JPH06201806A - Magnetic sensor device - Google Patents

Magnetic sensor device

Info

Publication number
JPH06201806A
JPH06201806A JP5000590A JP59093A JPH06201806A JP H06201806 A JPH06201806 A JP H06201806A JP 5000590 A JP5000590 A JP 5000590A JP 59093 A JP59093 A JP 59093A JP H06201806 A JPH06201806 A JP H06201806A
Authority
JP
Japan
Prior art keywords
magnetic sensor
voltage
sensor device
amplifier
resistance
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
JP5000590A
Other languages
Japanese (ja)
Inventor
Hiroshi Suzuki
洋 鈴木
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.)
Murata Manufacturing Co Ltd
Original Assignee
Murata 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 Murata Manufacturing Co Ltd filed Critical Murata Manufacturing Co Ltd
Priority to JP5000590A priority Critical patent/JPH06201806A/en
Publication of JPH06201806A publication Critical patent/JPH06201806A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To prevent the fluctuation in amplification degree due to the unevenness of characteristics of a magnetoresistance element and the differences of temperature-resistance characteristics. CONSTITUTION:Magnetoresistance elements M1, M2 are connected in series and the series circuit is connected to Vcc-Gnd terminals of a power source. After the voltage Va of the connection point of the magnetoresistance elements M1, M2 is buffered and amplified by a buffer B, the voltage is amplified by a reversal amplifier A1. The output of the reversal amplifier A1 is regarded as a detection voltage Vo. As a result, even when there are the unevenness of characteristics of the magnetoresistance elements and the differences of temperature-resistance characteristics, the fluctuation of amplification degree does not occur. Further, it is unnecessary to make the characteristics of the magnetoresistance elements uniform, thereby improving the manufacturing yield of the title devices.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】この発明は、磁気センサ装置に関
し、さらに詳しくは、磁気抵抗素子の特性のバラツキや
温度−抵抗特性の差異による不都合を解消した磁気セン
サ装置に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a magnetic sensor device, and more particularly to a magnetic sensor device which eliminates inconveniences due to variations in the characteristics of magnetoresistive elements and differences in temperature-resistance characteristics.

【0002】[0002]

【従来の技術】図5は、紙幣識別機に用いられている従
来の磁気センサ装置の一例を示す回路図である。この磁
気センサ装置51では、ソケットS内の紙幣挿入スリッ
ト付近に、紙幣Mの移動方向と平行に、磁気抵抗素子M
1,M2が内設されている。磁気抵抗素子M1,M2は
直列接続され、その直列回路は電源Vcc−Gnd間に
接続されている。そして、磁気抵抗素子M1,M2の接
続点の電圧VaをコンデンサCおよび入力抵抗Riを介
して反転増幅器A1の反転入力端子に入力する。その反
転増幅器A1の反転入力端子と出力端子の間には帰還抵
抗Rfが接続され、また、反転増幅器A1の非反転入力
端子には基準電圧Vrが入力されている。そして、反転
増幅器A1の出力端子から検出電圧Voが出力される。
2. Description of the Related Art FIG. 5 is a circuit diagram showing an example of a conventional magnetic sensor device used in a bill validator. In this magnetic sensor device 51, the magnetic resistance element M is provided in the vicinity of the bill insertion slit in the socket S in parallel with the moving direction of the bill M.
1, M2 are installed internally. The magnetoresistive elements M1 and M2 are connected in series, and the series circuit is connected between the power supply Vcc and Gnd. Then, the voltage Va at the connection point between the magnetoresistive elements M1 and M2 is input to the inverting input terminal of the inverting amplifier A1 via the capacitor C and the input resistor Ri. A feedback resistor Rf is connected between the inverting input terminal and the output terminal of the inverting amplifier A1, and the reference voltage Vr is input to the non-inverting input terminal of the inverting amplifier A1. Then, the detection voltage Vo is output from the output terminal of the inverting amplifier A1.

【0003】次に、この磁気センサ装置51の動作を説
明する。紙幣が挿入されるとき、接続点の電圧Vaの電
圧Vaは図6の(a)に示す波形となる。但し、Viは
中性電圧を示す。反転増幅器A1からの出力される検出
電圧Voは、 Vo=〔−Rf/{Ri+M1・M2/(M1+M2)}〕・k・Vcc…(1) なので、図6の(b)に示す波形となる。
Next, the operation of the magnetic sensor device 51 will be described. When a bill is inserted, the voltage Va of the voltage Va at the connection point has the waveform shown in (a) of FIG. However, Vi shows a neutral voltage. The detection voltage Vo output from the inverting amplifier A1 is Vo = [− Rf / {Ri + M1 · M2 / (M1 + M2)}] · k · Vcc (1), and thus has the waveform shown in (b) of FIG. .

