JPH032814Y2 - - Google Patents

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Publication number
JPH032814Y2
JPH032814Y2 JP18954682U JP18954682U JPH032814Y2 JP H032814 Y2 JPH032814 Y2 JP H032814Y2 JP 18954682 U JP18954682 U JP 18954682U JP 18954682 U JP18954682 U JP 18954682U JP H032814 Y2 JPH032814 Y2 JP H032814Y2
Authority
JP
Japan
Prior art keywords
fluid
measured
magnetic flux
eddy current
guide tube
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
JP18954682U
Other languages
Japanese (ja)
Other versions
JPS5992816U (en
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 filed Critical
Priority to JP18954682U priority Critical patent/JPS5992816U/en
Publication of JPS5992816U publication Critical patent/JPS5992816U/en
Application granted granted Critical
Publication of JPH032814Y2 publication Critical patent/JPH032814Y2/ja
Granted legal-status Critical Current

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Description

【考案の詳細な説明】 本考案は、導電性を有する被測定流体の流速を
被測定流体中に発生する渦電流に基づいて測定す
る渦電流式流速計の改良に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an improvement in an eddy current type current meter that measures the flow velocity of a conductive fluid to be measured based on eddy currents generated in the fluid to be measured.

第1図は、この種の装置の検出部を構成する検
出ユニツトDETの一例を示す構成説明図であつ
てCBはコイルボビン、WEXはコイルボビンCBに
巻回された励磁コイル、WD1,WD2は励磁コイル
WEXを挾むようにしてコイルボビンCBに巻回さ
れた検出コイルである。
FIG. 1 is a configuration explanatory diagram showing an example of a detection unit DET constituting the detection section of this type of device, in which CB is a coil bobbin, W EX is an excitation coil wound around the coil bobbin CB, W D1 , W D2 is the excitation coil
This is a detection coil wound around a coil bobbin CB so as to sandwich W EX .

このように構成された検出ユニツトDETを、
コイルボビンCBの中心軸が導電性の被測定流体
の流れの方向Fと一致するように流体中に配置さ
れた案内管(図示せず)に挿入し、励磁コイル
WEXに交流信号を加えると、この流体中に渦電流
が発生する。なお、被測定流体によつては、案内
管に挿入することなく、直接被測定流体中に挿入
することもある。この渦電流は、励磁コイルWEX
によつてできる磁束φによるものと、磁束φと流
体の流速とのベクトル積に対応した起電力による
ものとに大別できる。そして、流体がある流速で
移動すると、後者の渦電流にしたがつてできる新
しい磁束が励磁コイルWEXによつてできている主
磁束φと相互に干渉し合い、励磁コイルWEX付近
の磁束分布は第2実線φに示すような形状から点
線φ′に示すような形状に歪む。ここで、磁束分布
が歪む量Δφは被測定流体の流速に対応する。検
出コイルWD1,WD2には、これと鎖交する磁束に
対応した信号e1,e2が発生し、両信号e1,e2の差
を演算することによつて磁束分布の歪み量Δφ、
すなわち被測定流体の流速を求めることができ
る。
The detection unit DET configured in this way is
Insert the coil bobbin CB into a guide tube (not shown) placed in the fluid so that the center axis of the coil bobbin CB matches the flow direction F of the conductive fluid to be measured.
When an alternating current signal is applied to W EX , eddy currents are generated in this fluid. Note that depending on the fluid to be measured, the probe may be inserted directly into the fluid to be measured without being inserted into the guide tube. This eddy current is caused by the excitation coil W EX
It can be roughly divided into two types: one is caused by the magnetic flux φ generated by the magnetic flux φ, and the other is caused by an electromotive force corresponding to the vector product of the magnetic flux φ and the flow velocity of the fluid. When the fluid moves at a certain flow velocity, the new magnetic flux generated by the latter eddy current mutually interferes with the main magnetic flux φ created by the exciting coil W EX , and the magnetic flux distribution near the exciting coil W EX occurs. is distorted from the shape shown by the second solid line φ to the shape shown by the dotted line φ'. Here, the amount Δφ by which the magnetic flux distribution is distorted corresponds to the flow velocity of the fluid to be measured. Signals e 1 and e 2 corresponding to the magnetic flux interlinked with the detection coils W D1 and W D2 are generated, and the amount of distortion in the magnetic flux distribution can be determined by calculating the difference between the two signals e 1 and e 2 . Δφ,
In other words, the flow velocity of the fluid to be measured can be determined.

