KR101693726B1 - Ultrasonic transducing apparatus for measuring pipe thickness and caliber and for measuring fluid flow and velocity using the same - Google Patents
Ultrasonic transducing apparatus for measuring pipe thickness and caliber and for measuring fluid flow and velocity using the same Download PDFInfo
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- KR101693726B1 KR101693726B1 KR1020150103675A KR20150103675A KR101693726B1 KR 101693726 B1 KR101693726 B1 KR 101693726B1 KR 1020150103675 A KR1020150103675 A KR 1020150103675A KR 20150103675 A KR20150103675 A KR 20150103675A KR 101693726 B1 KR101693726 B1 KR 101693726B1
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- wedge
- ultrasonic transducer
- ultrasonic
- pipe
- attached
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01D—MEASURING NOT SPECIALLY ADAPTED FOR A SPECIFIC VARIABLE; ARRANGEMENTS FOR MEASURING TWO OR MORE VARIABLES NOT COVERED IN A SINGLE OTHER SUBCLASS; TARIFF METERING APPARATUS; MEASURING OR TESTING NOT OTHERWISE PROVIDED FOR
- G01D21/00—Measuring or testing not otherwise provided for
- G01D21/02—Measuring two or more variables by means not covered by a single other subclass
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01B—MEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
- G01B17/00—Measuring arrangements characterised by the use of infrasonic, sonic or ultrasonic vibrations
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01B—MEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
- G01B17/00—Measuring arrangements characterised by the use of infrasonic, sonic or ultrasonic vibrations
- G01B17/02—Measuring arrangements characterised by the use of infrasonic, sonic or ultrasonic vibrations for measuring thickness
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01F—MEASURING VOLUME, VOLUME FLOW, MASS FLOW OR LIQUID LEVEL; METERING BY VOLUME
- G01F1/00—Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow
- G01F1/66—Measuring 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
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01P—MEASURING LINEAR OR ANGULAR SPEED, ACCELERATION, DECELERATION, OR SHOCK; INDICATING PRESENCE, ABSENCE, OR DIRECTION, OF MOVEMENT
- G01P5/00—Measuring speed of fluids, e.g. of air stream; Measuring speed of bodies relative to fluids, e.g. of ship, of aircraft
- G01P5/24—Measuring speed of fluids, e.g. of air stream; Measuring speed of bodies relative to fluids, e.g. of ship, of aircraft by measuring the direct influence of the streaming fluid on the properties of a detecting acoustical wave
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- Physics & Mathematics (AREA)
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- Engineering & Computer Science (AREA)
- Acoustics & Sound (AREA)
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- Aviation & Aerospace Engineering (AREA)
- Electromagnetism (AREA)
- Fluid Mechanics (AREA)
- Measuring Volume Flow (AREA)
Abstract
The present invention relates to a method of manufacturing a pipe having a contact surface attached to an outer wall of a pipe and having a contact surface having a first length, an upper surface formed parallel to the contact surface and having a second length longer than the first length, The ultrasonic transducer attached to the upper surface of each wedge, and the ultrasonic signal output from the ultrasonic transducer attached to the first wedge, based on the time difference of the reflected wave reflected from the inner wall of the pipe The thickness and the inner diameter of the pipe are measured and the ultrasonic signals outputted from the ultrasonic transducer attached to the first wedge and the second wedge are reflected on the inclined surface and are transmitted to the ultrasonic transducer attached to the second wedge and the first wedge And a controller for measuring the flow rate and the flow rate of the fluid inside the pipe based on the time.
Description
The present invention relates to an ultrasonic transducer capable of simultaneously measuring the thickness, inner diameter, flow velocity and flow rate of a pipe.
Generally, an ultrasonic flowmeter or an anemometer includes a transmitting transducer and a receiving transducer that transmit and receive an ultrasonic signal by using a state change of fluid flowing in the pipe, and the transmission and reception of ultrasonic signals are repeated a predetermined number of times between the transmitting transducer and the receiving transducer The flow rate or the flow rate of the fluid is detected by measuring the propagation time according to the state change of the fluid while the transmission and reception of the ultrasonic signal is repeated.
