JPH0611368A - Karman's vortex flowmeter - Google Patents
Karman's vortex flowmeterInfo
- Publication number
- JPH0611368A JPH0611368A JP4169362A JP16936292A JPH0611368A JP H0611368 A JPH0611368 A JP H0611368A JP 4169362 A JP4169362 A JP 4169362A JP 16936292 A JP16936292 A JP 16936292A JP H0611368 A JPH0611368 A JP H0611368A
- Authority
- JP
- Japan
- Prior art keywords
- pressure
- flow rate
- thin portion
- flow
- measuring element
- 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.)
- Granted
Links
Landscapes
- Measuring Volume Flow (AREA)
- Measuring Fluid Pressure (AREA)
Abstract
Description
【0001】[0001]
【産業上の利用分野】この発明は、流体の流れの中に挿
入された柱状物体の下流側側面に発生するカルマン渦を
検出して、流体の流量を検出するカルマン渦流量計に関
するものである。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a Karman vortex flowmeter for detecting a flow rate of a fluid by detecting a Karman vortex generated on a downstream side surface of a columnar object inserted into a fluid flow. .
【0002】[0002]
【従来の技術】図8は、例えば特開昭60―22081
9号公報に示された従来のカルマン渦流量計を示す断面
図である。図において、2は流路、4は柱状体、6は導
圧管、8はシリコンチップ、9はピエゾ抵抗ゲージであ
る。2. Description of the Related Art FIG. 8 shows, for example, JP-A-60-22081.
It is sectional drawing which shows the conventional Karman vortex flowmeter shown by the 9th publication. In the figure, 2 is a flow path, 4 is a columnar body, 6 is a pressure guiding tube, 8 is a silicon chip, and 9 is a piezoresistive gauge.
【0003】従来のカルマン渦流量計は上記のように構
成され、柱状体4によって発生したカルマン渦による圧
力変化を導圧管6を用いてシリコンチップ8の薄肉部に
導き、この圧力差による薄肉部の振動をピエゾ抵抗ゲー
ジ9の抵抗値変化によって検出し、この抵抗値の変動周
波数から流速または流量を測定していた。このようなカ
ルマン渦流量計は比較的測定精度が高いという特徴を持
つ。The conventional Karman vortex flowmeter is constructed as described above, and the pressure change due to the Karman vortex generated by the columnar body 4 is introduced to the thin portion of the silicon chip 8 using the pressure guiding tube 6, and the thin portion due to this pressure difference. Was detected by the change in the resistance value of the piezoresistive gauge 9, and the flow velocity or the flow rate was measured from the fluctuation frequency of the resistance value. Such a Karman vortex flowmeter is characterized by relatively high measurement accuracy.
【0004】[0004]
【発明が解決しようとする課題】しかしながら、一般
に、渦による圧力変化を板状部材をたわませて歪を検出
する方式のカルマン渦流量計では原理的に以下の問題点
があった。圧力の変化が流速の2乗に比例するため感度
とレンジアビリティの両立が困難である。すなわち、低
速流量域においてはカルマン渦列が非常に弱くなるの
で、この領域での感度を上げるためには板上部材を薄く
する必要があるが、この場合高速流量域において渦によ
る圧力が大きくなると過大な変位や力が加わり精度よく
渦が検出できなくなる。逆に、板上部材を厚くすると高
速流量域での耐振性が向上するが、低速流量域での感度
が低くなる。また、いわゆる容積型であるため、気体流
量の測定においては温度や圧力による密度変化を補正す
るための温度検出素子を、渦の発生に影響を与えずしか
も流体温度を正確に測定できる位置に挿入する必要があ
った。そこで、低速流量域において高感度であり、高速
流量域でも充分な応答性をもつ渦検出器として、例えば
熱線が冷却されることを用いた方式のものがあるが、流
体中の混入物の接触や付着の影響を受けやすいという問
題点があった。上記のように従来のカルマン渦流量計に
おいては、渦の検出方法や測定素子に依存して充分な測
定精度を得るためには、測定対象や測定領域が限定され
たり、測定素子の出力に異常が発生したときの機能の保
障に問題があった。また、一般に流体計測においては種
々の流体物理量のうち、ひとつだけを必要とすることは
少なく、流量、絶対圧、温度など複数の物理量の同時測
定が要求されることが多い。ところが、従来の渦流量計
ではこのような測定は不可能であった。However, in general, the Karman vortex flowmeter of the type in which a plate-shaped member is deflected by a pressure change due to a vortex to detect a strain has the following problems in principle. Since the change in pressure is proportional to the square of the flow velocity, it is difficult to achieve both sensitivity and rangeability. That is, since the Karman vortex street becomes extremely weak in the low flow rate region, it is necessary to make the plate member thin in order to increase the sensitivity in this region, but in this case, the pressure due to the vortex becomes large in the high flow rate region. Excessive displacement