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JPS6329302B2 - - Google Patents
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JPS6329302B2 - - Google Patents

Info

Publication number
JPS6329302B2
JPS6329302B2 JP55046375A JP4637580A JPS6329302B2 JP S6329302 B2 JPS6329302 B2 JP S6329302B2 JP 55046375 A JP55046375 A JP 55046375A JP 4637580 A JP4637580 A JP 4637580A JP S6329302 B2 JPS6329302 B2 JP S6329302B2
Authority
JP
Japan
Prior art keywords
magnetic
information
magnetoresistive element
basic information
pitch information
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
JP55046375A
Other languages
Japanese (ja)
Other versions
JPS56143084A (en
Inventor
Noboru Masuda
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.)
Denki Onkyo Co Ltd
Original Assignee
Denki Onkyo 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 Denki Onkyo Co Ltd filed Critical Denki Onkyo Co Ltd
Priority to JP4637580A priority Critical patent/JPS56143084A/en
Publication of JPS56143084A publication Critical patent/JPS56143084A/en
Publication of JPS6329302B2 publication Critical patent/JPS6329302B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G06COMPUTING OR CALCULATING; COUNTING
    • G06KGRAPHICAL DATA READING; PRESENTATION OF DATA; RECORD CARRIERS; HANDLING RECORD CARRIERS
    • G06K7/00Methods or arrangements for sensing record carriers, e.g. for reading patterns
    • G06K7/08Methods or arrangements for sensing record carriers, e.g. for reading patterns by means detecting the change of an electrostatic or magnetic field, e.g. by detecting change of capacitance between electrodes
    • G06K7/082Methods or arrangements for sensing record carriers, e.g. for reading patterns by means detecting the change of an electrostatic or magnetic field, e.g. by detecting change of capacitance between electrodes using inductive or magnetic sensors
    • G06K7/087Methods or arrangements for sensing record carriers, e.g. for reading patterns by means detecting the change of an electrostatic or magnetic field, e.g. by detecting change of capacitance between electrodes using inductive or magnetic sensors flux-sensitive, e.g. magnetic, detectors

Landscapes

  • Engineering & Computer Science (AREA)
  • Artificial Intelligence (AREA)
  • Computer Vision & Pattern Recognition (AREA)
  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Theoretical Computer Science (AREA)
  • Character Input (AREA)
  • Image Processing (AREA)

Description

【発明の詳細な説明】 本発明は紙幣識別装置等に用いられる磁気情報
処理方法に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a magnetic information processing method used in banknote identification devices and the like.

従来、磁気インク等で印刷された紙幣等の文
字、記号、模様等の読取りに磁気抵抗素子を用い
た磁気検出器が多用されている。第1図は紙幣識
別装置の検出手段の原理を例示するもので、1は
紙またはプラスチツク等の非磁性材料からなる磁
性体保持媒体、2a,2bは保持媒体1上に粘
着、印刷等により固定された磁性インク、磁性粉
等の磁気ストライブである。3,4は1対の磁気
抵抗素子で、永久磁石5上に磁気ストライブ2
a,2bに対向して取り付けられ、第2図に示す
如く、直列に接続されている。ここで、永久磁石
5上に磁気抵抗素子3,4を取り付けた状態を磁
気検出器cと称す。磁気検出器cと磁気ストライ
ブ2a,2bの位置関係が定速度で相対的に変わ
り、磁気抵抗素子3に磁気ストライブ2aが近接
し、磁気抵抗素子4の対向面には磁気ストライプ
2bが近接していない状態では、磁気抵抗素子4
に比べ磁気抵抗素子3を貫通する磁束が多くな
り、その結果、磁気抵抗素子3の抵抗値が高くな
る。この状態を第2図の分圧回路について考える
と次式が成立する。
Conventionally, magnetic detectors using magnetoresistive elements have been widely used to read characters, symbols, patterns, etc. on banknotes printed with magnetic ink or the like. Figure 1 illustrates the principle of the detection means of a banknote identification device, in which 1 is a magnetic holding medium made of a non-magnetic material such as paper or plastic, and 2a and 2b are fixed on the holding medium 1 by adhesive, printing, etc. It is a magnetic stripe made of magnetic ink, magnetic powder, etc. 3 and 4 are a pair of magnetic resistance elements, and a magnetic stripe 2 is placed on the permanent magnet 5.
a and 2b, and are connected in series as shown in FIG. Here, the state in which the magnetic resistance elements 3 and 4 are attached on the permanent magnet 5 is referred to as a magnetic detector c. The positional relationship between the magnetic detector c and the magnetic stripes 2a and 2b changes relatively at a constant speed, so that the magnetic stripe 2a approaches the magnetoresistive element 3, and the magnetic stripe 2b approaches the opposing surface of the magnetoresistive element 4. In the state where it is not connected, the magnetoresistive element 4
The magnetic flux passing through the magnetoresistive element 3 is larger than that of the magnetoresistive element 3, and as a result, the resistance value of the magnetoresistive element 3 is increased. Considering this state with respect to the voltage dividing circuit shown in FIG. 2, the following equation holds true.