The pipe thickness is an important variable when calculating the flow rate and flow rate. Currently used ultrasonic flowmeters or anemometers are used either by inputting the thickness or inner diameter as specified in the pipe specification table or by measuring the thickness or inner diameter directly. However, the thickness and inner diameter of the pipe may be measured or different from the thickness when produced by scale or environmental factors, and the pipe may be installed in a position that is difficult to measure directly. If the thickness of the actual pipe is different from the thickness of the pipe, there is a problem in that an error occurs in the flow rate and flow velocity of the fluid.
In this regard, Korean Patent Registration No. 1513697 (entitled "Ultrasonic Transducer Capable of Measuring Pipe Thickness and Flow Rate Measurement Apparatus Using the Same") discloses an ultrasonic transducer which is attached to an outer wall of a pipe and has a contact surface with a pipe, An ultrasonic transducer for measuring the thickness of a pipe based on a time difference between two or more reflected waves re-transmitted to an ultrasonic transducer, including an ultrasonic transducer for propagating an ultrasonic signal into a pipe through a wedge, and a flow velocity measuring device using the ultrasonic transducer .
On the other hand, the conventional ultrasonic transducer has two reflection surfaces on the wedge, which has a disadvantage that the measurement path is distant. Accordingly, the influence of the error due to the shape was large, and a large amount of energy loss occurred due to a plurality of ultrasonic wave transmission and reflection.
The present invention provides an ultrasonic transducer capable of simultaneously changing the wedge shape of an ultrasonic transducer of a conventional ultrasonic flowmeter and simultaneously measuring the thickness, inner diameter, flow velocity and flow rate of the pipe through the wedge shape, There is a purpose.
It is to be understood, however, that the technical scope of the present invention is not limited to the above-described technical problems, and other technical problems may be present.
According to an aspect of the present invention, there is provided an ultrasonic transducer including a contact surface having a first length attached to an outer wall of a pipe, a contact surface formed parallel to the contact surface and having a second length longer than the first length, A first and a second wedge including an inclined surface formed by connecting the upper surface and the upper surface with the end of the contact surface and having a predetermined inclination angle, an ultrasonic transducer attached to the upper surface of each wedge, and an ultrasonic transducer The thickness and the inner diameter of the pipe are measured based on the time difference between the reflected waves reflected from the inner wall of the pipe and the ultrasonic signals output from the ultrasonic transducers attached to the first wedge and the second wedge are reflected Based on the time taken to be delivered to the second wedge and the ultrasonic transducer attached to the first wedge, And a control unit for measuring the flow rate and the flow rate of the fluid.
A contact surface having a first length according to an embodiment of the present invention, an upper surface formed parallel to the contact surface and having a second length longer than the first length, and an inclined surface formed to connect the upper surface and the end of the contact surface, The energy loss of the ultrasonic signal is minimized and the thickness and the inner diameter of the pipe can be measured and the flow velocity and the flow rate of the fluid inside the pipe can be accurately measured.
1 is a block diagram showing a configuration of an ultrasonic wave converting apparatus according to an embodiment of the present invention.
2 is a view for explaining the shapes of first and second wedges according to an embodiment of the present invention.
3 is a view for explaining a method of measuring a thickness and an inner diameter of a pipe according to an embodiment of the present invention.
4A and 4B are views for explaining flow velocity and flow rate measurement method according to an embodiment of the present invention.
5 is a view for explaining a method of measuring a flow velocity of a fluid in a pipe according to an embodiment of the present invention.
6 is a view for explaining an ultrasonic transducer arranged in two or more in parallel according to an embodiment of the present invention.
7 is a view for explaining a method of further coupling a wedge extension to a wedge shape according to an embodiment of the present invention.
