JPS61132824A - Ultrasonic flowmeter - Google Patents
Ultrasonic flowmeterInfo
- Publication number
- JPS61132824A JPS61132824A JP59255445A JP25544584A JPS61132824A JP S61132824 A JPS61132824 A JP S61132824A JP 59255445 A JP59255445 A JP 59255445A JP 25544584 A JP25544584 A JP 25544584A JP S61132824 A JPS61132824 A JP S61132824A
- Authority
- JP
- Japan
- Prior art keywords
- waves
- wall surface
- piping
- pipe
- ultrasonic
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Pending
Links
Classifications
-
- 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
- G01F1/662—Constructional details
Landscapes
- Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Fluid Mechanics (AREA)
- General Physics & Mathematics (AREA)
- Measuring Volume Flow (AREA)
Abstract
Description
【発明の詳細な説明】
〔発明の属する技術分野〕
本発明は、配管外壁から流体中へ超音波を発射させて配
管外1面で受信し、その伝搬時間が流体の流速あるいは
流量に比例することを原理とする超音波流量計に関する
。より詳しくは、配管外壁面より流体中へ斜めに超音波
を発射して、配管内壁面で流体中へ反射させた超音波を
配管外壁面で受信する形式の主に小口径用又は中口径用
とじて一般的な超音波流量計に関する。[Detailed Description of the Invention] [Technical Field to Which the Invention Pertains] The present invention emits ultrasonic waves from the outer wall of a pipe into a fluid and receives them on one surface outside the pipe, and the propagation time is proportional to the flow rate or flow rate of the fluid. This article relates to an ultrasonic flowmeter based on the principle of More specifically, it is mainly for small or medium diameters, in which ultrasonic waves are emitted diagonally into the fluid from the outer wall of the pipe, reflected into the fluid by the inner wall of the pipe, and then received at the outer wall of the pipe. Regarding general ultrasonic flowmeters.
従来のこの種の超音波流量計は、第5図ないし第7図の
ような構成となっている。すなわち、流体中に超音波を
発射し、配管内壁面で反射した超音波を受信する超音波
送受波器(以下略して送受波器と称す)2a、2bを、
流体を導く配管1の外壁に互いに位置をずらして音響力
、ブリング材4を介して配置している。送受波器2a、
2bは、図に示すように、超音波透過材として一般的に
用いラレるエポキシ系樹脂等のプロ、り(以下略シテ透
過材プロ、りと称す)5に、PZTのような圧電素子で
ある超音波振動子6を接着した構造となっている。A conventional ultrasonic flowmeter of this type has a configuration as shown in FIGS. 5 to 7. That is, ultrasonic transducers (hereinafter simply referred to as transducers) 2a and 2b that emit ultrasonic waves into the fluid and receive the ultrasonic waves reflected on the inner wall surface of the pipe,
They are placed on the outer wall of the pipe 1 that guides the fluid, with acoustic force and a bringing material 4 interposed therebetween, with their positions shifted from each other. Transducer/receiver 2a,
As shown in the figure, 2b is made of a material such as epoxy resin that is generally used as an ultrasonic transmitting material (hereinafter simply referred to as "shite transparent material professional") 5, and a piezoelectric element such as PZT. It has a structure in which a certain ultrasonic transducer 6 is bonded.
このような構成により、送受波器2aかも発射した超音
波が送受波器2bに到達するまでの時間と、送受波器2
bから発射した超音波が送受波器2aに到達する時間と
の差に基づいて配管1円を流れる流体の流速あるいは流
量を求める。したがって、測定原理上、送受波器から流
体中を伝磁し配管P131Ni面で反射して、再び流体
中を伝搬して他方の送受波器に裏って受信される超音波
(以下略して直接受波と称す)の伝搬時間が、この超音
波流量計本来の計測信号であり、流体の流速あるいは流
量に比例する。With this configuration, the time it takes for the ultrasonic waves emitted by the transducer 2a to reach the transducer 2b and the time taken by the transducer 2
The flow velocity or flow rate of the fluid flowing through one circle of piping is determined based on the difference in time between the ultrasonic wave emitted from b and the time it takes to reach the transducer 2a. Therefore, based on the measurement principle, ultrasonic waves (abbreviated as direct) are transmitted from a transducer through the fluid, reflected on the P131Ni surface of the pipe, propagated through the fluid again, and are received by the other transducer. The propagation time of the received wave (referred to as a received wave) is the original measurement signal of this ultrasonic flowmeter, and is proportional to the flow velocity or flow rate of the fluid.