Vout=R4/R3+R4Vin 但し、R3は磁気抵抗素子3の抵抗値、R4は磁
気抵抗素子4の抵抗値である。この式から抵抗値
R3の値が大きくなると、基準電圧1/2Vinより低
い電圧がVoutから取り出される。
Vout=R 4 /R 3 +R 4 Vin where R 3 is the resistance value of the magnetoresistive element 3 and R 4 is the resistance value of the magnetoresistive element 4. From this formula, the resistance value
As the value of R 3 increases, a voltage lower than the reference voltage 1/2Vin is taken from Vout.

基準電圧の条件:磁気抵抗素子3,4に等しい磁
気バイアスが印加されている次のAまたはBの
状態。
Reference voltage condition: the next A or B state in which equal magnetic bias is applied to the magnetoresistive elements 3 and 4.

A…RB4=RB3→両磁気抵抗素子3,4面に均等
に磁性体(磁気ストライブ)が対向する場合、 B…R4=R3→両磁気素子3,4面に全く磁性体
(磁気ストライブ)が対向していない場合。
A...R B4 = R B3 → When the magnetic material (magnetic stripe) is evenly opposed to both magnetic resistance elements 3 and 4, B...R 4 = R 3 → There is no magnetic material at all on both magnetic elements 3 and 4. (magnetic stripes) are not facing each other.

次に、磁気検出器cと磁気ストライブ2a,2
bの位置関係が相対的に更に変化し、磁気抵抗素
子3に比べ磁気抵抗素子4の方に磁束が多く加わ
つた場合、磁気抵抗素子4の抵抗値R4が増加し、
Voutは基準電圧1/2Vinより高い電圧となる。こ
の際、磁気ストライブ2a,2bと磁気検出器c
の位置関係が相対的に定速度で進むとすると、出
力特性は、第3図に示す如く、出力波形S1、S2
第1図の媒体1上の距離l1、l2に相対して対応関
係が得られる。しかし、磁気ストライブ2a,2
bと磁気検出器cの相対速度が変つた場合例え
ば、手持ちスキヤンナー或はリードペン等を用い
た場合には、出力波形は、第4図に示す如く、媒
体1上の距離l1、l2に相対せずt1>t2の関係とな
り、信号読取りエラーが生じることがあつた。
Next, magnetic detector c and magnetic stripes 2a, 2
When the relative positional relationship of b changes further and more magnetic flux is applied to the magnetoresistive element 4 than to the magnetoresistive element 3, the resistance value R 4 of the magnetoresistive element 4 increases,
Vout becomes a voltage higher than the reference voltage 1/2Vin. At this time, the magnetic stripes 2a, 2b and the magnetic detector c
Assuming that the positional relationship advances at a relatively constant speed, the output characteristics are as shown in Figure 3, where the output waveforms S 1 and S 2 are relative to the distances l 1 and l 2 on the medium 1 in Figure 1. The correspondence relationship can be obtained by However, the magnetic stripes 2a, 2
When the relative speed between b and magnetic detector c changes, for example when using a hand-held scanner or reed pen, the output waveform changes at distances l 1 and l 2 on the medium 1, as shown in Figure 4. There was a relationship of t 1 > t 2 without relative relationship, and a signal reading error sometimes occurred.

