and the like. If an elbow pipe or a valve exists at the upstream and the downstream of the ultrasonic water meter, fluid disturbance can generate a rotary flow field or an uneven flow field, so that the flow field stability of an ultrasonic signal acquisition area, namely a metering area is affected, and metering errors are generated. To obtain accurate flow metering, a rectifier is typically placed at the water inlet/outlet of the water meter or the cross-sectional area of the tube segment in the metering area is reduced, which results in a larger pressure loss and increases the energy consumption of water delivery.
Disclosure of Invention
Aiming at the defects and drawbacks existing in the prior art, the invention provides an ultrasonic water meter flow field design with small pressure loss and strong fluid disturbance resistance, which has higher fluid disturbance resistance capability while reducing the pressure loss, and realizes low water delivery energy consumption and accurate flow metering.
The object of the invention can be achieved by the following technical scheme.
An ultrasonic water meter flow field design with small pressure loss and strong fluid disturbance resistance comprises a flow stable metering area, a rectifying transition area and a straight pipe area.
Two ends of the flow stabilizing and metering area are respectively connected with a rectification transition area; the other ends of the two rectification transition areas are respectively connected with a straight pipe area.
Preferably, the longitudinal section shape of the flow stabilizing metering area adopts a rectangular shape or a shape formed by combining a rectangle, a trapezoid and an arc shape.
The sectional area of the longitudinal section is determined according to the continuity equation of incompressible fluid in fluid mechanics and the range ratio of an ultrasonic water meter.
Preferably, a Vitoxinesky curve horizontal stretching curved surface is adopted in the rectification transition region, so that smooth gradual reduction and curvature continuous transition between the straight pipe section region and the flow stable metering region are realized.
Preferably, a streamline rectifying blade for reducing pressure loss and resisting disturbance flow is arranged on the Vitocinsky curve horizontal stretching curved surface.
And a diversion channel for reducing pressure loss and resisting turbulence is arranged on the Vitoxineski curve horizontal stretching curved surface.
Preferably, the pressure loss and the fluid disturbance resistance of the ultrasonic water meter flow field can be adjusted by adjusting the length of the rectification transition area and the radial height of the cross section of the flow stabilizing and metering area.
The beneficial technical effects of the invention are as follows: the ultrasonic water meter flow channel is mainly divided into a flow stable metering area and a rectification transition area, smooth gradual shrinkage and curvature continuous transition between an uncontracted straight pipe section area and the flow stable metering area are realized by utilizing a Vitoxineski curve horizontal stretching curved surface, and the advantages of small pressure loss and strong fluid disturbance resistance are realized by introducing 4 degrees of freedom of the length of the rectification transition area, the radial height of the section of the flow stable metering area, streamline rectification blades and a diversion channel, so that the ultrasonic water meter has the advantages of low water delivery energy consumption and accurate flow metering.
Drawings
Fig. 1 is a three-dimensional schematic diagram of an ultrasonic water meter flow field structure in an embodiment of the invention.
Fig. 2 is a front cross-sectional view of an ultrasonic water meter flow field structure in an embodiment of the invention.
Fig. 3 is a side cross-sectional view of an ultrasonic water meter flow field structure in an embodiment of the invention.
Fig. 4 is a top cross-sectional view of an ultrasonic water meter flow field structure in an embodiment of the invention.
FIG. 5 is a Vetussi curve of the present invention.
Fig. 6 is a cloud chart of ultrasonic water meter flow field wall pressure distribution in an embodiment of the invention.
Fig. 7 is a three-dimensional perspective view of a half ultrasonic water meter flow field structure in an embodiment of the invention.
Reference numerals: 10 is a flow stabilizing and metering area, 20 is a rectifying transition area, 30 is a straight pipe area, 201, 202 and 203 are Vitoxinesky curve-shaped horizontal stretching curved surfaces, 204 and 205 are streamline rectifying blades, and 206 is a diversion channel.
Detailed Description
The present invention will be described in further detail with reference to the drawings and examples, in order to make the objects, technical solutions and advantages of the present invention more apparent. It should be understood that the specific embodiments described herein are for purposes of illustration only and are not intended to limit the scope of the invention.
Examples: as shown in FIG. 1, the ultrasonic water meter flow field design with small pressure loss and strong fluid disturbance resistance comprises an ultrasonic water meter flow field, and is mainly divided into a flow stabilizing and metering area 10, a rectifying transition area 20 and a straight pipe area 30.
