JPS5827017A - Vortex flowmeter - Google Patents

Vortex flowmeter

Info

Publication number
JPS5827017A
JPS5827017A JP56126972A JP12697281A JPS5827017A JP S5827017 A JPS5827017 A JP S5827017A JP 56126972 A JP56126972 A JP 56126972A JP 12697281 A JP12697281 A JP 12697281A JP S5827017 A JPS5827017 A JP S5827017A
Authority
JP
Japan
Prior art keywords
vortex
detected
flow speed
change
detect
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
JP56126972A
Other languages
Japanese (ja)
Inventor
Shunichi Wada
俊一 和田
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric Corp
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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP56126972A priority Critical patent/JPS5827017A/en
Publication of JPS5827017A publication Critical patent/JPS5827017A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To detect a stable vortex frequency signal and to detect an analog signal corresponding to a mean flow speed at the same time, by detecting the change in the flow of fluid due to the vortex by heat sensitive elements which are provided so as to widen an effective area. CONSTITUTION:A pair of heating wires 31, which are provided behind a vortex yielding body 2, are approximately vertically stretched within a lateral width D of the yielding body 2. Then the wires are bent and stretched to the outside of the lateral width D in a V shape. Thus the effective area is widened. The heating wires 31 are also provided at the opposite side. The detection is performed in the wider area in comparison with the case the change in the flow speed is detected by dot or a piece of wire. Therefore the stable detection of the vortex signal can be expected. An electric signal corresponding to the mean flow speed can be concurrently detected by a part protruded from the width D. As a result, the stable vortex frequency signal can be detected, and the analog signal corresponding to the mean flow speed can be also detected.

Description

【発明の詳細な説明】 本発明は渦流量針の改良に関し、特に渦の検出部に関す
るものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an improvement in a vortex flow needle, and more particularly to a vortex detection section.

この種渦流量計には力μマン渦式のものとスワール式の
ものが知られておシ、ともに流量又は流速に略比例した
周波数信号を出力する。渦は被測定流体中に渦発生体を
挿入するとその下流に安定に発生する。渦の発生に伴な
い、渦発生体の周シには規則的な流れの変化が発生し、
該変化を圧力の変化、流速の変化、超音波の伝搬の変化
、感熱素子の放熱の変化等により検出する方法が各種実
用化されている。
This kind of vortex flow meter is known as a force μ-man vortex type type or a swirl type type, and both output a frequency signal that is approximately proportional to the flow rate or flow velocity. When a vortex generator is inserted into the fluid to be measured, a vortex is stably generated downstream of the vortex generator. As vortices are generated, regular flow changes occur around the vortex generator,
Various methods have been put into practical use for detecting such changes based on changes in pressure, changes in flow velocity, changes in propagation of ultrasonic waves, changes in heat radiation of heat-sensitive elements, etc.

ただし、渦周波数に対応した電気信号を得る為のセンサ
ーの設置場所を適正位置にしないと安定な周波数信号を
得る事が出来ない。このセンサーを適当な位置に設置す
る方法については特公昭54−88518号公報に詳し
く説明されている。
However, it is not possible to obtain a stable frequency signal unless the sensor is installed in an appropriate position to obtain an electrical signal corresponding to the vortex frequency. A method for installing this sensor at an appropriate position is described in detail in Japanese Patent Publication No. 88518/1983.

第1図に渦発生体とその周囲の流体の流れの様子の一例
を示す。
FIG. 1 shows an example of a vortex generator and the flow of fluid around it.

図において、(1)は導管、(2)は渦発生体、(3)
は力μマン渦である。図において被測定流体が流れると
渦発生体(2)の後流に規則的なカルマン渦列(3)が
発生する。図中(4)、(5)の斜線で示した部分は、
力μマン渦の発生周波数に対応した流速変化が安定に観
測出来る部分である。この中で渦発生体(2)のの最後
尾の平板のすぐ後流の(6) (7)の部分は流速の変
化信号が最も明瞭に観測出来るが逆に不要なノイズ信号
の重畳する割合も大きい。逆に、(6)(7)の部分か
ら遠ざかるにしたがって流速の変化信号に重畳されるノ
イズ信号は小さくなるが、主流の流速が(6) (7)
の部分よシ速くなる為に得られる流速の変化信号は小さ
くなる。もちろん斜線(4) (6)の部分と(5) 
(7)の部分の流速の変化の方向はお互いに逆位相で、
幾可学的に左右対称である。
In the figure, (1) is a conduit, (2) is a vortex generator, and (3)
is a force μ-man vortex. In the figure, when the fluid to be measured flows, a regular Karman vortex street (3) is generated in the wake of the vortex generator (2). The shaded parts (4) and (5) in the figure are
This is the part where changes in flow velocity corresponding to the frequency of the force μ-Man vortex can be stably observed. Among these, the flow velocity change signal can be observed most clearly in the parts (6) and (7) immediately after the last flat plate of the vortex generator (2), but on the other hand, unnecessary noise signals are superimposed on the parts (6) and (7). It's also big. Conversely, as the distance from parts (6) and (7) increases, the noise signal superimposed on the flow velocity change signal becomes smaller;
Since the flow rate becomes faster than the flow rate, the obtained flow velocity change signal becomes smaller. Of course, the diagonal lines (4) and (6) and (5)
The directions of changes in flow velocity in part (7) are in opposite phase to each other,
Geometrically symmetrical.

