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JPS6236592B2 - - Google Patents
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JPS6236592B2 - - Google Patents

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Publication number
JPS6236592B2
JPS6236592B2 JP56159979A JP15997981A JPS6236592B2 JP S6236592 B2 JPS6236592 B2 JP S6236592B2 JP 56159979 A JP56159979 A JP 56159979A JP 15997981 A JP15997981 A JP 15997981A JP S6236592 B2 JPS6236592 B2 JP S6236592B2
Authority
JP
Japan
Prior art keywords
coin
value
standby
correction
frequency
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
JP56159979A
Other languages
Japanese (ja)
Other versions
JPS5860390A (en
Inventor
Ko Arai
Sadao Matsumoto
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.)
Sanyo Denki Co Ltd
Original Assignee
Sanyo Denki 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 Sanyo Denki Co Ltd filed Critical Sanyo Denki Co Ltd
Priority to JP15997981A priority Critical patent/JPS5860390A/en
Publication of JPS5860390A publication Critical patent/JPS5860390A/en
Publication of JPS6236592B2 publication Critical patent/JPS6236592B2/ja
Granted legal-status Critical Current

Links

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  • Testing Of Coins (AREA)
  • Sorting Of Articles (AREA)

Description

【発明の詳細な説明】 (イ) 産業上の利用分野 本発明は、検査硬貨による発振磁界への影響度
に基づきその適正を判別するための硬貨選別方法
に関する。
DETAILED DESCRIPTION OF THE INVENTION (A) Field of Industrial Application The present invention relates to a coin sorting method for determining suitability based on the degree of influence of a test coin on an oscillating magnetic field.

(ロ) 従来の技術 一般にかかる硬貨選別は、発振磁界中に検査硬
貨を置くことによつて生じる影響度をインダクタ
ンス・周波数・位相・誘起電圧等の変化により捉
えて、硬貨の特性を測定するものである。そして
従来の硬貨選別装置としては特公昭52−6200号公
報に開示されている構成があり、これは硬貨測定
器を検査用と基準用とで二通り設け基準用には予
め真硬貨を置き検査用に検査すべき硬貨が経過し
た時両者の測定結果を比較することでこの硬貨の
適正を判定するものである。また基準の設定とし
ては、可変抵抗或いは可変キヤパシターを用い
て、基準用硬貨の電気的条件と同一とするように
した例えば特公昭48−799号公報に示す構成もあ
る。しかしながら最近は特開昭49−95692号公報
で開示されているように、かかる基準用硬貨や基
準設定部品に代わり半導体メモリを用いて、適正
硬貨の受入範囲情報や許容誤差範囲等の基準情報
を設定するようになつてきている。
(B) Conventional technology In general, such coin sorting involves measuring the characteristics of coins by capturing the degree of influence caused by placing the test coin in an oscillating magnetic field by changes in inductance, frequency, phase, induced voltage, etc. It is. As a conventional coin sorting device, there is a configuration disclosed in Japanese Patent Publication No. 52-6200, in which coin measuring devices are installed in two ways, one for inspection and one for reference, and for the reference, real coins are placed in advance for inspection. When a coin to be inspected has passed, the suitability of the coin is determined by comparing the two measurement results. Further, as for setting the reference, there is also a configuration shown in Japanese Patent Publication No. 48-799, in which a variable resistor or a variable capacitor is used to make the electrical conditions the same as those of the reference coin. However, recently, as disclosed in Japanese Patent Application Laid-Open No. 49-95692, a semiconductor memory is used instead of such standard coins and standard setting parts to store standard information such as acceptance range information of appropriate coins and tolerance range. I'm starting to set it up.

