JPH092385A - Permanent magnetiszm removing method of ship - Google Patents

Permanent magnetiszm removing method of ship

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Publication number
JPH092385A
JPH092385A JP18212995A JP18212995A JPH092385A JP H092385 A JPH092385 A JP H092385A JP 18212995 A JP18212995 A JP 18212995A JP 18212995 A JP18212995 A JP 18212995A JP H092385 A JPH092385 A JP H092385A
Authority
JP
Japan
Prior art keywords
magnetic
ship
permanent
hull
current
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
Application number
JP18212995A
Other languages
Japanese (ja)
Other versions
JP2893165B2 (en
Inventor
Toshiji Kimura
利治 木村
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.)
Japan Steel Works Ltd
Technical Research and Development Institute of Japan Defence Agency
Original Assignee
Japan Steel Works Ltd
Technical Research and Development Institute of Japan Defence Agency
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Filing date
Publication date
Application filed by Japan Steel Works Ltd, Technical Research and Development Institute of Japan Defence Agency filed Critical Japan Steel Works Ltd
Priority to JP7182129A priority Critical patent/JP2893165B2/en
Publication of JPH092385A publication Critical patent/JPH092385A/en
Application granted granted Critical
Publication of JP2893165B2 publication Critical patent/JP2893165B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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  • Geophysics And Detection Of Objects (AREA)

Abstract

PURPOSE: To minimize the permanent magnetic moment through the constant monitoring by calculating the permanent magnetic moment in the longitudinal direction in the process of removing the permanent magnetism of a ship having a steel hull. CONSTITUTION: In a process in which a ring of windings is fitted approximately with equal intervals around a steel hull 2 of a ship 1, and the permanent magnetism in the longitudinal direction of the ship is canceled by carrying current to the ring 3 of windings by gradually reducing the current while the polarity of the current is alternately changed to positive or negative, the magnetic field in X, Y and Z directions of the hull 2 is measured by a plurality of magnetism detector 7 installed on the sea bed, and the permanent magnetic moment in the longitudinal direction is quantitatively calculated based on the measured values by a plurality of magnetism detectors 7 to minimize the value of the permanent magnetic moment through the constant monitoring.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は、磁性体の、例えば鋼鉄
製の船体を有する船舶から発生する永久磁気を脱磁でき
る船舶の永久磁気脱磁方法に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a permanent magnetic demagnetization method for a ship, which is capable of demagnetizing a permanent magnet generated from a magnetic material, for example, a ship having a steel hull.

【0002】[0002]

【従来の技術】従来、鋼材によって構成された船体を有
する船舶が保持する永久磁気を消去するために、船体の
外周に幾巻きかの胴巻線輪を装着し、該胴巻線輪に電流
の極性を正負に変えながら、その大きさを漸減して通電
しているが、その過程において、海底に設置されている
複数個の磁気検出器のうちの特定の磁気検出器の測定値
により所要の船体磁気諸元を間欠的に算出して、それに
基づいた永久磁気分を間欠的に監視しながら脱磁処理を
実施し、その効果を評価していた。
2. Description of the Related Art Conventionally, in order to erase the permanent magnetism retained by a ship having a hull made of steel, several windings are attached to the outer circumference of the hull and the polarity of the current is applied to the windings. While changing the sign to positive or negative, the size is gradually reduced to energize.In the process, the required hull is measured according to the measured value of a specific magnetic detector among the plurality of magnetic detectors installed on the seabed. The magnetic data was calculated intermittently, and the demagnetization process was carried out while the permanent magnetic component based on it was intermittently monitored, and the effect was evaluated.

【0003】[0003]

【発明が解決しようとする課題】上記の船体磁気測定に
基づく船舶の永久磁気の脱磁処理はある特定の磁気検出
器(例えば2個)の測定値から永久磁気分を抽出して監
視している磁界制御方法であるが、その際、測定海面の
潮の干満等による水深の変動及び船体と磁気検出器の相
対位置のずれ等による測定誤差が生じ、それらが脱磁効
果に大きく影響を及ぼしていた。
The demagnetization process of the permanent magnetism of a ship based on the above-mentioned hull magnetism measurement involves extracting and monitoring the permanent magnetism component from the measurement values of a certain specific magnetic detector (for example, two). This is a magnetic field control method, but at that time, fluctuations in water depth due to ebb and flow of the sea surface of the measurement surface and measurement errors due to displacement of the relative position between the hull and the magnetic detector, etc., greatly affect the demagnetization effect. Was there.