Hereinafter, embodiments of the present invention will be described in detail with reference to the accompanying drawings, which will be readily apparent to those skilled in the art. The present invention may, however, be embodied in many different forms and should not be construed as limited to the embodiments set forth herein. In order to clearly illustrate the present invention, parts not related to the description are omitted, and similar parts are denoted by like reference characters throughout the specification.
Throughout the specification, when a part is referred to as being "connected" to another part, it includes not only "directly connected" but also "electrically connected" with another part in between . Also, when an element is referred to as "including" an element, it is to be understood that the element may include other elements as well as other elements, And does not preclude the presence or addition of one or more other features, integers, steps, operations, components, parts, or combinations thereof.
FIG. 1 is a block diagram showing a configuration of an ultrasonic transducer according to an embodiment of the present invention, and FIG. 2 is a view for explaining the shapes of first and second wedges according to an embodiment of the present invention.
1, the
The
Also, the
The
The
The
Hereinafter, the shapes of the first and second wedges according to one embodiment of the present invention will be described.
As shown in FIG. 2A, the
The
The
The
2 (a), the inclination angle between the
[Equation 1]
Here,? Is an incident angle.
In addition, the energy transmittance of the
2 (b), the
The
The
The
The
2 (b), the
An
3 is a view for explaining a method of measuring a thickness and an inner diameter of a pipe according to an embodiment of the present invention.
The
The
3 (a), the ultrasonic wave output from the first
3, the
The
3, the
The
On the other hand, the thickness and the inner diameter of the
In the case of the
3B, ultrasonic waves output from the first
Accordingly, the
The description of the configuration shown in FIG. 3 (a) that performs the same function will be omitted.
FIGS. 4A and 4B are views for explaining a flow velocity and a flow rate measuring method according to an embodiment of the present invention, and FIG. 5 is a view for explaining a method of measuring a flow velocity of a fluid in a pipe according to an embodiment of the present invention. to be.
First, a description will be given of an
4A and 4B, a first
At this time, the
Hereinafter, a method of measuring the flow rate and flow rate of the internal fluid of the pipe will be described in detail.
The flow rate measurement formula of the fluid is shown in the following formula (2).
&Quot; (2) "
Where Q is the flow rate, A is the area inside the pipe, and V is the flow rate.
The internal area of the pipe has the same relationship as A = pi r i 2, and can be calculated as follows.
Where r i is the radius of the pipe bore.
Therefore, it is possible to calculate r i by multiplying the inner diameter of the pipe calculated by the
Further, the thickness of the pipe calculated by the
Where r 0 is the radius of the pipe outer diameter, and ℓ is the pipe thickness.
4A and 4B, the
5, the ultrasonic velocity u d within the
&Quot; (3) "
Here, u 0 is the initial ultrasonic velocity before the speed changes by the flow velocity, and? Is the ultrasonic incident angle in the pipe.
(3) can be expressed by Equation (3) as the ultrasonic wave propagation time t d within the
&Quot; (4) "
Here, S is the distance, V is the velocity, l is the ultrasonic travel distance in the pipe, u 0 is the initial ultrasonic velocity before the velocity changes by the velocity, and θ is the ultrasonic wave incident angle in the pipe.
Equations (3) to (4) are summarized by the time difference occurring in t d and t u , and the relationship is as shown in Equation (5).
&Quot; (5) "
Here, u d is the ultrasonic velocity inside the pipe transmitted from the first ultrasonic transducer to the second ultrasonic transducer, u u is the velocity of the ultrasonic wave transmitted from the second ultrasonic transducer to the first ultrasonic transducer, L is a horizontal moving distance of the ultrasonic wave inside the pipe and t d is a distance in the pipe passing from the first ultrasonic transducer portion to the second ultrasonic transducer portion. And t u is the ultrasonic wave propagation time inside the pipe transferred from the second ultrasonic transducer portion to the first ultrasonic transducer portion.