ところで、従来、このような検出ユニツトと外
部回路とを接続するにあたつては、第3図に示す
ように各コイル毎にツイスト線TWを用い、これ
らツイスト線相互を固着することなくフレキシブ
ル管FTに挿入し、このフレキシブル管FTを案内
管WL内に挿入することが行われている。
By the way, conventionally, when connecting such a detection unit to an external circuit, a twisted wire TW is used for each coil as shown in Fig. 3, and these twisted wires are connected to a flexible tube without being fixed to each other. FT, and this flexible tube FT is inserted into the guide tube WL.

しかし、このような構成によれば、ツイスト線
によりある程度の電磁誘導ノイズは低減できるも
のの、ツイスト線相互間の位置関係が被測定流体
の温度変化による構成部材の膨張、収縮や被測定
流体の流体振動による案内管WLへの押付力の経
時変化などによつて変化することから、残留電磁
誘導ノイズの大きさも変化することになり、高分
解能が得にくい。
However, with such a configuration, although the twisted wires can reduce electromagnetic induction noise to some extent, the positional relationship between the twisted wires may cause expansion or contraction of the constituent members due to temperature changes in the fluid to be measured, or the fluid flow of the fluid to be measured. Since the pressing force on the guide tube WL due to vibration changes over time, the magnitude of the residual electromagnetic induction noise also changes, making it difficult to obtain high resolution.

本考案は、このような従来の欠点を解決したも
のであつて、検出部の各コイルへのリード線とし
て金属シースツイスト線を用い、これらリード線
の金属シース相互を固着したことを特徴とする。
The present invention solves these conventional drawbacks, and is characterized by using metal sheath twisted wires as lead wires to each coil of the detection section, and fixing the metal sheaths of these lead wires to each other. .

以下、図面を用いて詳細に説明する。 Hereinafter, it will be explained in detail using the drawings.

第4図は、本考案の一実施例を示す構成説明図
であつて、第3図と同等部分には同一符号を付し
ている。
FIG. 4 is a configuration explanatory diagram showing one embodiment of the present invention, and the same parts as in FIG. 3 are given the same reference numerals.

第4図において、STWは金属シースツイスト
線であつて、これらツイスト線STWの金属シー
ス相互は例えばロウ付けにより固着され一体化さ
れている。このようにして金属シース相互間が固
着一体化されたツイスト線STWは、案内管WL
内に従来のようなフレキシブル管を用いることな
く直接挿入される。これは、複数のツイスト線
STWを一体化したことにより全体としての強度
が増して、案内管WL内で折れ曲がるおそれがな
いことによる。
In FIG. 4, STW is a metal sheath twisted wire, and the metal sheaths of these twisted wires STW are fixed and integrated by, for example, brazing. The twisted wire STW in which the metal sheaths are fixed and integrated in this way is connected to the guide tube WL.
It is inserted directly into the interior of the body without using a conventional flexible tube. It has multiple twisted wires
By integrating the STW, the overall strength is increased, and there is no risk of bending within the guide tube WL.