【0004】しかも、前記の作業における船体磁気諸元
の算出、通電量の決定及び脱磁効果の評価は、作業者の
豊富な経験と熟練した技量に依存するところが大きかっ
た。
Moreover, the calculation of the magnetic properties of the hull, the determination of the energization amount, and the evaluation of the demagnetization effect in the above-mentioned work depended largely on the abundant experience and skilled skill of the worker.

【0005】さらに、多数の磁気検出器が海底に設置さ
れている場合でも、船体磁気諸元の算出に用いるもの
は、特定の磁気検出器の測定値だけであり、残りの磁気
検出器の測定値は有効に利用されないきらいがあった。
これは、従来方法では、船体磁気諸元の算出に多数の磁
気検出器の測定値を利用しようとすると、演算等が極め
て複雑化すると考えられていたからである。
Further, even when a large number of magnetic detectors are installed on the seabed, only the measured values of a specific magnetic detector are used to calculate the ship's magnetic specifications, and the remaining magnetic detectors are measured. There is a tendency that the value is not used effectively.
This is because, in the conventional method, it was considered that the calculation and the like would be extremely complicated if the measured values of a large number of magnetic detectors were used to calculate the magnetic properties of the ship.

【0006】本発明は、これらの問題点に着目してなさ
れたものであって、海底等に設置された複数個の磁気検
出器の測定値からコンピュータを活用することにより船
体全体を磁気モーメントとして算出し、その値を定量的
に常時把握しながら脱磁処理を実施することを可能と
し、システムの自動化を図り得る船舶の永久脱磁方法を
提供することを目的としている。
The present invention has been made by paying attention to these problems, and by utilizing a computer from the measured values of a plurality of magnetic detectors installed on the seabed or the like, the entire hull is converted into a magnetic moment. An object of the present invention is to provide a permanent demagnetization method for a ship, which enables the demagnetization process to be performed while constantly calculating and calculating the value quantitatively, and enabling the system to be automated.

【0007】[0007]

【課題を解決するための手段】上記目的を達成するため
に、本発明の船舶の永久磁気脱磁方法は、船舶の磁性体
からなる船体に幾巻きかの胴巻線輪を装着し、該胴巻線
輪に、電流の極性を正負に変えながら当該電流の大きさ
を漸減して通電することにより、船首尾線方向の永久磁
気を消去する過程において、船体の磁界を複数個の磁気
検出器により測定し、前記複数個の磁気検出器の測定値
に基づいて船首尾線方向の永久磁気モーメントを定量的
に算出して、該永久磁気モーメントの値を監視しながら
最小にするようにしている。
In order to achieve the above object, the method of permanent magnetic demagnetization of a ship according to the present invention is such that a number of body winding wheels are attached to a hull made of a magnetic material of the ship, In the process of erasing the permanent magnetism in the direction of the bow-stern line, the magnetic field of the hull is detected by a plurality of magnetic detectors in the process of erasing the permanent magnetism in the bow-caudal direction by changing the polarity of the current to positive or negative and energizing the coil. The permanent magnetic moment in the bow and tail line direction is quantitatively calculated based on the measured values of the plurality of magnetic detectors, and the value of the permanent magnetic moment is minimized while being monitored.