and force are applied, and vortices cannot be detected accurately. On the contrary, when the plate member is thickened, the vibration resistance in the high flow rate range is improved, but the sensitivity in the low flow rate range is lowered. Also, because it is a so-called positive displacement type, when measuring the gas flow rate, insert a temperature detection element to correct the density change due to temperature and pressure at a position that can accurately measure the fluid temperature without affecting the generation of vortices. Had to do. Therefore, as a vortex detector that has high sensitivity in the low-speed flow rate range and has sufficient response in the high-speed flow rate range, for example, there is a system that uses cooling of the heat wire. However, there is a problem that it is easily affected by adhesion. As described above, in the conventional Karman vortex flowmeter, in order to obtain sufficient measurement accuracy depending on the vortex detection method and measurement element, the measurement target and measurement area are limited, and the output of the measurement element is abnormal. There was a problem in guaranteeing the function when the occurrence occurred. Generally, in fluid measurement, it is rare that only one of various physical quantities of fluid is required, and simultaneous measurement of a plurality of physical quantities such as flow rate, absolute pressure, and temperature is often required. However, such measurement is impossible with the conventional vortex flowmeter.
【0005】この発明は上記のような問題点を解消する
ためになされたもので、測定対象を限定せずに広い流量
範囲にわたって高精度な流量測定を行うことができるカ
ルマン渦流量計を得ることを目的としている。The present invention has been made in order to solve the above problems, and provides a Karman vortex flowmeter capable of highly accurate flow rate measurement over a wide flow rate range without limiting the measurement object. It is an object.
【0006】また、流路内における流体の絶対圧と流量
を同時に測定することができる複合カルマン渦流量計を
得ることを目的としている。Another object of the present invention is to obtain a compound Karman vortex flowmeter capable of simultaneously measuring the absolute pressure and the flow rate of the fluid in the flow channel.
【0007】[0007]
【課題を解決するための手段】この発明に係るカルマン
渦流量計は、カルマン渦による圧力変動の検出に圧力測
定素子と発熱素子を併用し、これら2つの検出信号から
流量を測定するようにしたものである。In the Karman vortex flowmeter according to the present invention, a pressure measuring element and a heating element are used together to detect pressure fluctuation due to Karman vortex, and the flow rate is measured from these two detection signals. It is a thing.
【0008】また、上記カルマン渦流量計は、ひとつの
半導体チップ上にエッチングによって形成された薄肉部
と貫通孔とを設け、前記薄肉部上に圧力測定素子を形成
し、前記貫通孔内に両端支持された発熱素子を、前記貫
通孔近傍の半導体チップ表面上に温度測定素子を形成す
るとよい。In the Karman vortex flowmeter, a thin portion formed by etching and a through hole are provided on one semiconductor chip, a pressure measuring element is formed on the thin portion, and both ends are formed in the through hole. The supported heat generating element may be formed with a temperature measuring element on the surface of the semiconductor chip near the through hole.
【0009】また、上記カルマン渦流量計は圧力測定素
子と、発熱素子及び温度測定素子とが圧力的に分離され
た導圧室、上記導圧室と流路を結ぶ導圧管、並びに薄肉
部を気密に保つ基準圧室を備えた構成としてもよい。In the Karman vortex flowmeter, a pressure measuring element, a pressure guiding chamber in which a heating element and a temperature measuring element are pressure-separated, a pressure guiding tube connecting the pressure guiding chamber and a flow path, and a thin portion are provided. A reference pressure chamber that keeps airtightness may be provided.
