JP2000046617A - Coriolis mass flowmeter - Google Patents

Coriolis mass flowmeter

Info

Publication number
JP2000046617A
JP2000046617A JP10217999A JP21799998A JP2000046617A JP 2000046617 A JP2000046617 A JP 2000046617A JP 10217999 A JP10217999 A JP 10217999A JP 21799998 A JP21799998 A JP 21799998A JP 2000046617 A JP2000046617 A JP 2000046617A
Authority
JP
Japan
Prior art keywords
vibration
vibrating tube
tube
vibrating
compensating
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
JP10217999A
Other languages
Japanese (ja)
Inventor
Norikazu Osawa
紀和 大沢
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
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 filed Critical Yokogawa Electric Corp
Priority to JP10217999A priority Critical patent/JP2000046617A/en
Publication of JP2000046617A publication Critical patent/JP2000046617A/en
Pending legal-status Critical Current

Links

Landscapes

  • Measuring Volume Flow (AREA)

Abstract

PROBLEM TO BE SOLVED: To realize a Coriolis mass flowmeter capable of aiming improvement of a mass flow measurement performance by improving insulatability of internal vibration, and simultaneously capable of improving stability of a density measurement performance or a mass flow measurement performance at the time of density change. SOLUTION: This flowmeter is so composed that measurement fluid flows in a vibrating tube 31, and that the vibrating tube 31 is deformedly vibrated by Coriolis force generated by the flow of the measurement fluid and angular vibration of the vibrating tube 31. In this case, this flowmeter is equipped with the vibrating tube 31 in which the measurement fluid flows and which vibrates in a resonance frequency, and plural compensating vibrators 32 having one end connected to the position of a node of the vibration or the periphery thereof of the vibrating tube 31 and having a resonance frequency different from the resonance frequency of the vibrating tube 31. And besides, the compensating vibrators 32 are equipped with compensating vibrator exciters 34, for shaking forcedly in the same frequency as the vibrating tube 31, so as to cancel the vibration of a joint between the compensating vibrators 32 and the vibrating tube 31 or of a fixed point 35 of the vibrating tube 31.

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【発明の属する技術分野】本発明は、内部振動の絶縁性
を向上させて、質量流量測定性能の向上を図りながら、
密度測定性能や、密度変化時の質量流量測定性能の安定
性が向上するコリオリ質量流量計に関するものである。
The present invention relates to a method for improving the mass flow measurement performance by improving the insulation of internal vibrations.
The present invention relates to a Coriolis mass flowmeter having improved density measurement performance and stability of mass flow measurement performance when density changes.

【0002】[0002]

【従来の技術】図5は、従来より一般に使用されている
従来例の構成説明図で、例えば、特開平6−10951
2号の従来例に示されている。図において、振動チュー
ブ1はフランジ2に、両端が取付けられ、内部に測定流
体FLoが流れる。
2. Description of the Related Art FIG. 5 is an explanatory view of the structure of a conventional example generally used in the prior art.
This is shown in the conventional example of No. 2. In the figure, the vibration tube 1 to the flange 2, both ends attached flow measurement fluid FL o therein.

【0003】フランジ2は、管路へ振動チューブ1を取
付けるためのものである。励振器3は、振動チューブ1
の中央部分に設けられ、振動チューブ1を励振する。
[0003] The flange 2 is for attaching the vibration tube 1 to a pipeline. The exciter 3 is a vibration tube 1
To excite the vibrating tube 1.

【0004】振動検出センサ4,5は振動チューブ1の
両側にそれぞれ設けられ、振動チューブ1の振動を検出
する。ハウジング6には、振動チューブ1の両端が固定
されている。
The vibration detecting sensors 4 and 5 are provided on both sides of the vibrating tube 1 and detect the vibration of the vibrating tube 1. Both ends of the vibration tube 1 are fixed to the housing 6.

【0005】以上の構成において、振動チューブ1に測
定流体が流され、励振器3が駆動される。励振器3の振
動方向の角速度『ω』、測定流体の流速『V』(以
下『』で囲まれた記号はベクトル量を表す。)とする
と、
[0005] In the above configuration, the measurement fluid is caused to flow through the vibration tube 1 and the exciter 3 is driven. Assuming that the angular velocity “ω” in the vibration direction of the exciter 3 and the flow velocity “V” of the measurement fluid (hereinafter, a symbol surrounded by “” represents a vector amount),

【0006】Fc=―2m『ω』×『V』 のコリオリ力が働く、コリオリ力に比例した振動の振幅
を測定すれば、質量流量が測定出来る。
The mass flow rate can be measured by measuring the amplitude of the vibration proportional to the Coriolis force where a Coriolis force of Fc = −2 m “ω” × “V” acts.

【0007】しかしながら、この様な装置においては、
振動チューブ1は近似的に両端固定条件で振動するが、
限られた大きさのコリオリ質量流量計では、端点を完全
固定にすることはできず、わずかに振動してしまう。
However, in such an apparatus,
The vibrating tube 1 vibrates approximately under the condition that both ends are fixed.
With a Coriolis mass flowmeter of limited size, the endpoints cannot be completely fixed and will vibrate slightly.