しかしながら前記基準情報は大幅に異なる情報
の硬貨を弁別する場合は受入許容誤差範囲を拡大
せしめることが可能であり実用上問題はないが、
硬貨の種類によつて硬貨検査情報が極めて酷似し
ていたり、また精巧な偽貨を投入された場合受入
許容範囲を他の正貨又は偽貨と弁別するため正貨
の受入率をあまり大きく低下させない程度に可能
な限り狭い範囲とする必要がある。この場合交番
磁界の周波数、電圧、温度又これらの測定回路に
於ける各種電気的素子の外的変化による影響はも
とより、硬貨の安定した転動による硬貨測定器か
らの測定情報を常に安定した条件となるよう回
路、素子、機構に工夫が施さなければならず装置
が複雑化する。そのため特開昭48−29499号公報
には、かかる検査条件の変動分を硬貨の測定値か
ら加減算することで、変動による影響を打消すよ
うにした硬貨選別方法についてが開示されてい
る。しかしこのような補正は必ずしも完全とはい
えず、以下の説明で明らかとなる。
However, when the standard information is used to discriminate between coins with significantly different information, it is possible to expand the acceptance tolerance range, and there is no problem in practical use.
If the coin inspection information is very similar depending on the type of coin, or if sophisticated counterfeit coins are inserted, the acceptance rate of genuine coins will be greatly reduced because the acceptance range will be differentiated from other genuine coins or counterfeit coins. It is necessary to keep the range as narrow as possible to the extent that it does not cause In this case, the measurement information from the coin measuring device due to the stable rolling of the coin is not affected by external changes such as the frequency of the alternating magnetic field, voltage, temperature, or various electrical elements in the measurement circuit, but is always kept under stable conditions. In order to achieve this, circuits, elements, and mechanisms must be devised, making the device complicated. For this reason, Japanese Patent Application Laid-Open No. 48-29499 discloses a coin sorting method in which the influence of the variation is canceled by adding or subtracting the variation in the inspection conditions from the measured value of the coin. However, such correction is not necessarily perfect, which will become clear from the description below.

(ハ) 発明が解決しようとする問題点 問題点を述べる前に硬貨選別装置の具体的な構
成を第1図から第3図までによつて説明する。第
1図で硬貨選別装置の上部の受口2より投入され
た硬貨は硬貨通路16の一側を構成する角度約10
゜の傾斜を持つた基板A2及び下方に位置するレ
ール上を他側の基板B9により構成される硬貨通
路16を転動し、順次配列された材質センサー
4、板厚センサー5、直径センサー6の各部を通
過しこれらの複数の検査器の情報が予め定められ
た基準値情報と各々一致した場合受入ゲート7を
吸引せしめ正貨通路8に導入するよう構成されて
いる。板厚センサーは基板3と基板9のそれぞれ
の壁に埋めこまれたポツト型のフエライト材で作
られたコア10とその内部に巻回されたコイル1
1及びコア12とその内部に巻回されたコイル1
3より構成され、その通路寸法Aは使用される硬
貨の最大厚みに若干の余裕を持つた寸法に設定さ
れている。投入された硬貨18の厚さはこの例の
構成に於いては硬貨のほぼ中央部の凹部の厚さT
が測定されることとなり、この寸法は基板9側セ
ンサーからの寸法Bと基板3からの寸法Cを測定
することにより硬貨中央部の厚さTを間接的に検
出することになる。
(c) Problems to be Solved by the Invention Before describing the problems, the specific structure of the coin sorting device will be explained with reference to FIGS. 1 to 3. In FIG. 1, the coins inserted from the upper socket 2 of the coin sorting device form one side of the coin passage 16 at an angle of about 10
The coins roll through a passageway 16 formed by the board A2 having an angle of 20° and the board B9 on the other side on the rail located below, and the coins are sent to the material sensor 4, plate thickness sensor 5, and diameter sensor 6 arranged in sequence. When the coin passes through each section and the information of the plurality of testers matches the predetermined reference value information, the receiving gate 7 is sucked and the genuine coin is introduced into the passage 8. The plate thickness sensor includes a pot-shaped core 10 made of ferrite material embedded in the walls of each of the substrates 3 and 9, and a coil 1 wound inside the core 10.
1 and core 12 and coil 1 wound inside it
3, and its passage dimension A is set to have a slight margin for the maximum thickness of the coins used. In the configuration of this example, the thickness of the inserted coin 18 is equal to the thickness T of the recessed portion approximately in the center of the coin.
will be measured, and this dimension will indirectly detect the thickness T of the center portion of the coin by measuring the dimension B from the substrate 9 side sensor and the dimension C from the substrate 3.

