JPS585683A - magnetic detection element - Google Patents
magnetic detection elementInfo
- Publication number
- JPS585683A JPS585683A JP10299881A JP10299881A JPS585683A JP S585683 A JPS585683 A JP S585683A JP 10299881 A JP10299881 A JP 10299881A JP 10299881 A JP10299881 A JP 10299881A JP S585683 A JPS585683 A JP S585683A
- Authority
- JP
- Japan
- Prior art keywords
- coil
- bobbin
- core
- magnetic field
- detection element
- 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.)
- Granted
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)
Abstract
(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.
Description
【発明の詳細な説明】
この発明は磁気検出素子、特にフラックスゲート形の磁
気検出素子に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a magnetic sensing element, particularly a fluxgate type magnetic sensing element.
これまでに地磁気中の微小磁気を検出するのにフラック
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ックスゲートの基本回路を示
している。Up to now, fluxgate-type magnetic detectors have often been used to detect minute magnetism in the earth's magnetism. Figure 1 shows the basic circuit of the open core type flux gate.
第1図に診いてca、cbはコア、1は励振室−源、
Wl a、−Wl bは励振電源1よりの励振信号を受
けてコアca、cbを励振する励振コイル。Looking at Figure 1, ca and cb are the core, 1 is the excitation chamber-source,
Wl a and -Wl b are excitation coils that receive an excitation signal from the excitation power source 1 and excite the cores ca and cb.
W2 a −W2 bは信号検出コイル、2は信号検出
コイ/l/W2 a −W 2bに検出された信号を増
幅する増幅回路、5は地磁気のベース分を打消すだめの
信号を発生する打消電源、 w3 a −w3 bは打
消コイルである。W2 a - W2 b are signal detection coils, 2 is an amplifier circuit that amplifies the signal detected by the signal detection coil/l/W2 a - W 2b, and 5 is a canceler that generates a signal to cancel the base component of the earth's magnetic field. Power supplies, w3a-w3b are cancellation coils.
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△H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)VW3 a
−W5 bで打消すとともに微小磁気は信号検出コイ/
L/W 2 a −W 2 b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 by the circuit shown in FIG.
-W5 b cancels out the micromagnetic signal detection coil/
Detection is performed using L/W 2 a - W 2 b.
ところで、第1図に示す基本回路に使用される従来の各
コア及びコイルの構成要素は第3図(a)のようにオー
プンコア4にボビン5を介シてコイル界の強さ分布は第
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ック等の合成樹脂を使用し
ているがプラスチックは熱i係数が大きいため、温度に
よってボビンの大きさが変イピする。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1.コイル長さをLとすると、H■
NI/Lで表わされコイル長さに反比例する。それゆえ
熱膨張によシボピン長連変化するとLも変化するので1
発生磁界Hは逆に小となる変化をする。したがってペー
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の検出は困轄であった。By the way, the conventional core and coil components used in the basic circuit shown in FIG. 1 are as shown in FIG. As shown in FIG. 3(b), the magnetic field becomes smaller at the ends, and a uniform magnetic field cannot be obtained, making it impossible to uniformly magnetize the core 4. Also, synthetic resin such as plastic is used as the material for the bobbin, but since plastic has a large thermal i coefficient, the size of the bobbin changes depending on the temperature. Generally, the strength H of the magnetic field generated in a coil when a current is passed through the coil is determined by the number of turns of the coil being N and the current being 1. If the coil length is L, then H■
It is expressed as NI/L and is inversely proportional to the coil length. Therefore, when the length of the grain pin changes due to thermal expansion, L also changes, so 1
On the contrary, the generated magnetic field H changes to become smaller. Therefore, cancellation of the pace magnetic field H becomes unstable when ΔH is small compared to H, and it is 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。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.
以上の目的を達成するためにこの発明の磁気検出素子は
、コイルの′巻線幅をオープンコアの長さよりも長くす
るとともに、併せてボビンを熱膨張係数の小さい材質の
もので構成するようにしている。In order to achieve the above object, the magnetic sensing element of the present invention has the winding width of the coil longer than the length of the open core, and the bobbin is made of a material with a small coefficient of thermal expansion. ing.
