JPH0341387A - Detection coil of article discrimination instrument - Google Patents

Detection coil of article discrimination instrument

Info

Publication number
JPH0341387A
JPH0341387A JP1175940A JP17594089A JPH0341387A JP H0341387 A JPH0341387 A JP H0341387A JP 1175940 A JP1175940 A JP 1175940A JP 17594089 A JP17594089 A JP 17594089A JP H0341387 A JPH0341387 A JP H0341387A
Authority
JP
Japan
Prior art keywords
detection coil
magnetic
coil
belt
diameter
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
JP1175940A
Other languages
Japanese (ja)
Inventor
Osamu Saito
修 斎藤
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.)
Fuji Electric Co Ltd
Original Assignee
Fuji Electric 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 Fuji Electric Co Ltd filed Critical Fuji Electric Co Ltd
Priority to JP1175940A priority Critical patent/JPH0341387A/en
Publication of JPH0341387A publication Critical patent/JPH0341387A/en
Pending legal-status Critical Current

Links

Landscapes

  • Geophysics And Detection Of Objects (AREA)

Abstract

PURPOSE:To enable a detection coil to be arranged so that a stable output voltage can be taken out by calculating and setting the diameter of the detection coil such that maximum output can be obtained. CONSTITUTION:The integral value phi of the normal component of a magnetic field vector in the direction of the center line of a detection coil 7 is represented by the function of the diameter (r) of the coil 7, that is, phi=F(r) can hold. Since the peak value of an output voltage is proportional to the value phi, the diameter (r0) of the coil 7 at which the output voltage takes the maximum value can be calculated from an expression phimax=F(r0) (phimax: maximum value of phi). Taking a fact into consideration that, when only one pair of the coils 7 with the diameters (r0) are used, the diameter (r0) of the coil 7 is too small as compared with the width of a belt and the output voltage is not generated depending on the passing position of a magnet marker 1, a plurality of pairs of the coils 7 should be arranged in the direction of the belt width. Thus, even when the marker 1 passes an AC magnetic field in any position above the belt, a stable and large output can be secured.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は物品にマーカーをとりつけ、その物品の数量や
種類を識別する装置に用いられる検出コイルに関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a detection coil used in a device for attaching a marker to an article and identifying the quantity and type of the article.

〔従来の技術〕[Conventional technology]

物品にマーカーをとりつけ、このマーカーをその物品の
数量や種類を検出、もしくは物品の盗難防止に利用する
ことが知られている。例えばアモルファス磁性薄帯や細
線をマーカーとして取り付けた物品を交流磁場を通過さ
せ、そのとき生ずる磁場の変動を検出する装置が用いら
れており、第8図はその装置の主な構成部を示した模式
図である。第8図において、アモルファス磁性薄帯また
は細線の磁気マーカー1の貼付された物品2が二つの滑
車3に張られているヘルド4上にあり、滑車3の回転に
よってベルト4の走行とともに矢印方向に移動する。
It is known to attach a marker to an article and use the marker to detect the quantity or type of the article or to prevent the article from being stolen. For example, a device is used that passes an alternating current magnetic field through an article to which an amorphous magnetic ribbon or thin wire is attached as a marker, and detects the fluctuations in the magnetic field that occur. Figure 8 shows the main components of this device. It is a schematic diagram. In FIG. 8, an article 2 to which an amorphous magnetic ribbon or thin wire magnetic marker 1 is attached is placed on a heald 4 stretched between two pulleys 3, and as the belt 4 runs due to the rotation of the pulleys 3, it moves in the direction of the arrow. Moving.

磁気マーカー1は例えばCo基アモルファス合金などの
磁性薄帯または細線からなり、そのB−H曲線は第9図
に示したような角形の特性を持つものが用いられる。こ
の磁気マーカーlを検出体である物品2に1本もしくは
複数本を貼着するが、状況に応じて磁気マーカー1をプ
ラスチック材料などに固定した検出素子として用いるこ
ともできる。
The magnetic marker 1 is made of a magnetic ribbon or thin wire made of, for example, a Co-based amorphous alloy, and its B-H curve has a rectangular characteristic as shown in FIG. 9. One or more magnetic markers 1 are attached to an article 2 as a detection object, but depending on the situation, the magnetic marker 1 can also be used as a detection element fixed to a plastic material or the like.