しかし、このような構成の従来形超音波流量計において
は、後述のように、直接受波のエネルギーは配管内壁面
での反射及び透過、及び干渉により弱められ、また、こ
の直接受波に配管内外壁に沿って、あるいは配管内f!
!#部で多電反射しながら伝搬するNt波(以下略して
回り込み波と称す)がノイズとしてX畳している。この
ため、送受波器2a、2bの受信波のS/Nが低下する
ので、流体の流速あるいは流量に比例する直接受波の伝
搬時間の計測精度が低下する。その結果、核超音彼流量
訂の測定精度が低下するという問題がある。However, in conventional ultrasonic flowmeters with such a configuration, as described later, the energy of directly received waves is weakened by reflection and transmission on the inner wall surface of the piping, and interference, and the energy of the directly received waves is weakened by Along internal and external walls or inside piping f!
! The Nt wave (hereinafter simply referred to as a wrap-around wave) propagating while undergoing multiple electrical reflections in the # section forms an X fold as noise. For this reason, the S/N ratio of the waves received by the transducers 2a and 2b decreases, and the measurement accuracy of the propagation time of the directly received waves, which is proportional to the flow velocity or flow rate of the fluid, decreases. As a result, there is a problem in that the measurement accuracy of nuclear ultrasonic flow correction is reduced.
本発明は、送受波器の受信波のS/Nを高め、上述の間
旭点を解決し、測定精度を向上させた超音波振動子を提
供することを目的とする。SUMMARY OF THE INVENTION An object of the present invention is to provide an ultrasonic transducer that improves the S/N ratio of waves received by a transducer, solves the above-mentioned problem, and improves measurement accuracy.
この目的は本発明によれば、直接受波の配管内壁面での
流体への反射面に対応する配管外壁面に、適当な材質と
厚さの薄板を密着させることにより、直接受波を太き(
し、送受波器の受111′波の△を高めることにより達
成される。According to the present invention, this purpose is achieved by attaching a thin plate of appropriate material and thickness to the outer wall surface of the pipe corresponding to the reflection surface of the fluid on the inner wall surface of the pipe for directly receiving waves. tree(
However, this is achieved by increasing the Δ of the received 111' wave of the transducer.
81図および第2図に本発明の実施例を示′す。 An embodiment of the present invention is shown in FIG. 81 and FIG.
図に示すように本発明の構成は、配管内壁での直接受波
の反射面に対応した配管外礒面に適当な材質と厚さの金
属薄板7を密着させたものである。As shown in the figure, the configuration of the present invention is such that a thin metal plate 7 of an appropriate material and thickness is closely attached to the outer surface of the pipe corresponding to the reflection surface of the directly received wave on the inner wall of the pipe.
このことによりTi[接受波の音圧レベルを高め、顎を
高くすることによって上述の目的を達成することができ
る。As a result, the above-mentioned purpose can be achieved by increasing the sound pressure level of the Ti [receiving wave] and heightening the chin.
第3図および第4図は本発明の原理を示し、これらの図
に基づいて本発明の詳細な説明する。図において、配°
管1の外壁面から超音波振動子6aにより流体中へ発射
した超音波は、配管1の内壁−115と外壁面16で反
射され、流体3を伝搬して配管1の肉厚部を透過して超
音波振動子6bで受信される。この場合、流体中を伝搬
してきた超音波iは配管1の内1! [i 15と外壁
面16で反射、透過して超音amenとなり、流体中を
伝搬して内壁面15で反射する超音vj、にと干渉する
。3 and 4 illustrate the principle of the present invention, and the present invention will be explained in detail based on these figures. In the figure,
Ultrasonic waves emitted from the outer wall of the pipe 1 into the fluid by the ultrasonic transducer 6a are reflected by the inner wall 115 and the outer wall 16 of the pipe 1, propagate through the fluid 3, and pass through the thick part of the pipe 1. and is received by the ultrasonic transducer 6b. In this case, the ultrasonic wave i that has propagated through the fluid is one of the pipes 1! [i 15 and is reflected and transmitted by the outer wall surface 16 to become an ultrasonic wave amen, which interferes with the ultrasonic wave vj that propagates through the fluid and is reflected by the inner wall surface 15.