【0010】[0010]
【作用】流路に測定流体が流されると、柱状体によりカ
ルマン渦が生じる。カルマン渦によって生じる圧力変動
による差圧を薄肉部に形成された圧力測定素子で検出
し、測定流体の流量を測定する。一方、温度検出素子に
よって測定した流体温度より一定温度高く発熱するよう
に制御された発熱体が、カルマン渦による圧力変動のた
め生じる流体の流れによって冷却されたときに、発熱体
に流れる加熱電流の大きさ、または変動周波数から測定
流体の流量を測定する。そして流量域に応じて、あるい
は出力の異常を検知し、上記各測定結果を選択して取り
出す。これにより、それぞれの素子の長所を活かした高
精度で広範囲な測定が可能となり、一方の測定素子に異
常が発生しても流量計としての機能が麻痺することが避
けられる。When the measurement fluid is flown through the flow path, Karman vortices are generated by the columnar body. The pressure difference caused by the pressure fluctuation caused by the Karman vortex is detected by the pressure measuring element formed in the thin portion, and the flow rate of the measurement fluid is measured. On the other hand, when the heating element controlled to generate heat at a temperature higher than the fluid temperature measured by the temperature detecting element is cooled by the flow of the fluid caused by the pressure fluctuation due to the Karman vortex, the heating current flowing through the heating element is The flow rate of the measuring fluid is measured from the magnitude or the fluctuating frequency. Then, according to the flow rate range, or an output abnormality is detected, and each of the above measurement results is selected and taken out. As a result, it is possible to perform high-accuracy and wide-range measurements by taking advantage of the merits of each element, and it is possible to prevent the function of the flowmeter from being paralyzed even if an abnormality occurs in one of the measuring elements.
【0011】また、ひとつの半導体チップ上にエッチン
グによって形成された薄肉部と貫通孔とを設け、前記薄
肉部上に圧力測定素子を形成し、前記貫通孔内に両端支
持された発熱素子を、前記貫通孔近傍の半導体チップ表
面上に温度測定素子を形成してカルマン渦流量計を構成
すると、高精度でかつ小形に構成することができ、しか
も、圧力測定素子、温度検出素子、発熱素子等を半導体
製造技術により一体形成できるので大量生産が可能で、
このため安価にできる。Further, a thin portion and a through hole formed by etching are formed on one semiconductor chip, a pressure measuring element is formed on the thin portion, and a heating element supported at both ends in the through hole is formed. When a Karman vortex flowmeter is formed by forming a temperature measuring element on the surface of the semiconductor chip in the vicinity of the through hole, the Karman vortex flowmeter can be formed with high accuracy and small size, and furthermore, a pressure measuring element, a temperature detecting element, a heating element, etc. Since it can be integrally formed by semiconductor manufacturing technology, mass production is possible,
Therefore, the cost can be reduced.
【0012】さらに、圧力測定素子と、発熱素子及び温
度測定素子とが圧力的に分離された導圧室、上記導圧室
と流路を結ぶ導圧管、並びに薄肉部を気密に保つ基準圧
室を備えた構成とすることにより、流路内における流体
の絶対圧も同時に測定でき、個々の物理量の測定だけで
は得られない流体の質量流量、エネルギーなどを得るこ
とができる。Further, a pressure guiding chamber in which the pressure measuring element and the heating element and the temperature measuring element are pressure-separated, a pressure guiding tube connecting the pressure guiding chamber and the flow path, and a reference pressure chamber for keeping the thin portion airtight. With the configuration including, it is possible to simultaneously measure the absolute pressure of the fluid in the flow path, and it is possible to obtain the mass flow rate of the fluid, energy, etc.