第3図は第2図に示した各々のコイル11,1
3の接続方法とその回路構成である。なお本回路
は説明上板厚検査回路のみを示しており他の検査
回路は省略している。コイル13とコイル11は
相互インダクタンスが負となるよう互に発振磁界
を打ち消すように直列逆相接続を行ない発振回路
19に入る。前記直列逆相接続は通路寸法Aが変
化した場合、例えば広くなつた場合にはコイル1
3とコイル11の合計のインダクタンスが大きく
なつて発振周波数が下がり、通路寸法の増加によ
る低下分を補償するよう作用するものである。
Figure 3 shows each coil 11, 1 shown in Figure 2.
This is the connection method of No. 3 and its circuit configuration. In this circuit, only the board thickness inspection circuit is shown for the sake of explanation, and other inspection circuits are omitted. The coils 13 and 11 enter the oscillation circuit 19 by making a series anti-phase connection so as to mutually cancel out the oscillating magnetic fields so that the mutual inductance becomes negative. The series anti-phase connection is used when the passage dimension A changes, for example when it becomes wider.
The total inductance of coil 3 and coil 11 increases, lowering the oscillation frequency, and acts to compensate for the decrease due to the increase in path size.

発振回路19は内蔵されたキヤパシターとコイ
ル13とコイル11により得られるインダクタン
スとで決定される発振周波数で発振するよう構成
され、更に発振波形を正弦波から論理回路レベル
になるよう波形整形回路を内蔵している。発振回
路19の出力は判定演算回路21に入力されてお
り、該回路では硬貨がコイル13とコイル11と
の間を通過したときの発振磁界の影響度である発
振周波数の値と記憶装置22に設定している基準
情報とを照合し、許容誤差範囲内で一致していれ
ば板厚センサー5による測定結果としては正貨で
あることを示す信号23或いは複数の硬貨種のう
ちのある特定種類であることを示す信号23を出
力する。
The oscillation circuit 19 is configured to oscillate at an oscillation frequency determined by the built-in capacitor, the coil 13, and the inductance obtained by the coil 11, and further includes a built-in waveform shaping circuit to change the oscillation waveform from a sine wave to a logic circuit level. are doing. The output of the oscillation circuit 19 is input to a judgment calculation circuit 21, which stores the value of the oscillation frequency, which is the degree of influence of the oscillation magnetic field when the coin passes between the coils 13 and 11, and the storage device 22. If the set standard information is checked and they match within the allowable error range, the measurement result by the plate thickness sensor 5 is a signal 23 indicating that the coin is a genuine coin, or a specific type among a plurality of coin types. It outputs a signal 23 indicating that.

