JPS6293675A - Apparatus for compensating magnetism - Google Patents

Apparatus for compensating magnetism

Info

Publication number
JPS6293675A
JPS6293675A JP23432285A JP23432285A JPS6293675A JP S6293675 A JPS6293675 A JP S6293675A JP 23432285 A JP23432285 A JP 23432285A JP 23432285 A JP23432285 A JP 23432285A JP S6293675 A JPS6293675 A JP S6293675A
Authority
JP
Japan
Prior art keywords
magnetic field
magnetometer
formula
compensating
external magnetic
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
JP23432285A
Other languages
Japanese (ja)
Inventor
Hiroyuki Yoshinari
吉成 碩之
Eiichi Suzuki
栄一 鈴木
Mitsuru Nakatani
中谷 充
Kanji Yoshioka
吉岡 寛二
Akikazu Beppu
別府 昭和
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.)
Shimadzu Corp
Japan Steel Works Ltd
Technical Research and Development Institute of Japan Defence Agency
Original Assignee
Shimadzu Corp
Japan Steel Works Ltd
Technical Research and Development Institute of Japan Defence Agency
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 Shimadzu Corp, Japan Steel Works Ltd, Technical Research and Development Institute of Japan Defence Agency filed Critical Shimadzu Corp
Priority to JP23432285A priority Critical patent/JPS6293675A/en
Publication of JPS6293675A publication Critical patent/JPS6293675A/en
Pending legal-status Critical Current

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  • Measuring Magnetic Variables (AREA)

Abstract

PURPOSE:To measure a compensated external magnetic field without using a compensating coil,by providing a subtraction circuit and compensating the induction magnetic field, permanent magnetic field and eddy current magnetic field generated from a vehicle itself according to a predetermined vector formula. CONSTITUTION:Three low sensitivity fluxmeters 1 detect an external magnetic field E in formula. Herein, HP, A and B in the formula are a constant and stored in a constant memory part 2. A noise quantity calculation circuit 3 takes in the value of the external magnetic field E and calculates the value D represented by the above mentioned formula. A subtraction circuit 5 takes in the output signal of a high sensitivity magnetometer and subtracts the calculated noise quantity to output a compensated magnetometer signal. By this constitution, a compensating coil is not required and an axial alignment process in the compensating coil becomes unnecessary.

Description

【発明の詳細な説明】 主粟上夏科凪分■ この発明は航空機に磁気探知機を搭載して地磁気の乱れ
を検出することにより、沈船等を探査する場合に、航空
機自身による地磁気の乱れを補償する目的で使用する磁
気補償装置に関する。
[Detailed description of the invention] Natsushina Nagibun by Shuawa ■ This invention detects disturbances in the earth's magnetic field by installing a magnetic detector on an aircraft, thereby compensating for disturbances in the earth's magnetic field caused by the aircraft itself when searching for shipwrecks, etc. The present invention relates to a magnetic compensation device used for the purpose of

従ス奥肢歪 一般に、乗物自体から発生する雑音磁界としては、永久
磁界、誘導磁界および渦電流磁界がある。
In general, noise magnetic fields generated from the vehicle itself include permanent magnetic fields, induced magnetic fields, and eddy current magnetic fields.

永久磁界は乗物自体の鋼鉄部品類により、誘導磁界は軟
鉄部品類により、また渦電流磁界は導電体により生じる
Permanent magnetic fields are generated by steel parts of the vehicle itself, induced magnetic fields by soft iron parts, and eddy current fields by electrical conductors.

しかして、乗物に搭載して磁界を計測するための高感度
磁力計が感知する乗物自体からの上記雑音磁界は次ぎの
ように表される。
Therefore, the noise magnetic field from the vehicle itself sensed by a highly sensitive magnetometer mounted on the vehicle to measure the magnetic field is expressed as follows.

まず、磁力計検知部における永久磁界をHp、誘導磁界
をH4、渦電流磁界をHeとする。ここで、永久磁界H
p 、誘導磁界Hiおよび渦電流磁界Heはともに三次
元のベクトル量である。
First, it is assumed that the permanent magnetic field in the magnetometer detection section is Hp, the induced magnetic field is H4, and the eddy current magnetic field is He. Here, the permanent magnetic field H
p, the induced magnetic field Hi, and the eddy current magnetic field He are all three-dimensional vector quantities.

