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JPH0454895B2 - - Google Patents
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JPH0454895B2 - - Google Patents

Info

Publication number
JPH0454895B2
JPH0454895B2 JP11776085A JP11776085A JPH0454895B2 JP H0454895 B2 JPH0454895 B2 JP H0454895B2 JP 11776085 A JP11776085 A JP 11776085A JP 11776085 A JP11776085 A JP 11776085A JP H0454895 B2 JPH0454895 B2 JP H0454895B2
Authority
JP
Japan
Prior art keywords
tube
mass flow
vibration
coriolis force
fixed
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.)
Expired
Application number
JP11776085A
Other languages
Japanese (ja)
Other versions
JPS61275621A (en
Inventor
Akira Takada
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.)
OBARA KIKI KOGYO KK
Original Assignee
OBARA KIKI KOGYO KK
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 OBARA KIKI KOGYO KK filed Critical OBARA KIKI KOGYO KK
Priority to JP11776085A priority Critical patent/JPS61275621A/en
Publication of JPS61275621A publication Critical patent/JPS61275621A/en
Publication of JPH0454895B2 publication Critical patent/JPH0454895B2/ja
Granted 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
    • G01F1/76Devices for measuring mass flow of a fluid or a fluent solid material
    • G01F1/78Direct mass flowmeters
    • G01F1/80Direct mass flowmeters operating by measuring pressure, force, momentum, or frequency of a fluid flow to which a rotational movement has been imparted
    • G01F1/84Coriolis or gyroscopic mass flowmeters
    • G01F1/8409Coriolis or gyroscopic mass flowmeters constructional details
    • 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
    • G01F1/76Devices for measuring mass flow of a fluid or a fluent solid material
    • G01F1/78Direct mass flowmeters
    • G01F1/80Direct mass flowmeters operating by measuring pressure, force, momentum, or frequency of a fluid flow to which a rotational movement has been imparted
    • G01F1/84Coriolis or gyroscopic mass flowmeters
    • G01F1/8409Coriolis or gyroscopic mass flowmeters constructional details
    • G01F1/8431Coriolis or gyroscopic mass flowmeters constructional details electronic circuits
    • 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
    • G01F1/76Devices for measuring mass flow of a fluid or a fluent solid material
    • G01F1/78Direct mass flowmeters
    • G01F1/80Direct mass flowmeters operating by measuring pressure, force, momentum, or frequency of a fluid flow to which a rotational movement has been imparted
    • G01F1/84Coriolis or gyroscopic mass flowmeters
    • G01F1/845Coriolis or gyroscopic mass flowmeters arrangements of measuring means, e.g., of measuring conduits
    • G01F1/8468Coriolis or gyroscopic mass flowmeters arrangements of measuring means, e.g., of measuring conduits vibrating measuring conduits
    • G01F1/849Coriolis or gyroscopic mass flowmeters arrangements of measuring means, e.g., of measuring conduits vibrating measuring conduits having straight measuring conduits
    • 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
    • G01F1/76Devices for measuring mass flow of a fluid or a fluent solid material
    • G01F1/78Direct mass flowmeters
    • G01F1/80Direct mass flowmeters operating by measuring pressure, force, momentum, or frequency of a fluid flow to which a rotational movement has been imparted
    • G01F1/84Coriolis or gyroscopic mass flowmeters
    • G01F1/845Coriolis or gyroscopic mass flowmeters arrangements of measuring means, e.g., of measuring conduits
    • G01F1/8468Coriolis or gyroscopic mass flowmeters arrangements of measuring means, e.g., of measuring conduits vibrating measuring conduits
    • G01F1/849Coriolis or gyroscopic mass flowmeters arrangements of measuring means, e.g., of measuring conduits vibrating measuring conduits having straight measuring conduits
    • G01F1/8495Coriolis or gyroscopic mass flowmeters arrangements of measuring means, e.g., of measuring conduits vibrating measuring conduits having straight measuring conduits with multiple measuring conduits

Landscapes

  • Physics & Mathematics (AREA)
  • Fluid Mechanics (AREA)
  • General Physics & Mathematics (AREA)
  • Measuring Volume Flow (AREA)

Description

【発明の詳細な説明】 (1) 産業上の利用分野 本願発明はコリオリの力を利用した質量流量計
に関する。
DETAILED DESCRIPTION OF THE INVENTION (1) Industrial Application Field The present invention relates to a mass flowmeter that utilizes Coriolis force.