Therefore, the flow velocity V of the inner fluid of the
5, the total ultrasonic traveling distance s t between the first and second
The total ultrasonic wave propagation time t t between the first and second
Hereinafter, a method of calculating the total ultrasonic traveling distance s t between the first and second
The travel distance s w in the wedge can directly measure the ultrasonic wave propagation distance based on the size of the wedge.
The moving distance s p of the pipe from the wall can be calculated using Snell's law, and the following formula (6) can be used.
&Quot; (6) "
Where p p is the pipe thickness, p is the ultrasound incident angle at the pipe wall, θ w is the ultrasound incident angle at the wedge, c P T is the sonic velocity at the pipe, c w L is the It is sound speed (sect).
The moving distance s f in the pipe can be calculated using Snell's law, and the following formula (7) can be used.
&Quot; (7) "
Here, L is the ultrasonic vertical movement distance (diameter) of the inner pipe, θ f is the ultrasonic wave incident angle of the inner pipe, θ p is the ultrasound angle of incidence of the pipe wall, c P T is the sound velocity (shear wave) in the pipe, c f L is the velocity of sound in the pipe.
Therefore, the ultrasonic traveling distance l in the pipe of the equation (5) can be calculated by the following equation (7).
Hereinafter, a method of measuring the total ultrasonic wave propagation time t t between the first and second
The propagation time t w in the wedge can be calculated by dividing the sound velocity in the wedge by the moving distance ( w w ) in the wedge, and has the relationship as shown in the following equation (8).
&Quot; (8) "
Where s w is the travel distance on the wedge and c w L is the sonic velocity on the wedge.
The propagation time t p at the pipe wall can be calculated by dividing the sound velocity at the pipe wall at the ultrasonic traveling distance (s p ) at the pipe wall, and has the relationship as shown in the following equation (9).
&Quot; (9) "
Where s p is the travel distance from the pipe wall, and c p T is the sound velocity (transverse wave) at the pipe wall.
The ultrasonic wave propagation time t f in the pipe has the relationship as shown in the following equation (10).
&Quot; (10) "
Here, t t is the total ultrasonic wave propagation time required to be transmitted from the first ultrasonic transducer unit to the second ultrasonic transducer unit or the entire ultrasonic wave propagation time required to be transmitted from the second ultrasonic transducer unit to the first ultrasonic transducer unit, t w is the propagation time at the wedge, and t p is the propagation time at the pipe wall.
The total ultrasonic wave propagation time t t required to be transmitted from the first
Therefore, t d and t u in the equation (5) can be calculated by the equation (10).
Illustratively, when it is desired to calculate the ultrasonic wave propagation time t d in the pipe transmitted from the first
[Equation 10 1 ]
Here, t t is the total ultrasonic propagation time required to be transferred from the first ultrasonic transducer to the second ultrasonic transducer, t w is the propagation time at the wedge, and t p is the propagation time at the pipe wall.
A second
[Equation 10 2 ]
Here, t t is the total ultrasonic wave propagation time required to be transmitted from the second ultrasonic transducer portion to the first ultrasonic transducer portion, t w is the propagation time at the wedge, and t p is the propagation time at the pipe wall.
6 is a view for explaining an ultrasonic transducer arranged in two or more in parallel according to an embodiment of the present invention.
The
The
The first electrode may be disposed above the plurality of ultrasonic transducers 135 and may be a (+) electrode.
The second electrode may be disposed under the plurality of ultrasonic transducers 135 and may be a negative electrode.
Here, the plurality of ultrasonic transducer units 135 are the same as those of the first
That is, the
Referring to FIG. 6, the
Accordingly, the
7 is a view for explaining a method of further coupling a wedge extension to a wedge shape according to an embodiment of the present invention.
Referring to FIG. 7, the first and
7A and 7B show side and front views of the
It will be understood by those skilled in the art that the foregoing description of the present invention is for illustrative purposes only and that those of ordinary skill in the art can readily understand that various changes and modifications may be made without departing from the spirit or essential characteristics of the present invention. will be. It is therefore to be understood that the above-described embodiments are illustrative in all aspects and not restrictive. For example, each component described as a single entity may be distributed and implemented, and components described as being distributed may also be implemented in a combined form.