永久磁界は乗物自体が半永久的に磁化されることに基づ
いて発生しているものであるから、■■pは一定である
Since the permanent magnetic field is generated because the vehicle itself is semi-permanently magnetized, ■■p is constant.

誘導磁界は、誘導磁化されやすい物体が外部磁界の中に
置かれたときに外部磁界の大きさに比例して、その方向
に磁化されるものであるから、Hi =AE     
      ・ ・ ・■と表される。ここに、Eは外
部磁界を表わす三次元のベクトル、Aは乗物固有の3×
3定数行列である。また、渦電流磁界は外部磁界の変化
に対して導電体中に電流が流れて2次的に磁界を発生す
るものであり、その大きさは当該外部磁界の時間的変化
率に比例する故、 He =B ・d E/dL    −・−■と表され
る。ここに、d E/dtは外部磁界Eの時間的微分、
Bは乗物固有の3×3定数行列である。
The induced magnetic field is such that when an object that is easily magnetized is placed in an external magnetic field, it will be magnetized in that direction in proportion to the magnitude of the external magnetic field, so Hi = AE
It is expressed as ・ ・ ・■. Here, E is a three-dimensional vector representing the external magnetic field, and A is the vehicle-specific 3×
It is a 3 constant matrix. In addition, an eddy current magnetic field is one in which a current flows in a conductor in response to a change in an external magnetic field, generating a secondary magnetic field, and its magnitude is proportional to the rate of change over time of the external magnetic field. It is expressed as He=B・dE/dL −・−■. Here, dE/dt is the time differential of the external magnetic field E,
B is a vehicle-specific 3×3 constant matrix.

したがって、磁力計検知部における乗物自体の雑音磁界
をHnとすると、I nは Hn=I(p +AE+B −d E/di ・・■で
表される。ここで、Hnは三次元のベクトルである。
Therefore, if the noise magnetic field of the vehicle itself in the magnetometer detection section is Hn, In is expressed as Hn=I(p + AE + B - d E/di...■. Here, Hn is a three-dimensional vector. .

従来の方式では、このHnと同じ大きさで逆向きの磁界
を補償用コイルで発生させ、磁力計検知部に与えること
により乗物自体の雑音を補償するように構成していた。
In the conventional system, a compensating coil generates a magnetic field of the same magnitude as Hn and in the opposite direction, and the magnetic field is applied to the magnetometer detection section to compensate for the noise of the vehicle itself.

上記の従来方式を図面に沿って説明する。The above conventional method will be explained with reference to the drawings.

第2図において、■は3つの直交した低感度磁束計、2
は定数記憶部、3は前記低感度磁束計1の出力と定数記
憶部2の出力に基づいて雑音磁界を計算する雑音磁界計
算回路、4は補償用コイル駆動回路、5は3([1i1
の直交した補償用コイル、6は高感度磁力計である。
In Figure 2, ■ indicates three orthogonal low-sensitivity magnetometers, 2
3 is a constant storage unit, 3 is a noise magnetic field calculation circuit that calculates a noise magnetic field based on the output of the low-sensitivity magnetometer 1 and the output of the constant storage unit 2, 4 is a compensation coil drive circuit, and 5 is 3 ([1i1
6 is a high-sensitivity magnetometer.

ここで、前記低感度磁束計1は0式中の外部磁界Eを検
出する。但し、0式中のHp、A、Bは定数であり、定
数記憶部2に記憶しておく。
Here, the low-sensitivity magnetometer 1 detects the external magnetic field E in equation 0. However, Hp, A, and B in the formula 0 are constants and are stored in the constant storage section 2.

雑音磁界計算回路3は低感度磁束計1の出力、すなわち
外部磁界Eの値を取り込み、■式で表されるH nを計
算する。補償用コイル駆動回路4はこの値を電流に変換
し、補償用コイル5が磁界を発生する。高感度磁力計6
は乗物自体の発生ずる磁界とこの補償磁界のベクトル和
を検出するので補償された外部磁界を測定する。
The noise magnetic field calculation circuit 3 takes in the output of the low-sensitivity magnetometer 1, that is, the value of the external magnetic field E, and calculates H n expressed by the formula (2). The compensation coil drive circuit 4 converts this value into a current, and the compensation coil 5 generates a magnetic field. High sensitivity magnetometer 6
detects the vector sum of the magnetic field generated by the vehicle itself and this compensation magnetic field, so it measures the compensated external magnetic field.