【0008】このように、振動絶縁が不十分だと、以下
のような問題点がある。 (1)Q値が低くなるので、コリオリ質量流量計内部の
振動が不安定になり、励振振動以外の余計な振動ノイズ
の影響を受けやすくなる。
As described above, if the vibration isolation is insufficient, there are the following problems. (1) Since the Q value becomes low, the vibration inside the Coriolis mass flowmeter becomes unstable, and it becomes susceptible to extra vibration noise other than the excitation vibration.

【0009】(2)励振に大きなエネルギーが必要にな
り、消費電力が増加する。 (3)設置方法や、配管応力、温度等の環境変化や外的
要因により、振動の漏れ程度も大きく変わり、振動チュ
ーブ1の振動状況も変化し、零点やスパンが変化しやす
くなる。
(2) Large energy is required for excitation, and power consumption increases. (3) The degree of vibration leakage greatly changes due to the installation method, environmental changes such as piping stress and temperature, and external factors, the vibration state of the vibrating tube 1 also changes, and the zero point and span easily change.

【0010】すなわち、これらの環境変化や外的要因に
対し、弱く、精度の悪いコリオリ流量計になりがちであ
る。
That is, Coriolis flowmeters which are weak and inaccurate with respect to these environmental changes and external factors tend to be formed.

【0011】図6は、この問題点に鑑み、本願出願人が
出願した、先願に係わる特願平9−186431号、発
明の名称「コリオリ質量流量計」である。図において、
図5と同一記号の構成は同一機能を表わす。以下、図5
と相違部分のみ説明する。
FIG. 6 shows a Coriolis mass flowmeter, filed by the applicant of the present invention, and filed by the present applicant in view of this problem. In the figure,
Configurations with the same symbols as those in FIG. 5 represent the same functions. Hereinafter, FIG.
Only the differences will be described.

【0012】振動チューブ11は、測定流体FLoが流
れる直管状の振動チューブである。補償振動体12は、
振動チューブ11に平行に設けられた、少なくとも1個
の補償振動体である。この場合は、1個の補償振動体1
2が使用されている。結合体13は、振動チューブ11
と補償振動体12の振動の節となる個所を連結する。
[0012] the vibration tube 11 is a vibrating tube straight tubular measuring fluid FL o flows. The compensation vibrator 12 is
At least one compensating vibrator provided in parallel with the vibrating tube 11. In this case, one compensation vibrator 1
2 are used. The combined body 13 includes the vibration tube 11
And a portion that serves as a node of vibration of the compensating vibrator 12 are connected.

【0013】励振器14は、振動チューブ11の中央部
分と、補償振動体12の中央部分との間に設けられ、振
動チューブ11と補償振動体12とを励振する。振動検
出センサ15は、振動チューブ11と補償振動体12と
の間に設けられ、振動チューブ11と補償振動体12と
の相対振動を検出する。
The exciter 14 is provided between the central part of the vibration tube 11 and the central part of the compensation vibration body 12, and excites the vibration tube 11 and the compensation vibration body 12. The vibration detection sensor 15 is provided between the vibration tube 11 and the compensation vibration body 12, and detects a relative vibration between the vibration tube 11 and the compensation vibration body 12.

【0014】以上の構成において、振動チューブ11に
測定流体が流され、励振器14が駆動されると、コリオ
リ力が働く、このコリオリ力に比例した振動チューブ1
1の振動の振幅を測定すれば、質量流量が測定出来る。
In the above configuration, when the measurement fluid is flowed through the vibrating tube 11 and the exciter 14 is driven, a Coriolis force acts. The vibrating tube 1 is proportional to the Coriolis force.
By measuring the amplitude of the vibration of No. 1, the mass flow rate can be measured.

【0015】而して、振動チューブ11と補償振動体1
2と結合体13との、振動系の振動の節となる場所で、
振動チューブ11と補償振動体12と結合体13とを、
流量計ハウジング6と接続させることで、振動チューブ
11と補償振動体12と結合体13からなる振動系の振
動を、内部に閉じこめることができる。
Thus, the vibration tube 11 and the compensation vibration body 1
In the place where the joint of the vibration body 2 and the coupling body 13 is a node of the vibration,
The vibration tube 11, the compensation vibration body 12, and the combined body 13
By connecting to the flow meter housing 6, the vibration of the vibration system including the vibration tube 11, the compensation vibration body 12, and the coupling body 13 can be confined inside.

【0016】すなわち、図6に示す如く、X,Y,Z軸
方向を決めると、励振器14により、振動チューブ11
と、補償振動体12は、図に示したようにY方向で互い
に逆向きに振動する。この振動系は、ちょうど結合体1
3が振動の節となるように作られるので、励振状態であ
っても、結合体13では、ほぼ動きがなくなる。
That is, as shown in FIG. 6, when the directions of the X, Y, and Z axes are determined, the exciter 14
The compensating vibrator 12 vibrates in the Y direction in opposite directions as shown in the figure. This vibration system is just
3 is formed so as to be a node of vibration, so that even in the excited state, the combined body 13 hardly moves.