? 交流磁界を発生する励磁コイル5が交流発振器6に接続
され、交流磁界によって生ずる磁気マーカー1の磁化反
転に伴なう磁束変化を、誘導起電圧として検出する検出
コイル7が計測器8に接続されている。励磁コイル5.
交流発振器6.検出コイル7および計測器8については
第10図(81,(b)にもそれぞれ拡大図として示し
た。検出コイル7は励磁コイル5によって検出コイル7
自体に発生する誘導起電圧を打ち消すために双子コイル
としである。計測器8は検出コイル7に生したパルス電
圧列をパターン認識により識別するものである。
? An excitation coil 5 that generates an alternating magnetic field is connected to an alternating current oscillator 6, and a detection coil 7 that detects as an induced electromotive voltage a change in magnetic flux accompanying magnetization reversal of the magnetic marker 1 caused by the alternating magnetic field is connected to a measuring device 8. ing. Excitation coil5.
AC oscillator6. The detection coil 7 and the measuring device 8 are also shown as enlarged views in FIG. 10 (81, (b)).The detection coil 7 is
Twin coils are used to cancel the induced electromotive force generated within the coil itself. The measuring device 8 identifies the pulse voltage train generated in the detection coil 7 by pattern recognition.

第11図(a)、(b)は検出コイル7に誘起されるパ
ルス電圧波形図であり、第11図(a)は1本の磁気マ
ーカー1.第11図(blは複数本の磁気マーカー1を
用いた場合を示す。
11(a) and 11(b) are pulse voltage waveform diagrams induced in the detection coil 7, and FIG. 11(a) shows one magnetic marker 1. FIG. 11 (bl shows the case where a plurality of magnetic markers 1 are used.

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

しかしながら、第8図に示した装置には検出コイル7に
関して次のような問題がある。
However, the device shown in FIG. 8 has the following problem regarding the detection coil 7.

即ち、第8図の装置では、検出コイル7は双子コイルと
して、ただ−組だけが物品2の通過するベルト4の下方
に設けられており、しかもその径を任意の大きさとして
いるため、必ずしも最大出力電圧が得られていないこと
と、磁気マーカー1を貼着した物品2の置かれる位置や
方向は必ずしも一定になっていないから、励磁コイル5
で発生する交流磁界領域を磁気マーカー1が通過すると
き、その位置、方向によって検出コイル7からの出力が
不安定になることである。
That is, in the apparatus shown in FIG. 8, the detection coil 7 is a twin coil, and only one set is provided below the belt 4 through which the article 2 passes, and its diameter is set to an arbitrary size. The excitation coil 5
When the magnetic marker 1 passes through an alternating current magnetic field region generated in the magnetic field, the output from the detection coil 7 becomes unstable depending on its position and direction.

本発明は上述の欠点を除去するためになされたものであ
り、その目的は最大出力が得られるように検出コイルの
直径を定めるとともに、磁気マーカーが貼着された物品
のベルト上に置かれる位置や方向の如何に拘らず、安定
な出力電圧を取り出すことができるように配置した物品
識別装置の検出コイルを提供することにある。
The present invention has been made to eliminate the above-mentioned drawbacks, and its purpose is to determine the diameter of the detection coil in such a way that maximum output is obtained and the position at which the magnetic marker is placed on the belt of the article affixed to it. It is an object of the present invention to provide a detection coil for an article identification device that is arranged so that a stable output voltage can be extracted regardless of the direction or orientation.

〔課題を解決するための手段〕[Means to solve the problem]

上記の課題を解決するために本発明の物品識別装置は、
最大出力が得られるように直径を算出した検出コイルを
用いて2個一対とし、ベルトの幅方向に複数対を配置し
たものである。
In order to solve the above problems, the article identification device of the present invention includes:
Detection coils whose diameters are calculated so as to obtain maximum output are used in pairs, and a plurality of pairs are arranged in the width direction of the belt.