このような構成によれば、ツイスト線STWの
金属シース相互が固着一体化されているので、被
測定流体の温度変化による構成部材の膨張、収縮
や被測定流体の流体振動による案内管WLへの押
付力の経時変化などによつてツイスト線STW相
互間の位置関係が従来のように大幅に変化するこ
とはなく、ツイスト線相互間の位置変化に起因す
る電磁誘導ノイズの変化を大幅に軽減することが
できる。従つて、残留電磁誘導ノイズを電気回路
処理により除去することができ、高分解能が得ら
れる。また、前述のように、従来のようなフレキ
シブル管が不要となつて構成の簡略化が図れ、案
内管内への挿入作業も容易になる。
According to this configuration, since the metal sheaths of the twisted wire STW are fixed and integrated, there is no possibility of expansion or contraction of the constituent members due to temperature changes of the fluid to be measured or vibrations of the fluid to be measured to the guide tube WL. Unlike conventional methods, the positional relationship between the twisted wires STW does not change significantly due to changes in pressing force over time, etc., and changes in electromagnetic induction noise caused by positional changes between the twisted wires are significantly reduced. be able to. Therefore, residual electromagnetic induction noise can be removed by electrical circuit processing, and high resolution can be obtained. Furthermore, as described above, the conventional flexible tube is not required, which simplifies the structure and facilitates insertion into the guide tube.

なお、金属シース相互の固着にあたつては、ロ
ウ付けに限るものではなく、接着剤や固定部材を
用いてもよい。
Note that fixing the metal sheaths to each other is not limited to brazing, and adhesives or fixing members may also be used.

以上説明したように、本考案によれば、電磁誘
導ノイズの変化が少なく、測定分解能が高い渦電
流式流速計が実現でき、液体ナトリウムのような
導電性の被測定流体の流速や流量測定に好適であ
る。
As explained above, according to the present invention, an eddy current current meter with little change in electromagnetic induction noise and high measurement resolution can be realized, and is suitable for measuring the flow velocity and flow rate of conductive fluids to be measured such as liquid sodium. suitable.

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

第1図はこの種の装置の検出部を構成する検出
ユニツトDETの一例を示す構成説明図、第2図
は第1図の動作説明図、第3図は従来のリード線
構造の一例を示す構成説明図、第4図は本考案に
係るリード線構造の一例を示す構成説明図であ
る。 STW……金属シースツイスト線、WL……案内
管。
Fig. 1 is a configuration explanatory diagram showing an example of the detection unit DET that constitutes the detection section of this type of device, Fig. 2 is an explanatory diagram of the operation of Fig. 1, and Fig. 3 shows an example of the conventional lead wire structure. FIG. 4 is an explanatory diagram showing an example of a lead wire structure according to the present invention. STW...Metal sheath twisted wire, WL...Guide tube.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] 導電性を有する被測定流体の流れ方向に沿つて
交流信号が印加される励磁コイルとこの励磁コイ
ルの近傍に少なくとも2個の検出コイルが配置さ
れた検出部を用い、任意の2個の検出コイルの出
力信号の差の信号に基づいて被測定流体の流速を
求めるように構成された渦電流式流速計におい
て、検出部の各コイルへのリード線として金属シ
ースツイスト線を用い、これらリード線の金属シ
ース相互を固着したことを特徴とする渦電流式流
速計。
Using a detection section that includes an excitation coil to which an alternating current signal is applied along the flow direction of the conductive fluid to be measured and at least two detection coils arranged near the excitation coil, any two detection coils can be used. In an eddy current anemometer configured to determine the flow velocity of a fluid to be measured based on the difference between the output signals of An eddy current current meter characterized by a metal sheath that is fixed to each other.
JP18954682U 1982-12-15 1982-12-15 Eddy current current meter Granted JPS5992816U (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP18954682U JPS5992816U (en) 1982-12-15 1982-12-15 Eddy current current meter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP18954682U JPS5992816U (en) 1982-12-15 1982-12-15 Eddy current current meter

Publications (2)

Publication Number Publication Date
JPS5992816U JPS5992816U (en) 1984-06-23
JPH032814Y2 true JPH032814Y2 (en) 1991-01-25

Family

ID=30408638

Family Applications (1)

Application Number Title Priority Date Filing Date
JP18954682U Granted JPS5992816U (en) 1982-12-15 1982-12-15 Eddy current current meter

Country Status (1)

Country Link
JP (1) JPS5992816U (en)

Also Published As

Publication number Publication date
JPS5992816U (en) 1984-06-23

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