【0017】[0017]

【発明が解決しようとする課題】しかしながら、図6の
先願例においては、振動絶縁に関しては、改善が図られ
る。しかし、ひとつの振動系内部に、補償振動体12が
存在するので、測定流体FLoの密度が変化したとき
に、振動チューブ11と、補償振動体12との振動バラ
ンスが崩れてしまい、振動絶縁性能が低下する。
However, in the prior application of FIG. 6, the vibration isolation is improved. However, within one of the vibration system, since the compensation vibrator 12 is present, when the density of the measuring fluid FL o is changed, the vibration tube 11, the vibration balance collapses the compensation vibrator 12, vibration isolation Performance decreases.

【0018】また補償振動体12は、振動チューブ11
と補償振動体12とで構成される一体の振動系として働
き、この一体の振動系全てが、共振状態振動をするのが
一般的であっる。
The compensating vibrator 12 includes a vibrating tube 11
Generally, the integrated vibration system functions as an integrated vibration system composed of the compensation vibration body 12 and the integrated vibration system.

【0019】例えば、測定流体FLoの密度変化がある
と、振動系全体の共振周波数が緩やかに変化する。密度
変化に直接関係ある振動チューブ11以外に、密度変化
とは無関係な補償振動体12があり、それらが一体の振
動系として振動する。
[0019] For example, when there is a change in density measurement fluid FL o, the resonant frequency of the whole vibration system changes gradually. In addition to the vibrating tube 11 that is directly related to the density change, there is a compensation vibrator 12 that is not related to the density change, and they vibrate as an integrated vibration system.

【0020】従って、振動チューブ11だけの場合に比
べ、測定流体FLoの密度が変わった時の共振周波数の
変化は緩やかになり、測定流体FLoの密度と共振周波
数の関係は非線形的になる。
[0020] Therefore, compared with the case of only the vibration tube 11, changes in the resonance frequency when the density of the measuring fluid FL o has changed becomes gradual, the relationship of the density and the resonance frequency of the measurement fluid FL o becomes nonlinear .

【0021】密度変化に対する共振周波数の変化率が小
さいので、S/N比が劣り、高分解能での密度計測が困
難であっる。また、非線形的なので高精度で安定した密
度計測が困難である。
Since the change rate of the resonance frequency with respect to the density change is small, the S / N ratio is inferior, and it is difficult to measure the density with high resolution. Further, it is difficult to measure the density with high accuracy and stability because of the nonlinearity.

【0022】本発明は、この問題点を解決するものであ
る。本発明の目的は、内部振動の絶縁性を向上させて、
質量流量測定性能の向上を図りながら、密度測定性能
や、密度変化時の質量流量測定性能の安定性が向上する
コリオリ質量流量計を提供するにある。
The present invention solves this problem. An object of the present invention is to improve the insulation of internal vibration,
It is an object of the present invention to provide a Coriolis mass flowmeter that improves the density measurement performance and the stability of the mass flow measurement performance when the density changes while improving the mass flow measurement performance.

【0023】[0023]

【課題を解決するための手段】この目的を達成するため
に、本発明は、 (1)振動チューブ内に測定流体が流れ、該測定流体の
流れと前記振動チューブの角振動によって生じるコリオ
リ力により、該振動チューブを変形振動させるコリオリ
質量流量計において、前記測定流体が流れ共振周波数で
振動する振動チューブと、この振動チューブの振動の節
となる位置あるいはその近傍に一端が接続され前記振動
チューブの共振周波数とは異なる共振周波数を有する複
数個の補償振動体と、この補償振動体と前記振動チュー
ブとの連結点或いは前記振動チューブの固定点の振動を
打ち消すようにこの補償振動体に前記振動チューブと同
一周波数で強制加振する補償振動体励振器とを具備した
ことを特徴とするコリオリ質量流量計。 (2)前記振動チューブの前記固定点近傍に設けられた
固定点振動検出センサと、この固定点振動検出センサの
検出出力が最小になるように前記補償振動体励振器の加
振力の大きさを制御する制御回路とを具備したことを特
徴とする(1)記載のコリオリ質量流量計。を構成した
ものである。
In order to achieve the above object, the present invention provides: (1) a measuring fluid flowing in a vibrating tube, and a flow of the measuring fluid and a Coriolis force generated by angular vibration of the vibrating tube; In a Coriolis mass flowmeter for deforming and vibrating the vibrating tube, a vibrating tube in which the measurement fluid flows and vibrates at a resonance frequency, and one end of which is connected to a position or a vicinity of a vibration node of the vibrating tube, A plurality of compensating vibrators having a resonance frequency different from the resonance frequency, and the vibrating tube being attached to the compensating vibrating body so as to cancel vibration at a connection point between the compensating vibrating body and the vibrating tube or at a fixed point of the vibrating tube. And a compensating vibrator exciter for forcibly exciting at the same frequency. (2) A fixed-point vibration detection sensor provided near the fixed point of the vibrating tube, and the magnitude of the excitation force of the compensating vibrator exciter so that the detection output of the fixed-point vibration detection sensor is minimized. A Coriolis mass flowmeter according to (1), further comprising a control circuit for controlling the mass flow rate. It is what constituted.

【0024】[0024]

【作用】以上の構成において、振動チューブに測定流体
が流され、励振器が駆動されると、コリオリ力が働く、
このコリオリ力に比例した振動の振幅を測定すれば、質
量流量が測定出来る。
In the above construction, when the measuring fluid is flowed through the vibrating tube and the exciter is driven, Coriolis force acts.
By measuring the amplitude of the vibration proportional to the Coriolis force, the mass flow rate can be measured.