〔作用〕[Effect]

検出コイルの中心線方向の磁界ベクトルの垂直成分であ
るHよの積分値Φは検出コイルの径rの関数で表わされ
、Φ−F (r)とおくことができ、このΦと出力電圧
のピーク値は比例関係にあるから、出力電圧が最大値と
なる検出コイルの径r0ば、Φの最大値Φ、−X= F
 (ro)から算出するこができる。モしてr。の径を
持つ検出コイルを2個一対として一対用いるだけでは、
検出コイルの径r。がベルトの幅に対して小さくなり、
磁気マーカーの通過位置によっては出力電圧が発生しな
くなる点を考慮して、この検出コイルをベルトの幅方向
に複数対配置することによって、磁気マーカーがベルト
上の如何なる位置で交流磁界中を通過しても、常に安定
な大きな出力を確保することができる。
The integral value Φ of H, which is the vertical component of the magnetic field vector in the direction of the center line of the detection coil, is expressed as a function of the diameter r of the detection coil, and can be set as Φ - F (r), and this Φ and the output voltage Since the peak value of is in a proportional relationship, if the diameter r0 of the detection coil where the output voltage is the maximum value is the maximum value of Φ, -X = F
It can be calculated from (ro). Mote r. Simply using a pair of detection coils with a diameter of
Diameter r of detection coil. becomes smaller relative to the belt width,
Considering that the output voltage may not be generated depending on the position where the magnetic marker passes, by arranging multiple pairs of detection coils in the width direction of the belt, it is possible to detect whether the magnetic marker passes through the alternating current magnetic field at any position on the belt. It is possible to always ensure a stable and large output even when the output is high.

〔実施例〕〔Example〕

以下、本発明を図面を参照して実施例に基づき説明する
Hereinafter, the present invention will be explained based on examples with reference to the drawings.

初めに検出コイル7の直径の大きさを決める手順を述べ
るために、磁気マーカー1から発生する磁束と検出コイ
ル7との関係を表わす模式図を第1図に示す。第1図で
はただ1個の検出コイル7を床面に平行に切断した斜視
図として示しであるが、第8図で述べたようにベルト4
上を走行する磁気マーカー1は、励磁コイル5により磁
化されて磁力m9を発生する。検出コイル7上に描いた
ベクトルは磁界強度Hで、検出コイル7の床面に対して
垂直な方向の成分H□を、斜線で示した領域について積
分した値Φと、検出コイル7に発生する誘導起電圧eは
次式で表わすことができる。
First, in order to describe the procedure for determining the diameter of the detection coil 7, a schematic diagram showing the relationship between the magnetic flux generated from the magnetic marker 1 and the detection coil 7 is shown in FIG. Although FIG. 1 shows only one detection coil 7 as a perspective view cut parallel to the floor, as described in FIG.
The magnetic marker 1 traveling above is magnetized by the excitation coil 5 and generates a magnetic force m9. The vector drawn on the detection coil 7 is the magnetic field strength H, and the component H□ in the direction perpendicular to the floor surface of the detection coil 7 is integrated over the shaded area, and the value Φ is generated in the detection coil 7. The induced electromotive voltage e can be expressed by the following equation.

dΦ e= −N         tl) dt 但し、Nは検出コイルの巻数 したがって、誘導起電圧e即ち磁気マーカー1により検
出コイル7に発生するパルス電圧の絶対値回は、dtを
一定とするとdΦが大きい程大きくなる。Φは前述のよ
うに、斜線部分の点Xにおける磁界強度Hの垂直方向成
分H工を斜線領域について積分した値であるから、Φの
大きさは検出コイル7の径に依存し、検出コイル7の径
でパルスミ圧のピーク値が異なる。
dΦ e= -N tl) dt However, N is the number of turns of the detection coil. Therefore, the induced electromotive force e, that is, the absolute value of the pulse voltage generated in the detection coil 7 by the magnetic marker 1, will increase as dΦ increases, assuming that dt is constant. growing. As mentioned above, Φ is the value obtained by integrating the vertical component H of the magnetic field strength H at the point The peak value of the pulse wave pressure differs depending on the diameter.