【0013】[0013]
実施例1.以下、この発明の実施例について図面に基づ
き、詳細に説明する。図1はこの発明の一実施例を表す
全体構成図で、図2は図1のA−A線に沿った断面図で
ある。各図において、2は流路で、その上流側には整流
格子1が設けられる。また、3、4で一対の渦発生体を
構成しており、図2に示すように断面二等辺三角形状に
形成された上流側柱状体3と、断面等脚台形状に形成さ
れた下流側柱状体4が一定間隙を隔てて流れに対して垂
直に挿入され、固定されている。上流側柱状体3によっ
て発生したカルマン渦Bの圧力変動は、下流側柱状体4
に設けられた導圧孔5から導圧管6a、6bを通ってそ
の内部に導入される。7はパイレックスガラスなどでで
きた台座である。この台座7上にシリコンチップ8が陽
極接合などにより接合されている。シリコンチップ8は
(100 )面の単結晶シリコンで形成され、薄肉部14、
貫通孔15が並んで形成されている。導圧管6aは途中
で2本に分岐し、この薄肉部14、貫通孔15に連通し
た後、再度1本に集束し、導圧管6bとなって下流側柱
状体4の反対側側面に導出される。Example 1. Hereinafter, embodiments of the present invention will be described in detail with reference to the drawings. 1 is an overall configuration diagram showing an embodiment of the present invention, and FIG. 2 is a sectional view taken along the line AA of FIG. In each figure, 2 is a flow path, and the rectifying grid 1 is provided on the upstream side thereof. Further, 3 and 4 constitute a pair of vortex generators, and as shown in FIG. 2, an upstream side columnar body 3 having an isosceles triangular cross section and a downstream side having an isosceles trapezoidal cross section. The columnar body 4 is inserted and fixed perpendicularly to the flow with a certain gap. The pressure fluctuation of the Karman vortex B generated by the upstream columnar body 3 is
It is introduced from the pressure guiding hole 5 provided in the inside through the pressure guiding tubes 6a and 6b. 7 is a pedestal made of Pyrex glass or the like. The silicon chip 8 is bonded to the pedestal 7 by anodic bonding or the like. The silicon chip 8 is made of (100) plane single crystal silicon, and has a thin portion 14,
The through holes 15 are formed side by side. The pressure guiding tube 6a branches into two in the middle, communicates with the thin portion 14 and the through hole 15, and then converges again into one pressure guiding tube 6b which is led out to the side surface on the opposite side of the downstream side columnar body 4. It
【0014】次に、図3は図2のシリコンチップ8を表
し、(a)はその斜視図、(b)は図3(a)のC−C
線に沿った断面図である。シリコンチップ8は裏面より
エッチングを施した薄肉部14をもつ。この薄肉部14
の表面には圧力検出素子9があり、この実施例ではピエ
ゾ抵抗ゲージが用いられており、例えば不純物拡散など
の半導体技術によって(110 )方向に形成されている。
この4個のピエゾ抵抗ゲージはホイートストンブリッジ
を形成している。10は配線取り出し用のアルミニウム
ボンディングパッドである。11は温度検出素子であっ
て、この実施例では白金薄膜抵抗を用いている。12は
アルミニウム配線である。13は発熱素子であって、こ
の実施例では白金薄膜抵抗を用いており、その周囲はエ
ッチングによって打ち抜かれ、矩形状の貫通孔15を構
成している。Next, FIG. 3 shows the silicon chip 8 of FIG. 2, (a) is a perspective view thereof, and (b) is CC of FIG. 3 (a).
It is sectional drawing which followed the line. The silicon chip 8 has a thin portion 14 that is etched from the back surface. This thin part 14
A pressure detecting element 9 is provided on the surface of the element, and a piezoresistive gauge is used in this embodiment, and is formed in the (110) direction by a semiconductor technique such as impurity diffusion.
The four piezoresistive gauges form a Wheatstone bridge. Reference numeral 10 is an aluminum bonding pad for taking out the wiring. Reference numeral 11 is a temperature detecting element, and a platinum thin film resistor is used in this embodiment. Reference numeral 12 is an aluminum wiring. Reference numeral 13 is a heating element, which uses a platinum thin film resistor in this embodiment, and the periphery thereof is punched by etching to form a rectangular through hole 15.