(2) 従来技術 流管を流れる流体流に対して振動を与えると、
流体流の流れの向きと、流管の振動軸とに対して
直角方向にコリオリの力が発生し、このコリオリ
の力が振動周波数と流体の質量流量に比例するこ
とが知られており、特開昭54−52570号公報にお
いてコリオリの力を利用した質量流量計が開示さ
れている。この従来例は支持部材に入口及び出口
部分をもつたU字形の管体を固着した本体形状を
しており、流体は入口部よりU字形管体を通つて
流出する。U字形管体をU字形管体面に対して垂
直の方向に上記固着に対応する固着線を軸として
回転を与えると、U字形管体を流れる流体による
コリオリの力が作用し、固着線に対して垂直なU
字形管体軸に関してコリオリの力に比例した捩り
振動が生ずる。このコリオリの力を管体が基準面
を通過する時間差から求めるものである。
(2) Prior art When vibration is applied to a fluid flow flowing through a flow tube,
It is known that a Coriolis force is generated in a direction perpendicular to the direction of the fluid flow and the vibration axis of the flow tube, and that this Coriolis force is proportional to the vibration frequency and the mass flow rate of the fluid. Japanese Patent Publication No. 54-52570 discloses a mass flowmeter that utilizes the Coriolis force. This conventional example has a body shape in which a U-shaped tube having an inlet and an outlet is fixed to a support member, and fluid flows out from the inlet through the U-shaped tube. When the U-shaped tube is rotated in a direction perpendicular to the surface of the U-shaped tube about the fixation line corresponding to the fixation mentioned above, Coriolis force due to the fluid flowing through the U-shaped tube acts on the fixation line. vertical U
Torsional vibrations proportional to the Coriolis force occur about the axis of the shaped tube. This Coriolis force is determined from the time difference when the tube passes through the reference plane.

(3) 発明が解決しようとする問題点 上述の従来例はコリオリの力を管体の捩りとし
て検出するものであるが、捩りを生じさせるため
流体に往復路を直通させるU字管体としている。
即ち流体は管体に流入するとき及び流出するとき
に、流体は直角に曲げられる。コリオリの力を有
効的に検出するためには、固定線軸まわりの管体
の腕の長さを長くし、U字形管体軸のまわりのモ
ーメントを大きくすることが必要である。このこ
とはU字形管体の面積を大きくする結果を生み、
流量計の取付面積を大きくする結果となつた。ま
た管体の肉厚は薄くした方が有利であるが、この
ことは耐圧強度の低下をまねき高圧の流体計側に
は不向きであり、更に固着部分の耐疲労強度が低
下し長期間安定な流量計測ができない等の問題点
がある。
(3) Problems to be solved by the invention In the conventional example described above, the Coriolis force is detected as the torsion of the tube body, but in order to cause the torsion, the U-shaped tube body is used to pass the reciprocating path directly through the fluid. .
That is, the fluid is bent at right angles as it enters and exits the tube. In order to effectively detect the Coriolis force, it is necessary to increase the length of the arms of the tube about the fixed line axis and to increase the moment about the U-shaped tube axis. This results in increasing the area of the U-shaped tube,
This resulted in the installation area of the flowmeter being increased. Furthermore, it is advantageous to make the wall thickness of the tube thinner, but this leads to a decrease in pressure resistance, making it unsuitable for high-pressure fluid gauges.Furthermore, the fatigue resistance of fixed parts decreases, resulting in long-term stability. There are problems such as the inability to measure flow rate.