【0008】[0008]

【作用】本発明に係る船舶の永久磁気脱磁方法において
は、例えば海底等に設置された複数個の磁気検出器の測
定値から、船体磁気モーメントを算出して、それらに基
づいて船首尾線方向の永久磁気モーメントを抽出し、そ
の値を監視しながら最小にさせようとするものである。
船舶のX,Y,Z方向の船体磁気モーメントの算出は長
球調和関数の展開式を用いて実行することができる。磁
性体からなる船体の磁界の測定値から長球調和関数の展
開式により算出した船体磁気モーメントは、永久磁気モ
ーメントと誘導磁気モーメントが混在しており、これら
を分離することは、船首を北及び南方向に向けた状態に
おいてそれぞれ算出したモーメントから可能である。そ
して、分離して得られた永久磁気モーメントの値を常時
監視(胴巻線輪に脱磁用の電流を通電後、通電をオフし
た毎に監視)することにより永久磁気の消去状態を定量
的に評価できることになる。この場合、海底等に設置さ
れた磁気検出器の全ての測定データを有効に利用でき、
特定の磁気検出器の測定値のみを用いる従来方法に比し
て測定誤差を少なくし、脱磁効果の向上を図れる。
In the permanent magnetic demagnetization method for a ship according to the present invention, the ship's magnetic moment is calculated from the measured values of a plurality of magnetic detectors installed on the seabed or the like, and the bow-tail line is calculated based on the magnetic moments. It is intended to extract the permanent magnetic moment in the direction and minimize it while monitoring its value.
The calculation of the ship magnetic moments in the X, Y, and Z directions of the ship can be performed using the expansion formula of the elliptic harmonic function. The hull magnetic moment calculated from the measured value of the magnetic field of the hull made of magnetic material by the expansion formula of the ellipsoidal harmonic function is a mixture of the permanent magnetic moment and the induced magnetic moment. It is possible from the moments calculated in the state facing south. Then, the value of the permanent magnetic moment obtained by the separation is constantly monitored (monitoring every time the energizing current is turned off after the demagnetizing current is applied to the body winding wheel) to quantitatively determine the erased state of the permanent magnetism. Can be evaluated. In this case, you can effectively use all the measurement data of the magnetic detector installed on the seabed,
It is possible to reduce the measurement error and improve the demagnetization effect as compared with the conventional method in which only the measured value of a specific magnetic detector is used.

【0009】[0009]

【実施例】以下、本発明に係る船舶の永久磁気脱磁方法
の実施例を図面に従って説明する。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS An embodiment of a ship permanent magnetic demagnetization method according to the present invention will be described below with reference to the drawings.

【0010】図1は本発明に係る船舶の永久磁気脱磁方
法の実施例において用いる船舶の永久磁気脱磁施設の概
略図である。この図において、1は船舶であり、磁性
体、例えば鋼鉄製等の船体2を有するものであり、船体
2の外周には幾巻きかの胴巻線輪3が巻回、装着されて
いる。該胴巻線輪3の巻線ピッチは等間隔であることが
望ましいが、多少の間隔のずれは許容される。脱磁工程
において、船舶1は係留用ワイヤー4で海底側に固定の
係留用台5に繋がれるようになっている。前記胴巻線輪
3は脱磁用電流を流すための電源を有する脱磁処理用電
源室6に電源ケーブル9を介し接続される。
FIG. 1 is a schematic diagram of a ship permanent magnetic demagnetization facility used in an embodiment of the ship permanent magnetic demagnetization method according to the present invention. In the figure, reference numeral 1 denotes a ship, which has a hull 2 made of a magnetic material, such as steel, and several body winding wheels 3 are wound and mounted on the outer circumference of the hull 2. It is desirable that the winding pitches of the body winding wheel 3 be evenly spaced, but a slight gap can be allowed. In the demagnetization process, the ship 1 is connected to the mooring table 5 fixed on the seabed side by the mooring wire 4. The body winding wheel 3 is connected to a demagnetization processing power supply chamber 6 having a power supply for supplying a demagnetization current via a power cable 9.

【0011】多数の磁気検出器7は船舶1の係留位置の
下方に位置する海底に固定されている。例えば、磁気検
出器7は船体2の船首尾線方向に幾つか配置され、さら
に、船首尾線方向の両側に幾つか配置されている。そし
て、各磁気検出器7は、それらの測定値を受けるコンピ
ュータを有する測定室8に接続される。なお、図1で
は、船体2の船首尾線方向をX方向、水平面内でX方向
に垂直な向きをY方向、鉛直方向をZ方向とする。
A large number of magnetic detectors 7 are fixed to the seabed below the mooring position of the ship 1. For example, some magnetic detectors 7 are arranged in the fore-and-aft direction of the hull 2, and further several are arranged on both sides in the fore-and-aft direction. Then, each magnetic detector 7 is connected to a measuring chamber 8 having a computer for receiving those measured values. In FIG. 1, the bow-tail direction of the hull 2 is the X direction, the direction perpendicular to the X direction in the horizontal plane is the Y direction, and the vertical direction is the Z direction.

