JPS5916847Y2 - Magnetic field sensing transformer - Google Patents

Magnetic field sensing transformer

Info

Publication number
JPS5916847Y2
JPS5916847Y2 JP1978159684U JP15968478U JPS5916847Y2 JP S5916847 Y2 JPS5916847 Y2 JP S5916847Y2 JP 1978159684 U JP1978159684 U JP 1978159684U JP 15968478 U JP15968478 U JP 15968478U JP S5916847 Y2 JPS5916847 Y2 JP S5916847Y2
Authority
JP
Japan
Prior art keywords
magnetic
magnetic field
magnetic body
cylindrical metal
transformer
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
JP1978159684U
Other languages
Japanese (ja)
Other versions
JPS5577191U (en
Inventor
登 伊藤
Original Assignee
大井電気株式会社
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 大井電気株式会社 filed Critical 大井電気株式会社
Priority to JP1978159684U priority Critical patent/JPS5916847Y2/en
Publication of JPS5577191U publication Critical patent/JPS5577191U/ja
Application granted granted Critical
Publication of JPS5916847Y2 publication Critical patent/JPS5916847Y2/en
Expired legal-status Critical Current

Links

Description

【考案の詳細な説明】 本考案は、磁界検知器(フィールド・センサー)として
使用する磁性線等の磁性体を用いた変成器に関するもの
である。
[Detailed Description of the Invention] The present invention relates to a transformer using a magnetic material such as a magnetic wire, which is used as a magnetic field sensor.

従来のこの種の変成器は、第1図に示すように、磁性線
1の両端から直接リード線を引き出し、駆動電流供給端
子a、bに接続している。
In a conventional transformer of this kind, as shown in FIG. 1, lead wires are drawn out directly from both ends of a magnetic wire 1 and connected to drive current supply terminals a and b.

4は磁性線1に巻回された2次巻線で、c、dは2次巻
線端子である。
4 is a secondary winding wound around the magnetic wire 1, and c and d are secondary winding terminals.

2は、2次巻線4を巻回した磁性線1の外周を保護する
高分子系絶縁チューブで、その外周に3次巻線5が巻回
されている。
A polymer insulating tube 2 protects the outer periphery of the magnetic wire 1 around which the secondary winding 4 is wound, and the tertiary winding 5 is wound around the outer periphery of the polymer insulating tube.

そして、端子36間に交流電源を接続し、3次巻線5に
直流バイアス電流を流し、2次巻線4の端子c、dに現
われる偶数高調波出力を測定している(第3図参照)。
Then, an AC power source is connected between the terminals 36, a DC bias current is passed through the tertiary winding 5, and the even harmonic output appearing at terminals c and d of the secondary winding 4 is measured (see Figure 3). ).

しかし、従来のかような変成器は、その出力波形に基本
波成分が多く含まれ信号対雑音比(S/N)、すなわち
出力波形の信号(第2高調波)と雑音(基本波)との比
が余りよくない欠点があった。
However, with such conventional transformers, the output waveform contains many fundamental wave components, and the signal-to-noise ratio (S/N), that is, the ratio between the signal (second harmonic) and the noise (fundamental wave) of the output waveform, is low. There was a drawback that the ratio was not very good.

本考案は、従来のこの種の変成器のS/Nを向上すべく
改良したものであり、その実施例を第2図に示す。
The present invention is an improvement of the conventional transformer of this type in order to improve the S/N ratio, and an embodiment thereof is shown in FIG.

第2図において、第1図に対応する同一の部分には同一
の符号を付しである。
In FIG. 2, the same parts corresponding to FIG. 1 are given the same reference numerals.

3は銅などの両端が開放した筒状金属体で、その内側に
は絶縁チューブ2で被う。
3 is a cylindrical metal body made of copper or the like with both ends open, and the inside thereof is covered with an insulating tube 2.

筒状金属体3のほぼ中心軸に位置するように磁性線1を
挿入し、その一端を柔軟な例えば細い導電性線材6で筒
状金属体3の一端に接続し、筒状金属体3の他端から端
子aを引き出す。
A magnetic wire 1 is inserted so as to be located approximately at the central axis of the cylindrical metal body 3, and one end of the magnetic wire 1 is connected to one end of the cylindrical metal body 3 with a flexible, e.g., thin conductive wire 6. Pull out terminal a from the other end.

端子すは、従来どおり磁性線1の他端から引き出す。The terminal is pulled out from the other end of the magnetic wire 1 as before.

こうすると、磁性線1は筒状金属体3内の空間に自由に
維持されることになる。
In this way, the magnetic wire 1 is freely maintained in the space within the cylindrical metal body 3.

そして、第3図に示すように、端子a、l)間に交流電
源epを接続し、3次巻線5に直流バイアス電流を流す
ことは、従来と同様である。
As shown in FIG. 3, connecting an AC power source ep between the terminals a and l) and flowing a DC bias current to the tertiary winding 5 is the same as in the conventional case.

本実施例において使用した磁性線1は、銅にパーマロイ
を1μmだけメッキしたもので、軸方向に異方性をもつ
ものである。
The magnetic wire 1 used in this example is made of copper plated with permalloy to a thickness of 1 μm, and has anisotropy in the axial direction.

かような構成の変成器においては、実験により、基本波
が抑圧され偶数高調波が出力に現われることが判った。
Experiments have shown that in a transformer with such a configuration, the fundamental wave is suppressed and even harmonics appear in the output.