The scope of the present invention is defined by the appended claims rather than the detailed description and all changes or modifications derived from the meaning and scope of the claims and their equivalents are to be construed as being included within the scope of the present invention do.
10: pipe 100: ultrasonic transducer
111: contact surface 112: upper surface
113 slope 115: wedge extension
110: first wedge 120: second wedge
130: ultrasonic transducer 131: first ultrasonic transducer
132: second ultrasonic transducer
140:
Claims (7)
An upper surface attached to the outer wall of the pipe and having a first length, a top surface formed parallel to the contact surface and having a second length longer than the first length, and an inclined surface formed to connect the top surface and the end of the contact surface, A first and a second wedge comprising:
A wedge extension formed adjacent to a point where said sloped surface starts from said upper surface and extending in a vertical direction from said upper surface to contact said pipe outer wall;
An ultrasonic transducer attached to a region of an upper surface of each wedge corresponding to the inclined surface and an upper surface of the wedge extension; And
Measuring a thickness and an inner diameter of the pipe based on a time difference between reflected waves reflected from the inner wall of the pipe and an ultrasonic signal output from the ultrasonic transducer attached to the first wedge; The flow rate and the flow rate of the fluid inside the pipe are measured based on the time required for the ultrasonic signal output from the attached ultrasonic transducer portion to be reflected from the inclined surface and transferred to the ultrasonic transducer portion attached to the second wedge or the first wedge And a controller,
The ultrasonic transducer unit
A plurality of ultrasonic transducers arranged in parallel at least two;
A first electrode disposed on an upper portion of the plurality of ultrasonic transducers; And
And a second electrode disposed below the plurality of ultrasonic transducers,
And a plurality of ultrasonic transducers are operated as one ultrasonic transducer unit at a time by giving signals to the first and second electrodes,
The ultrasonic wave output from the ultrasonic transducer attached to the upper surface of the wedge expansion portion passes through a region where the contact surface between the upper surface of the wedge expansion portion and the pipe overlaps,
Wherein the second wedge is disposed to be spaced apart from the first wedge by a predetermined distance in a direction in which the pipe extends,
Wherein an inclination angle between the inclined surface of each wedge and a surface extending in a direction perpendicular to the wedge expansion portion is set such that an ultrasonic wave output from an ultrasonic transducer attached to an upper surface of each wedge is reflected on the inclined surface, Wherein the ultrasonic transducer has an acute angle range.
Wherein an angle of inclination between the inclined surface of the first and second wedges and the upper surface of the wedge is smaller than an incident angle of the ultrasonic wave output from the ultrasonic transducer attached to the upper surface when the ultrasonic wave is reflected by the inclined surface, (1). ≪ EMI ID = 1.0 >
[Equation 1]
(Where &thetas; is an incident angle).
Wherein,
The ultrasonic signal output from the first ultrasonic transducer attached to the first wedge enters the upper surface and is vertically reflected toward the upper surface at the interface between the first wedge and the outer wall of the pipe, The ultrasonic signal output from the first ultrasonic transducer portion is incident on the upper surface and is transmitted through the interface between the first wedge and the outer wall of the pipe, Wherein the thickness of the pipe is calculated on the basis of a difference in a second time required to be vertically reflected from the interface between the first inner wall and the inner fluid toward the upper surface to be transmitted to the first ultrasonic transducer portion, Device.
Wherein,
Wherein an ultrasonic signal output from a first ultrasonic transducer attached to the first wedge is incident on the upper surface and is transmitted through an interface between the first wedge and an outer wall of the pipe, And a second time required for the ultrasonic wave to be transmitted to the first ultrasonic transducer unit and the ultrasonic signal outputted from the first ultrasonic transducer unit are incident on the upper surface, After passing through the interface between the first wedge and the outer wall of the pipe and the interface between the first inner wall and the inner fluid of the pipe and then reflected vertically toward the upper surface at the interface between the second inner wall and the inner fluid, Wherein the inner diameter of the pipe is calculated on the basis of a difference of a third time required to be transmitted to the first ultrasonic transducer unit. Value.