【0012】次に、船舶1が有する磁性体、例えば鋼鉄
製等の船体2の磁気モーメントを算出する手法について
述べると、伝導電流を含まない空間領域に船体が存在し
ているものとすると、外部磁界は渦なしであるため、磁
界のスカラ・ポテンシャルすなわち磁位はラプラスの方
程式を満足する。
Next, a method of calculating the magnetic moment of the magnetic body of the vessel 1, for example, the vessel 2 made of steel, will be described. Assuming that the vessel exists in a spatial region that does not include conduction current, Since the magnetic field is vortex-free, the scalar potential or magnetic field of the magnetic field satisfies the Laplace equation.

【0013】図2に示すように、図1の船体2の幾何学
的中心線上両端の位置に点c1及び点c2を置き、これ
らを焦点とする回転楕円体座標(η,ξ,φ)を設け
る。任意の点P(η,ξ,φ)は回転楕円体面η(η≧
1)、回転双曲面ξ(−1≦ξ≦1)及び半平面φ(0
≦φ≦2π)の交点として表される。もし、点Pが船体
に外接する回転楕円体面の外側に存在していれば、そこ
での磁位Fは
As shown in FIG. 2, points c1 and c2 are placed at both ends on the geometrical center line of the hull 2 of FIG. 1, and the spheroid coordinates (η, ξ, φ) with these points as the focal points are set. Set up. An arbitrary point P (η, ξ, φ) is a spheroidal surface η (η ≧
1), rotating hyperboloid ξ (-1 ≦ ξ ≦ 1) and half plane φ (0
≦ φ ≦ 2π). If the point P exists outside the spheroidal surface circumscribing the hull, the magnetic field F there is

【数1】 となり、長球調和関数の無限級数で展開することができ
る。
[Equation 1] And can be expanded by an infinite series of spherical spherical harmonics.

【0014】一方、点Pの回転楕円体座標(η,ξ,
φ)を直角座標で表すと
On the other hand, the coordinates of the spheroid of the point P (η, ξ,
φ) in Cartesian coordinates

【数2】 となる。[Equation 2] Becomes

【0015】したがって、各展開係数は船首の南北各方
位(船首を南向きに係留した場合と北向きに係留した場
合)において各磁気検出器7で測定されたデータを[数
1]を元にした負の導関数(磁位Fの負の導関数は磁界
に相当する)にあてはめることによって、最小2乗法に
より求めることができる。具体的な数値計算に当たって
は、nを適当な値に選ばなくてはならないが、関数が収
束した定量的な評価法としては、平均二乗誤差の測定磁
界最大値に対する相対値として求めることができる。こ
こで、平均二乗誤差σi
Therefore, each expansion coefficient is based on [Equation 1] based on the data measured by each magnetic detector 7 in each north-south direction of the bow (when the bow is moored in the south direction and in the north direction). It is possible to obtain by the method of least squares by applying the above-mentioned negative derivative (the negative derivative of the magnetic potential F corresponds to the magnetic field). In specific numerical calculation, n must be selected as an appropriate value, but as a quantitative evaluation method in which the function converges, it can be obtained as a relative value of the mean square error with respect to the maximum measured magnetic field value. Where the mean square error σ i is

【数3】 である。但し、Hi:各展開係数を用いて求めた計算
値、Hid:各磁気検出器7の測定値、N:測定数であ
り、i=X,Y,Zである。平均二乗誤差σiの測定磁界
最大値に対する相対値P(%)は P=(σi/Himax)×100 である。但し、Himax:測定磁界の最大値である。前記
平均二乗誤差σiと相対値Pは、各磁気検出器7のX方
向、Y方向及びZ方向の船体磁界測定値から、X方向、
Y方向及びZ方向のそれぞれについて求めることができ
る。
(Equation 3) It is. However, H i : a calculated value obtained by using each expansion coefficient, H id : a measured value of each magnetic detector 7, N: a measured number, and i = X, Y, Z. The relative value P (%) of the mean square error σ i with respect to the maximum value of the measured magnetic field is P = (σ i / H imax ) × 100. Where H imax is the maximum value of the measured magnetic field. The mean square error σ i and the relative value P are calculated based on the hull magnetic field measurement values of the magnetic detectors 7 in the X, Y and Z directions.
It can be obtained for each of the Y direction and the Z direction.