According to different measuring range ratio requirements, combining a continuity equation of incompressible fluid in fluid mechanics to determine the sectional area of a flow stable measuring area, wherein the flow stable measuring area 10 is in a shape formed by combining a rectangle, a trapezoid and an arc, and the sectional area of the rectangular chamfer is 106.4mm 2 R500 meter meeting ultrasonic water meter range ratioThe amount is required.
The rectification transition region 20 is determined according to the radial height difference between the flow stabilizing and metering region 10 and the straight pipe section region 30, as shown in fig. 2 and 4, the transition curved surface in the rectification transition region 20 adopts the Vitoxinesky curve-shaped horizontal stretching curved surfaces 201, 202 and 203 to realize smooth gradual reduction and curvature continuous transition between the straight pipe section region 30 and the flow stabilizing and metering section region 10, and has the functions of low pressure loss transition and flow field pulsation reduction.
As shown in fig. 5, the victims curve equation is as follows.
Wherein: r is (r) 1 Expressed as the radius of the cross section before shrinkage, r 2 The radial height of the cross-section of the flow stabilization metering zone 10 is denoted by L, the length of the transition zone 20 is rectified, r, the radius of the cross-section, and L, the contracted length.
In this embodiment, parameters of the vicocinsky curve horizontal stretching curved surface 201 are: l=6.12 mm, r 1 =6.87mm,r 2 =5.37 mm; the parameters of the transition surface 202 are: l=21 mm, r 1 =7.5mm,r 2 =0.28 mm; the parameters of the transition surface 203 are: l=7.5 mm, r 1 =7.5mm,r 2 =4mm。
As shown in fig. 3, rectifying blades 204, 205 with anti-rotation turbulence function and a diversion channel 206 with reduced pressure loss and anti-turbulence function are placed on the Vetoski curve horizontal stretching curved surfaces 201, 202. The streamline blade 204 height maximum is about 1.1mm and the streamline blade height 205 maximum is about 7mm; the channel 206 has a depth of about 1.2mm and a width of about 2.34mm.
Fig. 7 is a perspective view of a three-dimensional structure of a half ultrasonic water meter flow field with small pressure loss and strong fluid disturbance resistance, wherein the three-dimensional structure of the ultrasonic water meter flow field is an axisymmetric structure.
Further, a Comsol Multiphysics multi-physical-field simulation software CFD module is utilized, a turbulence model 'k-epsilon model' commonly used in industry is adopted, all split-flow field models with the structure shown in fig. 7 are adopted, the water inlet flow of the model is set to be 2.5L/h, the corresponding inlet speed is 3.94m/s, the total pressure of a water outlet is one atmosphere, and a wall pressure cloud pattern is calculated in a simulation mode.
Further, the water inlet flow is determined according to national standard GBT 778.1-2018 drinking cold water meter and hot water meter pressure loss test rules.
As shown in fig. 5, the pressure of the flow guide channel 206 is smaller when the flow guide channel 206 exists compared with the pressure of the flow guide channel 206 or not when the flow guide channel 206 exists on the curved horizontal stretching curved surface 202 of the victims curve shape, and the resistance of the transition curved surface to water flow is reduced due to the existence of the flow guide channel 206.
Further, in fig. 5, the average pressures of the water inlet and the water outlet are calculated under the two-medium model, and the average pressures are subtracted to obtain the pressure loss, wherein the pressure loss is 25.8kPa without a diversion channel 206, and the pressure loss is 22kPa with a diversion channel 206.
Further, according to the pressure loss test rule in national standard GBT 778.1-2018 drinking cold water meter and hot water meter, the pressure loss of 23kPa of the flow channel model with the flow guide channel 206 is measured under the condition of 2.5L/h. This embodiment has a smaller pressure loss than the like product.
Further, according to the fluid disturbance test of the national standard GBT 778.1-2018 drinking cold water meter and the hot water meter, the flow field sensitivity level U0D0 is set in a specified experimental setting mode, and under the condition of 2.5L/h of flow, the k coefficient deviation rate of the graph-flow channel structure and the flow after the spoiler is added is tested.
Further, the method comprises the steps of,wherein Q represents the water flow in the experimental process, which is obtained by a weighing method, and delta t represents the propagation time difference of the upstream and downstream receiving signals of the ultrasonic water meter.
Table 1 the results of the spoiler deviation,
turbulence type Front right-hand screw Rear right-hand screw Front speed profile Post velocity profile
Deviation ratio (%) 0.7 0.26 0.67 0.4
As shown in Table 1, the deviation rate result is smaller than that of the national standard GBT 778.1-2018 drinking cold water meter, and the error is not more than +/-2% of the maximum allowable error. The ultrasonic meter flow channel embodiment thus has a high resistance to fluid disturbance.
The above embodiments are illustrative of the specific embodiments of the present invention, and not restrictive, and various changes and modifications may be made by those skilled in the relevant art without departing from the spirit and scope of the invention, so that all such equivalent embodiments are intended to be within the scope of the invention.