【0025】しかして、振動チューブは、1次モード共
振状態で振動するように、励振器で加振される。
Thus, the vibrating tube is excited by the exciter so as to vibrate in the first mode resonance state.

【0026】一方、補償振動体は、振動チューブの振動
周波数と全く等しい周波数で、かつ逆位相に振動するよ
うに、補償振動体励振器によって、加振される。
On the other hand, the compensating vibrator is vibrated by the compensating vibrator exciter so as to vibrate at a frequency exactly equal to the vibration frequency of the vibrating tube and in the opposite phase.

【0027】補償振動体励振器は、振動検出センサの出
力をもとに、それと同周波数の信号を作成して、加振力
を発生する。
The compensating vibrator exciter generates a signal having the same frequency as the signal based on the output of the vibration detecting sensor to generate an exciting force.

【0028】最終的には、振動チューブと補償振動体と
が、逆方向に振動して、打ち消し合うことで、連結部、
あるいは、固定点で、振動がほとんどなくなるように、
補償振動体を加振させることを目標とする。
Finally, the vibration tube and the compensating vibrator vibrate in opposite directions and cancel each other, so that the connecting portion,
Alternatively, at the fixed point, so that there is almost no vibration,
The goal is to vibrate the compensating vibrator.

【0029】而して、振動チューブと補償振動体との、
振動系の振動の節となる場所で、振動チューブと補償振
動体とを、流量計ハウジングに接続させることで、振動
チューブと補償振動体と結合体からなる振動系の振動
を、内部に閉じこめるようにした。以下、実施例に基づ
き詳細に説明する。
Thus, the vibration tube and the compensation vibration body
By connecting the vibrating tube and the compensating vibrator to the flowmeter housing at a location that is a node of the vibration of the vibrating system, the vibration of the vibrating system consisting of the vibrating tube, the compensating vibrator, and the combined body can be confined inside. I made it. Hereinafter, a detailed description will be given based on embodiments.

【0030】[0030]

【発明の実施の形態】図1は、本発明の一実施例の要部
構成説明図である。図において、図6と同一記号の構成
は同一機能を表わす。以下、図6と相違部分のみ説明す
る。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS FIG. 1 is an explanatory diagram of a main part configuration of an embodiment of the present invention. In the figure, the configuration of the same symbol as FIG. 6 represents the same function. Hereinafter, only differences from FIG. 6 will be described.

【0031】図において、振動チューブ31は、測定流
体FLoが流れ共振周波数で振動する振動チューブであ
る。
[0031] In Figure, the vibration tube 31 is a vibrating tube measuring fluid FL o flows oscillates at the resonance frequency.

【0032】補償振動体32は、振動チューブ31の振
動の節となる位置、あるいは、その近傍に一端が連結接
続33され、振動チューブ31の共振周波数とは異なる
共振周波数を有する複数個の補償振動体である。
One end of the compensating vibrator 32 is connected or connected 33 at or near a node of vibration of the vibrating tube 31, and a plurality of compensating vibrators having a resonance frequency different from the resonance frequency of the vibrating tube 31 are provided. Body.

【0033】この場合は、2個の補償振動体32が使用
されている。補償振動体励振器34は、補償振動体32
と振動チューブ31との連結点33、或いは、振動チュ
ーブ31の固定点35の振動を、打ち消すように、補償
振動体32に振動チューブ31と同一周波数で強制加振
する。
In this case, two compensation vibrators 32 are used. The compensating vibrator exciter 34 includes the compensating vibrating body 32
A vibration is applied to the compensation vibrator 32 at the same frequency as the vibration tube 31 so as to cancel the vibration at the connection point 33 between the vibration tube 31 and the fixed point 35 of the vibration tube 31.

【0034】以上の構成において、図2に示す如く、振
動チューブ31は、1次モード共振状態で振動するよう
に、励振器14で加振される。
In the above configuration, as shown in FIG. 2, the vibration tube 31 is vibrated by the exciter 14 so as to vibrate in a first-order mode resonance state.

【0035】一方、補償振動体32は、振動チューブ3
1の振動周波数と全く等しい周波数で、かつ逆位相(図
2に示したように連結部33にて振動を打ち消し合う、
振動の節になるように逆方向に振動する。)に振動する
ように、補償振動体励振器34によって、加振される。
On the other hand, the compensation vibrator 32 is
1 and at the opposite phase (the vibrations cancel each other out at the connecting portion 33 as shown in FIG.
Vibrates in the opposite direction to become a node of vibration. ) Is vibrated by the compensating vibrator exciter 34 so as to vibrate.

【0036】補償振動体励振器34は、振動検出センサ
15の出力をもとに、それと同周波数の信号を作成し
て、加振力を発生する。位相に関しては、振動チューブ
31が共振状態であるのに対し、補償振動体32は非共
振状態である。
The compensating vibrator exciter 34 generates a signal having the same frequency as that of the output of the vibration detecting sensor 15 based on the output of the vibration detecting sensor 15 to generate an exciting force. As for the phase, the vibration tube 31 is in a resonance state, while the compensation vibration body 32 is in a non-resonance state.

【0037】従って、励振器14と、補償振動体励振器
34の加振力は90度異なる位相で振動させる必要があ
る。
Therefore, the exciting forces of the exciter 14 and the compensating vibrator exciter 34 need to be oscillated at phases different from each other by 90 degrees.