第4図は上記した構成の硬貨選別装置におい
て、硬貨の存在しないとき及び厚さ1.0mm・1.5
mm・2.0mmの各硬貨が存在するときの周波数変化
を示すもので、この特性図により検査条件の変動
に応じて硬貨の測定値を有効に補正しなければな
らないことが理解できる。即ち、同図において、
横軸Tは各種投入硬貨又は相当する偽貨等の中央
部の厚さ寸法を表わし縦軸は第3図に於ける発振
回路19の出力20である発振周波数を示してお
り、T0点は硬貨の投入が無い場合の発振周波数
であり待機時周波数である。この待機時周波数は
前述のようにコイル13,11と発振回路19の
内部のコンデンサー及び発振器の特性によつて決
定される周波数である。T0線上の
は待機時周波数であり、は工場等での調
整時に記憶装置22に基準情報を設定した時の発
振周波数であり、はいずれも外的要因
例えばポツトコア10又は12のフエライト等の
透磁率や発振回路内部のコンデンサーの容量変化
や通路寸法Aの経時変化等による検査条件の変化
に伴ない待機発振周波数が変化した状態を示して
いる。の関係は周波数で
であり、は周波数の上昇、
周波数の下降を夫々示している。この例では説明
上理解しやすいように()=(
)としている。このような条件に於いて硬貨厚
みTを種々変えた場合その発振周波数の変化はグ
ラフのようになり、例えば2.0mmの厚さの硬貨を
投入した場合各々の待機周波数に応じて待機周波
数がの場合は0T2.0の場合は1T2.
0の場合は2T2.0となり、その各々の差
2T2.0)−(0T2.0)は(0T2.0)−(1T2.0

り大きくなる。またそれぞれの差は待機周波数の
それぞれの差すなわち()−()や(
)−()よりも大きくなつていることが理解
出来る。また、1.0mmの硬貨を投入した場合の同
様の差も同じ傾向を示しているが(2T2.0)−
0T2.0)より同条件のT1.0部の発振周波数の差
は小さい。この理由は待機発振周波数に対し硬貨
投入時の変化は等比変化をすることと、厚い硬貨
の方が特に基板9側のセンサーに近ずくためコイ
ル13の変化が大きくなつて、インダクタンス変
化が指数函数的に増大する傾向にあることを示し
ている。
Figure 4 shows the coin sorting device with the above configuration, when there are no coins and when the thickness is 1.0 mm/1.5 mm.
This shows the frequency change when there are mm and 2.0 mm coins, and this characteristic diagram allows you to understand that the measured value of the coin must be effectively corrected in response to fluctuations in the inspection conditions. That is, in the same figure,
The horizontal axis T represents the thickness of the central part of various inserted coins or equivalent counterfeit coins, etc., and the vertical axis represents the oscillation frequency, which is the output 20 of the oscillation circuit 19 in FIG. 3, and the T 0 point is This is the oscillation frequency when no coins are inserted, and is the standby frequency. As described above, this standby frequency is determined by the characteristics of the coils 13, 11, the capacitors inside the oscillation circuit 19, and the oscillator. 1 , 0 , on the T 0 line
2 is the standby frequency, 0 is the oscillation frequency when reference information is set in the storage device 22 during adjustment at the factory, etc., and 1 and 2 are both caused by external factors such as ferrite of pot core 10 or 12. This shows a state in which the standby oscillation frequency changes due to changes in inspection conditions due to changes in magnetic permeability, capacitance of the capacitor inside the oscillation circuit, changes in passage dimension A over time, etc. The relationship between 2 , 0 , 1 is 2 > in frequency
0 > 1 , 2 indicates an increase in frequency, and 1 indicates a decrease in frequency. In this example, ( 20 ) = ( 0
1 ). Under these conditions, if the coin thickness T is varied, the change in the oscillation frequency will be as shown in the graph.For example, if a coin with a thickness of 2.0 mm is inserted, the standby frequency will change to 0 depending on the standby frequency. 0 T 2 . 0 for , 1 T 2 . for 1 .
In the case of 0 and 2 , it becomes 2 T 2 . 0 , and the difference between them ( 2 T 2 . 0 ) − ( 0 T 2 . 0 ) is ( 0 T 2 . 0 ) − ( 1 T 2 . 0 )
Become bigger. Also, each difference is the difference in standby frequency, that is, ( 2 ) - ( 0 ) or (
It can be seen that it is larger than 0 )-( 1 ). Also, the same difference when inserting a 1.0 mm coin shows the same trend, but ( 2 T 2.0 )−
( 0 T 2 . 0 ), the difference in oscillation frequency in the T 1 . 0 part under the same conditions is small. The reason for this is that the change in the standby oscillation frequency when a coin is inserted is a geometric change, and the thicker coin is closer to the sensor on the board 9 side, so the change in the coil 13 becomes larger, and the inductance change becomes exponential. This shows that there is a tendency to increase functionally.

