JPS58154617A - Vortex flow meter - Google Patents

Vortex flow meter

Info

Publication number
JPS58154617A
JPS58154617A JP57036490A JP3649082A JPS58154617A JP S58154617 A JPS58154617 A JP S58154617A JP 57036490 A JP57036490 A JP 57036490A JP 3649082 A JP3649082 A JP 3649082A JP S58154617 A JPS58154617 A JP S58154617A
Authority
JP
Japan
Prior art keywords
force
vibration
bending moment
fixed
receiving body
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
Application number
JP57036490A
Other languages
Japanese (ja)
Inventor
Takehiro Sawayama
沢山 武弘
Toshio Aga
阿賀 敏夫
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Yokogawa Electric Corp
Original Assignee
Yokogawa Electric Corp
Yokogawa Hokushin Electric Corp
Yokogawa Electric Works Ltd
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Yokogawa Electric Corp, Yokogawa Hokushin Electric Corp, Yokogawa Electric Works Ltd filed Critical Yokogawa Electric Corp
Priority to JP57036490A priority Critical patent/JPS58154617A/en
Publication of JPS58154617A publication Critical patent/JPS58154617A/en
Pending legal-status Critical Current

Links

Classifications

    • 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
    • G01F1/20Measuring 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 detection of dynamic effects of the flow
    • G01F1/32Measuring 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 detection of dynamic effects of the flow using swirl flowmeters
    • G01F1/325Means for detecting quantities used as proxy variables for swirl
    • G01F1/3259Means for detecting quantities used as proxy variables for swirl for detecting fluid pressure oscillations
    • G01F1/3266Means for detecting quantities used as proxy variables for swirl for detecting fluid pressure oscillations by sensing mechanical vibrations

Landscapes

  • Physics & Mathematics (AREA)
  • Fluid Mechanics (AREA)
  • General Physics & Mathematics (AREA)

Abstract

PURPOSE:To improve vibration resisting performance and to produce a vortex flow meter with improved SN, by fixing a detecting sensor on a position where noise due to disturbance is about zero. CONSTITUTION:A force receiving body 2a has a free end at its insersion point and is fixed on a conduit 1 at its intermediate part. A fixing body 5 is inserted into a recessed part 21 with a gap 51 to press and fix a stress detecting part 3 to/on the required position of the recessed part 21. Bending moment M, force F and tare weight W act on the lower part of the fixing body 5 by the disturbance vibration, bending moments M21-M23 based upon said loads are generated and M2 is generated as a composite bending moment. If the stress detecting part 3 is arranged on a position A or B where vibration bending moment M2 O is formed, noises due to disturbance vibration can be reduced.

Description

【発明の詳細な説明】 本発明は、カルマン渦を利用して流体の流速1九は流量
を測定する渦流量計K11lするものであゐ。
DETAILED DESCRIPTION OF THE INVENTION The present invention is a vortex flowmeter K11l that measures the flow rate of fluid by utilizing Karman vortices.

流体中に物体を置くと、物体の両後備面から交互Kかつ
規則的に渦が発生し、下流に満月となって流れることが
古くから知られている。こO渦列はカルマン渦列といわ
れ、単位時間amりの渦の生成数(渦周波数)が流体の
流速に比例している。
It has been known for a long time that when an object is placed in a fluid, vortices are generated regularly and alternately from both rear surfaces of the object, and flow downstream in the form of a full moon. This O vortex street is called a Karman vortex street, and the number of vortices generated per unit time am (vortex frequency) is proportional to the flow velocity of the fluid.

そこで、測定流体を導く管路内に渦発生体を配置し、渦
の生成による揚力変化を渦発生体(tたは受力体)K設
けた圧電素子、ストレンゲージ、容量やインダクタンス
等のセンナで検出した後信号変換して流体の流速や流量
を測定する渦流量計が実用化されている。ところでこの
種の渦流量計においては、ポンプなどにより励起される
配管振動等の外tm動による影響を受ff、4tK低流
速時。
Therefore, a vortex generator is placed in the pipe that guides the fluid to be measured, and a piezoelectric element, a strain gauge, a capacitance, an inductance, etc. equipped with a vortex generator (t or force receiving body) absorbs the lift change caused by the generation of the vortex. Vortex flowmeters have been put into practical use that measure the flow velocity and flow rate of fluids by detecting and converting signals. By the way, this type of vortex flowmeter is affected by external tm movements such as piping vibrations excited by pumps etc. at low flow rates of ff and 4tK.

I比が悪化するという欠点があった。There was a drawback that the I ratio deteriorated.