(4) 問題解決の手段 本願発明は上述の問題点を解決するためになさ
れたものである。即ち流量計の取付面積を小さく
するために流体の振動を与える管体を流体管路に
沿つた直管としておいてコリオリの力を測定でき
るようにし、且つ管体の肉厚を薄くしても高圧流
体の計測にも耐えるように管体を密閉容器内に内
挿した本体形状とするようにしている。
(4) Means for solving the problem The present invention has been made in order to solve the above-mentioned problems. In other words, in order to reduce the installation area of the flowmeter, the tube that vibrates the fluid is made a straight tube along the fluid pipeline, and the Coriolis force can be measured, and even if the wall thickness of the tube is made thinner, The main body shape is such that the tube is inserted into a closed container to withstand measurement of high-pressure fluid.

実施例 第1図に本願発明の実施例をしめす。イ図は平
面図、ロ図は側面図、ハ図はロ図のAA′矢視断面
をしめす。密閉容器1は図示しない外部流管から
流入する流体の流入口5をもち、該密閉容器内に
他端51を開放する管体2を内挿し、流出口6を
配設した容器である。管体2は薄肉円筒状に構成
され、駆動コイルによりYY′軸上に単振駆動され
るようにされる。従つて駆動が電磁的に行われる
場合、管体は磁性材料で構成されるが、駆動コイ
ルと対向する面に磁性片を固着するようにする。
駆動手段が電磁力によらない、例えば偏心カムを
電動機駆動する場合は磁性材料の必要はない。管
体2は密閉容器1との固着点を支点とした片持ば
りを形成するが、開口端51近傍に駆動コイルを
配設し、ハ図YY′軸上で後述する手段により単振
動駆動する。尚駆動エネルギ効率からみて共振周
波数で駆動するのが好ましい。叙上の導管振動は
大きさに比例した電気量として検出器4で検出さ
れる。リブ7は振動方向に対して剛性が小さく、
直角方向に大きくし、外部振動の影響を軽減させ
るものである。流体が矢印の方向に流れるとし、
管体が上記のように駆動されると、管体内流体に
コリオリの力が発生する。コリオリの力は流体の
流れベクトルと振動ベクトルとのベクトル積に比
例する向きのベクトル量として作用する。振動ベ
クトルはハ図ZZ′軸上にあるのでコリオリの力は
YY′軸上に振動周波数と流体の質量流量とに比例
した大きさであらわれる。即ち振動周波数が一定
であれば質量流量に比例して振幅を減少させるよ
うに働く。
Embodiment FIG. 1 shows an embodiment of the present invention. Figure A shows a plan view, Figure B shows a side view, and Figure C shows a cross section taken along the AA′ arrow in Figure B. The closed container 1 has an inlet 5 for fluid to flow in from an external flow tube (not shown), a tube 2 with an open other end 51 is inserted into the closed container, and an outlet 6 is provided. The tube body 2 is formed into a thin cylindrical shape, and is driven by a drive coil on the YY′ axis in a single vibration. Therefore, when the drive is performed electromagnetically, the tube is made of a magnetic material, and a magnetic piece is fixed to the surface facing the drive coil.
If the driving means does not rely on electromagnetic force, for example, when an eccentric cam is driven by an electric motor, there is no need for a magnetic material. The tube body 2 forms a cantilever beam with the fixed point with the closed container 1 as a fulcrum, and a drive coil is disposed near the open end 51, and is driven by a simple vibration on the YY' axis in Figure C by means described later. . Note that from the viewpoint of drive energy efficiency, it is preferable to drive at a resonant frequency. The above-mentioned conduit vibration is detected by the detector 4 as an electric quantity proportional to the magnitude. The rib 7 has low rigidity in the vibration direction,
It is made larger in the right angle direction to reduce the influence of external vibrations. Assuming that the fluid flows in the direction of the arrow,
When the tube is driven as described above, a Coriolis force is generated in the fluid within the tube. The Coriolis force acts as a vector quantity whose direction is proportional to the vector product of the fluid flow vector and the vibration vector. Since the vibration vector is on the ZZ′ axis of the diagram, the Coriolis force is
It appears on the YY' axis with a magnitude proportional to the vibration frequency and the mass flow rate of the fluid. That is, if the vibration frequency is constant, it works to reduce the amplitude in proportion to the mass flow rate.