このように検査条件の変動に対して測定周波数
の変化は一様ではなく、上記した特開昭48−
29499号公報で示されているような硬貨投入時の
発振周波数より待機時の発振周波数の変動分をそ
のまま加減算する補正の方法や、待機時の発振周
波数の変動分に一率の補正係数を乗じて補正する
方法は不完全である。したがつてかかる補正の下
では正貨のみを受け入れようとして、許容誤差範
囲を狭く設定することは非常に困難となる。
In this way, the change in the measurement frequency is not uniform as the inspection conditions change;
There is a correction method that directly adds or subtracts the variation in the oscillation frequency during standby from the oscillation frequency when coins are inserted, as shown in Publication No. 29499, or a correction method in which the variation in the oscillation frequency during standby is multiplied by a correction coefficient of 1%. This method of correction is incomplete. Therefore, under such correction, it is extremely difficult to set a narrow tolerance range in order to accept only genuine coins.

したがつて本発明は、検査硬貨により得られた
測定値を、待機周波数の変動の具合や硬貨の特性
(例えば厚さ)の違いから派生する測定の不均衡
の度合に応じて補正することができる硬貨選別方
法を提供するものである。
Therefore, the present invention makes it possible to correct the measurement values obtained from the test coins according to the degree of measurement imbalance resulting from variations in the standby frequency and differences in coin characteristics (e.g., thickness). The present invention provides a method for sorting coins.

(ニ) 問題点を解決するための手段 上記の問題点を解決するために本発明に依る硬
貨選別方法は、第4図の特性図で説明すると、装
置の調整時において発振磁界に硬貨が存在しない
ときの測定値である第1待機値を予め設定し
ておき、装置の稼動時において発振磁界に検査硬
貨が存在する直前の測定値である第2待機値
を検出すると、第1待機値と第2待機値との差
)に所定の第1の補正係数αを掛け
て検査条件の変動度を示す第1補正値(
)・αを演算し、装置の稼動時において発振磁
界に検査硬貨が存在すると、そのときの前記影響
度を示す硬貨の測定値2T2.0と前記第2待機値
との差(2T2.0)に所定の第2の補正係
数βを掛けて硬貨の特性変化に原因する変動度を
示す第2補正値(2T2.0)・βを演算し、
次に硬貨測定値2T2.0を第1補正値(
)・α,第2補正値(2T2.0)・β及び
第1待機値と第2待機値との差(
)にて次式を演算し、 x=2T2.0−〔()・α +(2T2.0)・β+()〕
…… この補正による演算値xに基づき検査硬貨の
適正を判別する。
(d) Means for Solving the Problems In order to solve the above problems, the coin sorting method according to the present invention is explained using the characteristic diagram of FIG. A first standby value 0 is set in advance, which is the measured value when the test coin is not present, and a second standby value 2 is set in advance, which is the measured value immediately before the test coin is present in the oscillating magnetic field when the device is operating.
When detected, the difference ( 2-0 ) between the first standby value and the second standby value is multiplied by a predetermined first correction coefficient α to obtain a first correction value ( 2-0 ) indicating the degree of variation in the inspection conditions.
0 )・α is calculated, and if a test coin is present in the oscillating magnetic field during operation of the device, the difference between the measured value 2 T 2.0 of the coin indicating the degree of influence at that time and the second standby value ( 2 T 2 . 02 ) is multiplied by a predetermined second correction coefficient β to calculate a second correction value ( 2 T 2 . 02 ) β indicating the degree of fluctuation caused by changes in the coin characteristics,
Next, the coin measurement value 2 T 2 . 0 is converted to the first correction value ( 2
0 )・α, the second correction value ( 2 T 2 . 02 )・β, and the difference between the first standby value 0 and the second standby value 2 ( 2
0 ), calculate the following formula, x= 2 T 2 . 0 − [( 20 ) α + ( 2 T 2 .
... The suitability of the test coin is determined based on the calculated value x resulting from this correction.