食品用等に使用される場合に、衛生上O観点から管路0
底聞儒の渦発生体端爾を自由端としなければならないが
、この場合に、4IK上記欠点の除去がむずかしい。以
下、図によって1!明するO第1図は、便乗よシ一般に
使用されている従来例の構成説明図である。
When used for food, etc., the pipe line is 0 from a sanitary O point of view.
The end of the vortex generator of the base must be made a free end, but in this case, it is difficult to eliminate the above-mentioned drawbacks of 4IK. Below, according to the diagram 1! FIG. 1 is a diagram illustrating the configuration of a conventional example that is commonly used.

図において、1は測定流体の流れる円筒状の管路、2は
管路1に挿入された柱状の受力体で、ステンレス材より
なり一端は管路IKl[l定され、他端は自由端状態と
なっている。21は受力体1に設けられた凹部であるa
sh凹郁凹部に設けられ九円板状の応力検出部で、その
中心軸は受力体2の中心軸上にある。応力検出部5はこ
の場合は第2図に示す如く円板状の素子本体31と電極
32.33.34よりなる。電極32は薄円板状をなし
、素子本体31の一面側に設けられている〇一方、電極
33.34はほぼ弓形をなし、素子本体31の他面側に
素子本体31の中心を挾んで、測定流体の流れに直角方
向に対称形に設けられている。素子本体31はこの場合
は圧電素子が使用されている。4は絶縁材よりな転、応
力検出部Sを凹部21内に凹部21よシ絶縁して封着す
石對着体で、この場合は、ガラス材が用いられている。
In the figure, 1 is a cylindrical pipe through which the fluid to be measured flows, and 2 is a columnar force receiving body inserted into the pipe 1. It is made of stainless steel, and one end is fixed to the pipe IKl [l], and the other end is a free end. It is in a state. 21 is a recess provided in the force receiving body 1;
This is a nine-disk-shaped stress detecting section provided in the shallow recess, and its center axis is on the center axis of the force receiving body 2. In this case, the stress detection section 5 consists of a disk-shaped element body 31 and electrodes 32, 33, and 34, as shown in FIG. The electrode 32 has a thin disk shape and is provided on one side of the element body 31. On the other hand, the electrodes 33 and 34 are approximately arcuate and have the center of the element body 31 sandwiched between them on the other side of the element body 31. They are arranged symmetrically in a direction perpendicular to the flow of the measuring fluid. In this case, a piezoelectric element is used as the element body 31. Reference numeral 4 denotes a stone-bonded body which is not made of an insulating material, but which seals the stress detection part S in the recess 21 insulatingly from the recess 21. In this case, a glass material is used.

以上の構−成において、管路1内に測定流体が流れると
14ユ力体21にはカルマン渦によセ第1図に示す矢印
Xのような交番力が作用する。(以下、この方向を「揚
力方向」と称する0)この交番力は、封着体4を介して
応力検出s5に伝達される。
In the above configuration, when the fluid to be measured flows into the pipe 1, an alternating force as indicated by the arrow X shown in FIG. 1 acts on the 14-force body 21 due to the Karman vortex. (Hereinafter, this direction will be referred to as the "lift direction") This alternating force is transmitted to the stress detection s5 via the sealing body 4.

この場合、受力体2には第1図に示す如く、受力体2の
中心軸をはさんで逆方向の応力変化が発生する。而して
、応力検出部5の電極32−電極33゜電極32−電極
34関にはこの応力変化に対応した電気信号(たとえば
電荷の変化)が生ずる。この変化の回数を検出するとと
Kよp渦発生周波数が検出で龜る。而して、電極32−
電極33.電極32−電極34間の電気出力を差動的に
処理すれば、2倍の電気出力を得ることができる〇 一方、管路を伝播してくる振動ノイズ、たとえばポンプ
、コンプレ、サー、ポンプ;−の開閉等による振動ノイ
ズの影響により管路全体が振れる。
In this case, as shown in FIG. 1, stress changes occur in the force-receiving body 2 in opposite directions across the central axis of the force-receiving body 2. An electric signal (for example, a change in electric charge) corresponding to this stress change is generated between the electrodes 32 and 33 and the electrodes 32 and 34 of the stress detection section 5. If the number of times of this change is detected, the detection frequency of K and P vortices will be delayed. Therefore, the electrode 32-
Electrode 33. If the electrical output between the electrodes 32 and 34 is processed differentially, twice the electrical output can be obtained.On the other hand, vibration noise propagating through the pipes, such as pumps, compressors, The entire pipeline vibrates due to vibration noise caused by the opening and closing of the -.