第2図は振幅の変化をなくすように帰還を施
し、質量流量に比例した帰還量を指示させる手段
をしめすブロツク図である。管体の振動は検出器
4により電気量として検出され、移相回路101
により検出信号の位相を所定量移相し、増幅器1
02と駆動コイル3とからなる閉ループが共振す
るように設定する。移相された検出器出力は抵抗
R1,R2により分圧され増幅器102に入力され
るが、増幅器102の入力は可変抵抗R1を変化
させることにより、管体の振幅、即ち検出信号を
一定にするようにする。可変抵抗R1は例へば
光・抵抗変換器103を用いている。該光・抵抗
変換素子103は、検出信号を整流器104によ
り整流した所の検出信号に比例した直流電圧と基
準直流電圧105を希望する振幅値になるように
分圧器106で分圧した直流電圧と比較した偏差
信号107を増幅する比較増幅器108に負荷と
して接続される。質量流量が増大して管体振幅が
減少すると光量が増大し、抵抗R1が減少し増幅
器102のゲインを上げ、振幅を増大させる。比
較増幅器108の出力はコリオリの力に比例する
ことになるので指示計109でこれを表示する。
FIG. 2 is a block diagram showing a means for performing feedback so as to eliminate changes in amplitude and instructing a feedback amount proportional to the mass flow rate. The vibration of the tube body is detected as an electric quantity by the detector 4, and the vibration is detected as an electric quantity by the detector 4, and
The phase of the detection signal is shifted by a predetermined amount by
02 and the drive coil 3 is set so that it resonates. The phase shifted detector output is resistor
The voltage is divided by R 1 and R 2 and input to the amplifier 102, and the input to the amplifier 102 is made to keep the amplitude of the tube constant, that is, the detection signal, by changing the variable resistor R 1 . For example, a light-to-resistance converter 103 is used as the variable resistor R1 . The photoresistance conversion element 103 has a DC voltage proportional to the detection signal obtained by rectifying the detection signal by a rectifier 104, and a DC voltage obtained by dividing a reference DC voltage 105 by a voltage divider 106 so as to have a desired amplitude value. It is connected as a load to a comparison amplifier 108 that amplifies the compared deviation signal 107. As the mass flow rate increases and the tube amplitude decreases, the amount of light increases and the resistance R 1 decreases, increasing the gain of amplifier 102 and increasing the amplitude. Since the output of the comparator amplifier 108 is proportional to the Coriolis force, the indicator 109 indicates this.

叙上の方法は一具体例であるが指示方式は本願
による解決課題ではなく上記以外の他の手段でも
可能である。尚叙上の説明において管体断面を円
としているが、これをZ軸方向の辺が長い矩形断
面とすることにより、管体の曲げ剛性を小さくで
き、検出感度をあげることができる。更にZ軸方
向の剛性が大きくなるので信号検出に不要なZ軸
方向振動影響を軽減できる。
Although the method described above is a specific example, the instruction method is not a problem to be solved by the present application, and other means other than the above are also possible. In the above description, the cross section of the tube is circular, but by making it a rectangular cross section with long sides in the Z-axis direction, the bending rigidity of the tube can be reduced and the detection sensitivity can be increased. Furthermore, since the rigidity in the Z-axis direction is increased, the influence of vibration in the Z-axis direction that is unnecessary for signal detection can be reduced.