第2図はベルト4上の磁気マーカー1 (物品2は図示
を省略する)と1個の検出コイル7の位置関係を示した
模式斜視図であり、磁気マーカーlの一端の真下に検出
コイル7aの中心が位置し、その位置で検出コイル7a
の径が7bまで変化したとき、Φは式(2)〜(5)か
ら計算により求められ、第3図(alに式(2)〜(5
)に用いられるH I+ H!+ Hよのベクトル図を
示し、第3図(1))はその拡大図として示したもので
ある。
FIG. 2 is a schematic perspective view showing the positional relationship between the magnetic marker 1 on the belt 4 (the article 2 is not shown) and one detection coil 7. The center of the detection coil 7a is located at that position.
When the diameter of
) used for H I+ H! +H vector diagram is shown, and Fig. 3 (1)) is shown as an enlarged view.

φ=μf f HA d s        −−−−
・−・・・−(2)H=H+ Xcos θ、 +Hz
 Xcos θz ’−’−−−−−’(31l 但し、μ:透磁率、  m、:磁荷 r、:A、x間距離+ rz: B1  X間距離θ、
:Hlと第1図斜線部の法線とのなす角θ2 :H2と
第1図斜線部の法線とのなす角kI :定数 第4図は式(2)〜(5)を用いて算出したΦと検出コ
イル7の径との関係を示した線図であり、Φが最大とな
る最適検出コイル径r0があることがわかる。
φ=μf f HA ds -----
・−・・・−(2) H=H+ Xcos θ, +Hz
Xcos θz '-'-------' (31l, μ: magnetic permeability, m,: magnetic charge r,: A, distance between x + rz: B1 distance between X, θ,
: Angle θ2 between Hl and the normal to the shaded area in Figure 1 : Angle kI between H2 and the normal to the shaded area in Figure 1 : Constant Figure 4 is calculated using equations (2) to (5) It is a diagram showing the relationship between Φ and the diameter of the detection coil 7, and it can be seen that there is an optimum detection coil diameter r0 at which Φ is maximum.

したがって、出力の大きいパルス電圧を得るためには、
Φを計算することにより検出コイル径の最適値r0を決
定することができる。
Therefore, in order to obtain a pulse voltage with a large output,
By calculating Φ, the optimum value r0 of the detection coil diameter can be determined.

第5図(111〜(C1は検出コイル7の縦断面図に、
磁気マーカー1および磁気マーカー1から発生する磁力
線9を併記した模式図である。第5図(a)は検出コイ
ル7が磁気マーカー1に対して大き過ぎる場合であり、
磁力線9が互いに検出コイル7の断面図と逆方向に交差
する箇所が生しるため、Φはその最大値Φ、□より小さ
くなる。第5図中)は検出コイル7がほぼ最適な大きさ
の径を持ち、ΦはΦ□つとなる。第5図fc)は検出コ
イル7が磁気マーカー1に対して小さ過ぎ、検出コイル
7の断面部も小さくなるのでΦはΦ、Xより小さい。そ
こで本発明では第5図中)のように磁気マーカー1に対
してΦが最も大きな値となるときの検出コイル径r0を
計算から求め、検出コイル7の大きさを決定することに
より、物品識別装置の出力を高め安定させることができ
るのである。
FIG. 5 (111-(C1 is a vertical cross-sectional view of the detection coil 7,
2 is a schematic diagram showing a magnetic marker 1 and lines of magnetic force 9 generated from the magnetic marker 1. FIG. FIG. 5(a) shows a case where the detection coil 7 is too large for the magnetic marker 1,
Since there are places where the lines of magnetic force 9 cross each other in directions opposite to the cross-sectional view of the detection coil 7, Φ becomes smaller than its maximum value Φ, □. In FIG. 5), the detection coil 7 has a diameter of approximately the optimum size, and Φ becomes Φ□. In FIG. 5fc), the detection coil 7 is too small relative to the magnetic marker 1, and the cross section of the detection coil 7 is also small, so Φ is smaller than Φ and X. Therefore, in the present invention, as shown in FIG. This makes it possible to increase and stabilize the output of the device.