第4図は、第2図のものを用いて第3図のように結線し
て測定した結果を示すものである。
FIG. 4 shows the results of measurement using the device shown in FIG. 2 and connecting the wires as shown in FIG. 3.

図において、i、は、端子a、bに接続された交流電源
e、による駆動電流で、(P−P)/2に、すなわちピ
ーク・ツウ・ピークの1/2の値で示しである。
In the figure, i is a drive current from an AC power source e connected to terminals a and b, and is expressed as (P-P)/2, that is, 1/2 of the peak-to-peak value.

図は、バイアス磁場(A/m・・・・・・1m当たりア
ンペア・ターン)をパラメータとし、点線が従来品、実
線が本考案による場合を示す。
In the figure, the bias magnetic field (A/m . . . ampere turns per meter) is used as a parameter, the dotted line shows the conventional product, and the solid line shows the case according to the present invention.

この図から明らかなように、駆動電流ipを変化した場
合、バイアス磁場が60 A/mのときも800 A/
mのときも、出力波形の信号(第2高調波)と雑音(基
本波)の比S/Nは、本考案によるものが従来のものよ
り極めて良好である。
As is clear from this figure, when the drive current ip is changed, the bias magnetic field is 800 A/m even when the bias magnetic field is 60 A/m.
Even when m, the ratio S/N between the signal (second harmonic) and the noise (fundamental wave) of the output waveform is extremely better in the present invention than in the conventional one.

また、本考案では、磁性線1を空中に浮かして外力が加
わらないようにしているので、日数が経過しても出力が
低下することはない。
Furthermore, in the present invention, the magnetic wire 1 is suspended in the air so that no external force is applied to it, so the output does not decrease even after days have passed.

なお、本実施例では磁性線を用いたが、他の形状の磁性
体を用いても同様の結果が得られるものである。
Although magnetic wires were used in this example, similar results can be obtained by using magnetic bodies of other shapes.

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

第1図は従来の磁界検知用変成器の構成を、第2図は本
考案の実施例の構成をそれぞれ示す一部断面図、第3図
は磁界検知変成器の結線図、第4図は本考案の実施例の
測定結果を示す曲線図である。 1・・・・・・磁性体、3・・・・・・筒状金属体、4
・・・・・・2次巻線、6・・・・・・柔軟な導電性線
材、a・・・・・・磁性体の他端に接続された端子、b
・・・・・・筒状金属体の他端に接続された端子、i、
・・・・・・駆動電流。
Figure 1 shows the configuration of a conventional magnetic field sensing transformer, Figure 2 is a partial sectional view showing the configuration of an embodiment of the present invention, Figure 3 is a wiring diagram of the magnetic field sensing transformer, and Figure 4 is a diagram of the magnetic field sensing transformer. FIG. 3 is a curve diagram showing measurement results of an example of the present invention. 1... Magnetic material, 3... Cylindrical metal body, 4
...Secondary winding, 6...Flexible conductive wire, a...Terminal connected to the other end of the magnetic body, b
・・・・・・Terminal connected to the other end of the cylindrical metal body, i,
・・・・・・Drive current.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] 磁性線等の磁性体を用いた磁界検知用変成器において、
2次巻線を巻回した磁性体を両端が開放した筒状金属体
のほぼ中心軸に位置するように配置し、柔軟な導電性線
材で、上記磁性体の一端を上記筒状金属体の一端に接続
すると共に、上記磁性体の他端を端子に接続することに
より、上記磁性体を空間に自由に維持し、上記磁性体の
他端に接続された端子と上記筒状金属体の他端に接続さ
れた端子とから駆動電流を供給することを特徴とする磁
界検知用変成器。
In magnetic field detection transformers using magnetic materials such as magnetic wires,
A magnetic body around which a secondary winding is wound is placed approximately at the central axis of a cylindrical metal body with both ends open, and one end of the magnetic body is connected to the cylindrical metal body using a flexible conductive wire. By connecting one end of the magnetic body and the other end of the magnetic body to a terminal, the magnetic body can be maintained freely in space, and the terminal connected to the other end of the magnetic body and the other end of the cylindrical metal body can be connected to the other end of the magnetic body. A transformer for detecting a magnetic field, characterized in that a drive current is supplied from a terminal connected to one end of the transformer.
JP1978159684U 1978-11-20 1978-11-20 Magnetic field sensing transformer Expired JPS5916847Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1978159684U JPS5916847Y2 (en) 1978-11-20 1978-11-20 Magnetic field sensing transformer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1978159684U JPS5916847Y2 (en) 1978-11-20 1978-11-20 Magnetic field sensing transformer

Publications (2)

Publication Number Publication Date
JPS5577191U JPS5577191U (en) 1980-05-28
JPS5916847Y2 true JPS5916847Y2 (en) 1984-05-17

Family

ID=29152716

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1978159684U Expired JPS5916847Y2 (en) 1978-11-20 1978-11-20 Magnetic field sensing transformer

Country Status (1)

Country Link
JP (1) JPS5916847Y2 (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP7249789B2 (en) * 2019-01-23 2023-03-31 協立電機株式会社 Fluxgate Sensors and Fluxgate Sensor Phasing Methods
JP2020118523A (en) * 2019-01-23 2020-08-06 協立電機株式会社 Flux gate sensor
JP7245662B2 (en) * 2019-01-30 2023-03-24 笹田磁気計測研究所株式会社 Quadrature fluxgate sensor

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5310180Y2 (en) * 1972-02-15 1978-03-17

Also Published As

Publication number Publication date
JPS5577191U (en) 1980-05-28

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