第3図は本願発明の他の実施例であり第1図と
同一番号の構成要素は同一としてしめす。上記第
1図の実施例に対して管体2と同形同大の管体2
1を追加し、該管体21を管体2に対し並列に配
設したものである。密閉容器1内には支切板8を
流入流体に対向し、流体室9を形成するように密
閉容器内壁に固着している。該支切板8には管体
2及び21を貫通固着する等大の貫通孔53,5
4が穿孔されている。また各々の貫通孔の位置は
管体2及び21に等流量が流れるよう流入口に対
して等間隔にする方がよい。駆動手段3は電磁石
で導管開口部51,52近傍中間部に配設され、
各々の管体をYY′軸上で単振動駆動する。検出器
4及び41は管体の振幅を検出する検出器である
が、各管体が全く等しい振幅で振動する場合はい
ずれか一方のみでよい。通常、管体の各々に同一
流量が流れているときは、この条件を充たしてい
る。従つて第2図と同様な計測手段を適用するこ
と可能である。叙上第3図の実施例においては管
体が並列になつているので、流体の圧力損失が
1/4となり効果的である。従つて同一の圧力損
失では4倍の流量が得られる。同様に管体を多数
の並列配管で行えば、圧損効果は更に向上する。
FIG. 3 shows another embodiment of the present invention, and components having the same numbers as those in FIG. 1 are shown as being the same. A tube body 2 having the same shape and size as the tube body 2 in the embodiment shown in FIG.
1 is added, and the tubular body 21 is arranged in parallel with the tubular body 2. Inside the closed container 1, a dividing plate 8 is fixed to the inner wall of the closed container so as to face the inflowing fluid and form a fluid chamber 9. The dividing plate 8 has equal-sized through holes 53 and 5 through which the tubes 2 and 21 are fixed.
4 is perforated. Further, it is preferable that the positions of the respective through holes be arranged at equal intervals with respect to the inlet so that the same flow rate flows into the pipe bodies 2 and 21. The driving means 3 is an electromagnet and is arranged in the intermediate part near the conduit openings 51 and 52,
Each tube is driven in simple harmonic motion on the YY′ axis. The detectors 4 and 41 are detectors for detecting the amplitude of the tube bodies, but if the tube bodies vibrate with exactly the same amplitude, only one of them may be used. Normally, this condition is satisfied when the same flow rate flows through each tube. Therefore, it is possible to apply a measuring means similar to that shown in FIG. In the embodiment shown in FIG. 3, since the pipe bodies are arranged in parallel, the pressure loss of the fluid is reduced to 1/4, which is effective. Therefore, four times the flow rate can be obtained with the same pressure loss. Similarly, if the pipe body is constructed with a large number of parallel pipes, the pressure drop effect will be further improved.

(6) 効果 以上説明したように本発明によれば、流体の流
れ方向にコリオリの力を発生する管体が配設され
るので、計測のため流体を曲げることがなく、圧
力損失も少なく取付面積も小さくなる。更に管体
は直管であるため加工し易く、感度を高めるため
の薄肉管とすることができ、しかもこの管体は密
閉容器内に開口しているため流体圧力の影響を受
ける心配がないので安価で高感度の質量流量計を
提供できる。
(6) Effects As explained above, according to the present invention, the pipe body that generates the Coriolis force in the direction of fluid flow is provided, so the fluid does not bend for measurement and the installation can be performed with less pressure loss. The area also becomes smaller. Furthermore, since the tube is a straight tube, it is easy to process and can be made into a thin-walled tube to increase sensitivity.Furthermore, since the tube opens into a sealed container, there is no need to worry about it being affected by fluid pressure. It is possible to provide an inexpensive and highly sensitive mass flow meter.

また管体が単純な直管であるため流量計測範囲
を拡大する場合に同形同大の並列管体を構成する
ことも容易で適用範囲の拡大を容易に可能とす
る。
Furthermore, since the tube is a simple straight tube, when expanding the flow rate measurement range, it is easy to configure parallel tubes of the same shape and size, making it easy to expand the range of application.

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

第1図は本願発明の実施例であり、イは平面
図、ロは側面図、ハは正面図である。第2図は第
1図の振動、検出指示等本願発明を具現するため
の計測手段を説明するブロツク図、第3図は本発
明の他の実施例をしめすものである。 図中、1は密閉容器、2は管体、3は駆動コイ
ル、4は検出器、5は流入口、6は流出口を表
す。
FIG. 1 shows an embodiment of the present invention, in which A is a plan view, B is a side view, and C is a front view. FIG. 2 is a block diagram illustrating a measuring means for implementing the present invention such as vibration and detection instructions shown in FIG. 1, and FIG. 3 shows another embodiment of the present invention. In the figure, 1 is a closed container, 2 is a tube body, 3 is a drive coil, 4 is a detector, 5 is an inlet, and 6 is an outlet.