【0015】次に、上記のような構造をもつカルマン渦
流量計の動作について図2、図3を基に説明する。測定
流体Qが流路に流入すると、上流側柱状体3によってカ
ルマン渦が発生する。今、渦が図中Bの位置にあるとす
ると導圧管6a、6bの開口部付近にそれぞれ正圧、負
圧が生じる。その結果、導圧管6aから流入して導圧管
6bを通って流出する流体の流れRが発生する。この圧
力変動、流れRはシリコンチップ上の薄肉部14、貫通
孔15に導かれる。薄肉部14は、カルマン渦による圧
力変動のため振動を起こす。この振動による応力変動の
ため薄肉部表面に形成されたピエゾ抵抗ゲージ9の抵抗
値が変化する。この抵抗値変化をブリッジを構成して検
出するが、その変動周波数は流速に比例しているので、
この周波数から流速あるいは流量を測定することができ
る。一方、貫通孔15内に突出した発熱用白金薄膜抵抗
13は温度検出用白金薄膜抵抗11によって測定した流
体温度より一定温度高く発熱するように制御されてい
る。そこに流れRが流入すると発熱用白金薄膜抵抗13
は冷却される。このとき白金薄膜抵抗13に流れる加熱
電流の変動周波数を検出することにより流速あるいは流
量を測定することができる。上記のように出力信号はピ
エゾ抵抗ゲージ9、白金薄膜抵抗13の双方から得られ
るが、外部制御回路によって出力信号の切り換えを行
う。すなわち、微小流量域で高い感度が求められるとき
や、白金薄膜抵抗13に流体中の混入物が付着してその
出力に異常が検知されるときはピエゾ抵抗ゲージ9から
の出力信号を取り出し、大流量域で高速応答性が求めら
れるときや、薄肉部に過大な圧力が加わりピエゾ抵抗ゲ
ージの出力に異常が検知されるときは発熱用白金薄膜抵
抗13の出力信号を取り出す。これにより、それぞれの
素子の長所を活かした高精度で広範囲な測定が可能とな
り、一方の測定素子に異常が発生しても流量計としての
機能が麻痺することが避けられる。Next, the operation of the Karman vortex flowmeter having the above structure will be described with reference to FIGS. When the measurement fluid Q flows into the flow path, Karman vortices are generated by the upstream columnar body 3. Now, assuming that the vortex is at the position B in the figure, positive pressure and negative pressure are generated near the openings of the pressure guiding tubes 6a and 6b, respectively. As a result, a fluid flow R that flows in from the pressure guiding tube 6a and flows out through the pressure guiding tube 6b is generated. This pressure fluctuation and flow R are guided to the thin portion 14 and the through hole 15 on the silicon chip. The thin portion 14 vibrates due to pressure fluctuation due to Karman vortex. Due to the stress variation due to this vibration, the resistance value of the piezoresistive gauge 9 formed on the surface of the thin portion changes. This resistance value change is detected by configuring a bridge. Since the fluctuation frequency is proportional to the flow velocity,
The flow velocity or flow rate can be measured from this frequency. On the other hand, the heat-generating platinum thin-film resistor 13 protruding into the through hole 15 is controlled to generate heat at a constant temperature higher than the fluid temperature measured by the temperature-detecting platinum thin-film resistor 11. When the flow R flows in there, the platinum thin film resistor 13 for heat generation
Is cooled. At this time, the flow velocity or flow rate can be measured by detecting the fluctuating frequency of the heating current flowing through the platinum thin film resistor 13. As described above, the output signal is obtained from both the piezoresistive gauge 9 and the platinum thin film resistor 13, but the output signal is switched by the external control circuit. That is, when high sensitivity is required in a minute flow rate range, or when an abnormality is detected in the output due to contaminants in the fluid adhering to the platinum thin film resistor 13, the output signal from the piezoresistive gauge 9 is taken out and set to a large value. When high-speed response is required in the flow rate range or when an abnormal pressure is detected on the thin-walled portion and the output of the piezoresistive gauge is detected, the output signal of the platinum thin-film resistor 13 for heat generation is taken out. As a result, it is possible to perform high-accuracy and wide-range measurements by taking advantage of the merits of each element, and it is possible to prevent the function of the flowmeter from being paralyzed even if an abnormality occurs in one of the measuring elements.
【0016】実施例2.上記実施例1では(100)面の
シリコン基板に(110)方向にピエゾ抵抗ゲージを4個
配列しているが、その配列、個数は何でもよい。例え
ば、(110 )面シリコン基板に(110 )方向にピエゾ抵
抗ゲージを配列しても同様の効果が得られる。また、温
度検出素子として白金薄膜抵抗11を用いたが、ダイオ
ードを定電流駆動したものを用いても同様の効果が得ら
れる。さらに、発熱素子として白金薄膜抵抗13を用い
ているが、拡散抵抗、トランジスタなどを用いてもよ
い。Example 2. Although four piezoresistive gauges are arranged in the (110) direction on the silicon substrate having the (100) plane in the first embodiment, the arrangement and the number may be arbitrary. For example, the same effect can be obtained by arranging piezoresistive gauges in the (110) direction on a (110) plane silicon substrate. Further, although the platinum thin film resistor 11 is used as the temperature detecting element, the same effect can be obtained by using a diode driven by a constant current. Further, although the platinum thin film resistor 13 is used as the heating element, a diffused resistor, a transistor or the like may be used.