【0016】ここで、上記で求めた各展開係数はn=1
とすると
Here, each expansion coefficient obtained above is n = 1.
And

【数4】 となり、各展開係数は船体のX,Y,Z各方向の磁気モ
ーメントMx,My,Mzに対応している。
(Equation 4) Thus, each expansion coefficient corresponds to the magnetic moments M x , M y , and M z of the hull in the X, Y, and Z directions.

【0017】これら各方位において算出した各展開係数
は、永久磁気分と地球磁界による誘導磁気分に相当する
磁気モーメントが混在しており、前者は船体磁気の経時
変化等によって変化するが、後者は同一場所、同方向に
存在する限りほぼ一定とみなしてよい。
Each expansion coefficient calculated in each of these directions contains a magnetic moment corresponding to a permanent magnetic component and an induced magnetic component due to the earth's magnetic field. The former changes due to changes in ship magnetism over time, but the latter changes. As long as they exist in the same place and in the same direction, they may be regarded as almost constant.

【0018】したがって、船首尾線方向の磁気モーメン
トに相当する各展開係数を永久磁気分と誘導磁気分に分
離すると
Therefore, if each expansion coefficient corresponding to the magnetic moment in the direction of the bow and tail is separated into the permanent magnetic component and the induced magnetic component,

【数5】 となる。ここで、添字pは永久磁気分、添字iは誘導磁気
分を、N,Sは北、南方位(船首北向きに係留した場合
と南向きに係留した場合)においてそれぞれ算出した各
展開係数である。
(Equation 5) Becomes Here, the subscript p is the permanent magnetic component, the subscript i is the induced magnetic component, and N and S are the respective expansion coefficients calculated in the north and south directions (when moored to the north of the bow and moored to the south). is there.

【0019】これにより、船首尾線方向の永久磁気モー
メントに相当する展開係数
As a result, the expansion coefficient corresponding to the permanent magnetic moment in the bow and tail line direction

【数6】 が最小になるように通電を繰り返せば、船全体の船首尾
線方向の永久磁気が脱磁できる。
(Equation 6) By repeating the energization to minimize, the permanent magnetism in the bow-caudal direction of the entire ship can be demagnetized.

【0020】図3は、本発明に係る実施例の一連の手順
を示したフローチャートである。まず、船首が北及び南
向きになるように図1の船舶1を係留して、図3のステ
ップ#1を実行し、各磁気検出器7の測定値を測定室8
内のコンピュータに取り込む。そして、ステップ#2を
実行して各方位(船首北向きと南向き)における船底下
磁界の測定値から長球調和関数展開式による各展開係数
FIG. 3 is a flow chart showing a series of procedures of the embodiment according to the present invention. First, the ship 1 of FIG. 1 is moored so that the bow faces north and south, and step # 1 of FIG. 3 is executed to measure the measured values of the magnetic detectors 7 in the measurement chamber 8
To the computer inside. Then, step # 2 is executed and each expansion coefficient is calculated from the measured values of the magnetic field under the bottom of the ship in each direction (north and south of the bow) using the spherical harmonic expansion formula.

【数7】 を算出し、ステップ#3で船首尾線方向の誘導磁気分と
永久磁気分に分離する。
(Equation 7) Is calculated, and in step # 3, it is separated into an inductive magnetic component in the bow and tail line direction and a permanent magnetic component.