(ホ) 作用 式において、硬貨の測定値2T2.0から待機
時の発振周波数の変動分()を引算す
るのは従来の補正であり、これにより待機周波数
の変化に比例して変化した分が補正される。そし
て更に2T2.0から第1補正値()・α
を引算することで、待機周波数の変化にて指数函
数的に変化した部分が補正されることになる。し
かもこのとき待機周波数の変動()に
応じて第1補正値を演算することで、検査周波数
の全ての領域で有効な補正となる。同時に2T2.
0から第2補正値(2T2.0)・βを引算す
ることで、硬貨の特性の差による不均衡に対する
補正が成される。
(e) Effect In the formula, the conventional correction is to subtract the variation in the oscillation frequency during standby ( 2 - 0 ) from the coin measurement value 2 T 2 . The amount of change is corrected. Then, from 2 T 2. 0 , the first correction value ( 20 )・α
By subtracting , the part that changes exponentially due to the change in standby frequency is corrected. Moreover, by calculating the first correction value according to the variation ( 2-0 ) of the standby frequency at this time, the correction becomes effective in all regions of the test frequency. 2 T 2 at the same time.
By subtracting the second correction value ( 2 T 2 . 02 )·β from 0 , the imbalance caused by the difference in the characteristics of the coins is corrected.