本発明は上記点に鑑み成されたもので、基礎情
報とピツチ情報を保持媒体に併設し、これを同時
に読取ることにより基礎情報信号の範囲を明確に
する磁気情報処理方法を提供するものである。
The present invention has been made in view of the above points, and provides a magnetic information processing method that clarifies the range of the basic information signal by providing basic information and pitch information on a holding medium and reading them simultaneously. .

以下本発明磁気情報処理方法を第5図乃至第8
図に用いて詳細に説明する。
The magnetic information processing method of the present invention is illustrated in FIGS. 5 to 8 below.
This will be explained in detail with reference to the drawings.

第5図は本発明磁気情報処理方法に用いる基本
的な原理構成図であり、同図において、6a,6
b,6c,6dはそれぞれ基礎情報用磁気ストラ
イブ、7は基礎情報用磁気ストライブ6a乃至6
bに近接すると共にその配列方向へ連続して延び
て基礎情報用磁気ストライブ6a乃至6dが存在
する範囲を明確にする如く付与されたピツチ情報
用磁気ストライブで、それぞれ磁性材料からな
り、保持媒体(図示せず)上に相対的位置関係が
変わることなく併設されている。8a,8bは磁
気検出器を構成する一対の磁気抵抗素子で、磁界
印加手段、例えば永久磁石、電磁コイル等は図示
していない。
FIG. 5 is a basic principle configuration diagram used in the magnetic information processing method of the present invention, and in the same figure, 6a, 6
b, 6c, and 6d are basic information magnetic stripes, and 7 is basic information magnetic stripes 6a to 6.
The magnetic stripes for pitch information are provided so as to be close to b and extend continuously in the arrangement direction to clarify the range in which the magnetic strips 6a to 6d for basic information exist, each of which is made of a magnetic material and is held. They are placed side by side on a medium (not shown) without changing their relative positional relationship. Reference numerals 8a and 8b denote a pair of magnetoresistive elements constituting a magnetic detector, and magnetic field applying means, such as a permanent magnet or an electromagnetic coil, are not shown.

斯かる構成において、ピツチ情報用磁気ストラ
イブ7を用いた動作を説明する。第6図はピツチ
情報用磁気ストライブ7と一対の磁気抵抗素子8
a,8bが相対的に位置変化したものを示し、磁
気抵抗素子8bのみにピツチ情報用磁気ストライ
ブ7が対向している状態をT1、磁気抵抗素子8
a,8bにピツチ情報用磁気ストライブ7が対向
している状態をT2、磁気抵抗素子8aのみにピ
ツチ情報用磁気ストライブ7が対向している状態
をT3で表わす。ここで、磁気抵抗素子8a,8
bの結線は第2図に待応するもので、磁気抵抗素
子8aは第2図の磁気抵抗素子3に、磁気抵抗素
子8bは同じく磁気抵抗素子4に置き換えられる
ものである。斯かる状態における出力電圧は、次
のようになる。
In such a configuration, the operation using the pitch information magnetic stripe 7 will be explained. Figure 6 shows a pitch information magnetic stripe 7 and a pair of magnetoresistive elements 8.
a and 8b indicate relative positional changes, and the state where the pitch information magnetic stripe 7 faces only the magnetoresistive element 8b is T 1 , and the state where the magnetic stripe 7 for pitch information is opposed only to the magnetoresistive element 8b is indicated by T 1 .
The state in which the pitch information magnetic stripe 7 faces a and 8b is represented by T2, and the state in which the pitch information magnetic stripe 7 faces only the magnetoresistive element 8a is represented by T3 . Here, the magnetoresistive elements 8a, 8
The connection b corresponds to that shown in FIG. 2, and the magnetoresistive element 8a is replaced by the magnetoresistive element 3 shown in FIG. 2, and the magnetoresistive element 8b is replaced by the magnetoresistive element 4. The output voltage in such a state is as follows.