【数8】 ここで、その場所における地球磁界によって誘導される
前記誘導磁気分を図1の船体2に巻かれた胴巻線輪3に
通電することにより見かけ上零にする必要がある。その
ためにステップ#4を実行する。すなわち、前記誘導磁
気分を打ち消す電流値を決定するには、通電していない
状態の船底下磁界からある電流を通電した状態の船底下
磁界を差し引くことによって、胴巻線輪3による単位電
流当たりの起磁力が算出でき、前記誘導磁気分を消去す
る電流は起磁力に比例するので容易に決定できる。以
後、この誘導磁気分を消去する電流をベース電流と呼
ぶ。
(Equation 8) Here, it is necessary to make the induced magnetic component induced by the earth's magnetic field at that location apparently zero by energizing the body winding wheel 3 wound around the hull 2 of FIG. Therefore, step # 4 is executed. That is, in order to determine the current value for canceling the induced magnetic component, by subtracting the underfloor magnetic field under a certain current from the underfloor magnetic field under a non-energized state, The magnetomotive force can be calculated, and the current for eliminating the induced magnetic component is proportional to the magnetomotive force, so that it can be easily determined. Hereinafter, the current for erasing the induced magnetic component will be referred to as the base current.

【0021】この状態から、ステップ#5,#6,#
7,#8を実行する。すなわち、最大通電量、例えば+
3000A、次に−2800A、+2600Aというよ
うに極性を正負に変えながら、胴巻線輪3の電流の大き
さをある減衰率に従って漸減して、最終段階に近づくに
つれて上記で求めたベース電流を基準として漸減しなが
ら通電することは従来の技術と同じであるが、その過程
において、図4に示すように、各通電後に通電をオフし
て前記永久磁気分を算出し(ステップ#6)、その値を
常時監視しながら最小になるまで脱磁処理を実施するこ
とになる。ステップ#8で永久磁気分の最小値が得られ
たと判定したら、ステップ#9を実行して脱磁効果の合
否を判定し、永久磁気の脱磁が良好に行われたと判断さ
れた場合(例えば、前記永久磁気分が一定値以下の場
合)に処理が終了する。
From this state, steps # 5, # 6, #
7 and # 8 are executed. That is, the maximum energization amount, for example +
While changing the polarity to positive / negative such as 3000A, then −2800A, + 2600A, the magnitude of the current of the body winding wheel 3 is gradually reduced according to a certain attenuation rate, and the base current obtained above is used as a reference as approaching the final stage. Energizing while gradually decreasing is the same as the conventional technique, but in the process, as shown in FIG. 4, energization is turned off after each energization to calculate the permanent magnetic component (step # 6), and the value is calculated. Will be constantly monitored, and demagnetization processing will be carried out until it becomes minimum. If it is determined in step # 8 that the minimum value of the permanent magnetism has been obtained, step # 9 is executed to determine whether or not the demagnetization effect is successful, and it is determined that the demagnetization of the permanent magnetism has been performed satisfactorily (for example, If the permanent magnetic component is less than a certain value), the process ends.

【0022】図3に示す一連の作業はコンピュータを活
用することによりシステムの自動化が図れる。
The series of operations shown in FIG. 3 can be automated by utilizing a computer.

【0023】[0023]

【発明の効果】以上説明したように、本発明に係る船舶
の永久磁気脱磁方法によれば、脱磁状況を船体全体の磁
気モーメントとして算出するので、永久磁気モーメント
を定量的に把握することが可能となり、それにより最適
な脱磁処理が実施でき、脱磁効果の向上が図れる。ま
た、この脱磁処理は、コンピュータを用いて自動化する
のに適し、作業者の高度の熟練が不要となり、コンピュ
ータ導入による作業の効率化を図ることができる。
As described above, according to the permanent magnetic demagnetization method for a ship according to the present invention, the demagnetization state is calculated as the magnetic moment of the entire hull, so that the permanent magnetic moment can be quantitatively grasped. This makes it possible to carry out an optimum demagnetization treatment and improve the demagnetization effect. Further, this demagnetization process is suitable for automation using a computer, does not require a high level of skill of an operator, and can improve the efficiency of the work by introducing the computer.

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

【図1】本発明に係る船舶の永久磁気脱磁方法の実施例
で用いる船舶の永久磁気脱磁処理施設の概略図である。
FIG. 1 is a schematic view of a permanent magnetic demagnetization treatment facility for a ship used in an embodiment of a ship permanent magnetic demagnetization method according to the present invention.

