JPS586581A - magnetic bubble detector - Google Patents
magnetic bubble detectorInfo
- Publication number
- JPS586581A JPS586581A JP56104468A JP10446881A JPS586581A JP S586581 A JPS586581 A JP S586581A JP 56104468 A JP56104468 A JP 56104468A JP 10446881 A JP10446881 A JP 10446881A JP S586581 A JPS586581 A JP S586581A
- Authority
- JP
- Japan
- Prior art keywords
- noise
- phase
- detector
- magnetic field
- pattern
- 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
Links
Abstract
Description
【発明の詳細な説明】
本実−はIII気パノ#憤出器0検出出方位−の改良に
胸するものである。DETAILED DESCRIPTION OF THE INVENTION The purpose of this invention is to improve the 0-detection direction of the air pump III.
$1111状、本発明に−わる磁気抵抗効果音利用した
S―朧磁気バブル検出器の構成図〇−例を示す。A configuration diagram of an S-blur magnetic bubble detector using a magnetoresistive sound effect according to the present invention is shown.
岡−Ks?いて、Dは検出器を形成する検出器ライン、
BTは磁気バブルをひも状に拡大するバブルストレッチ
ャで642、これらのパターンD 、gTはパーw c
14等の軟m−銖体薄編で形成される。また、H翼は同
平面内で1転すみ一転侮界、Haは紙HIrc鵬瓢に加
えられているバイアス磁界である。Oka-Ks? , D is a detector line forming a detector,
BT is a bubble stretcher that expands magnetic bubbles into a string shape642, and these patterns D and gT are par w c
It is made of soft m-tube thin knitting such as No. 14. In addition, the H blade is a bias magnetic field that is applied to the paper HIrc in each turn in the same plane.
こO励転磁」■によシ、磁気バブル鉱矢印P方向に転送
されるeaf4バブルがバブルストレッチャー8Tの下
を転送・されるとき、lll4yj向に拡大されてひも
社バブルになる。Bはζうして拡大されえひも状バブル
の一つである。また、同813において、■は外部から
検出器ラインに印′IIAiIれている検出器電流であ
る。−出出力紘、ひも状バブルlが検出器ラインDの下
を通過するとき、−出器うインDOilimlKtE出
力として祷られる。When the eaf4 bubble transferred in the direction of the magnetic bubble arrow P is transferred under the bubble stretcher 8T, it is expanded in the ll4yj direction and becomes a string bubble. B is one of the string-like bubbles expanded by ζ. Also, in 813, ■ is a detector current that is externally marked on the detector line. When the string-like bubble l passes under the detector line D, the output is taken as the output.
このような構成Ols気バブル検出−において、検出出
力のサインwLま九a三角波で態動した1例を嬶211
(&)に例示する。同図において、Na@01出力、S
嬬@1”出力t″示す。“l”出力として紘、1個のバ
ブルかも一転一界HRKよjlPlからP4の4種類の
安定なピークliI形が祷られる。これら4種類の安定
なピークa形P1〜?40中の一つま九は二つを用いて
、情報O“O”、“l嘴*1行なう。In such a configuration for air bubble detection, an example in which the detection output sign wL is a triangular wave is shown in 211.
(&) is an example. In the same figure, Na@01 output, S
嬬@1 Indicates “output t”. As the "l" output, four kinds of stable peaks from P4 to P4 are expected. These four types of stable peaks a-type P1~? One or nine out of 40 will use two to carry out the information O "O", "l beak*1.
tた、同図において、SWNは、−転磁界系から入るノ
イズである。バブルf:纒勤するため外部から加える關
−磁界HRとして、菖3図(a)〜(e)に例示し良、
3柚−のものがよく用いられる。總3wA←)。In addition, in the same figure, SWN is noise that enters from the -magnetic field system. Bubble f: As a magnetic field HR applied from the outside for winding, examples are shown in Figures 3 (a) to (e).
Three yuzu citrons are often used. 3wA←).
(b)o−y″イン款三角献IIA鋤の場合、醜2図(
a)に示したように、ノイX8WNi90°きざみの位
相で検出出力に入るeIia図(C)の台形鎖駆動の場
合、論2園−)VC示したように、ノイズ8WNは30
龜ざみ0位−で−山出力に入る。(b) In the case of o-y''in-section triangular IIA plow, Ugly 2 figure (
As shown in a), the noise X8WNi enters the detection output in 90° increments. In the case of the trapezoidal chain drive in diagram (C), the noise 8WN is 30
Enter the -yama output at the 0th position of the knob.
この15に、この−転磁外系ノイズ畠WNのために、I
IA出^力によh111輯0−0”、11″判走が安定
にfi2にえなくなる揚台がある0例え猷、慕2図−〕
の11a#5出力tiL彫りにおいて、鶴4ビークP4
を利用して@五″、101定を行なうシステムでは、2
70位@osWNノイメのために、安定なl”−〇1定
が不可能となる。また、1i12鵬−)O例O場合、8
■ノイメのために、鶴l−魅4のいずれのと−クPI−
P4も@1”、@O”判定に利用で亀ない。In this 15, due to this -magnetization external noise field WN, I
Due to the IA output power, h111 0-0", 11" has a platform where the 11" size cannot be stably changed to fi2.