Claims (1)

【特許請求の範囲】 1 流入口および流出口を配設した容器と、該容
器内に上記流入口に一端が連通固着しかつ他端が
開口する管体を配設した本体部と、該管体の固着
点近傍を軸として該管体を振動させる駆動手段
と、該振動により管体内を流れる流体に作用する
コリオリの力を検出する検出手段とをそなえ、上
記コリオリの力に比例する質量流量を測定するこ
とを特徴とする質量流量計。 2 管体を複数とし該管体を音叉を形成するよう
に並列に配設し、該管体開口部を反対位相で駆動
する駆動手段を配設したことを特徴とする特許請
求の範囲第1項記載の質量流量計。 3 管体の断面形状を矩形としたことを特徴とす
る特許請求の範囲第1項または第2項記載の質量
流量計。 4 管体の固着近傍において、該管体の振動方向
及び振動方向と直角方向に管体軸に平行して該管
体と容器とに連結するリブを固着したことを特徴
とする特許請求の範囲囲第1項ないし第3項のい
ずれか記載の質量流量計。 5 検出手段からの検出信号を上記駆動手段側に
帰還させ、上記管体の駆動を制御するようにした
ことを特徴とする特許請求の範囲第1項ないし第
4項のいずれか記載の質量流量計。
[Scope of Claims] 1. A container having an inlet and an outlet, a main body having a tube disposed in the container, one end of which communicates with and is fixed to the inlet, and the other end of which is open, and the tube. A mass flow rate proportional to the Coriolis force is provided, comprising a driving means for vibrating the tube body around an axis near the fixed point of the body, and a detection means for detecting the Coriolis force acting on the fluid flowing inside the tube due to the vibration. A mass flow meter characterized by measuring. 2. Claim 1, characterized in that a plurality of tube bodies are arranged in parallel to form a tuning fork, and a driving means for driving the tube openings in opposite phases is provided. Mass flow meter as described in section. 3. The mass flowmeter according to claim 1 or 2, wherein the tube body has a rectangular cross-sectional shape. 4. Claims characterized in that a rib connecting the tube and the container is fixed in the vibration direction of the tube and in a direction perpendicular to the vibration direction and parallel to the tube axis in the vicinity of the tube where the tube is fixed. The mass flowmeter according to any one of items 1 to 3. 5. The mass flow rate according to any one of claims 1 to 4, characterized in that the detection signal from the detection means is fed back to the driving means to control the driving of the tube body. Total.
JP11776085A 1985-05-31 1985-05-31 Mass flowmeter Granted JPS61275621A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP11776085A JPS61275621A (en) 1985-05-31 1985-05-31 Mass flowmeter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP11776085A JPS61275621A (en) 1985-05-31 1985-05-31 Mass flowmeter

Publications (2)

Publication Number Publication Date
JPS61275621A JPS61275621A (en) 1986-12-05
JPH0454895B2 true JPH0454895B2 (en) 1992-09-01

Family

ID=14719643

Family Applications (1)

Application Number Title Priority Date Filing Date
JP11776085A Granted JPS61275621A (en) 1985-05-31 1985-05-31 Mass flowmeter

Country Status (1)

Country Link
JP (1) JPS61275621A (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0749980B2 (en) * 1987-08-20 1995-05-31 トキコ株式会社 Vibration measuring device
DE4138840C2 (en) * 1991-11-26 2003-02-06 Abb Patent Gmbh Holder for a pipe to be flowed through in a mass flow meter
US6606573B2 (en) * 2001-08-29 2003-08-12 Micro Motion, Inc. Sensor apparatus, methods and computer program products employing vibrational shape control

Also Published As

Publication number Publication date
JPS61275621A (en) 1986-12-05

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