以下さらに図面に示す実施例によりこの発明の詳細な説
明する。The present invention will be further explained in detail below with reference to embodiments shown in the drawings.
第4図は、この発明の一実施例のコイル装置であって(
−)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 (
-) is a sectional view of the coil device, and (b) is a characteristic diagram showing the distribution of the 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/1/9を巻回している点では第3図(a)の
ものと変りはない。しかしコイル9の巻回幅を成するこ
とによシ、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)に示すようになシ。In FIG. 4(a), there is no difference from that in FIG. 3(a) in that a carp/1/9 is wound around an open core 7 via a bobbin 8. However, by adjusting the winding width of the coil 9, the distribution of the magnetic field strength H on the central axis of the coil becomes as shown in FIG. 4(b).
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lv9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アワコア7とコイ/
l/9の位置関係を厳密に固定する必要がない。A uniform magnetic field strength can be obtained at least within the length range of the open core 7. 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 lv9 and core 7 are slightly shifted, the strength of the magnetic field applied to core 7 will hardly change.
There is no need to strictly fix the positional relationship of l/9.
さらにボビン8は材質としてセラミック、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、非常に小姓な△H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 the conventional system, 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。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.
ボビン数を必要数だけ重ね合せて磁気検出素子を構成し
てもよい。The magnetic detection element may be constructed by stacking a required number of bobbins.
以上のようにこの発明の磁気検出素子によれば。As described above, according to the magnetic detection element of the present invention.
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。The winding width of the coil that makes up the magnetic sensing element is longer than the length of the open core, and the bobbin is made of a material with a small coefficient of thermal expansion.
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。When detecting variations in geomagnetism, the base component of geomagnetism can be canceled out with high stability, and the core can be magnetized uniformly, so core noise can also be reduced.
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。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ッ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△H“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)Uコイ/l/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
lv’lj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。
5・・・打消電源、 Wla−Wlb・・・励振コイ
p。
W2 a −W2 bH”検出コイ/L/。
W′5a 、w5 b−打消コイル。
4・7・・・コア、 5・8・10・・・ボビン。
6・9・11・・・コイμ。
特許出願人 株式会社島津製作所代理人 弁
理士 中 村 茂 信
第 1 図
一一一一一一り
第 2 図Figure 1 is a circuit connection diagram showing the basic circuit of an open-core fluxgate, 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 of a conventional magnetic detection element. A cross-sectional view of the device (a) U-coy/l/device;
(b) is a diagram showing the distribution of magnetic field strength. FIG. 4 shows a coil lv'lj device for a magnetic detection element showing one 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 FIG. 5 shows a coil device according to another embodiment of the present invention. 1...Excitation power supply, 2...Amplification circuit. 5...Cancelling power supply, Wla-Wlb... Excitation coil p. W2 a - W2 bH" detection carp /L/. W'5a, w5 b-cancellation coil. 4, 7...core, 5, 8, 10...bobbin. 6, 9, 11... carp μ Patent applicant Shimadzu Corporation Representative Patent attorney Shigeru Nakamura Nobu No. 1 Figure 11 Figure 2
Claims (2)
要素より構成される磁気検出素子において前記コイルの
巻線幅を前記コアの長さよシも長くするとともに、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。(1) In a magnetic sensing element composed of an element in which a coil is wound around a core via a bobbin, the winding width of the coil is made longer than the length of the core, and the bobbin has a thermal expansion coefficient. A magnetic detection element characterized in that it is made of a material with a small size.
れた導体であることを特徴とする特許請求の範囲第1項
記載の磁気検出素子。(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 true JPS585683A (en) | 1983-01-13 |
| JPH0155427B2 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) |
Citations (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
Patent Citations (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS445187Y1 (en) * | 1965-08-21 | 1969-02-25 |
Also Published As
| Publication number | Publication date |
|---|---|
| JPH0155427B2 (en) | 1989-11-24 |
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