この振動によって受力体2に1前述交番力Xが作用する
方向に受力体2の質量分布に基ずく交書の曲げモーメン
ト〜が作用するOこO交番の―げ毫−メント〜により受
力体2に生ずる応力は応力検出部5においてノイズとし
て検出される。
Due to this vibration, an alternating bending moment based on the mass distribution of the force receiving body 2 acts on the force receiving body 2 in the direction in which the aforementioned alternating force X acts. The stress generated in the force body 2 is detected as noise by the stress detection section 5.

第S図はこの曲げモーメント〜を示したも、ので、M8
社貴見生によって生じた交番O蘭は毫−メントである0 この場合、渦発生によって生じた交書O―げ毫−メント
M8と振動ノイズモーメント〜とはその作用形態がほぼ
同様であるので、輩、〉〜の条件下でしか使用できない
。したがって、耐振性能を重視( すると、測定可能流速の下限が汎用される領域に達する
ことができない。一方、測定下限を重視すると、耐振性
能が汎用される領域に達しない。、本発明は、この問題
点を解決するものである。
Figure S shows this bending moment ~, so M8
The police box O-ran caused by the company employee is a moment 0 In this case, the mode of action of the police box O-game M8 caused by the vortex generation and the vibration noise moment is almost the same. It can only be used under the following conditions. Therefore, if emphasis is placed on vibration resistance performance, the lower limit of measurable flow velocity will not reach the range where it is commonly used.On the other hand, if emphasis is placed on the lower limit of measurement, vibration resistance performance will not reach the range where it is commonly used. It is a solution to a problem.

本発明の目的は、耐振性能が向上し、8/N比の良好な
渦流量針を提供するにある〇 第4図は、本発明の一実施例の構成説明図である。
An object of the present invention is to provide a vortex flow needle with improved vibration resistance and a good 8/N ratio. FIG. 4 is an explanatory diagram of the configuration of an embodiment of the present invention.

図にシいて、第1図と同一記号は同一機能を示す。以下
、第1図と相違部分のみ説明する。
In the figure, the same symbols as in FIG. 1 indicate the same functions. Hereinafter, only the differences from FIG. 1 will be explained.

2aは、管路1に挿入された柱状の受力体で、ステンレ
スよしなる。受力体2mの挿入先端は自由端状態にあり
、その途中が管路1に固定されている。
2a is a columnar force receiving body inserted into the conduit 1, and is made of stainless steel. The insertion tip of the force receiving body 2m is in a free end state, and the middle part thereof is fixed to the conduit 1.

Sは凹部21に隙間51をもって挿入され、応力検出部
5を、凹部21の所要位置(後述する)K抑圧固定する
固定体である。固定体5は凹部21の開口端で固定され
、この場合は、溶接固定52されている。
S is a fixed body that is inserted into the recess 21 with a gap 51 and fixes the stress detection section 5 in a predetermined position (described later) K in the recess 21 while suppressing it. The fixed body 5 is fixed at the open end of the recess 21, and in this case, it is fixed by welding 52.

以上の構成において、受力体2K、渦発生に基づ〈文書
力が作用すると、受力体2は、ある瞬間においては、第
5図に示す如く変位する。、図中矢印Xは作用する力を
表わす。而して、固定体5に着目すると、第6図に示す
如く、固定体5の下端には、曲げモーメン)Mと、受力
体20造中が固定されていることに基づく力Fが作用し
、それぞれに基づく曲げモーメン)M工19M□2が生
ずイ。
In the above configuration, when a document force acts on the force receiving body 2K based on the generation of a vortex, the force receiving body 2 is displaced at a certain moment as shown in FIG. , the arrow X in the figure represents the acting force. Focusing on the fixed body 5, as shown in FIG. 6, a bending moment M and a force F due to the fact that the force receiving body 20 is fixed are applied to the lower end of the fixed body 5. However, bending moment based on each) M engineering 19M□2 is generated.

これらの合成曲げモーメントとして町が発生する。A town is generated as a resultant bending moment of these.

一方、管路振動等によっては、受力体2は、全体として
振動し、そのある瞬間の変位は、第7図に示す如くなる
。前述と同様に1固定体![着目すると、第8図に示す
如く、外乱振動に基づき、固定体50下端には、曲げモ
ーメントM、力Fと自重Wが作用し、それぞれに基づく
曲げモーメントM2□t M2□9M23  が生ずる
。これらの合成曲げモーメントとしてM2が発生する。
On the other hand, due to pipe vibration etc., the force receiving body 2 vibrates as a whole, and its displacement at a certain moment becomes as shown in FIG. 1 fixed body as mentioned above! [If we pay attention to this, as shown in FIG. 8, a bending moment M, a force F, and its own weight W act on the lower end of the fixed body 50 based on the disturbance vibration, and a bending moment M2□t M2□9M23 is generated based on each of them. M2 is generated as a resultant bending moment.