T1の場合……1/2Vin+α,(R8a<R8b) T2の場合……1/2Vin、(R8a=R8b) T3の場合……1/2Vin−α,(R8a>R8b) 但し、R8aは磁気抵抗素子8aの抵抗値、R8b
は磁気抵抗素子8bの抵抗値、αは電圧変化分で
ある。この場合、出力波形は、第7図に示す如
く、ピツチ情報用磁気ストライブ7の寸法l3に対
応し、正負の波形(tP1P1)が対をなし、走査
時間(低速度・高速度)に関係なく、対の状態は
維持される。即ち、磁気検出器がピツチ情報用磁
気ストライブ7の長手方向に相対的に移動すると
き、ピツチ情報用磁気ストライブの先端部分で始
端信号tP1が発生し、末端部分で終端信号P1が発
生する。
For T 1 ...1/2Vin+α, (R 8a < R 8b ) For T 2 ...1/2Vin, (R 8a = R 8b ) For T 3 ...1/2Vin-α, (R 8a > R 8b ) However, R 8a is the resistance value of the magnetoresistive element 8a, R 8b
is the resistance value of the magnetoresistive element 8b, and α is the voltage change. In this case, the output waveform corresponds to the dimension l 3 of the pitch information magnetic stripe 7, as shown in FIG. The state of the pair is maintained regardless of the speed). That is, when the magnetic detector moves relatively in the longitudinal direction of the pitch information magnetic stripe 7, the start signal t P1 is generated at the tip of the pitch information magnetic strip 7, and the termination signal P1 is generated at the end. do.

第8図は基礎情報用磁気ストライブ6a乃至6
dとピツチ情報用磁気ストライブ7を組合せた場
合の出力波形を示す。ピツチ情報信号tP1P1
ピツチ情報用磁気ストライブ7により発生したも
の、基礎情報信号tj1、tj2、tj3、tj4は基礎情報用
磁気ストライブ6a乃至6dによつて発生したも
ので、tj1乃至tj4は正負の波形対を構成し、tj1
tP1は基礎情報信号6a乃至6dの前後に生じ、
基礎情報信号の範囲を明確にしている。即ち、ピ
ツチ情報信号tP1P1の間にある基礎情報信号の
みが有効信号である。
Figure 8 shows magnetic stripes 6a to 6 for basic information.
d and the pitch information magnetic stripe 7 are combined. The pitch information signals t P1 and P1 are generated by the pitch information magnetic stripe 7, and the basic information signals t j1 , t j2 , t j3 and t j4 are generated by the basic information magnetic stripes 6a to 6d. t j1 to t j4 constitute a positive and negative waveform pair, and t j1 and
t P1 occurs before and after the basic information signals 6a to 6d,
The range of basic information signals is clarified. That is, only the basic information signal between the pitch information signals t P1 and P1 is a valid signal.

叙上の如く、本発明の磁気情報処理方法によれ
ば、媒体上に基礎情報とピツチ情報を併設してこ
れを磁気検出器で同時に読取り、ピツチ情報信号
で有効となる基礎情報信号の範囲を明確にするも
のであり、磁気検出器に対する媒体の相対速度が
どのように変化しようとも基礎情報の意味を正確
に判別することができる。
As described above, according to the magnetic information processing method of the present invention, basic information and pitch information are provided on the medium and read simultaneously by a magnetic detector, and the range of the basic information signal that is effective in the pitch information signal is determined. This makes it possible to accurately determine the meaning of the basic information no matter how the relative velocity of the medium to the magnetic detector changes.