(ヘ) 実施例 第5図は硬貨選別の制御回路を示しており、装
置の構成及び板厚センサー5の構造は第1図及び
第2図と同じである。硬貨が受口2より投入され
ると先ず材質センサー4を通過し、この材質セン
サー4の出力にて材質判別回路15は材質の面か
らこの硬貨の適正を判別するが、本発明とは直接
には係りをもたないために説明を省略する。同時
に材質判別回路15は待機周波数取り込み回路2
6に硬貨投入信号14を出力する。該信号14の
入力により待機周波数取り込み回路26は発振回
路19の周波数を取り込む。硬貨が材質センサー
4を通過しそれにより材質判別回路15が硬貨投
入信号14を出力している状態は、板厚センサー
5にとつては硬貨が通過する直前の待機状態であ
り、待機周波数取り込み回路26は装置の稼動時
における板厚センサー5の待機周波数を取り込ん
だことになる。記憶装置22の待機周波数記憶部
28には装置の生産時等の調整時における板厚セ
ンサー5の待機周波数が設定されており、待機周
波数変動分演算回路27は調整時と稼動時におけ
る待機周波数の変化を演算して、その結果を補正
回路30に出力する。しかして材質センサー4を
通過した硬貨が板厚センサー5に達し、ピーク値
検出回路29はそのときの最大周波数を検出する
と、これを硬貨による影響度を示す測定値として
補正回路30に出力する。補正回路30は、調整
時の待機周波数即ち第1待機値と稼動時の待機周
波数即ち第2待機値との差を算出し、その差の値
に待機周波数の変化に対する補正用係数αを掛け
て第1補正値を演算する。また補正回路30は測
定値と第2待機値との差を演出し、その差の値に
硬貨の厚さの差による不均衡に対する補正用係数
βを掛けて第2補正値を演算する。そして補正回
路30は、測定値から第1補正値と第2補正値と
待機周波数の変化値を引いて測定値を補正する。
この補正用係数α,βの値はセンサーの感度、通
路寸法の大小、複数の硬貨厚さによる差等で決定
される定数である。このようにして補正回路30
にて補正された測定値は、照合回路32で記憶装
置22の受入許容範囲情報記憶部3に設定されて
いる基準情報と比較される。そして照合回路32
は補正測定値が受入許容範囲内にあれば板厚測定
に関して正貨又は金種を示す信号23Aを出力す
る。
(F) Embodiment FIG. 5 shows a control circuit for coin sorting, and the configuration of the device and the structure of the plate thickness sensor 5 are the same as those in FIGS. 1 and 2. When a coin is inserted into the socket 2, it first passes through the material sensor 4, and based on the output of the material sensor 4, the material discrimination circuit 15 determines whether the coin is suitable from the viewpoint of the material, but this is not directly related to the present invention. The explanation will be omitted because it is unrelated. At the same time, the material discrimination circuit 15 is connected to the standby frequency acquisition circuit 2.
A coin insertion signal 14 is output to 6. Upon input of the signal 14, the standby frequency acquisition circuit 26 acquires the frequency of the oscillation circuit 19. The state in which the coin passes through the material sensor 4 and the material discrimination circuit 15 outputs the coin insertion signal 14 is a standby state for the plate thickness sensor 5 just before the coin passes, and the standby frequency acquisition circuit 26 is the standby frequency of the plate thickness sensor 5 when the device is in operation. The standby frequency of the plate thickness sensor 5 at the time of adjustment, such as during production of the device, is set in the standby frequency storage section 28 of the storage device 22, and the standby frequency fluctuation calculation circuit 27 stores the standby frequency at the time of adjustment and operation. The change is calculated and the result is output to the correction circuit 30. The coin that has passed through the material sensor 4 reaches the plate thickness sensor 5, and when the peak value detection circuit 29 detects the maximum frequency at that time, it outputs this to the correction circuit 30 as a measured value indicating the degree of influence by the coin. The correction circuit 30 calculates the difference between the standby frequency during adjustment, that is, the first standby value, and the standby frequency during operation, that is, the second standby value, and multiplies the value of the difference by a correction coefficient α for the change in standby frequency. A first correction value is calculated. Further, the correction circuit 30 produces a difference between the measured value and the second standby value, and calculates a second correction value by multiplying the value of the difference by a correction coefficient β for the imbalance due to the difference in the thickness of the coin. Then, the correction circuit 30 corrects the measured value by subtracting the first correction value, the second correction value, and the standby frequency change value from the measured value.
The values of the correction coefficients α and β are constants determined by the sensitivity of the sensor, the size of the passage, the difference due to the thickness of a plurality of coins, etc. In this way, the correction circuit 30
The corrected measurement value is compared with reference information set in the acceptance range information storage section 3 of the storage device 22 in the comparison circuit 32. and verification circuit 32
outputs a signal 23A indicating the specie or denomination for plate thickness measurement if the corrected measured value is within the acceptable range.

本例では適用した場合に最も効果的である板厚
センサー5にて説明したが、材質センサー4でも
直径センサー6でも同じである。
In this example, the description has been made using the plate thickness sensor 5, which is most effective when applied, but the same applies to the material sensor 4 and the diameter sensor 6.

(ト) 発明の効果 本発明によると、検査条件の変動に応じて全て
の領域での有効な補正が可能となるために、許容
誤差範囲を狭く設定でき正確な硬貨選別を行なう
ことができる。しかも周波数の変動に加えて、硬
貨の厚さ等による特性差によつて影響が出過ぎた
分も補正するために、誤差範囲をとり入れた適確
な判定動作を行なうことが出来るものである。
(G) Effects of the Invention According to the present invention, since effective correction can be made in all areas according to variations in inspection conditions, the allowable error range can be set narrowly and accurate coin sorting can be performed. Furthermore, in addition to frequency fluctuations, it is possible to perform accurate judgment operations that take into account error ranges in order to compensate for excessive influences due to differences in characteristics due to coin thickness, etc.