【0038】最終的には、振動チューブ31と補償振動
体32とが、逆方向に振動して、打ち消し合うことで、
連結部33、あるいは、固定点35で、振動がほとんど
なくなるように、補償振動体34を加振させることを目
標とする。
Finally, the vibrating tube 31 and the compensating vibrating body 32 vibrate in opposite directions and cancel each other,
The purpose is to vibrate the compensating vibrator 34 so that the vibration is almost eliminated at the connecting portion 33 or the fixed point 35.

【0039】この結果、本発明では、基本的には、振動
チューブ31だけの振動系で、共振状態が形成できる。
補償振動体のような、余計な質量が振動系に存在しない
ので、測定流体FLoの密度が変化すると共振周波数も
大きく変化し、測定流体FLoの密度と共振周波数の関
係は、より線形的にできる。
As a result, in the present invention, a resonance state can be basically formed by a vibration system including only the vibration tube 31.
Compensation as a vibrating body, since the extra weight does not exist in the vibration system, the resonance frequency and the density change in the measured fluid FL o be greatly changed, the relationship between the density and the resonance frequency of the measurement fluid FL o, more linear Can be.

【0040】測定流体FLoの密度計測は、共振周波数
から求める。従って、密度変化に対する共振周波数の変
化率が大きければ、S/N比に優れ、高分解能で密度計
測が可能になるコリオリ質量流量計が得られる。
[0040] Density measurements of the measuring fluid FL o is determined from the resonant frequency. Therefore, if the change rate of the resonance frequency with respect to the density change is large, a Coriolis mass flowmeter having an excellent S / N ratio and capable of measuring the density with high resolution can be obtained.

【0041】また、線形性が高まることで、より高精度
で安定した密度計測が可能になる。さらに、質量流量の
密度補正や体積流量測定には、密度計測値を用いる。従
って、質量流量や体積流量測定も高精度、高安定性が期
待できるコリオリ質量流量計が得られる。
Further, by increasing the linearity, more accurate and stable density measurement becomes possible. Further, the density measurement value is used for density correction of the mass flow rate and measurement of the volume flow rate. Therefore, a Coriolis mass flowmeter that can expect high accuracy and high stability in mass flow rate and volume flow rate measurement can be obtained.

【0042】共振状態となる振動系が振動チューブ31
のみであっても、非共振状態にある補償振動体32に、
共振振動をしている振動チューブ31と同期させたアク
ティブな強制加振をすることによって、補償振動体32
を有効な振動状態にさせ、それらの連結部分33では、
振動がキャンセルしあって、外部との振動絶縁を可能に
することができる。
The vibrating system in the resonance state is the vibrating tube 31.
Even if only the compensation vibrator 32 in the non-resonant state,
By performing active forced vibration synchronized with the vibration tube 31 that is performing resonant vibration, the compensation vibrator 32 is
To an effective vibration state, and at their connecting portions 33,
The vibrations cancel each other, and the vibration isolation from the outside can be made possible.

【0043】振動絶縁を実現し、振動系の振動を内部に
閉じこめることで、以下の利点が生まれる。 (1)内部振動系は高Q値を実現でき、外部ノイズが加
わってもその影響が相対的に少なく、振動が安定なの
で、外部振動ノイズに強いコリオリ質量流量計が得られ
る。
By realizing vibration isolation and confining the vibration of the vibration system inside, the following advantages are obtained. (1) Since the internal vibration system can realize a high Q value, the influence of external noise is relatively small even if external noise is applied, and the vibration is stable, a Coriolis mass flowmeter resistant to external vibration noise can be obtained.

【0044】(2)少ないエネルギで、安定した励振を
実現できるので、低消費電流のコリオリ質量流量計が得
られる。
(2) Since stable excitation can be realized with small energy, a Coriolis mass flowmeter with low current consumption can be obtained.

【0045】(3)外部への振動エネルギの散逸量が変
化したり、上下流で散逸量のバランスが崩れると、内部
の振動系に影響が及び、ゼロ点やスパンが変動してしま
う。本発明では、常に内部に振動を閉じ込める事が出来
るので、その心配がなく、高精度なコリオリ質量流量計
が得られる。
(3) If the amount of vibration energy dissipated to the outside changes, or if the balance of the amount dissipated upstream and downstream is disturbed, the internal vibration system is affected, and the zero point and span fluctuate. In the present invention, the vibration can always be confined inside, so that there is no need to worry about this, and a highly accurate Coriolis mass flowmeter can be obtained.

【0046】図3は本発明の他の実施例の要部構成説明
図である。本実施例において、固定点振動検出センサ4
1は、振動チューブ31の固定点35近傍に設けられて
いる。
FIG. 3 is an explanatory diagram of a main part configuration of another embodiment of the present invention. In this embodiment, the fixed point vibration detection sensor 4
1 is provided near the fixed point 35 of the vibration tube 31.

【0047】制御回路42は、図4に示す如く、固定点
振動検出センサ41の検出出力が最小になるように、固
定点振動検出センサ41の検出出力信号に基づき、補償
振動体励振器34の加振力の大きさを制御する。
As shown in FIG. 4, the control circuit 42 controls the compensation vibrator exciter 34 based on the detection output signal of the fixed-point vibration detection sensor 41 so that the detection output of the fixed-point vibration detection sensor 41 is minimized. Controls the magnitude of the excitation force.