従つて、本発明方法を例えば磁気カード等に応
用すれば、ダミーの磁気ストライブを付与するこ
とにより、秘匿性の高い情報処理方法とすること
ができる。
Therefore, if the method of the present invention is applied to, for example, a magnetic card, by adding a dummy magnetic stripe, it is possible to obtain a highly confidential information processing method.

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

第1図は磁気ストライブを読み取る周知の検出
手段の概略構成図、第2図は同じく検出手段に用
いられる磁気抵抗素子の接続状態を示す結線図、
第3図は同じく検出手段によつて生ずる相対的に
定速度時の出力特性図、第4図は同じく相対速度
が変つた場合の出力特性図、第5図は本発明磁気
情報処理方法に用いられる検出手段の基本原理構
成図、第6図は同じくピツチ情報ストライブと磁
気抵抗素子対との位置関係を示す説明図、第7図
は第6図に示した位置関係における出力特性図、
第8図はピツチ情報ストライブと情報用磁気スト
ライブを組み合わせた状態の出力特性図を示す。 6a,6b,6c,6d……情報用磁気ストラ
イブ(基板情報)、7……ピツチ情報ストライブ、
8a,8b……磁気抵抗素子。
FIG. 1 is a schematic configuration diagram of a well-known detection means for reading magnetic stripes, and FIG. 2 is a wiring diagram showing the connection state of a magnetoresistive element used in the detection means.
FIG. 3 is a diagram of the output characteristics generated by the detection means at a relatively constant speed, FIG. 4 is a diagram of the output characteristics when the relative speed changes, and FIG. 5 is a diagram of the output characteristics used in the magnetic information processing method of the present invention. FIG. 6 is an explanatory diagram showing the positional relationship between the pitch information stripe and the magnetoresistive element pair, and FIG. 7 is an output characteristic diagram in the positional relationship shown in FIG. 6.
FIG. 8 shows an output characteristic diagram of a combination of pitch information stripes and information magnetic stripes. 6a, 6b, 6c, 6d...Magnetic stripe for information (board information), 7...Pitch information stripe,
8a, 8b... Magnetoresistive elements.

Claims (1)

【特許請求の範囲】[Claims] 1 媒体上に基礎情報を配列すると共に、該基礎
情報の配列方向へ連続して延びるピツチ情報を前
記基礎情報に近接して設け、これら2つの情報を
分圧回路を構成する一対の磁気抵抗素子を用いて
読取り、前記ピツチ情報の始端信号と終端信号の
間の期間に所定の基礎情報信号を発生させるよう
にしたことを特徴とする磁気情報処理方法。
1 Arrange basic information on a medium, provide pitch information that extends continuously in the direction in which the basic information is arranged, and provide adjacent to the basic information, and connect these two pieces of information to a pair of magnetoresistive elements that constitute a voltage divider circuit. 1. A magnetic information processing method, characterized in that a predetermined basic information signal is generated during a period between a start signal and an end signal of the pitch information.
JP4637580A 1980-04-09 1980-04-09 Magnetic information processing method Granted JPS56143084A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP4637580A JPS56143084A (en) 1980-04-09 1980-04-09 Magnetic information processing method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP4637580A JPS56143084A (en) 1980-04-09 1980-04-09 Magnetic information processing method

Publications (2)

Publication Number Publication Date
JPS56143084A JPS56143084A (en) 1981-11-07
JPS6329302B2 true JPS6329302B2 (en) 1988-06-13

Family

ID=12745392

Family Applications (1)

Application Number Title Priority Date Filing Date
JP4637580A Granted JPS56143084A (en) 1980-04-09 1980-04-09 Magnetic information processing method

Country Status (1)

Country Link
JP (1) JPS56143084A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS59216278A (en) * 1983-05-24 1984-12-06 Tdk Corp Stationary setting type magnetic signal reading device

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6036628B2 (en) * 1977-08-10 1985-08-21 神鋼電機株式会社 Segment method in pattern recognition

Also Published As

Publication number Publication date
JPS56143084A (en) 1981-11-07

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