第2図の他の渦発生柱を用いた場合のその周囲の流体の
流れの様子を示す。渦発生体(2)の形状が異なる為に
斜線部の領域は明らかに異なるが、斜線部(4) (6
)、斜線部(s) (7)の特性は第1図で説明した通
りである。
This figure shows how the fluid flows around the vortex generating column when the other vortex generating column shown in FIG. 2 is used. The shaded area is obviously different because the shape of the vortex generator (2) is different, but the shaded area (4) (6
), the characteristics of the shaded area (s) (7) are as explained in FIG.

さて、渦による流速変化を感熱素子を用いて電気信号に
変換する場合にサーミスタ又は熱線を用いたとする。こ
れらの感熱素子は設置された狭い範囲の流速変化しか検
出する事が出来ず、設置場所のずれに敏感である。又左
右対称位置に感熱素子を配し、その差信号によシ渦信号
を検出する場合にも、対称位置からのずれの影響も非常
に大きく位置精度を十分に押さえなければならないと云
う欠点がある。
Now, assume that a thermistor or a hot wire is used when converting a change in flow velocity due to a vortex into an electrical signal using a heat-sensitive element. These heat-sensitive elements can only detect changes in flow velocity within a narrow range in which they are installed, and are sensitive to misalignment of the installation location. In addition, even when heat-sensitive elements are arranged in symmetrical positions and a vortex signal is detected based on the difference signal between them, the influence of deviation from the symmetrical position is very large, and the positional accuracy must be maintained sufficiently. be.

さらに感熱素子の電気信号の中から流速に対応したアナ
ログ信号を検出しようとすると、渦発生体(2)の横幅
以内のかげの部分(6) (7)では良好な信号が得ら
れない欠点がある。
Furthermore, when trying to detect an analog signal corresponding to the flow velocity from among the electrical signals of the heat-sensitive element, there is a drawback that good signals cannot be obtained in the shaded areas (6) and (7) within the width of the vortex generator (2). be.

この発明は上記欠点を除去しようとするもので、その第
1の目的は乱れのない安定な渦周波数信号の検出であシ
、その第2の目的は流量べ対応した周波数信号と同時に
アナログ信号も検出する為である。
This invention attempts to eliminate the above-mentioned drawbacks; its first purpose is to detect a stable, undisturbed vortex frequency signal, and its second purpose is to detect a frequency signal corresponding to a flow rate as well as an analog signal. This is for the purpose of detection.

第8図は本発明の一実施例の部分説明図であり、図にお
いて釦)は熱線である。熱線rAOは渦発生体(2)の
最後尾の後方に1対設けられ、設置方法は渦発生体(2
)の横幅ID1以内の所に略垂直にA −A’と張シ、
さらに折シ返して、上記横幅TD)よシも外側へA’ 
−eA“と「Vの字」形に張っている。反対側は対称で
ある。
FIG. 8 is a partial explanatory diagram of one embodiment of the present invention, and in the figure, the button) is a hot wire. A pair of hot wires rAO are installed behind the rearmost part of the vortex generator (2), and the installation method is as follows:
) is approximately perpendicular to the area within width ID1 of A-A',
Then turn around and move the width TD above to the outside as well.
-eA" and are stretched in a "V" shape. The opposite side is symmetrical.

上記の様に設置された熱線においては、点又は1本の線
で流速の変化を検出する場合に比べて幅の広い面で検出
出来る事になりよシ安定な渦信号の検出が期待出来る。
With the hot wire installed as described above, it is possible to detect changes in flow velocity over a wider surface than when detecting changes in flow velocity at a point or a single line, and stable detection of vortex signals can be expected.

