JPH0155427B2 - - Google Patents
Info
- Publication number
- JPH0155427B2 JPH0155427B2 JP56102998A JP10299881A JPH0155427B2 JP H0155427 B2 JPH0155427 B2 JP H0155427B2 JP 56102998 A JP56102998 A JP 56102998A JP 10299881 A JP10299881 A JP 10299881A JP H0155427 B2 JPH0155427 B2 JP H0155427B2
- Authority
- JP
- Japan
- Prior art keywords
- coil
- bobbin
- core
- magnetic
- magnetic field
- 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
Links
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
- G01R33/00—Arrangements or instruments for measuring magnetic variables
- G01R33/02—Measuring direction or magnitude of magnetic fields or magnetic flux
Landscapes
- Physics & Mathematics (AREA)
- Condensed Matter Physics & Semiconductors (AREA)
- General Physics & Mathematics (AREA)
- Measuring Magnetic Variables (AREA)
Description
【発明の詳細な説明】
(イ) 産業上の利用分野
この発明は磁気検出素子、特にフラツクスゲー
ト形の磁気検出素子に関する。DETAILED DESCRIPTION OF THE INVENTION (a) Field of Industrial Application This invention relates to a magnetic sensing element, particularly a flux gate type magnetic sensing element.
(ロ) 従来の技術
これまで地磁気中の微小磁気を検出するのにフ
ラツクスゲート形の磁気検出器がよく用いられて
いる。第1図にそのオープンコア形フラツクスゲ
ートの基本回路を示している。(b) Conventional technology Until now, flux gate type magnetic detectors have been often used to detect minute magnetism in the earth's magnetism. Figure 1 shows the basic circuit of the open-core flux gate.
第1図において、Ca,Cbはコア、1は励振電
源、W1a,W1bは励振電源1よりの励振信号
を受けコアCa,Cbを励振する励振コイル、W2
a,W2bは信号検出コイル、2は信号検出コイ
ルW2a,W2bに検出された信号を増幅する増
幅回路、3は地磁気のベース分を打消すための信
号を発生する打消電源、W3a,W3bは打消コ
イルである。 In Figure 1, C a and C b are cores, 1 is an excitation power source, W1a and W1b are excitation coils that receive excitation signals from excitation power source 1 and excite cores C a and C b , and W2
a and W2b are signal detection coils, 2 is an amplifier circuit that amplifies the signals detected by the signal detection coils W2a and W2b, 3 is a cancellation power supply that generates a signal to cancel the base component of the earth's magnetic field, and W3a and W3b are cancellations. It is a coil.
地磁気は一般に、第2図に示すようにベース分
Hと、微小磁気ΔHを有しているので、第1図に
示す回路により、ベース分Hは打消電源3及び打
消コイルW3a,W3bで打消すとともに微小磁
気は信号検出コイルW2a,W2bで検出するよ
うにしている。 Earth's magnetism generally has a base component H and a minute magnetism ΔH as shown in FIG. 2, so the base component H is canceled by the canceling power supply 3 and canceling coils W3a and W3b using the circuit shown in FIG. At the same time, minute magnetism is detected by signal detection coils W2a and W2b.
(ハ) 発明が解決しようとする課題
第1図に示す基本回路に使用される従来の各コ
ア及びコイル構成要素は第3図aのようにオープ
ンコア4にボビン5を介してコイル6が巻回され
ており、コイルの巻線幅とコア4の長さがほぼ同
一であるか巻線幅の方が短かつた。そのため、コ
イル中心軸上の磁界の強さ分布は第3図bに示す
ように、端部で小さくなり均一な磁界が得られず
コア4を均一に磁化することができない。又ボビ
ンの材質としてプラスチツク等の合成樹脂を使用
しているがプラスチツクは熱膨張係数が大きいた
め、温度によつてボビンの大きさが変化する。一
般にコイルに電流を流した時のコイル内に生じる
磁界の強さHはコイルの巻数をN、電流をI、コ
イル長さをLとすると、H∞NI/Lで表されコ
イル長さに反比例する。それゆえ熱膨張によりボ
ビン長が変化するとLも変化するので、発生磁界
Hは逆に小となる変化をする。したがつて、ベー
ス磁界Hの打消もHに比しΔHが小さいと不安定
となり、非常に小さなΔHの検出は困難であつ
た。(c) Problems to be Solved by the Invention The conventional core and coil components used in the basic circuit shown in FIG. 1 are as shown in FIG. The winding width of the coil and the length of the core 4 were either approximately the same or shorter. Therefore, as shown in FIG. 3b, the strength distribution of the magnetic field on the central axis of the coil becomes smaller at the ends, and a uniform magnetic field cannot be obtained, making it impossible to uniformly magnetize the core 4. Furthermore, synthetic resin such as plastic is used as the material for the bobbin, but since plastic has a large coefficient of thermal expansion, the size of the bobbin changes depending on the temperature. In general, the strength of the magnetic field H generated in a coil when current is passed through it is expressed as H∞NI/L, where N is the number of turns in the coil, I is the current, and L is the length of the coil, and is inversely proportional to the length of the coil. do. Therefore, when the bobbin length changes due to thermal expansion, L also changes, so the generated magnetic field H changes to become smaller. Therefore, the cancellation of the base magnetic field H also becomes unstable when ΔH is small compared to H, making it difficult to detect a very small ΔH.