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

第1図は、硬貨選別装置の概略図、第2図は、
板厚センサーの断面図、第3図は制御回路、第4
図は、硬貨に対する板厚特性、第5図は、本発明
に依る制御回路を示す。 5……板厚センサー、13,11……コイル、
29……ピーク値検出回路、30……補正回路。
Figure 1 is a schematic diagram of the coin sorting device, Figure 2 is
Cross-sectional view of the plate thickness sensor, Figure 3 is the control circuit, Figure 4 is the control circuit.
The figure shows plate thickness characteristics for coins, and FIG. 5 shows a control circuit according to the present invention. 5... Plate thickness sensor, 13, 11... Coil,
29...Peak value detection circuit, 30...Correction circuit.

Claims (1)

【特許請求の範囲】[Claims] 1 発振磁界を形成し、検査硬貨による発振磁界
への影響度を測定して該検査硬貨の適正を判別す
る硬貨選別装置における硬貨選別方法であつて、
装置の調整時において発振磁界に硬貨が存在しな
いときの測定値である第1待機値を予め設定して
おき、装置の稼動時において発振磁界に検査硬貨
が存在する直前の測定値である第2待機値を検出
すると、第1待機値と第2待機値との差に所定の
第1の補正係数を掛けて検査条件の変動度を示す
第1補正値を演算し、装置の稼動時において発振
磁界に検査硬貨が存在すると、そのときの前記影
響度を示す硬貨の測定値と前記第2待機値との差
に所定の第2の補正係数を掛けて硬貨の特性変化
に原因する変動度を示す第2補正値を演算し、次
に前記硬貨測定値を第1補正値・第2補正値及び
第1待機値と第2待機値との差の値とに基づき補
正して、該補正による演算値に基づき検査硬貨の
適正を判別することを特徴とした硬貨選別方法。
1. A coin sorting method in a coin sorting device that forms an oscillating magnetic field and determines the suitability of the test coin by measuring the influence of the test coin on the oscillating magnetic field,
A first standby value, which is a measured value when no coin is present in the oscillating magnetic field, is set in advance when adjusting the device, and a second standby value, which is a measured value immediately before a coin exists in the oscillating magnetic field, is set in advance when the device is operating. When the standby value is detected, a first correction value indicating the degree of variation in the inspection conditions is calculated by multiplying the difference between the first standby value and the second standby value by a predetermined first correction coefficient, and oscillation is detected when the device is operating. When a test coin exists in the magnetic field, the difference between the measured value of the coin indicating the degree of influence at that time and the second standby value is multiplied by a predetermined second correction coefficient to calculate the degree of variation caused by the change in the characteristics of the coin. The coin measurement value is then corrected based on the first correction value, the second correction value, and the difference between the first standby value and the second standby value, and A coin sorting method characterized by determining the suitability of test coins based on calculated values.
JP15997981A 1981-10-06 1981-10-06 Selection of coin Granted JPS5860390A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP15997981A JPS5860390A (en) 1981-10-06 1981-10-06 Selection of coin

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP15997981A JPS5860390A (en) 1981-10-06 1981-10-06 Selection of coin

Publications (2)

Publication Number Publication Date
JPS5860390A JPS5860390A (en) 1983-04-09
JPS6236592B2 true JPS6236592B2 (en) 1987-08-07

Family

ID=15705344

Family Applications (1)

Application Number Title Priority Date Filing Date
JP15997981A Granted JPS5860390A (en) 1981-10-06 1981-10-06 Selection of coin

Country Status (1)

Country Link
JP (1) JPS5860390A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
ZA851248B (en) * 1984-03-01 1985-11-27 Mars Inc Self tuning coin recognition system

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5426200B2 (en) * 1974-01-31 1979-09-03
JPS56110194A (en) * 1980-02-05 1981-09-01 Sanyo Jido Hanbaiki Kk Compensation method of electronic coin selector

Also Published As

Publication number Publication date
JPS5860390A (en) 1983-04-09

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