【0048】この結果、測定流体FLoの密度や温度変
化等があっても、補償振動体32の振動の大きさを調整
することで、振動チューブ3と流量計ハウジング6の固
定点35の付近の振動を、常にゼロあるいは、ゼロに近
い値に制御することが可能となる。
The vicinity of this result, even if the density or the temperature change or the like of the measurement fluid FL o, by adjusting the magnitude of the vibration of the compensation vibrator 32, the fixed point 35 of the vibration tube 3 and the flow meter housing 6 Can always be controlled to zero or a value close to zero.

【0049】すなわち、環境変化に安定で、より高いレ
ベルで振動絶縁が可能になるので、更に、外部振動ノイ
ズに強く、低消費電流で、高精度なコリオリ質量流量計
が得られる。
That is, since the vibration isolation can be performed at a higher level, which is stable to environmental changes, a Coriolis mass flowmeter which is resistant to external vibration noise, consumes low current, and has high accuracy can be obtained.

【0050】[0050]

【発明の効果】以上説明したように、本発明の請求項1
によれば、基本的には、振動チューブだけの振動系で、
共振状態が形成できる。補償振動体のような、余計な質
量が振動系に存在しないので、測定流体の密度が変化す
ると共振周波数も大きく変化し、測定流体の密度と共振
周波数の関係は、より線形的に出来る。
As described above, according to the first aspect of the present invention,
According to, basically, the vibration system only vibration tube,
A resonance state can be formed. Since there is no extra mass in the vibration system, such as a compensating vibrator, when the density of the measurement fluid changes, the resonance frequency also changes greatly, and the relationship between the density of the measurement fluid and the resonance frequency can be made more linear.

【0051】測定流体の密度計測は、共振周波数から求
める。従って、密度変化に対する共振周波数の変化率が
大きければ、S/N比に優れ、高分解能で密度計測が可
能になるコリオリ質量流量計が得られる。
The density of the measurement fluid is determined from the resonance frequency. Therefore, if the change rate of the resonance frequency with respect to the density change is large, a Coriolis mass flowmeter having an excellent S / N ratio and capable of measuring the density with high resolution can be obtained.

【0052】また、線形性が高まることで、より高精度
で安定した密度計測が可能になる。さらに、質量流量の
密度補正や体積流量測定には、密度計測値を用いる。従
って、質量流量や体積流量測定も高精度、高安定性が期
待できるコリオリ質量流量計が得られる。
In addition, the increased linearity enables more accurate and stable density measurement. Further, the density measurement value is used for density correction of the mass flow rate and measurement of the volume flow rate. Therefore, a Coriolis mass flowmeter that can expect high accuracy and high stability in mass flow rate and volume flow rate measurement can be obtained.

【0053】共振状態となる振動系が振動チューブのみ
であっても、非共振状態にある補償振動体に、共振振動
をしている振動チューブと同期させたアクティブな強制
加振をすることによって、補償振動体を有効な振動状態
にさせ、それらの連結部分では、振動がキャンセルしあ
って、外部との振動絶縁を可能にすることが出来る。
Even if the vibration system that is in the resonance state is only the vibration tube, it is possible to apply active forced vibration synchronized with the vibration tube that is performing resonance vibration to the non-resonant compensation vibration body, The compensating vibrator is brought into an effective vibrating state, and the vibrations are canceled at the connecting portions thereof, so that the vibration can be isolated from the outside.

【0054】振動絶縁を実現し、振動系の振動を内部に
閉じこめることで、以下の利点が生まれる。 (1)内部振動系は高Q値を実現でき、外部ノイズが加
わってもその影響が相対的に少なく、振動が安定なの
で、外部振動ノイズに強いコリオリ質量流量計が得られ
る。
By realizing vibration isolation and confining the vibration of the vibration system inside, the following advantages are obtained. (1) Since the internal vibration system can realize a high Q value, the influence of external noise is relatively small even if external noise is applied, and the vibration is stable, a Coriolis mass flowmeter resistant to external vibration noise can be obtained.

【0055】(2)少ないエネルギで、安定した励振を
実現できるので、低消費電流のコリオリ質量流量計が得
られる。
(2) Since stable excitation can be realized with a small amount of energy, a Coriolis mass flowmeter with low current consumption can be obtained.

【0056】(3)外部への振動エネルギの散逸量が変
化したり、上下流で散逸量のバランスが崩れると、内部
の振動系に影響が及び、ゼロ点やスパンが変動してしま
う。本発明では、常に内部に振動を閉じ込める事が出来
るので、その心配がなく、高精度なコリオリ質量流量計
が得られる。
(3) If the amount of vibration energy dissipated to the outside changes, or if the balance of the amount dissipated upstream and downstream is disturbed, the internal vibration system is affected and the zero point and span fluctuate. In the present invention, the vibration can always be confined inside, so that there is no need to worry about this, and a highly accurate Coriolis mass flowmeter can be obtained.