In the 11a #5 output tiL carving, Tsuru 4 beak P4
In a system that uses @5'', 101 constant, 2
70th place @osWN Because of the noise, a stable l”-〇1 constant is impossible.Also, in the case of 1i12Peng-)O example O, 8
■For Noime, any of Tsuru I-Mi 4 and Ku PI-
P4 can also be used for @1" and @O" judgment.
上記し九ように、従来の磁気パプルー一−におい′C憾
−転−界畢ノイメswxoために、脣定の出力波形ピー
クP1を有用した安定な@1′、″″O”I#4J定が
不可能であった。As mentioned above, for the conventional magnetic papulus swxo, a stable output waveform peak P1 is used to obtain a stable was not possible.
したがって、本発明の目的は上記した問題点を解消し、
“l”、”0”判定に有用する出力波形ピーク位相に、
回転磁界系ノイズ5WIIJが重なることのない磁気バ
ブル検出器を提供しようとするものである。Therefore, an object of the present invention is to solve the above-mentioned problems,
For the output waveform peak phase useful for “l” and “0” judgment,
The present invention aims to provide a magnetic bubble detector in which rotating magnetic field noise 5WIIJ does not overlap.
以下、本発明の詳細な説明する。The present invention will be explained in detail below.
11図に例示した磁気バブル検出器ラインDlj、第4
図に例ボした基本セルパターンを基本構成要素として、
この基本セルを左右に繰〉返して配列することによシ構
成されている。The fourth magnetic bubble detector line Dlj illustrated in FIG.
Using the basic cell pattern shown in the figure as the basic component,
It is constructed by repeatedly arranging these basic cells left and right.
#14図に例示したように、基本セルパターン祉、二つ
のシェブロンパターン1,2J−1こレラシェブロンパ
ターン1,2をショートスルショートパー3,4とで形
成される。As illustrated in FIG. #14, the basic cell pattern is formed by two chevron patterns 1 and 2J-1 and short through shorts 3 and 4.
このようなパターンから構成される磁気バブル検出器に
おいて、出力II形ビータPlO位相を決める形状パラ
メJりを買験釣に究−しえ。検討し、た形状パラメータ
として次のような項目を選んだ。In a magnetic bubble detector composed of such a pattern, the shape parameter J that determines the phase of the output type II beater PlO should be thoroughly investigated. The following items were selected as shape parameters.
■ ショートパー3,4の結合位置
■ シェブロンパターン1,2の形
■ パターン−
■ パターン調厚
こO結果、出力波形ビークPiの位相に直接影響を4え
るキーバラメータは、84図において示す角度−であゐ
ことが明らかになった。ζO角W1#拡、シェブロンパ
ターン1,2を形成する!811110素片10.2@
と素片11,21のうちで、検出器電流IO流れる電流
径路となる素片It、21が一1方向(位相O基準点)
となる角度である。ここ、で、こO素片It、21を電
流径路素片と名付けるととにする。まえ、この角度0の
ことを電流径路素片O方向と呼ぶととにする。■ Combined position of shorters 3 and 4 ■ Shape of chevron patterns 1 and 2 ■ Pattern - ■ Pattern thickness adjustment As a result, the key parameter that directly influences the phase of the output waveform peak Pi is the angle shown in Figure 84. It became clear that this was the case. ζO angle W1# is expanded to form chevron patterns 1 and 2! 811110 piece 10.2@
Among the elements 11 and 21, the elements It and 21, which are the current paths through which the detector current IO flows, are in the 11th direction (phase O reference point)
This is the angle. Here, the element It,21 is named the current path element. First, let us say that this angle 0 is called the current path segment O direction.
鏑5mは、−出出力筐形のII3ビーク位1ivaと上
記電流−路素片の方向0との関係を実験的に求めえ紬呆
O−例である。本夷験結果よシ明らかなように、第3ピ
ーク位@ダ3と電m径路素片の方向0と0111に1対
10対応があシ、93=Q)関係のあることが明らかに
なりた。5m is an example of experimentally determining the relationship between the II3 peak position 1iva of the -output output housing type and the direction 0 of the current path segment. As is clear from the results of this experiment, there is a 1:10 correspondence between the third peak position @da3 and the directions 0 and 0111 of the electric m path element, and there is a relationship (93=Q). Ta.
し九がって、本発明の!1本的な考え方は、磁気バブル
検出器を構成するシェブロンノ(ターンの電流径路素片
の方向0が、回転磁界系ノイズSWN位相から最も遠く
なる方向となるようにシェブロンパターン形状を設定し
ようとするものである。After all, the present invention! One way of thinking is to set the chevron pattern shape so that the direction 0 of the current path element of the chevron (turn) that makes up the magnetic bubble detector is the direction that is farthest from the rotating magnetic field system noise SWN phase. It is something to do.
第6図け、本発明による一気)(プル検出器の実施例の
一例を示す図でわシ、台形波駆動の場合における、検m
eの基本命ルノリーン例を示す。同図中には、台形波駆
動の回転磁界軌跡も参考に+1記した。同図から4明ら
かなように、基本セル/<ターンの電流径路素片11.