しかしながら、以上の如く検出コイル7の径を最適な値
に設定することができても、磁気マーカー1のベルト4
上を通過する位置によっては、双子コイルを一対だけ用
いたのでは出力が得られない場合が生ずる。次にこれに
対処する手段について述べる。
However, even if the diameter of the detection coil 7 can be set to an optimal value as described above, the belt 4 of the magnetic marker 1
Depending on the position over which the coil passes, there may be cases where no output can be obtained by using only one pair of twin coils. Next, we will discuss ways to deal with this.

第6図(alはベルト4上の磁気マーカー1 (物品2
は図示を省略)と一対の検出コイル7の位置関係を示し
た模式図であり、ベルト4の幅方向を矢印Xで表わしX
座標の中心の位置0を付記しである。第6図(b)は第
6図(a)に対応して、磁気マーカー1の位置がベルト
4上でX方向に変化した場合のパルス電圧ピーク値の変
化を示した線図であり、縦軸はパルス電圧ピーク値、横
軸はベルト′AM方向をX軸としたときの磁気マーカー
1の中心の座標を表わしており、このX座標が0のとき
は、検出コイル7の中心点の真上に磁気マーカー1の中
心慮がある場合である。第7図(al、(b)は第6図
FB+に出力電圧波形を書き加えた模式図であり、第7
図(alは双子の検出コイル7を一対とし、第7図中)
は双子の検出コイル7を複数対用いたことを示すもので
ある。第7図(alから例えば一対の検出コイル7によ
り、ある一定値以上の出力電圧を得ようとするとき、出
力電圧波形上の線分AB、線分CDの範囲を磁気マーカ
ー1が通過しなければ所定の出力が得られないことが解
る。しかし、第7図(blのように双子の検出コイル7
を複数対用いることにより、磁気マーカー1がベルト上
の如何なる位置を通過しても、必ず複数対のうちの何れ
か一対の検出コイル7には安定な大きいパルス出力電圧
が得られることになる。
Figure 6 (al is magnetic marker 1 on belt 4 (article 2)
(not shown) is a schematic diagram showing the positional relationship between a pair of detection coils 7, and the width direction of the belt 4 is indicated by an arrow X.
The position 0 of the center of the coordinates is added. FIG. 6(b), corresponding to FIG. 6(a), is a diagram showing changes in the pulse voltage peak value when the position of the magnetic marker 1 changes in the X direction on the belt 4, and The axis represents the pulse voltage peak value, and the horizontal axis represents the coordinate of the center of the magnetic marker 1 when the belt'AM direction is the X axis. When this X coordinate is 0, the true value of the center point of the detection coil 7 is shown. This is a case where the magnetic marker 1 is centered on the top. Figure 7 (al, (b) is a schematic diagram in which the output voltage waveform is added to Figure 6 FB+.
Figure (al indicates a pair of twin detection coils 7, in Figure 7)
indicates that a plurality of pairs of twin detection coils 7 are used. Fig. 7 (When trying to obtain an output voltage of a certain value or more from a pair of detection coils 7, for example, the magnetic marker 1 must pass through the range of line segment AB and line segment CD on the output voltage waveform. However, as shown in Fig. 7 (bl), if the twin detection coils 7
By using a plurality of pairs, no matter what position on the belt the magnetic marker 1 passes, a stable and large pulse output voltage will always be obtained in one of the detection coils 7 of the plurality of pairs.

以上のように、物品識別装置に用いられる本発明の検出
コイルは、磁気マーカーからの磁束を受けて最大パルス
出力電圧を発生する径の大きさを算出し、さらにヘルド
幅方向に対して2個で一対とする検出コイルを複数対配
置することにより、物品がベルト上の如何なる位置を通
過しても、安0 定なしかも大出力のパルス電圧を得られるようにしたも
のである。
As described above, the detection coil of the present invention used in the article identification device calculates the diameter size that generates the maximum pulse output voltage by receiving the magnetic flux from the magnetic marker, and also has two coils in the heald width direction. By arranging a plurality of pairs of detection coils, it is possible to obtain a high-output pulse voltage with no stability, no matter where the article passes on the belt.