【0057】本発明の請求項2によれば、制御回路によ
り、固定点振動検出センサの検出出力が最小になるよう
に、固定点振動検出センサの検出出力信号に基づき、補
償振動体励振器の加振力の大きさを制御するようにし
た。
According to the second aspect of the present invention, the control circuit controls the compensation vibrator exciter based on the detection output signal of the fixed point vibration detection sensor so that the detection output of the fixed point vibration detection sensor is minimized. The magnitude of the excitation force is controlled.

【0058】この結果、測定流体の密度や温度変化等が
あっても、補償振動体の振動の大きさを調整すること
で、振動チューブと流量計ハウジングの固定点の付近の
振動を、常にゼロあるいは、ゼロに近い値に制御するこ
とが可能となる。
As a result, even if there is a change in the density or temperature of the measurement fluid, the vibration near the fixed point between the vibrating tube and the flow meter housing is always reduced to zero by adjusting the magnitude of the vibration of the compensating vibrator. Alternatively, it can be controlled to a value close to zero.

【0059】すなわち、環境変化に安定で、より高いレ
ベルで振動絶縁が可能になるので、更に、外部振動ノイ
ズに強く、低消費電流で、高精度なコリオリ質量流量計
が得られる。
That is, since the vibration isolation can be performed at a higher level, which is stable against environmental changes, a Coriolis mass flowmeter which is resistant to external vibration noise, consumes low current, and has high accuracy can be obtained.

【0060】従って、本発明によれば、内部振動の絶縁
性を向上させて、質量流量測定性能の向上を図りなが
ら、密度測定性能や、密度変化時の質量流量測定性能の
安定性が向上するコリオリ質量流量計を実現することが
出来る。
Therefore, according to the present invention, the density measurement performance and the stability of the mass flow measurement performance at the time of density change are improved while improving the insulation of the internal vibration and improving the mass flow measurement performance. A Coriolis mass flow meter can be realized.

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

【図1】本発明の一実施例の要部構成説明図である。FIG. 1 is an explanatory diagram of a main part configuration of an embodiment of the present invention.

【図2】図1の動作説明図である。FIG. 2 is an operation explanatory diagram of FIG. 1;

【図3】本発明の他の実施例の要部構成説明図である。FIG. 3 is an explanatory diagram of a main part configuration of another embodiment of the present invention.

【図4】図3の要部構成説明図である。FIG. 4 is an explanatory diagram of a main part configuration of FIG. 3;

【図5】従来より一般に使用されている従来例の構成説
明図である。
FIG. 5 is an explanatory diagram of a configuration of a conventional example generally used in the related art.

【図6】従来より一般に使用されている他の従来例の構
成説明図である。
FIG. 6 is an explanatory view of the configuration of another conventional example generally used in the prior art.

【符号の説明】[Explanation of symbols]

2 フランジ 6 ハウジング 14 励振器 15 振動検出センサ 31 振動チューブ 32 補償振動体 33 連結部 34 補償振動体励振器 35 固定点 41 固定点振動検出センサ 42 制御回路 2 Flange 6 Housing 14 Exciter 15 Vibration detection sensor 31 Vibration tube 32 Compensating vibrator 33 Connecting part 34 Compensating vibrator exciter 35 Fixed point 41 Fixed point vibration detecting sensor 42 Control circuit

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】振動チューブ内に測定流体が流れ、該測定
流体の流れと前記振動チューブの角振動によって生じる
コリオリ力により、該振動チューブを変形振動させるコ
リオリ質量流量計において、 前記測定流体が流れ共振周波数で振動する振動チューブ
と、 この振動チューブの振動の節となる位置あるいはその近
傍に一端が接続され前記振動チューブの共振周波数とは
異なる共振周波数を有する複数個の補償振動体と、 この補償振動体と前記振動チューブとの連結点或いは前
記振動チューブの固定点の振動を打ち消すようにこの補
償振動体に前記振動チューブと同一周波数で強制加振す
る補償振動体励振器とを具備したことを特徴とするコリ
オリ質量流量計。
1. A Coriolis mass flowmeter for deforming and vibrating a vibrating tube by a flow of a measuring fluid in a vibrating tube and a Coriolis force generated by the flow of the measuring fluid and an angular vibration of the vibrating tube. A vibrating tube that vibrates at a resonance frequency, a plurality of compensation vibrators having one end connected to or near a position serving as a node of vibration of the vibration tube and having a resonance frequency different from the resonance frequency of the vibration tube; The compensating vibrator is provided with a compensating vibrator exciter that forcibly vibrates at the same frequency as the vibrating tube so as to cancel vibration at a connecting point between the vibrating body and the vibrating tube or a fixed point of the vibrating tube. Features a Coriolis mass flow meter.
【請求項2】前記振動チューブの前記固定点近傍に設け
られた固定点振動検出センサと、 この固定点振動検出センサの検出出力が最小になるよう
に前記補償振動体励振器の加振力の大きさを制御する制
御回路とを具備したことを特徴とする請求項1記載のコ
リオリ質量流量計。
2. A fixed-point vibration detecting sensor provided near the fixed point of the vibrating tube; and a vibrating force of the compensating vibrator exciter so that a detection output of the fixed-point vibration detecting sensor is minimized. The Coriolis mass flowmeter according to claim 1, further comprising a control circuit for controlling the size.
JP10217999A 1998-07-31 1998-07-31 Coriolis mass flowmeter Pending JP2000046617A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP10217999A JP2000046617A (en) 1998-07-31 1998-07-31 Coriolis mass flowmeter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP10217999A JP2000046617A (en) 1998-07-31 1998-07-31 Coriolis mass flowmeter