Wherein,
A time t required for transmitting the ultrasonic signal output from the first ultrasonic transducer attached to the first wedge to the second ultrasonic transducer attached to the second wedge, d and the ultrasonic signal output from the second ultrasonic transducer attached to the second wedge is transmitted to the first ultrasonic transducer attached to the first wedge during the fifth time Wherein the flow velocity of the fluid in the pipe is measured according to the following equation (2) as a relational expression of the difference between the time t u and the time t u .
&Quot; (2) "
(Where u d is the ultrasonic velocity in the pipe that is transmitted from the first ultrasonic transducer unit to the second ultrasonic transducer unit and u u is the velocity of ultrasonic waves transmitted from the second ultrasonic transducer unit to the first ultrasonic transducer unit, L is the horizontal travel distance of the ultrasonic wave inside the pipe, t d is the distance between the first ultrasonic transducer and the second ultrasonic transducer, And t u is the ultrasonic wave propagation time inside the pipe which is transmitted from the second ultrasonic transducer portion to the first ultrasonic transducer portion)
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Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN113167618A (en) * | 2018-12-13 | 2021-07-23 | 恩德斯+豪斯流量技术股份有限公司 | Ultrasonic transducer device for a clamped ultrasonic flow measuring point, clamped ultrasonic flow measuring point and method for putting a clamped ultrasonic flow measuring point into operation |
US20220113175A1 (en) * | 2019-01-30 | 2022-04-14 | Labtrino Ab | Coupling Member for Clamp on Flow Metering |
Citations (4)
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JPH05209766A (en) * | 1991-12-10 | 1993-08-20 | Tokimec Inc | Ultrasonic transmitter-receiver |
KR101022407B1 (en) * | 2009-04-20 | 2011-03-15 | (주)씨엠엔텍 | Non-intrusive ultrasonic flowmeter |
KR101302645B1 (en) * | 2012-02-29 | 2013-09-03 | 한국표준과학연구원 | Multi path ultrasonic flowmeter |
KR101513697B1 (en) * | 2014-06-10 | 2015-04-22 | 숭실대학교산학협력단 | Ultrasonic transducing apparatus for measuring pipe thickness and apparatus for measuring flow velocity using the same |
-
2015
- 2015-07-22 KR KR1020150103675A patent/KR101693726B1/en active IP Right Grant
Patent Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
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JPH05209766A (en) * | 1991-12-10 | 1993-08-20 | Tokimec Inc | Ultrasonic transmitter-receiver |
KR101022407B1 (en) * | 2009-04-20 | 2011-03-15 | (주)씨엠엔텍 | Non-intrusive ultrasonic flowmeter |
KR101302645B1 (en) * | 2012-02-29 | 2013-09-03 | 한국표준과학연구원 | Multi path ultrasonic flowmeter |
KR101513697B1 (en) * | 2014-06-10 | 2015-04-22 | 숭실대학교산학협력단 | Ultrasonic transducing apparatus for measuring pipe thickness and apparatus for measuring flow velocity using the same |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN113167618A (en) * | 2018-12-13 | 2021-07-23 | 恩德斯+豪斯流量技术股份有限公司 | Ultrasonic transducer device for a clamped ultrasonic flow measuring point, clamped ultrasonic flow measuring point and method for putting a clamped ultrasonic flow measuring point into operation |
US20220113175A1 (en) * | 2019-01-30 | 2022-04-14 | Labtrino Ab | Coupling Member for Clamp on Flow Metering |
US11982559B2 (en) * | 2019-01-30 | 2024-05-14 | Labtrino Ab | Coupling member for clamp on flow metering |
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