【0017】実施例3.上記実施例1、2では、シリコ
ンチップ8は下流側柱状体4の内部に設置されている
が、流路2の外部に置くことで保守、点検を容易にする
こともできる。Embodiment 3. In the first and second embodiments, the silicon chip 8 is installed inside the downstream columnar body 4, but it can be placed outside the flow path 2 to facilitate maintenance and inspection.
【0018】実施例4.図4は圧力測定素子9で流路の
絶対圧を測定するように構成した実施態様を示す全体構
成図である。1〜15は上記実施例1〜3と全く同一で
ある。16は導圧管、17は渦検出部である。図5は渦
検出部を流れ方向から見た拡大断面図であり、図6は渦
検出部の側面断面図である。この実施例では圧力測定素
子9を温度測定素子11、発熱素子13と圧力的に分離
した導圧室18内に設置し、この導圧室18と流路2と
を導圧管16によって連通させている。また、薄肉部1
4の裏面は台座7と陽極接合などにより気密に接合し基
準圧室19としている。基準圧室19内部は密閉される
ため湿度の影響を極小にすることができる。このような
実施例によれば圧力測定素子9によって流路2を流れる
流体の絶対圧を測定できるようになる。一方、上記実施
例1〜3と同様に発熱素子によって流速または流量を測
定することができる。すなわち、流路の絶対圧と流量と
いう流体計測において重要な2つの物理量が同時に測定
できる。Example 4. FIG. 4 is an overall configuration diagram showing an embodiment configured to measure the absolute pressure of the flow path by the pressure measuring element 9. 1 to 15 are exactly the same as those in Examples 1 to 3 above. Reference numeral 16 is a pressure guiding tube, and 17 is a vortex detector. FIG. 5 is an enlarged cross-sectional view of the vortex detector as seen from the flow direction, and FIG. 6 is a side sectional view of the vortex detector. In this embodiment, the pressure measuring element 9 is installed in a pressure guiding chamber 18 that is pressure-separated from the temperature measuring element 11 and the heating element 13, and the pressure guiding chamber 18 and the flow path 2 are connected by a pressure guiding tube 16. There is. Also, the thin portion 1
The back surface of 4 is hermetically bonded to the base 7 by anodic bonding or the like to form a reference pressure chamber 19. Since the inside of the reference pressure chamber 19 is sealed, the influence of humidity can be minimized. According to such an embodiment, the absolute pressure of the fluid flowing through the flow path 2 can be measured by the pressure measuring element 9. On the other hand, the flow velocity or flow rate can be measured by the heating element as in the first to third embodiments. That is, two physical quantities that are important in fluid measurement, that is, the absolute pressure of the flow path and the flow rate, can be measured simultaneously.
【0019】実施例5.上記実施例4では圧力検出素子
としてピエゾ抵抗ゲージを用いているが、図7に示すよ
うな方法で圧力検出素子を構成しても所期の目的を達成
することができる。すなわち、シリコンチップの薄肉部
14に不純物拡散層20を形成し、これを可動電極と
し、基準圧室内19の台座7の表面にアルミニウム電極
21を蒸着し、これを固定電極とすることで、薄肉部の
偏位にともなうキャパシタの容量が変化することを利用
した容量型の圧力検出素子を構成できる。Example 5. Although the piezoresistive gauge is used as the pressure detecting element in the fourth embodiment, the intended purpose can be achieved by forming the pressure detecting element by the method shown in FIG. That is, the impurity diffusion layer 20 is formed in the thin portion 14 of the silicon chip, and this is used as a movable electrode, and the aluminum electrode 21 is vapor-deposited on the surface of the pedestal 7 in the reference pressure chamber 19, and this is used as a fixed electrode. It is possible to configure a capacitive pressure detecting element that utilizes the change in the capacitance of the capacitor due to the displacement of the part.