【図2】船体磁気モーメントを算出する数学モデルを示
す説明図である。
FIG. 2 is an explanatory diagram showing a mathematical model for calculating a ship magnetic moment.

【図3】本発明の実施例のフローチャート図である。FIG. 3 is a flowchart of an embodiment of the present invention.

【図4】船舶の脱磁処理の過程における船首尾線方向の
永久磁気の減衰状況を示した説明図である。
FIG. 4 is an explanatory diagram showing a decay state of permanent magnetism in the bow-tail direction in the course of demagnetization processing of the ship.

【符号の説明】[Explanation of symbols]

1 船舶 2 船体 3 胴巻線輪 7 磁気検出器 1 Ship 2 Hull 3 Body Winding Wheel 7 Magnetic Detector

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】 船舶の磁性体からなる船体に幾巻きかの
胴巻線輪を装着し、該胴巻線輪に、電流の極性を正負に
変えながら当該電流の大きさを漸減して通電することに
より、船首尾線方向の永久磁気を消去する過程におい
て、船体の磁界を複数個の磁気検出器により測定し、前
記複数個の磁気検出器の測定値に基づいて船首尾線方向
の永久磁気モーメントを定量的に算出して、該永久磁気
モーメントの値を監視しながら最小にすることを特徴と
する船舶の永久磁気脱磁方法。
1. A hull made of a magnetic material of a ship, to which several body winding wheels are attached, and the body winding wheel is energized by gradually reducing the magnitude of the current while changing the polarity of the current to positive or negative. Thus, in the process of erasing the permanent magnetism in the bow-tail direction, the magnetic field of the hull is measured by a plurality of magnetic detectors, and the permanent magnetic moment in the bow-tail direction is measured based on the measured values of the plurality of magnetic detectors. Is calculated quantitatively and is minimized while monitoring the value of the permanent magnetic moment.
JP7182129A 1995-06-26 1995-06-26 Permanent magnetic demagnetization method for ships Expired - Lifetime JP2893165B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP7182129A JP2893165B2 (en) 1995-06-26 1995-06-26 Permanent magnetic demagnetization method for ships

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP7182129A JP2893165B2 (en) 1995-06-26 1995-06-26 Permanent magnetic demagnetization method for ships

Publications (2)

Publication Number Publication Date
JPH092385A true JPH092385A (en) 1997-01-07
JP2893165B2 JP2893165B2 (en) 1999-05-17

Family

ID=16112843

Family Applications (1)

Application Number Title Priority Date Filing Date
JP7182129A Expired - Lifetime JP2893165B2 (en) 1995-06-26 1995-06-26 Permanent magnetic demagnetization method for ships

Country Status (1)

Country Link
JP (1) JP2893165B2 (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2007106140A (en) * 2005-10-11 2007-04-26 Yo Engineering Kk Demagnetization processing system for vessel
JP2007237997A (en) * 2006-03-10 2007-09-20 Hitachi Ltd Magnetic processing system, and magnetism control device
KR20190085405A (en) * 2018-01-10 2019-07-18 국방과학연구소 Apparatus and method for controlling deperm, deperming apparatus and deperming method

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6445108A (en) * 1987-08-13 1989-02-17 Shimadzu Corp Treatment of magnetism of magnetic body
JPH04182129A (en) * 1990-11-16 1992-06-29 Tokai Shoji Kk Full automatic screen printer

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6445108A (en) * 1987-08-13 1989-02-17 Shimadzu Corp Treatment of magnetism of magnetic body
JPH04182129A (en) * 1990-11-16 1992-06-29 Tokai Shoji Kk Full automatic screen printer

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2007106140A (en) * 2005-10-11 2007-04-26 Yo Engineering Kk Demagnetization processing system for vessel
JP2007237997A (en) * 2006-03-10 2007-09-20 Hitachi Ltd Magnetic processing system, and magnetism control device
KR20190085405A (en) * 2018-01-10 2019-07-18 국방과학연구소 Apparatus and method for controlling deperm, deperming apparatus and deperming method

Also Published As

Publication number Publication date
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