第6図の振動曲げモーメン) M24零の位置即ち、図
示のム又はBK応力検出部5を配電すれば、外乱振動ノ
イズを小さくすることができる。
(Vibration Bending Moment in FIG. 6) By distributing power to the M24 zero position, that is, the illustrated M or BK stress detection unit 5, the disturbance vibration noise can be reduced.

この結果、外乱振動に対するBIN比が改善できる0 なお、前述の!!l!施例においては、検出センサとし
て、圧電素子よりなる応力検出部5を使用した−のKつ
いて説明し九が、これに限ることはなく、たとえば、ス
トレンゲージでもよく、要するに、渦発生により受力体
21Lに作用する交番力を検出できるものであればよい
As a result, the BIN ratio against disturbance vibration can be improved. ! l! In the embodiment, a stress detection section 5 made of a piezoelectric element is used as a detection sensor. However, the present invention is not limited to this, and a strain gauge may be used, for example. Any device that can detect the alternating force acting on the body 21L may be used.

また、前述の実施例において、受力体2aは渦発生体を
も兼ね九ものについて説明したが、渦発生体を受力体2
鼠と別体に作や、受力体2aの上流側に渦発生体番配置
したものであってもよいことは勿論である。
In addition, in the above-mentioned embodiment, nine examples have been described in which the force receiving body 2a also serves as a vortex generating body, but the vortex generating body is
It goes without saying that the vortex generating body may be made separately from the body or the vortex generating body may be placed upstream of the force receiving body 2a.

以上説明したように、本発#4によれば、耐振性能が向
上され、87N比の良好な渦流量針を実現することがで
きる。
As explained above, according to the present invention #4, it is possible to realize a vortex flow needle with improved vibration resistance and a good 87N ratio.

【図面の簡単な説明】[Brief explanation of drawings]

第1図は従来より一般に使用されている従来例実施例の
構成説明図、第5図〜第8図は第4図の動作説明図であ
る。 1・・・管路、2a・・・受力体、21・・・凹部、5
・・・応力検出部、5・・・固定体、51・・・隙間、
52・・・固定。 代理人   弁理士  小 沢 信 靭第1  [ll
              夢 3 口′440  
    第5図    捧6圓!J 7 図    2
43 図
FIG. 1 is an explanatory diagram of the configuration of a conventional example embodiment that has been generally used in the past, and FIGS. 5 to 8 are explanatory diagrams of the operation of FIG. 4. DESCRIPTION OF SYMBOLS 1... Pipeline, 2a... Force receiving body, 21... Recessed part, 5
... Stress detection part, 5 ... Fixed body, 51 ... Gap,
52...Fixed. Agent: Patent Attorney Nobuo Kozawa No. 1 [ll
Dream 3 Mouth'440
Figure 5: 6 yen! J7 Figure 2
43 Figure

Claims (1)

【特許請求の範囲】[Claims] 測定流体の流れる管路と、咳管路に一端が自由端状態に
挿入され途中が該管路に取付けられた柱状の受力体と、
骸受力体の他端側に設けられた凹部と、該凹部に配置さ
れた検出センナと、前記凹部に隙間をもって挿入されそ
の一端が前記凹部の開口端部で固定され前記センナを外
乱力に基づくノイズがほぼ零となる位置に固定する固定
体とを具備してなる渦流量計〇
a pipe line through which a measurement fluid flows; a columnar force-receiving body having one end inserted into the cough pipe line in a free end state and a part thereof attached to the pipe line;
A recess provided on the other end side of the body force receiving body, a detection senna disposed in the recess, and a detection senna inserted into the recess with a gap, one end of which is fixed at the open end of the recess, and the senna is subjected to disturbance force. A vortex flowmeter that is equipped with a fixed body that is fixed at a position where the based noise is almost zero.
JP57036490A 1982-03-10 1982-03-10 Vortex flow meter Pending JPS58154617A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP57036490A JPS58154617A (en) 1982-03-10 1982-03-10 Vortex flow meter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP57036490A JPS58154617A (en) 1982-03-10 1982-03-10 Vortex flow meter

Publications (1)

Publication Number Publication Date
JPS58154617A true JPS58154617A (en) 1983-09-14

Family

ID=12471259

Family Applications (1)

Application Number Title Priority Date Filing Date
JP57036490A Pending JPS58154617A (en) 1982-03-10 1982-03-10 Vortex flow meter

Country Status (1)

Country Link
JP (1) JPS58154617A (en)

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