したがって、超音波m 、 nと内壁面15での反射超
音波j、にとの位相が合えば互いの音波が強め合うこと
になるので、内壁面15での反射音圧レベルが増し、ま
た、超音波m 、 nと内壁面15での反射超音波j、
にとの位相が逆になれば互いの音波が打ち消し合うこと
になるので、内壁面15での反射音圧は小さくなる。Therefore, if the phases of the ultrasonic waves m, n and the ultrasonic waves j, reflected on the inner wall surface 15 match, the sound waves will strengthen each other, so the reflected sound pressure level on the inner wall surface 15 will increase, and Ultrasonic waves m, n and reflected ultrasonic waves j at the inner wall surface 15,
If the phases of the two waves are reversed, the sound waves cancel each other out, so the reflected sound pressure on the inner wall surface 15 becomes smaller.
本発明は、前記のような音波の干渉を利用して、直接受
波の音圧レベルを高めたものである。すなわち、超音波
m 、 nと内壁面15での反射超音波j。The present invention utilizes the interference of sound waves as described above to increase the sound pressure level of directly received waves. That is, ultrasonic waves m, n and reflected ultrasonic waves j at the inner wall surface 15.
kとの位相が合うように、配管内壁での直接受波の反射
面に対応した外壁面16に適度な厚さの金属薄機を密着
させて、内壁面15での反射音圧レベルを高めて受信波
の音圧レベルを高(したことである。この場合、金属薄
板は配管と同系読の材質を選ぶことが好ましい。In order to match the phase with k, a thin metal plate of an appropriate thickness is brought into close contact with the outer wall surface 16 corresponding to the reflection surface of the direct reception wave on the inner wall of the pipe, thereby increasing the reflected sound pressure level on the inner wall surface 15. This is to increase the sound pressure level of the received wave. In this case, it is preferable to select a material for the thin metal plate that has the same type of reading as the piping.
第4図は、材質SGP、口径IB、厚さ3.2 % (
7)配管に、エポキシ樹脂製の透過材プロ、りを介して
42度の角度で超音波を打ち込み、前記配管外壁面16
ニステンレス製の金属薄板を密着させた場合の薄板厚さ
と受信波の音圧レベル(相対値)との関係の実験確認結
果、および薄板厚さと内壁面15での音圧反射高(相対
値)との関係の計算結果の一例について示した。図に示
すように、受信波の音圧レベル12(相対値)と内壁面
15での音圧反射車13(計算結果で相対値)とは、特
性が同一で、金属薄板厚さに対し周期特性を持ち、受信
波の音圧レベルを高くする薄板厚さが存在する。この受
信波の音圧レベルを高くする金属薄板の厚さを選定して
、この金属薄板を直接受波の配管内壁での反射面に対応
した配管外壁面に密着させれば、受信波の音圧レベルを
高めることができる。Figure 4 shows the material SGP, diameter IB, and thickness 3.2% (
7) Ultrasonic waves are applied to the pipe at an angle of 42 degrees through a transparent material made of epoxy resin, and the outer wall surface 16 of the pipe is
Experimental confirmation results of the relationship between the thin plate thickness and the sound pressure level (relative value) of the received wave when thin metal plates made of stainless steel are brought into close contact with each other, and the thickness of the thin plate and the sound pressure reflection height (relative value) at the inner wall surface 15. An example of the calculation result of the relationship between As shown in the figure, the sound pressure level 12 (relative value) of the received wave and the sound pressure reflection wheel 13 (relative value in the calculation result) on the inner wall surface 15 have the same characteristics and have a periodicity relative to the thickness of the metal thin plate. There is a thin plate thickness that has characteristics and increases the sound pressure level of the received wave. If the thickness of the thin metal plate is selected to increase the sound pressure level of the received wave, and this thin metal plate is brought into close contact with the outer wall surface of the pipe corresponding to the reflection surface on the inner wall of the pipe for direct reception, the sound pressure level of the received wave will be increased. Pressure levels can be increased.