【0020】[0020]
【発明の効果】以上のように、この発明によれば、カル
マン渦による圧力変動の検出に圧力測定素子と発熱素子
を併用し、これら2つの検出信号から流量を測定するよ
うにしたので、微小流量域で高い感度が求められるとき
や、発熱素子に流体中の混入物が付着してその出力に異
常が検知されるときは、圧力検出素子から出力信号を取
り出し、大流量域で高速応答性が求められるときや、薄
肉部に過大な圧力が加わり圧力検出素子の出力に異常が
検知されるときは、発熱素子から出力信号を取り出す、
という2つの検出方式を併用でき、それぞれの長所を活
かした高精度で広範囲な測定が可能になるとともに、一
方の検出方式に異常が発生しても他方が動作していれば
機能が完全に麻痺してしまうことも避けられる効果があ
る。As described above, according to the present invention, the pressure measuring element and the heating element are used together to detect the pressure fluctuation due to the Karman vortex, and the flow rate is measured from these two detection signals. When high sensitivity is required in the flow rate range, or when abnormalities in the output are detected due to contaminants in the fluid adhering to the heating element, the output signal is taken out from the pressure detection element and high-speed response is achieved in the large flow rate range. Is required, or when an excessive pressure is applied to the thin portion and an abnormality is detected in the output of the pressure detection element, the output signal is taken from the heating element,
These two detection methods can be used together, making it possible to perform high-accuracy and wide-range measurements by taking advantage of their respective strengths, and even if one of the detection methods fails, the other function is completely paralyzed. There is also an effect that it can be avoided.
【0021】また、ひとつの半導体チップ上にエッチン
グによって形成された薄肉部と貫通孔とを設け、前記薄
肉部上に圧力測定素子を形成し、前記貫通孔内に両端支
持された発熱素子を、前記貫通孔近傍の半導体チップ表
面上に温度測定素子を形成してカルマン渦流量計を構成
すれば、高精度でかつ小形に構成することができ、しか
も、圧力測定素子、温度検出素子、発熱素子等を半導体
製造技術により一体形成できるので大量生産が可能で、
安価にできる効果がある。するとよい。Further, a thin portion and a through hole formed by etching are provided on one semiconductor chip, a pressure measuring element is formed on the thin portion, and a heat generating element supported at both ends in the through hole is formed. If a Karman vortex flowmeter is formed by forming a temperature measuring element on the surface of the semiconductor chip in the vicinity of the through hole, the Karman vortex flowmeter can be formed with high accuracy and small size, and further, the pressure measuring element, the temperature detecting element, and the heat generating element. Etc. can be integrally formed by semiconductor manufacturing technology, so mass production is possible,
There is an effect that it can be made cheap. Good to do.
【0022】また、圧力測定素子と、発熱素子及び温度
測定素子とが圧力的に分離された導圧室、上記導圧室と
流路を結ぶ導圧管、並びに薄肉部を気密に保つ基準圧室
を備えた構成とすることにより、流体計測において重要
な物理量である流体の絶対圧、流速、温度を同時に測定
することができ、個々の物理量の測定だけでは得られな
い流体の質量流量、エネルギーなどを得ることができ
る。Further, a pressure guiding chamber in which the pressure measuring element and the heating element and the temperature measuring element are pressure-separated, a pressure guiding tube connecting the pressure guiding chamber and the flow path, and a reference pressure chamber for keeping the thin portion airtight. By including the configuration, it is possible to simultaneously measure the absolute pressure, flow velocity, and temperature of the fluid, which are important physical quantities in fluid measurement, and the mass flow rate, energy, etc. of the fluid that cannot be obtained by measuring individual physical quantities. Can be obtained.
【図1】この発明の実施例1を示す全体構成図である。FIG. 1 is an overall configuration diagram showing a first embodiment of the present invention.
【図2】図1のA―A線に沿った断面図である。FIG. 2 is a sectional view taken along the line AA of FIG.
【図3】この発明の実施例1におけるシリコンチップの
斜視図及び断面図である。FIG. 3 is a perspective view and a cross-sectional view of a silicon chip according to a first embodiment of the present invention.
【図4】この発明の実施例4を示す全体構成図である。FIG. 4 is an overall configuration diagram showing a fourth embodiment of the present invention.
