JPS5830557B2 - How to detect magnetic substances - Google Patents

How to detect magnetic substances

Info

Publication number
JPS5830557B2
JPS5830557B2 JP54069952A JP6995279A JPS5830557B2 JP S5830557 B2 JPS5830557 B2 JP S5830557B2 JP 54069952 A JP54069952 A JP 54069952A JP 6995279 A JP6995279 A JP 6995279A JP S5830557 B2 JPS5830557 B2 JP S5830557B2
Authority
JP
Japan
Prior art keywords
magnetic field
magnetic
axis
curve
detection output
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
JP54069952A
Other languages
Japanese (ja)
Other versions
JPS55162078A (en
Inventor
富代 山洞
祐司 野沢
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.)
Kyosan Electric Manufacturing Co Ltd
Original Assignee
Kyosan Electric Manufacturing Co Ltd
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 Kyosan Electric Manufacturing Co Ltd filed Critical Kyosan Electric Manufacturing Co Ltd
Priority to JP54069952A priority Critical patent/JPS5830557B2/en
Publication of JPS55162078A publication Critical patent/JPS55162078A/en
Publication of JPS5830557B2 publication Critical patent/JPS5830557B2/en
Expired legal-status Critical Current

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  • Geophysics And Detection Of Objects (AREA)

Description

【発明の詳細な説明】 本発明は磁性体が定点から一定範囲内を通過したかどう
かを磁性体通過物体の大小にかかわらず正確に検出する
方法(こ関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method for accurately detecting whether a magnetic body has passed within a certain range from a fixed point, regardless of the size of the object passing through the magnetic body.

地磁気中の強磁性体は磁性体自身の磁化あるいは、地磁
気によって磁化されている。
A ferromagnetic substance in the earth's magnetism is magnetized by the magnetic substance itself or by the earth's magnetism.

従がって、磁性体からの磁気を検出して、当該磁性体物
体の存否を検出することができるが、磁性体の磁化の程
度がさまざまの場合には検知器の側方どの程度の距離を
通過したかを検出することは不可能であった。
Therefore, it is possible to detect the presence or absence of a magnetic object by detecting the magnetism from a magnetic material, but if the degree of magnetization of the magnetic material varies, the distance to the side of the detector may vary. It was impossible to detect what had passed.

たとえば、磁界検知器がある一定のレベルで待ち受けて
いる場合、磁性体が一定の側方距離を通過しても、磁性
体が大きい場合は十分検出するが、小さい場合は検出で
きない。
For example, if a magnetic field detector is waiting at a certain level, even if a magnetic object passes a certain lateral distance, it will be sufficiently detected if the magnetic object is large, but it will not be detected if it is small.

本発明はかかる点に注目し、磁性体の通過物体の大小に
かかわらず、測定位置から水平方向一定の範囲内を通過
した場合に確実に検出する磁性体の検出方法を提供する
ものである。
The present invention has focused on this point, and provides a method for detecting a magnetic body that reliably detects an object passing within a certain range in the horizontal direction from a measurement position, regardless of the size of the object passing through the magnetic body.

以下本発明の実施例を具体的に説明する。Examples of the present invention will be specifically described below.

今磁気能率Mを持った磁性体があり、その位置を直交座
標の原点にとり、磁性体から距離rを離れた点Pの磁位
は■は(1)式となる。
Now, there is a magnetic body with a magnetic efficiency M, and if its position is taken as the origin of the rectangular coordinates, the magnetic potential at a point P at a distance r from the magnetic body is expressed by equation (1).

ここで12 + m 、 nは磁気能率Mのy軸、y軸
、軸えの方向余弦である。
Here, 12 + m and n are the y-axis of the magnetic efficiency M, the y-axis, and the direction cosine of the axis.

またP点のy軸、y軸、Z軸の磁界成分HxHy、Hz
、は(2)式のよう(こなる。
In addition, the magnetic field components HxHy, Hz of the y-axis, y-axis, and Z-axis at point P
, is as shown in equation (2).