以上の説明から明らかなよ、うに、本発明によれば、配
管内壁面での直接受波の反射面に対応した配管外壁面に
、適当な材質と厚さの金属薄板を密着させるだけで受信
波の音圧レベルを高めることができ、その結果、受信波
の味が高くなり、測定精度を向上させることができる。As is clear from the above description, according to the present invention, reception can be received simply by closely adhering a thin metal plate of an appropriate material and thickness to the outer wall surface of the pipe corresponding to the reflection surface of the direct received wave on the inner wall surface of the pipe. The sound pressure level of the waves can be increased, and as a result, the received waves have a higher quality, and the measurement accuracy can be improved.
第1図、第2図はそれぞれ本発明の実施例による超音波
流量計を配管とともに示す側面図および径方向断面図、
第3図は配管における超音波の伝搬形態を模式的に示す
概略図、第4図は本発明を説明するためのグラフ、第5
図、第6図はそれぞれ従来の超音波流量計を配管ととも
に示す側面図および径方向断面図、第7図は送受波器の
構成を示す断面図である。
1:配管、2.2m、2b :送受波器、3:流体、4
:音響力、プリング材、9:金属薄板、15:配管内壁
面、16:配管外壁面。FIG. 1 and FIG. 2 are a side view and a radial cross-sectional view showing an ultrasonic flowmeter according to an embodiment of the present invention together with piping, respectively;
FIG. 3 is a schematic diagram schematically showing the propagation mode of ultrasonic waves in piping, FIG. 4 is a graph for explaining the present invention, and FIG.
6 are a side view and a radial cross-sectional view showing a conventional ultrasonic flowmeter together with piping, respectively, and FIG. 7 is a cross-sectional view showing the configuration of a transducer. 1: Piping, 2.2m, 2b: Transducer, 3: Fluid, 4
: Acoustic force, pulling material, 9: Metal thin plate, 15: Piping inner wall surface, 16: Piping outer wall surface.
Claims (1)
受信部とを配置し、配管外壁面から超音波を流体中に発
射し配管内壁面で流体中へ反射させた超音波を配管外壁
面で受信するようにした超音波流量計において、前記流
体中へ発射させた超音波が反射する配管内壁面に対応す
る配管外壁面に金属薄板を密着して取付けたことを特徴
とする超音波流量計。An ultrasonic transmitting part and a receiving part are arranged at different positions on the outer wall of the pipe, and the ultrasonic waves are emitted from the outer wall of the pipe into the fluid and reflected into the fluid by the inner wall of the pipe. An ultrasonic flowmeter configured to receive ultrasonic waves on a wall surface, characterized in that a thin metal plate is attached in close contact with the outer wall surface of the pipe corresponding to the inner wall surface of the pipe where the ultrasonic waves emitted into the fluid are reflected. Flowmeter.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP59255445A JPS61132824A (en) | 1984-12-03 | 1984-12-03 | Ultrasonic flowmeter |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP59255445A JPS61132824A (en) | 1984-12-03 | 1984-12-03 | Ultrasonic flowmeter |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS61132824A true JPS61132824A (en) | 1986-06-20 |
Family
ID=17278865
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP59255445A Pending JPS61132824A (en) | 1984-12-03 | 1984-12-03 | Ultrasonic flowmeter |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS61132824A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2005214820A (en) * | 2004-01-30 | 2005-08-11 | Fuji Electric Systems Co Ltd | Ultrasonic transceiving unit for doppler type ultrasonic flow velocity distribution meter |
-
1984
- 1984-12-03 JP JP59255445A patent/JPS61132824A/en active Pending
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2005214820A (en) * | 2004-01-30 | 2005-08-11 | Fuji Electric Systems Co Ltd | Ultrasonic transceiving unit for doppler type ultrasonic flow velocity distribution meter |
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