■が”ンしよ゛と る、jp占 従来の方式においては、前記3個の低感度磁束計と補償
用コイル相互の軸合わせが必要であり、しかもこの軸合
わせの精度は雑音補償の性能に直接的な影響を与える一
方、上記軸合わせの精度確保は困難であるという問題が
ある。
In the conventional method, it is necessary to align the three low-sensitivity magnetometers and the compensation coil with each other, and the accuracy of this alignment is limited by the performance of noise compensation. There is a problem in that while it has a direct effect on the alignment, it is difficult to ensure the accuracy of the axis alignment.

本発明は上記事情に鑑みて創案されたもので、従来必要
としていた補償用コイルを用いないで、従って軸合わせ
等を必要としない磁気補償装置を提供することを目的と
している。
The present invention was devised in view of the above-mentioned circumstances, and an object of the present invention is to provide a magnetic compensation device that does not use the conventionally required compensation coil and therefore does not require axis alignment or the like.

皿匙吏 lするための 西 本発明は引算回路を設け、乗物自体から発生する誘導磁
界Hi、永久磁界Hp、渦電流磁界Heを補償する磁気
補償装置であって、3×3定数行列をA、B、三次元の
ベクトルをEとした場合で計算される値りを前記引算回
路でもって高感度磁力計の信号から電気的に差し引くこ
とにより、補償を行うようにした磁気補償装置である。
The present invention is a magnetic compensation device that includes a subtraction circuit and compensates for an induced magnetic field Hi, a permanent magnetic field Hp, and an eddy current magnetic field He generated from a vehicle itself, in which a 3×3 constant matrix is , B. This magnetic compensation device performs compensation by electrically subtracting the value calculated when a three-dimensional vector is E from the signal of the high-sensitivity magnetometer using the subtraction circuit. .

皿 引算回路により、高感度磁力計の信号から上記のDを引
算する。
A dish subtraction circuit subtracts the above D from the signal of the high-sensitivity magnetometer.

災施皿 高感度磁力計は磁界の絶対値を検出するものであるから
、補償を行わない場合にこの磁力計が検出する乗物自体
の雑音量をDとすると、D=E−Hn/E      
 ・・・■即ち、 として表される。
Since the high-sensitivity magnetometer detects the absolute value of the magnetic field, if the amount of noise from the vehicle itself detected by this magnetometer without compensation is D, then D=E-Hn/E.
...■That is, it is expressed as.

ここに、・は内積、EはEの絶対値、Dはスカラー量で
ある。この発明は高感度磁力計から上記りの値を差し引
くことにより乗物自体の雑音を補償するものである。以
下回路図に基づいて具体的に説明する。
Here, . is an inner product, E is an absolute value of E, and D is a scalar quantity. The present invention compensates for the vehicle's own noise by subtracting the above values from a sensitive magnetometer. A detailed explanation will be given below based on a circuit diagram.

第1図において、1は3個の直交した低感度磁束計、2
は定数記憶部、3は雑音量計算回路、4は高感度磁力計
、5は引算回路である。
In Figure 1, 1 indicates three orthogonal low-sensitivity magnetometers, 2
3 is a constant storage unit, 3 is a noise amount calculation circuit, 4 is a high-sensitivity magnetometer, and 5 is a subtraction circuit.

前記3111i1の低感度磁束計1は0式における外部
磁界Eを検出する。また、0式中のHp、A、Bは定数
であり、これを予め前記定数記す、9部2に記憶してお
く。雑音量計算回路3は外部磁界Eの値を取り込み、0
式で表されるDを計算する。−万引算回路5は高感度磁
力計の出力信号を取り込み、計算された雑音量を引算し
て、補償された磁力計信号を出力する。以上述べた構成
により、補償された外部磁界を測定することができる。
The low sensitivity magnetometer 1 of the 3111i1 detects the external magnetic field E in the 0 type. Further, Hp, A, and B in the formula 0 are constants, and these are stored in advance in part 9 2 where the constants are written. The noise amount calculation circuit 3 takes in the value of the external magnetic field E and sets it to 0.
Calculate D expressed by the formula. - The subtraction circuit 5 takes in the output signal of the high-sensitivity magnetometer, subtracts the calculated amount of noise, and outputs a compensated magnetometer signal. With the configuration described above, a compensated external magnetic field can be measured.