ここで2式を計算して、 Hx 、 Hy 、Hzは(3)式 %式% ここで説明上第1図のごとく水平のアクリル板1の下に
垂直に取付けた磁界検知子2と水平に取付けた磁界検知
子Xを設け、アクリル板1の上を磁性体の小磁石4をX
方向に平行Qこ置きX方向に移動させX軸上から順次y
方向にづらしてX方向(こ移動させた場合を考える。
Here, calculate Hx, Hy, and Hz using the formula (3) (% formula) For the sake of explanation, as shown in Figure 1, the magnetic field detector 2 is installed vertically under the horizontal acrylic plate 1, and the magnetic field detector 2 is installed horizontally. Install the attached magnetic field detector X, and place a small magnetic magnet 4 on the acrylic plate 1
Parallel to the direction Q
Consider the case where the object is moved in the X direction.

この場合磁気能率Mの方向がX方向を向いているので(
3)式OこA=1 、m=n=0と置いて、Z軸の磁界
成分Hzは(4)式のようになる。
In this case, the direction of magnetic efficiency M is in the X direction, so (
3) Setting the formula OkoA=1 and m=n=0, the Z-axis magnetic field component Hz becomes as shown in formula (4).

となる。becomes.

第2図はMを任意の値とし、y二〇CTL1およびy
= 30 cm、のときの移動方向Xに対するZ軸の磁
界成分Hzと、Xの磁界成分Hxの曲線であり、曲線5
はy = Ocm、曲線6はy=−30cTLのXHz
曲線であり、曲線7はy−OCrrL1曲線3はy二3
0CTlのときのx−Hx曲線である。
In Figure 2, M is an arbitrary value, y20CTL1 and y
= 30 cm, it is a curve of the magnetic field component Hz of the Z axis with respect to the moving direction X and the magnetic field component Hx of X, and the curve 5
is y = Ocm, curve 6 is XHz of y = -30cTL
Curve 7 is y-OCrrL1 Curve 3 is y23
This is an x-Hx curve at 0CTl.

y=Oc1′rLの曲線4においてHzの最大値はA1
点であり、65 m G (ミリガウス)である。
In curve 4 of y=Oc1'rL, the maximum value of Hz is A1
point, 65 mG (milligauss).

そのときのHxは曲線6のA2点であり、12mGであ
る。
Hx at that time is point A2 of curve 6, which is 12 mG.

又y30cIrLの曲線6においてHzの最大値は81
点であり、35mGである。
Also, the maximum value of Hz in curve 6 of y30cIrL is 81
point and is 35mG.

そのときのHxは曲線8のB2点であり22ミリガウス
である。
Hx at that time is point B2 of curve 8 and is 22 milligauss.

このようにy=10Cr/′L、 y=20cmのとき
のHzの最大値(Hz)maxをHxの値を計算し、y
=OCr/′L1y=10crrL、 y=20crr
L、 y=30cm、のときの(Hz )max/Hx
を求め、y 二〇 cmのときの(Hz )max/H
zを100%としてy−10CrrL1y=20Cr/
′L、y=307mの比を求めると下表の表1のように
なる。
In this way, calculate the maximum value of Hz (Hz) max when y = 10Cr/'L and y = 20 cm, and calculate the value of Hx, and set y
=OCr/'L1y=10crrL, y=20crr
(Hz)max/Hx when L, y=30cm
Find (Hz)max/H when y is 20 cm
y-10CrrL1y=20Cr/, where z is 100%
The ratio of 'L, y=307m is determined as shown in Table 1 below.

表1から比の値が69.6%以上であるときのみを選べ
ば、側方距離が20crI1以内であることが判定でき
る。
If only the cases where the ratio value is 69.6% or more are selected from Table 1, it can be determined that the lateral distance is within 20 crI1.