〔発明の効果〕〔Effect of the invention〕

磁気マーカーを利用する物品識別装置に用いる双子の検
出コイルは、従来これらの径の大きさを適切に定めてお
らず、また検出コイルをただ一対しか設けていないため
に、磁気マーカーを取り付けた物品の置かれる位置や方
向によっては、検出コイルからの出力が不安定であった
のに対して、本発明では実施例で述べたように、検出コ
イルの径を最大出力が得られるように算出して設定し、
この検出コイルを用いて双子コイルの複数対をベルトの
幅方向に配置したことにより、交流磁界を走行中の磁気
マーカーから発生する磁束の大きい領域が、必ず検出コ
イルの何れかと交差するようになり、その結果、磁気マ
ーカーの位置や方向の如何に拘らず、検出コイルには常
に大きな誘導起電圧を生じ、安定な出力を取り出すこと
ができ、物品の数量や識別をより容易で確実にするとい
う利点が得られる。
Conventionally, the diameters of the twin detection coils used in article identification devices that use magnetic markers have not been determined appropriately, and only one pair of detection coils is provided, which makes it difficult to identify articles with magnetic markers attached. The output from the detection coil was unstable depending on the position and direction in which it was placed, but in the present invention, as described in the embodiment, the diameter of the detection coil is calculated so as to obtain the maximum output. and set
By using this detection coil and arranging multiple pairs of twin coils in the width direction of the belt, a region with large magnetic flux generated from a magnetic marker running in an alternating magnetic field will always intersect with one of the detection coils. As a result, regardless of the position or direction of the magnetic marker, a large induced electromotive force is always generated in the detection coil, and a stable output can be obtained, making it easier and more reliable to identify the quantity and identification of items. Benefits can be obtained.

【図面の簡単な説明】 第1図は磁気マーカーの磁束と検出コイルとの関係を表
わす模式図、第2図はベルト上の磁気マーカーと1個の
検出コイルの位置関係を示した模式斜視図、第3図(I
f)はH,、H,、H□のベクトル図第3図(blはそ
の拡大図、第4図はΦと検出コイル径との関係を示した
線図、第5図f8j〜(C1は検出コイルの径と磁気マ
ーカーの磁力線との関係を示した模式図、第6図(al
はヘルド上の磁気マーカーと一対の検出コイルの位置関
係を示した模式図、第6図(b)は磁気マーカーの位置
変化とパルス電圧ピーク値の変化との関係を示した線図
、第7図fa+は第6図falに一対の検出コイルの出
力電圧波形を書き加えて表わした模式図、第7図(b)
は同じく複数対の検出コイルとしたときの模式図、第8
図は物品識別装置の主な構成部を示した模式図、第9図
は磁気マーカーのB−H曲線図、第10図fa)、(b
)は第9図の装置の一部拡大図、第11図(a)、 (
blは検出コイルに誘起されるパルス電圧波形図である
。 1:磁気マーカー、2:物品、4:ベルト5:励磁コイ
ル。 7:検出コイル 9 : 磁力線。 3 所ト ((1) 特開平3 41387(6) / ! 2 ゲ 第8図 第7図 第10図 (Q) (b) 第11図
[Brief explanation of the drawings] Figure 1 is a schematic diagram showing the relationship between the magnetic flux of a magnetic marker and a detection coil, and Figure 2 is a schematic perspective view showing the positional relationship between the magnetic marker on the belt and one detection coil. , Figure 3 (I
f) is a vector diagram of H,, H,, H A schematic diagram showing the relationship between the diameter of the detection coil and the lines of magnetic force of the magnetic marker, FIG. 6 (al.
6(b) is a schematic diagram showing the positional relationship between the magnetic marker on the heald and a pair of detection coils, FIG. 6(b) is a diagram showing the relationship between the change in the position of the magnetic marker and the change in the pulse voltage peak value, Figure fa+ is a schematic diagram that shows the output voltage waveform of a pair of detection coils added to Figure 6 fal, Figure 7 (b)
is also a schematic diagram when multiple pairs of detection coils are used, No. 8
The figure is a schematic diagram showing the main components of the article identification device, Figure 9 is a B-H curve diagram of the magnetic marker, and Figure 10 fa), (b
) is a partially enlarged view of the device in Fig. 9, Fig. 11(a), (
bl is a pulse voltage waveform diagram induced in the detection coil. 1: Magnetic marker, 2: Article, 4: Belt 5: Excitation coil. 7: Detection coil 9: Lines of magnetic force. 3 Toko ((1) JP-A-3 41387 (6) /! 2 Ge Figure 8 Figure 7 Figure 10 (Q) (b) Figure 11