21c1方向−がθz15°±30Xn (n :!l
1l)” ” ’(1)表っている。Figure 6 shows an example of an embodiment of a pull detector according to the present invention.
An example of the basic order of e is shown. In the figure, the locus of the rotating magnetic field driven by the trapezoidal wave is also marked with +1 for reference. As is clear from the figure, the basic cell/<turn current path segment 11.
21c1 direction - is θz15°±30Xn (n:!l
1l) ” ” '(1) It is expressed.
回転磁界系ノイズI削は、台y#波駆動の場合に311
1M)K示すようニ30°t1ざみの位相に乗った。Rotating magnetic field system noise I reduction is 311 in case of y# wave drive
1M) It rode on the phase of 230°t1 to indicate K.
−を式(1)のようにノイズIWN位相の中央部に選ぶ
ことによシ、ピーク位相をノイズ8WN位相から最も遠
く離せることになる。By selecting - at the center of the noise IWN phase as in equation (1), the peak phase can be separated farthest from the noise 8WN phase.
以上は台形波I動の例であるが、サイン波駆動、三角波
駆動の場合は・5(1)は・ ・−レウ1o24?
±90Xn、(n:警WjI)・・・(21となる。The above is an example of trapezoidal wave I motion, but in the case of sine wave drive and triangular wave drive, 5(1) is... - Leu 1o24?
±90Xn, (n: WjI)...(21).
このように、本実@によると、シェブロンパターンの電
流径路素片の方向を回転磁界系ノイズ位相間の中央部に
くるようにし九ととによ〕、ノイズに影響畜れず安定に
情報O”QZIIIIII判定が検出できるという優れ
九効来がある。In this way, according to Honjitsu@, by arranging the direction of the current path element of the chevron pattern to be in the center between the noise phases of the rotating magnetic field system, information can be stably transmitted without being influenced by noise. It has nine excellent effects: it can detect QZIIIIII judgment.
si図は磁気バブル検出lIO構成図の一例を示す図、
第2図は検出出力波形例を示す図、第3図は番程駆動磁
界の例を示す図、第4図は検出器を横威す石基本セルパ
ターン例を示す図、115図は本発明の基本的な考え方
を示す0とlsO関係図、第6wJは本実l!j10冥
膣例を示す基本セルパターンの図である。
1.2・・・・シェブロンパターン、S、4・・・・シ
ョートパー、11,21・・・・電流径路素片、0・・
・−電[11路素片の方向。
第1図si diagram is a diagram showing an example of a magnetic bubble detection lIO configuration diagram,
Fig. 2 is a diagram showing an example of a detection output waveform, Fig. 3 is a diagram showing an example of a pulse drive magnetic field, Fig. 4 is a diagram showing an example of a stone basic cell pattern that dominates the detector, and Fig. 115 is a diagram showing an example of the present invention. 0 and lsO relationship diagram showing the basic idea of , 6th wJ is the real l! FIG. 2 is a diagram of a basic cell pattern showing an example of a j10 hypovagina. 1.2... Chevron pattern, S, 4... Shorter, 11, 21... Current path element, 0...
・-Electric [11 direction of the element. Figure 1
Claims (1)
cをいて、基本−Ig畳嵩となゐ基本セルパターンをシ
ェブロンパターンとショートパーとで形成し、このシェ
ブロンパターンの検出器電流が流れる亀滝徴路素片07
3向を、紬転磁界系ノイメ位相の閏の中**rcなるよ
うに設定し九磁気バブル検崩器。Rhinoceros-shaped magnetic bubble detection using am birth cage effect @II
c, a basic cell pattern with basic-Ig bulk is formed by a chevron pattern and a shortper, and the detector current of this chevron pattern flows through the Kametaki Choro element piece 07.
Set the three directions so that they are in the leap of the Neume phase of the Tsumugi rotating magnetic field system**rc, and use a nine-magnetic bubble detector.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56104468A JPS586581A (en) | 1981-07-06 | 1981-07-06 | magnetic bubble detector |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56104468A JPS586581A (en) | 1981-07-06 | 1981-07-06 | magnetic bubble detector |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPS586581A true JPS586581A (en) | 1983-01-14 |
Family
ID=14381411
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP56104468A Pending JPS586581A (en) | 1981-07-06 | 1981-07-06 | magnetic bubble detector |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS586581A (en) |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS6082223A (en) * | 1983-10-04 | 1985-05-10 | Iwata Denko Kk | Production of reel spring for cassette |
| JPH0323023A (en) * | 1989-06-20 | 1991-01-31 | Sankoo:Kk | Assembly parts manufacturing method and assembly parts |
-
1981
- 1981-07-06 JP JP56104468A patent/JPS586581A/en active Pending
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS6082223A (en) * | 1983-10-04 | 1985-05-10 | Iwata Denko Kk | Production of reel spring for cassette |
| JPH0323023A (en) * | 1989-06-20 | 1991-01-31 | Sankoo:Kk | Assembly parts manufacturing method and assembly parts |
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