さらに横幅ID)よシもはみ出して張られたX→ム“の
部分によ多流体の平均流速に対応した電気信号も同時に
検出する事が出来る。、この検出原理は通常の熱線流速
計の原理と全く同一である。なお上記実施例では熱線を
直列に「Vの字」型に張る場合に・ついて述べたが「W
の字」型、その他の任意の張り で良い。又直列でなく
並列であっても良い、又熱線のかわシに複数個のサーミ
スタであっても良−・。
In addition, it is possible to simultaneously detect electrical signals corresponding to the average flow velocity of multiple fluids at the part of X → M which extends beyond the width ID).This detection principle is the same as that of a normal hot wire anemometer. In the above embodiment, the case where the hot wires are stretched in series in a "V" shape is described, but the "W"
” shape or any other tension is fine. Also, they may be connected in parallel instead of in series, or there may be multiple thermistors in place of the hot wire.

さらに、上記実施例ではカルマン渦列を検出する場合に
ついて述べたが、スワール式の渦流量計の場合にでも同
様の効果が期待出来る事は云うまでもない。
Further, in the above embodiment, the case of detecting the Karman vortex street was described, but it goes without saying that similar effects can be expected in the case of a swirl type vortex flow meter.

以上説明したとうシ本発明によれが渦による流体の流れ
の規則的変化を、16面積を広げる様に設置された感熱
素子で検出すると云う簡単な構成で、安定な渦周波数信
号を検出出来ると同時に、平均流速に対応したアナログ
信号も同時に検出出来る効果がある。
As explained above, according to the present invention, a stable vortex frequency signal can be detected with a simple configuration in which regular changes in fluid flow caused by vortices are detected using heat-sensitive elements installed to spread over 16 areas. At the same time, there is an effect that an analog signal corresponding to the average flow velocity can also be detected at the same time.

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

第1図は渦発生体その周囲の流体の流れの様子を示す図
、第2図は他の渦発生体とその周囲の流体の流れの様子
を示す図、第8図は本発明の一実施例を示す構造図であ
る。 なお図中(1)は導管、(2)は渦発生体、(3)は熱
線である。 代理人 葛野信−(ほか1名)
FIG. 1 is a diagram showing the flow of fluid around the vortex generator, FIG. 2 is a diagram showing another vortex generator and the flow of fluid around it, and FIG. 8 is an embodiment of the present invention. FIG. 2 is a structural diagram showing an example. In the figure, (1) is a conduit, (2) is a vortex generator, and (3) is a hot wire. Agent Shin Kuzuno (1 other person)

Claims (2)

【特許請求の範囲】[Claims] (1)被測定流体中に設けられ、渦発生体によシ該空気
流量を流体的な渦の変化としてとらえ、上記流体的な渦
の変化を少なくとも1個の感熱素子により電気信号の周
波数の変化信号としてとらえるものにおいて、上記流体
の流通方向において渦発生体の幅内に設けられた第1の
素子と上記幅より外側に設けられた第2の素子から成る
感熱素子を備えた事を特命とする渦流量計。
(1) A vortex generator installed in the fluid to be measured captures the air flow rate as a change in the fluid vortex, and changes the frequency of the electrical signal by using at least one heat-sensitive element to detect the change in the fluid vortex. For signals to be detected as change signals, it is specially mandated that a heat-sensitive element consisting of a first element provided within the width of the vortex generator in the flow direction of the fluid and a second element provided outside the said width is provided. Vortex flowmeter with.
(2)感熱素子を第1の熱線と第2の熱線とから構成し
た事を特徴とする特許請求の範囲第1項記載の渦流量計
(2) The vortex flowmeter according to claim 1, wherein the heat-sensitive element is composed of a first heating wire and a second heating wire.
JP56126972A 1981-08-11 1981-08-11 Vortex flowmeter Pending JPS5827017A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56126972A JPS5827017A (en) 1981-08-11 1981-08-11 Vortex flowmeter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56126972A JPS5827017A (en) 1981-08-11 1981-08-11 Vortex flowmeter

Publications (1)

Publication Number Publication Date
JPS5827017A true JPS5827017A (en) 1983-02-17

Family

ID=14948447

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56126972A Pending JPS5827017A (en) 1981-08-11 1981-08-11 Vortex flowmeter

Country Status (1)

Country Link
JP (1) JPS5827017A (en)

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