仝皿少凱且 以上述べたように、本発明によれば、予め、Hp、Aお
よびBを定数記憶部に記憶しておき、雑音量計算回路が
外部磁界の値を取り込んだあと、その出力を引算回路に
入力し、−万引算回路に高感度磁力計の出力信号を取り
込んで、雑音量を引算してその出力を補償された磁力計
信号として出力するようにしたので、?1li(R用コ
イルを必要としない。したがって当然、補償用コイルに
おける軸合わせの工程は必要とせず、ひいては補償性能
の高い磁気補償装置を得ることができる。
As described above, according to the present invention, Hp, A, and B are stored in the constant storage section in advance, and after the noise amount calculation circuit takes in the value of the external magnetic field, the output is input to the subtraction circuit, the output signal of the high-sensitivity magnetometer is taken into the -yen subtraction circuit, the amount of noise is subtracted, and the output is output as a compensated magnetometer signal, so ? 1li (does not require an R coil. Therefore, of course, the process of aligning the axis of the compensation coil is not required, and as a result, a magnetic compensator with high compensation performance can be obtained.

さらに、補償コイルがないので、磁気補償装置全体とし
ての重量、寸法の軽減を図ることができる。
Furthermore, since there is no compensation coil, it is possible to reduce the weight and size of the entire magnetic compensation device.

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

第1図は本発明による方式のプロ、り図、第2図は従来
の方式のブロック図である。 1・・・低感度磁束計、2・・・定数記憶部、3・・・
雑音量計算回路、4・・・高感度磁力計5・・・引算回
路。 特許出願人  防衛庁技術研究本部長 両下 徹
FIG. 1 is a schematic diagram of the system according to the present invention, and FIG. 2 is a block diagram of the conventional system. 1...Low sensitivity magnetometer, 2...Constant storage unit, 3...
Noise amount calculation circuit, 4...high sensitivity magnetometer 5...subtraction circuit. Patent applicant: Toru Ryoshita, Director General, Technology Research Headquarters, Defense Agency

Claims (1)

【特許請求の範囲】[Claims] (1)乗物自体から発生する誘導磁界Hi、永久磁界H
p、渦電流磁界Heを補償する磁気補償装置であって、
3×3定数行列をA、B、三次元のベクトルをEとした
場合 D=1/|E|{E・[Hp+AE+B(dB/dt)
]}で計算される値Dを高感度磁力計の信号から電気的
に差し引くことにより、補償を行うことを特徴とする磁
気補償装置。
(1) Induced magnetic field Hi, permanent magnetic field H generated from the vehicle itself
p, a magnetic compensation device for compensating an eddy current magnetic field He,
If A and B are 3×3 constant matrices and E is a three-dimensional vector, then D=1/|E|{E・[Hp+AE+B(dB/dt)
]} A magnetic compensation device characterized in that compensation is performed by electrically subtracting a value D calculated from a signal of a high-sensitivity magnetometer.
JP23432285A 1985-10-18 1985-10-18 Apparatus for compensating magnetism Pending JPS6293675A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP23432285A JPS6293675A (en) 1985-10-18 1985-10-18 Apparatus for compensating magnetism

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP23432285A JPS6293675A (en) 1985-10-18 1985-10-18 Apparatus for compensating magnetism

Publications (1)

Publication Number Publication Date
JPS6293675A true JPS6293675A (en) 1987-04-30

Family

ID=16969190

Family Applications (1)

Application Number Title Priority Date Filing Date
JP23432285A Pending JPS6293675A (en) 1985-10-18 1985-10-18 Apparatus for compensating magnetism

Country Status (1)

Country Link
JP (1) JPS6293675A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH01209391A (en) * 1988-02-17 1989-08-23 Tech Res & Dev Inst Of Japan Def Agency Demagnetizer for eddy current magnetic field
CN109765506A (en) * 2018-12-29 2019-05-17 中国船舶重工集团公司第七一0研究所 A kind of screening arrangement internal magnetic field noise compensation apparatus

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH01209391A (en) * 1988-02-17 1989-08-23 Tech Res & Dev Inst Of Japan Def Agency Demagnetizer for eddy current magnetic field
CN109765506A (en) * 2018-12-29 2019-05-17 中国船舶重工集团公司第七一0研究所 A kind of screening arrangement internal magnetic field noise compensation apparatus

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