Publications (1)

Publication Number Publication Date
JP2000046617A true JP2000046617A (en) 2000-02-18

Family

ID=16713044

Family Applications (1)

Application Number Title Priority Date Filing Date
JP10217999A Pending JP2000046617A (en) 1998-07-31 1998-07-31 Coriolis mass flowmeter

Country Status (1)

Country Link
JP (1) JP2000046617A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN113710992A (en) * 2019-04-30 2021-11-26 恩德斯+豪斯流量技术股份有限公司 Measuring device and method for characterizing a non-uniform flowable medium
CN118111540A (en) * 2024-04-30 2024-05-31 上海宝宬冶金科技有限公司 AI intelligent flowmeter for blast furnace leak detection

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN113710992A (en) * 2019-04-30 2021-11-26 恩德斯+豪斯流量技术股份有限公司 Measuring device and method for characterizing a non-uniform flowable medium
CN113710992B (en) * 2019-04-30 2024-05-17 恩德斯+豪斯流量技术股份有限公司 Measuring device and method for characterizing non-uniform flowable media
CN118111540A (en) * 2024-04-30 2024-05-31 上海宝宬冶金科技有限公司 AI intelligent flowmeter for blast furnace leak detection

Similar Documents

Publication Publication Date Title
CA1234705A (en) Angular velocity sensor
US6164140A (en) Solid state transducer for Coriolis flowmeter
US4957005A (en) Coriolis-type flowmeter
JP2004538449A (en) Vibration transducer
JP3565588B2 (en) Vibration type measuring instrument
JP3547527B2 (en) Mass flow meter
KR20010030791A (en) Combined pickoff and oscillatory driver for use in coriolis flowmeters and method of operating the same
JP3327325B2 (en) Coriolis mass flowmeter
JPH04291119A (en) Colioris mass flowmeter
JP2012510072A (en) Method and apparatus for vibrating a flow tube of a vibratory flow meter
US6363794B1 (en) Method and apparatus for Coriolis flowmeter having an accuracy enhancing balance bar
JP2000046617A (en) Coriolis mass flowmeter
JP3336927B2 (en) Coriolis mass flowmeter
JP2000046613A (en) Coriolis mass flowmeter
JP2012526987A (en) Flow meter with a balanced reference member
US20010045133A1 (en) Coriolis flowmeter
JP3757559B2 (en) Coriolis mass flow meter
JPH1123341A (en) Coriolis mass flowmeter
JPH10104040A (en) Mass flowmeter converter
JP3555652B2 (en) Coriolis mass flowmeter
JP2000055710A (en) Coriolis mass flowmeter
JP2951460B2 (en) Coriolis mass flowmeter
JPH08313321A (en) Coriolis mass flow meter
JP2000111380A (en) Coriolis-type mass flowmeter
US20010049971A1 (en) Coriolis flowmeter

Legal Events

Date Code Title Description
A621 Written request for application examination

Free format text: JAPANESE INTERMEDIATE CODE: A621

Effective date: 20041224

A977 Report on retrieval

Effective date: 20061221

Free format text: JAPANESE INTERMEDIATE CODE: A971007

A131 Notification of reasons for refusal

Effective date: 20070206

Free format text: JAPANESE INTERMEDIATE CODE: A131

A521 Written amendment

Effective date: 20070502

Free format text: JAPANESE INTERMEDIATE CODE: A523

A02 Decision of refusal

Free format text: JAPANESE INTERMEDIATE CODE: A02

Effective date: 20070911

A521 Written amendment

Free format text: JAPANESE INTERMEDIATE CODE: A523

Effective date: 20071129

A911 Transfer of reconsideration by examiner before appeal (zenchi)

Free format text: JAPANESE INTERMEDIATE CODE: A911

Effective date: 20080312

TRDD Decision of grant or rejection written
A01 Written decision to grant a patent or to grant a registration (utility model)

Free format text: JAPANESE INTERMEDIATE CODE: A01

Effective date: 20080425

A01 Written decision to grant a patent or to grant a registration (utility model)

Free format text: JAPANESE INTERMEDIATE CODE: A01

A61 First payment of annual fees (during grant procedure)

Effective date: 20080523

Free format text: JAPANESE INTERMEDIATE CODE: A61

R150 Certificate of patent (=grant) or registration of utility model

Free format text: JAPANESE INTERMEDIATE CODE: R150

FPAY Renewal fee payment (prs date is renewal date of database)

Year of fee payment: 3

Free format text: PAYMENT UNTIL: 20110530

FPAY Renewal fee payment (prs date is renewal date of database)

Year of fee payment: 4

Free format text: PAYMENT UNTIL: 20120530

FPAY Renewal fee payment (prs date is renewal date of database)

Year of fee payment: 5

Free format text: PAYMENT UNTIL: 20130530

FPAY Renewal fee payment (prs date is renewal date of database)

Free format text: PAYMENT UNTIL: 20140530

Year of fee payment: 6

R250 Receipt of annual fees

Free format text: JAPANESE INTERMEDIATE CODE: R250