又別の磁気能力をもった小磁石の場合でも表1の(Hz
)max/Hxの値を満足する。
In addition, even in the case of a small magnet with a different magnetic ability, the (Hz
) satisfies the value of max/Hx.

従って通過する磁性体の大小に関係なく、すなわち磁気
能率の大小Gこ関係なく、磁界検知器からの側方距離一
定範囲内を通過した場合の検出が可能である。
Therefore, regardless of the size of the passing magnetic body, that is, regardless of the magnitude of the magnetic efficiency, detection is possible when the magnetic body passes within a certain range of lateral distance from the magnetic field detector.

上記実施例では磁性体小磁石をX軸に平行に置きX軸(
こ平行に移動させて説明したが、磁性体小磁石の移動方
向がX軸に平行でなく、X軸y軸からなる水平面と平行
に移動した場合には、(B2)maxと Hx +Hy
との比を求めれば実施例同様に、磁界検知器の配置さ
れたX軸y軸の水平面の原点から、X軸y軸からなる水
平面に平行な平面内の水平方向一定の距離範囲内を磁性
体が通過した場合の検出が可能である。
In the above embodiment, a small magnetic magnet is placed parallel to the X axis (
Although the explanation was given by moving the small magnet parallel to this, if the moving direction of the small magnetic magnet is not parallel to the X axis but parallel to the horizontal plane consisting of the X and y axes, (B2) max and Hx + Hy
As in the example, if we calculate the ratio of It is possible to detect when a body passes through.

又小磁石磁性体がX軸y軸2軸Gこ対して一定の傾きを
もっている場合には、理論的には(3)式(こ方向余弦
z 、 m 、 nの値を代入し、(Hz)maxと
Hx +Hy0との比を求めることにより説明づけられ
、この場合でも、磁界検知器の配置されたX軸y軸の原
点から、X軸y軸からなる水平面Gこ平行な平面内の、
水平方向一定距離範囲内を磁性体が通過した場合の検出
が可能である。
In addition, if the magnetic material of the small magnet has a certain inclination with respect to the )max and
This can be explained by finding the ratio of Hx + Hy0, and in this case, in a plane parallel to the horizontal plane G consisting of the X and y axes from the origin of the X and y axes where the magnetic field detector is placed,
Detection is possible when a magnetic body passes within a certain distance range in the horizontal direction.

上記の実施例を実験したところ表1の値を十分満足した
値が得られた。
When the above examples were tested, values that fully satisfied the values in Table 1 were obtained.

本発明は以上のように、水平面上を通過する磁性体が、
磁性体の大小にかかわらず、測定地点から水平方向一定
の範囲内を通過した場合に確実に検出する磁性体の検出
方法であり、磁界検知器を海中に沈めて、海面上一定の
範囲を通過する船を検出する等その応用範囲は広いもの
である。
As described above, in the present invention, a magnetic body passing on a horizontal plane,
Regardless of the size of the magnetic object, it is a detection method that reliably detects magnetic objects when they pass within a certain range in the horizontal direction from the measurement point. Its range of applications is wide, including detecting ships that are moving.

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

第1図は本発明実施例の説明図であり、1はアクリル板
、2,3は磁界検知子、4は小磁石を示す。 第2図はy = 0 (m、およびy=30cIrLの
ときの移動方向X(こ対するZ軸の磁界成分Hzと、移
動方向Xに対するXの磁界成分Hxの曲線であり曲線5
はy−OCIrL1曲線6はy−30c/rtのXHz
曲線、曲線γはy = Ocm、曲線8はy−307の
ときのx −Hx曲線である。
FIG. 1 is an explanatory diagram of an embodiment of the present invention, in which 1 represents an acrylic plate, 2 and 3 represent magnetic field detectors, and 4 represents a small magnet. Figure 2 is a curve of the magnetic field component Hz of the Z axis in the moving direction X (against the moving direction X) and the magnetic field component Hx of X in the moving direction
is y-OCIrL1 curve 6 is y-30c/rt XHz
The curve γ is the x-Hx curve when y=Ocm, and the curve 8 is y-307.