この発明の目的は、上記従来の磁気検出素子の
欠点を解消し、微小磁気でも安定して検出し得る
磁気検出素子を提供するにある。 SUMMARY OF THE INVENTION An object of the present invention is to eliminate the drawbacks of the conventional magnetic detection elements described above and to provide a magnetic detection element capable of stably detecting even minute magnetism.
(ニ) 課題を解決するための手段及び作用
この発明の磁気検出素子は、ボビンのコイルの
巻線幅を前記コアの長さよりも1.2倍以上長くす
るとともに、併せてボビンを熱膨張係数の小さい
材質で構成している。(d) Means and Effects for Solving the Problems In the magnetic sensing element of the present invention, the winding width of the coil of the bobbin is at least 1.2 times longer than the length of the core, and the bobbin has a small coefficient of thermal expansion. It is made up of materials.
この磁気検出素子では、コイルの巻線幅をコア
の長さよりも1.2倍以上長くしているので、コイ
ルの軸方向の磁界分布が均一になる。また、熱膨
張係数の小さい材質でボビンを構成しているの
で、温度によつて磁界分布が変化することも少な
い。 In this magnetic sensing element, the winding width of the coil is at least 1.2 times longer than the length of the core, so the magnetic field distribution in the axial direction of the coil is uniform. Furthermore, since the bobbin is made of a material with a small coefficient of thermal expansion, the magnetic field distribution is less likely to change depending on temperature.
(ホ) 実施例
以下、実施例により、この発明をさらに詳細に
説明する。(E) Examples The present invention will be explained in more detail below with reference to Examples.
第4図は、この発明の一実施例のコイル装置で
あつてaはコイル装置の断面図、bは磁界の分布
を示す特性図である。 FIG. 4 shows a coil device according to an embodiment of the present invention, in which a is a cross-sectional view of the coil device and b is a characteristic diagram showing the distribution of a magnetic field.
第4図aにおいて、オープンコア7にボビン8
を介してコイル9を巻回している点では第3図a
のものと変わりはない。しかしコイル9の巻回幅
をオープンコア7の長さに比して十分に長くなる
ようにしていることが特徴である。コイル9の巻
回幅はコア7の1.2倍以上の長さであることが効
果達成上望ましい。このように構成することによ
り、コイルの中心軸上における磁界の強さHの分
布は第4図bに示すようになり、少なくともオー
プンコア7の長さの範囲では均一磁界の強さを得
ることができる。そのためコアを均一に磁化する
ことができるから、均一に磁化できないことによ
る雑音を大幅に軽減することができる。またコイ
ル9とコア7の位置が若干ずれたとしてもコア7
に加えられる磁界の強さはほとんど変わらないの
で、コア7とコイル9の位置関係を厳密に固定す
る必要がない。 In Fig. 4a, the bobbin 8 is attached to the open core 7.
Figure 3a shows that the coil 9 is wound through the
It's no different from the one. However, a feature is that the winding width of the coil 9 is made sufficiently longer than the length of the open core 7. It is desirable that the winding width of the coil 9 is at least 1.2 times the length of the core 7 in order to achieve the effect. With this configuration, the distribution of the magnetic field strength H on the central axis of the coil becomes as shown in FIG. 4b, and a uniform magnetic field strength can be obtained at least within the length range of the open core 7. Can be done. Therefore, since the core can be magnetized uniformly, noise caused by not being able to magnetize uniformly can be significantly reduced. Also, even if the positions of coil 9 and core 7 are slightly shifted, core 7
Since the strength of the magnetic field applied to the core 7 and the coil 9 hardly changes, there is no need to strictly fix the positional relationship between the core 7 and the coil 9.
さらにボビン8は材質としてセラミツク、石英
等熱膨張係数の小さいものを使用している。これ
により、温度変化による発生磁界の変化は従来の
ものに比べて2桁以上の比率で改善され、非常に
小さなΔHをも検出可能となる。 Furthermore, the bobbin 8 is made of a material with a small coefficient of thermal expansion, such as ceramic or quartz. As a result, changes in the generated magnetic field due to temperature changes are improved by more than two orders of magnitude compared to conventional systems, and even extremely small ΔH can be detected.
なお上記実施例において、コイルはボビンの上
に導線を巻回しているが、第5図に示すようにボ
ビン10上に直接に導体11を螺旋状に蒸着して
もよい。コイルの巻線の機械的移動が少ないので
安定度がより増長される。 In the above embodiment, the coil is formed by winding a conductive wire on a bobbin, but the conductor 11 may be spirally deposited directly on the bobbin 10 as shown in FIG. Stability is further enhanced because there is less mechanical movement of the coil windings.