Claims (5)

1. The ultrasonic water meter flow field design with small pressure loss and strong fluid disturbance resistance is characterized by comprising a flow stable metering area (10), a rectifying transition area (20) and a straight pipe area (30);
two ends of the flow stabilizing and metering area (10) are respectively connected with a rectification transition area (20); the other ends of the two rectification transition areas (20) are respectively connected with a straight pipe section area (30).
2. The ultrasonic water meter flow field design with small pressure loss and strong fluid disturbance resistance according to claim 1, wherein the longitudinal section shape of the flow stabilizing and metering area (10) adopts a shape formed by combining a rectangle or a rectangle, a trapezoid and an arc;
the sectional area of the longitudinal section is determined according to the continuity equation of incompressible fluid in fluid mechanics and the range ratio of an ultrasonic water meter.
3. The ultrasonic water meter flow field design with small pressure loss and strong fluid disturbance resistance according to claim 1, wherein the rectification transition region (20) adopts a Vitoxinesky curve type horizontal stretching curved surface (201, 202, 203) to realize smooth gradual reduction and curvature continuous transition between the straight pipe section region (30) and the flow stable metering region (10).
4. An ultrasonic water meter flow field design with low pressure loss and high immunity to fluid disturbance according to claim 3, characterized in that said victims curve shaped horizontal stretching curved surface (201, 202) is placed with streamline rectifying blades (204, 205) for reducing pressure loss and immunity to disturbance flow;
and a diversion channel (206) for reducing pressure loss and resisting turbulence is arranged on the Vitoxineski curve horizontal stretching curved surface (202).
5. The ultrasonic water meter flow field design with small pressure loss and strong fluid disturbance resistance according to claim 1, wherein the pressure loss and the fluid disturbance resistance of the ultrasonic water meter flow field can be adjusted by adjusting the length of the rectifying transition region (20) and the radial height of the cross section of the flow stabilizing metering region (10).
CN202311376647.XA 2023-10-24 2023-10-24 Ultrasonic water meter flow field design with small pressure loss and strong fluid disturbance resistance Active CN117109676B (en)

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CN202410481642.1A CN118190095A (en) 2023-10-24 2023-10-24 Ultrasonic water meter flow field with small pressure loss and strong fluid disturbance resistance
CN202311376647.XA CN117109676B (en) 2023-10-24 2023-10-24 Ultrasonic water meter flow field design with small pressure loss and strong fluid disturbance resistance

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Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN204313901U (en) * 2015-01-05 2015-05-06 上海迪纳声科技股份有限公司 Multi-paths Ultrasonic water meter, calorimeter are with measuring pipeline section
CN110793580A (en) * 2019-11-06 2020-02-14 宁波水表股份有限公司 Circular arc transition structure on two sides of measuring section of ultrasonic water meter
CN115265689A (en) * 2022-09-30 2022-11-01 济南沛华信息科技有限公司 Ultrasonic reflection structure, measurement pipeline section and ultrasonic flowmeter

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN204313901U (en) * 2015-01-05 2015-05-06 上海迪纳声科技股份有限公司 Multi-paths Ultrasonic water meter, calorimeter are with measuring pipeline section
CN110793580A (en) * 2019-11-06 2020-02-14 宁波水表股份有限公司 Circular arc transition structure on two sides of measuring section of ultrasonic water meter
CN115265689A (en) * 2022-09-30 2022-11-01 济南沛华信息科技有限公司 Ultrasonic reflection structure, measurement pipeline section and ultrasonic flowmeter

Non-Patent Citations (3)

* Cited by examiner, † Cited by third party
Title
WU, NIANCHU: "NUMERICAL INVESTIGATION OF HVAF-SPRAYED Fe-BASED AMORPHOUS COATINGS", 《MATERIALI IN TEHNOLOGIJE》, vol. 56, no. 6, 5 February 2023 (2023-02-05) *
严渊达: "维托辛斯基收敛曲线在大口径 超声波水表流道设计中的应用", 《仪表技术》, no. 1 *
杨敏官: "轴流泵叶轮导水锥型式设计及其流道水力特性模拟", 《农业工程学报》, vol. 31, no. 11, 30 June 2015 (2015-06-30) *

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