Claims (1)

【特許請求の範囲】[Claims] 1 z軸を垂直にもつ直角座標のX軸y軸2軸の各々の
軸上に指向性を有する磁界検知子を配置し、水平面上を
任意の方向に移動する磁化している磁性体からの磁界を
上記配置された磁界検知子で同時に検知し、Z軸の磁界
検知子の検知出力が正又は負の最大値になったときの上
記Z軸の磁界検知出力値と、そのときの上記x m y
軸上の磁界検知出力値から求められる水平面の磁界検知
出力値の絶対値との比を計算することにより、上記水平
面の原点から上記水平面上の一定距離範囲内の磁性体の
通過の有無を検出することを特徴とした磁性体の検出方
法。
1. Magnetic field detectors with directivity are placed on each of the two axes of the X, Y, and 2 axes of rectangular coordinates with the Z axis perpendicular, and magnetic field detectors with directivity are placed on each of the two axes of rectangular coordinates with the Z axis perpendicular. The magnetic field is simultaneously detected by the magnetic field detector arranged above, and the Z-axis magnetic field detection output value when the detection output of the Z-axis magnetic field detector reaches the maximum positive or negative value, and the above x at that time. m y
By calculating the ratio of the absolute value of the magnetic field detection output value on the horizontal plane determined from the magnetic field detection output value on the axis, it is detected whether or not a magnetic material has passed within a certain distance range on the horizontal plane from the origin of the horizontal plane. A method for detecting magnetic substances characterized by:
JP54069952A 1979-06-06 1979-06-06 How to detect magnetic substances Expired JPS5830557B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP54069952A JPS5830557B2 (en) 1979-06-06 1979-06-06 How to detect magnetic substances

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP54069952A JPS5830557B2 (en) 1979-06-06 1979-06-06 How to detect magnetic substances

Publications (2)

Publication Number Publication Date
JPS55162078A JPS55162078A (en) 1980-12-17
JPS5830557B2 true JPS5830557B2 (en) 1983-06-29

Family

ID=13417489

Family Applications (1)

Application Number Title Priority Date Filing Date
JP54069952A Expired JPS5830557B2 (en) 1979-06-06 1979-06-06 How to detect magnetic substances

Country Status (1)

Country Link
JP (1) JPS5830557B2 (en)

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6261285A (en) * 1985-09-10 1987-03-17 サン−ゴバン ビトラ−ジユ Electric heating window glass for automobile
JPS62150658U (en) * 1986-03-14 1987-09-24
JPS6322725A (en) * 1986-06-26 1988-01-30 ピルキントン・ブラザ−ズ・ピ−エルシ− Glass window module, end edge of which is wrapped
JPS6369393U (en) * 1986-10-21 1988-05-10
JPH043851Y2 (en) * 1985-05-22 1992-02-05

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0274892A (en) * 1988-09-10 1990-03-14 Kyosan Electric Mfg Co Ltd Method and apparatus for detecting overhead passage of magnetic body
JPH0786532B2 (en) * 1990-03-30 1995-09-20 株式会社日立製作所 Magnetic substance detection method

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH043851Y2 (en) * 1985-05-22 1992-02-05
JPS6261285A (en) * 1985-09-10 1987-03-17 サン−ゴバン ビトラ−ジユ Electric heating window glass for automobile
JPS62150658U (en) * 1986-03-14 1987-09-24
JPS6322725A (en) * 1986-06-26 1988-01-30 ピルキントン・ブラザ−ズ・ピ−エルシ− Glass window module, end edge of which is wrapped
JPS6369393U (en) * 1986-10-21 1988-05-10

Also Published As

Publication number Publication date
JPS55162078A (en) 1980-12-17

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