また第5図の導体11がボビン10上に蒸着さ
れてなるコイル上に、他の導線を重ね巻きしても
よいし、さらにボビン径の種々のものを組合せ、
ボビン数を必要数だけ重ね合わせ磁気検出素子を
構成してもよい。 Further, other conductive wires may be wound over the coil formed by depositing the conductor 11 on the bobbin 10 shown in FIG. 5, or bobbins of various diameters may be combined.
The magnetic detection element may be constructed by stacking a required number of bobbins.
(ヘ) 発明の効果
この発明の磁気検出素子によれば、磁気検出素
子を構成するコイルの巻線幅をオープンコアの長
さよりも1.2倍以上長くするとともに、併せてボ
ビンを熱膨張係数の小さい材質で構成したので、
地磁気の変化分を検出する場合には、地磁気のベ
ース分を高安定度に打消すことができるし、コア
を均一に磁化できるから、コア雑音も低減でき
る。さらにコアとコイルの機械的位置のずれによ
る不安定性も低減除去できるという効果がある。(F) Effects of the Invention According to the magnetic sensing element of the present invention, the winding width of the coil constituting the magnetic sensing element is at least 1.2 times longer than the length of the open core, and the bobbin is also made of a material having a small coefficient of thermal expansion. Since it is made of materials,
When detecting changes in geomagnetism, the base component of geomagnetism can be canceled with high stability, and the core can be magnetized uniformly, so core noise can also be reduced. Furthermore, there is an effect that instability caused by mechanical positional deviation between the core and the coil can be reduced and eliminated.
第1図はオープンコア形フラツクスゲートの基
本回路を示す回路接続図、第2図は地磁気のベー
ス分Hと微小変化分ΔHを示す特性図、第3図は
従来の磁気検出素子のコイル装置でありaはコイ
ル装置の断面図、bは磁界の強さの分布を示す
図、第4図はこの発明の一実施例を示す磁気検出
素子のコイル装置であり、aはコイル装置の断面
図、bは磁界の強さの分布を示す図、第5図は、
この発明の他の実施例のコイル装置を示してい
る。
1…励振電源、2…増幅回路、3…打消電源、
W1a,W1b…励振コイル、W2a,W2b…
検出コイル、W3a,W3b…打消コイル、4,
7…コア、5,8,10…ボビン、6,9,11
…コイル。
Figure 1 is a circuit connection diagram showing the basic circuit of an open-core flux gate, Figure 2 is a characteristic diagram showing the base component H and minute change ΔH of the earth's magnetic field, and Figure 3 is a coil device of a conventional magnetic detection element. 4 is a cross-sectional view of the coil device, b is a diagram showing the distribution of magnetic field strength, FIG. 4 is a coil device of a magnetic detection element showing an embodiment of the present invention, and a is a cross-sectional view of the coil device. , b is a diagram showing the distribution of magnetic field strength, and Figure 5 is,
Fig. 7 shows a coil device according to another embodiment of the invention. 1... Excitation power supply, 2... Amplification circuit, 3... Cancellation power supply,
W1a, W1b...excitation coil, W2a, W2b...
Detection coil, W3a, W3b...cancellation coil, 4,
7... Core, 5, 8, 10... Bobbin, 6, 9, 11
…coil.
Claims (1)
消用の打消コイル及び信号検出コイルが巻回さ
れ、かつ前記励磁コイルに励振電源が接続され、
地磁気打消コイルに打消電源が接続され、前記信
号検出コイルより磁気検出信号が導出されるフラ
ツクスゲート型の磁気検出素子において、 前記ボビンのコイルの巻線幅を前記コアの長さ
よりも1.2倍以上長くするとともに、併せて前記
ボビンを熱膨張係数の小さい材質で構成したこと
を特徴とする磁気検出素子。 2 前記コイルは前記ボビンに直接ラセン状に蒸
着された導体であることを特徴とする特許請求の
第1項記載の磁気検出素子。[Claims] 1. An excitation coil, a cancellation coil for canceling the earth's magnetic field, and a signal detection coil are wound around the core via a bobbin, and an excitation power source is connected to the excitation coil,
In a flux gate type magnetic detection element in which a canceling power source is connected to a geomagnetism canceling coil and a magnetic detection signal is derived from the signal detecting coil, the winding width of the coil of the bobbin is 1.2 times or more larger than the length of the core. A magnetic sensing element characterized in that the bobbin is made of a material having a small coefficient of thermal expansion. 2. The magnetic sensing element according to claim 1, wherein the coil is a conductor deposited directly on the bobbin in a spiral shape.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP10299881A JPS585683A (en) | 1981-06-30 | 1981-06-30 | magnetic detection element |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP10299881A JPS585683A (en) | 1981-06-30 | 1981-06-30 | magnetic detection element |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS585683A JPS585683A (en) | 1983-01-13 |
| JPH0155427B2 true JPH0155427B2 (en) | 1989-11-24 |
Family
ID=14342348
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP10299881A Granted JPS585683A (en) | 1981-06-30 | 1981-06-30 | magnetic detection element |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS585683A (en) |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS445187Y1 (en) * | 1965-08-21 | 1969-02-25 |
-
1981
- 1981-06-30 JP JP10299881A patent/JPS585683A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS585683A (en) | 1983-01-13 |
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