【図5】この発明の実施例4における渦検出部を流体の
流れ方向から見た拡大断面図である。FIG. 5 is an enlarged cross-sectional view of a vortex detector according to a fourth embodiment of the present invention as viewed in the fluid flow direction.
【図6】この発明の実施例4における渦検出部の側面断
面図である。FIG. 6 is a side sectional view of a vortex detector in a fourth embodiment of the present invention.
【図7】この発明の実施例5におけるシリコンチップ及
び台座の断面図である。FIG. 7 is a sectional view of a silicon chip and a pedestal according to a fifth embodiment of the present invention.
【図8】従来の渦流量計の全体構成図である。FIG. 8 is an overall configuration diagram of a conventional vortex flowmeter.
2 流路 3 上流側柱状体 4 下流側柱状体 6a 導圧管 6b 導圧管 8 シリコンチップ 9 圧力測定素子 11 温度測定素子 13 発熱素子 14 薄肉部 15 貫通孔 16 導圧管 18 導圧室 19 基準圧室 2 flow path 3 upstream columnar body 4 downstream columnar body 6a pressure guiding tube 6b pressure guiding tube 8 silicon chip 9 pressure measuring element 11 temperature measuring element 13 heat generating element 14 thin portion 15 through hole 16 pressure guiding tube 18 pressure guiding chamber 19 reference pressure chamber
Claims (3)
るカルマン渦に対応して変化する2点間の圧力差を検出
するととともに、上記圧力差によって生じる流れを熱的
検出手段を用いて検出し、これら2つの検出信号から流
量を測定するようにしたカルマン渦流量計。1. A pressure difference between two points, which changes corresponding to a Karman vortex generated near a columnar body inserted in a flow path, is detected, and a flow generated by the pressure difference is detected by a thermal detection means. Karman vortex flowmeter that detects the flow rate and measures the flow rate from these two detection signals.
測定素子と、上記薄肉部の近傍に形成された貫通孔と、
この貫通孔内に両端支持され、流体温度よりも一定温度
高く発熱する発熱素子と、上記貫通孔近傍に形成された
温度測定素子とをひとつの半導体チップ上に一体形成し
た請求項1記載のカルマン渦流量計。2. A thin portion, a pressure measuring element formed in the thin portion, a through hole formed in the vicinity of the thin portion,
The Kalman according to claim 1, wherein a heating element, which is supported at both ends in the through hole and generates heat at a constant temperature higher than the fluid temperature, and a temperature measuring element formed near the through hole are integrally formed on one semiconductor chip. Vortex flow meter.
素子とが圧力的に分離された導圧室、上記導圧室と流路
を結ぶ導圧管、並びに薄肉部を気密に保つ基準圧室を備
えた請求項1または2記載のカルマン渦流量計。3. A pressure guiding chamber in which a pressure measuring element and a heating element and a temperature measuring element are pressure-separated, a pressure guiding tube connecting the pressure guiding chamber and a flow path, and a reference pressure chamber for keeping a thin portion airtight. The Karman vortex flowmeter according to claim 1 or 2, further comprising:
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP4169362A JP3024364B2 (en) | 1992-06-26 | 1992-06-26 | Karman vortex flowmeter |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP4169362A JP3024364B2 (en) | 1992-06-26 | 1992-06-26 | Karman vortex flowmeter |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH0611368A true JPH0611368A (en) | 1994-01-21 |
| JP3024364B2 JP3024364B2 (en) | 2000-03-21 |
Family
ID=15885178
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP4169362A Expired - Fee Related JP3024364B2 (en) | 1992-06-26 | 1992-06-26 | Karman vortex flowmeter |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP3024364B2 (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2016191655A (en) * | 2015-03-31 | 2016-11-10 | アズビル株式会社 | Vortex flow velocity meter |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP5724492B2 (en) | 2011-03-16 | 2015-05-27 | セイコーエプソン株式会社 | Atomic oscillator |
-
1992
- 1992-06-26 JP JP4169362A patent/JP3024364B2/en not_active Expired - Fee Related
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2016191655A (en) * | 2015-03-31 | 2016-11-10 | アズビル株式会社 | Vortex flow velocity meter |
Also Published As
| Publication number | Publication date |
|---|---|
| JP3024364B2 (en) | 2000-03-21 |
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