Claims (1)

【特許請求の範囲】[Claims] 1)複数個の磁性薄帯または細線を磁気マーカーとして
これらを長手方向に並列に取り付けた物品をベルトに載
せて走行中に交流磁界を通過させ前記磁気マーカーの磁
束変化で生ずるパルス電圧を、前記交流磁界を発生させ
る励磁コイルからの誘電起電力を相殺する2個一対とし
た双子の検出コイルによって取り出す物品識別装置の検
出コイルであって、前記磁気マーカーの磁束に対して最
大出力パルス電圧の得られる径を有し、前記ベルトの幅
方向に亘って複数対を配置したことを特徴とする物品識
別装置の検出コイル。
1) An article in which a plurality of magnetic ribbons or thin wires are used as magnetic markers and these are attached in parallel in the longitudinal direction is placed on a belt and passed through an alternating magnetic field while running, and the pulse voltage generated by the magnetic flux change of the magnetic markers is A detection coil for an article identification device that uses a pair of twin detection coils to offset the induced electromotive force from an excitation coil that generates an alternating magnetic field, the detection coil being capable of obtaining a maximum output pulse voltage with respect to the magnetic flux of the magnetic marker. 1. A detection coil for an article identification device, wherein a plurality of pairs are arranged across the width direction of the belt.
JP1175940A 1989-07-07 1989-07-07 Detection coil of article discrimination instrument Pending JPH0341387A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1175940A JPH0341387A (en) 1989-07-07 1989-07-07 Detection coil of article discrimination instrument

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1175940A JPH0341387A (en) 1989-07-07 1989-07-07 Detection coil of article discrimination instrument

Publications (1)

Publication Number Publication Date
JPH0341387A true JPH0341387A (en) 1991-02-21

Family

ID=16004919

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1175940A Pending JPH0341387A (en) 1989-07-07 1989-07-07 Detection coil of article discrimination instrument

Country Status (1)

Country Link
JP (1) JPH0341387A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2006523823A (en) * 2002-12-31 2006-10-19 カリプソー メディカル テクノロジーズ インコーポレイテッド Device for finding the position of an implantable wireless marker

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2006523823A (en) * 2002-12-31 2006-10-19 カリプソー メディカル テクノロジーズ インコーポレイテッド Device for finding the position of an implantable wireless marker

Similar Documents

Publication Publication Date Title
JPS5853396B2 (en) Target of magnetic detection system
TW363171B (en) Verifier device for a magnetic security thread for verifying the authenticity of a document having a security thread associated therewith
US5440296A (en) Coil assembly for electronic article surveillance system
JPH0341387A (en) Detection coil of article discrimination instrument
JPH09512362A (en) Electronic label encoding method and apparatus
JPH04157588A (en) Magnetic marker for object identification
JPS6247241B2 (en)
JPH07260492A (en) Angular velocity detector
TW311210B (en)
JP2806743B2 (en) Single-pulse magnetic marker
JPH02157682A (en) Detection coil for article identification device
JPH02173591A (en) Exciting coil of article identifying device
JPH04174086A (en) Identifying method for magnetic marker
JPH07198407A (en) Magnetism measuring instrument
JPH0450691A (en) Detection coil of article discrimination apparatus
JPS6379633A (en) Eyeball motion measuring apparatus
JPH0711582B2 (en) Magnetic marker
JPH05247839A (en) Needle detector
RU2136035C1 (en) Method and device for vehicle control
JP2503658B2 (en) Magnetic sensor
JPH0492988A (en) Discriminating method for magnetic marker
JP2535503B2 (en) Geomagnetic direction sensor
JPH04149683A (en) Identifying method for magnetic marker
JPH05250530A (en) Method for determining dimensions of magnetic narrow wire for magnetic marker
JPS58142203A (en) Magnetic body detecting device