【0004】[0004]

【発明が解決しようとする課題】上記従来の磁気センサ
装置51では、上記(1)式から判るように反転増幅器A
1の増幅度が磁気抵抗素子M1,M2に依存するので、
入力抵抗Riや帰還抵抗Rfを等しくしても、磁気抵抗
素子M1,M2のバラツキや温度−抵抗特性により増幅
度にバラツキを生じる問題点がある。また、この増幅度
にバラツキをなくすために、磁気抵抗素子M1,M2の
特性を揃えようとすると、歩留りが低くなる問題点があ
る。そこで、この発明の目的は、磁気抵抗素子の特性の
バラツキや温度−抵抗特性の差異があっても検出電圧が
変動しない磁気センサ装置を提供し、歩留りを向上させ
ることにある。
In the conventional magnetic sensor device 51 described above, the inverting amplifier A is used as can be seen from the equation (1).
Since the amplification factor of 1 depends on the magnetoresistive elements M1 and M2,
Even if the input resistance Ri and the feedback resistance Rf are made equal, there is a problem in that the amplification degree varies due to variations in the magnetoresistive elements M1 and M2 and temperature-resistance characteristics. Further, if the characteristics of the magnetoresistive elements M1 and M2 are made uniform in order to eliminate the variation in the amplification degree, there is a problem that the yield is reduced. Therefore, an object of the present invention is to provide a magnetic sensor device in which the detection voltage does not fluctuate even if there are variations in the characteristics of the magnetoresistive elements or differences in temperature-resistance characteristics, and to improve the yield.

【0005】[0005]

【課題を解決するための手段】この発明による磁気セン
サ装置は、2個の磁気抵抗素子の直列接続からなる磁気
センサを電源Vcc−Gnd間に接続し、前記2個の磁
気抵抗素子の接続点から信号電圧を取り出し、前記信号
電圧をバッファを介して増幅器に入力するか,または前
記磁気センサに対して高入力インピーダンスの増幅器に
入力し、前記増幅器の出力を検出信号として取り出すこ
とを構成上の特徴とするものである。
In the magnetic sensor device according to the present invention, a magnetic sensor consisting of two magnetoresistive elements connected in series is connected between a power source Vcc and Gnd, and the connection point of the two magnetoresistive elements is connected. A signal voltage is taken out from the device, and the signal voltage is inputted to an amplifier via a buffer, or is inputted to an amplifier having a high input impedance with respect to the magnetic sensor, and the output of the amplifier is taken out as a detection signal. It is a feature.

【0006】[0006]

【作用】この発明による磁気センサ装置は、2個の磁気
抵抗素子の接続点からの信号電圧をバッファを介して増
幅器に入力するか,または前記磁気センサに対して高入
力インピーダンスの増幅器を用いる。このため、増幅器
の増幅度に磁気抵抗素子の特性のバラツキや温度−抵抗
特性の差異が影響しなくなる。また、磁気抵抗素子M
1,M2の特性を揃える必要がなくなるため、歩留りが
向上する。
In the magnetic sensor device according to the present invention, the signal voltage from the connection point of the two magnetoresistive elements is input to the amplifier via the buffer, or an amplifier having a high input impedance is used for the magnetic sensor. Therefore, variations in the characteristics of the magnetoresistive element and differences in temperature-resistance characteristics do not affect the amplification degree of the amplifier. In addition, the magnetic resistance element M
Since it is not necessary to match the characteristics of 1 and M2, the yield is improved.

【0007】[0007]

【実施例】以下、図に示す実施例によりこの発明をさら
に詳しく説明する。なお、これによりこの発明が限定さ
れるものではない。
The present invention will be described in more detail with reference to the embodiments shown in the drawings. The present invention is not limited to this.

【0008】−第1実施例− この発明の第1実施例の磁気センサ装置であって、紙幣
識別機に用いられているものを、図1に示す。この磁気
センサ装置1では、ソケットS内の紙幣挿入スリット付
近に、紙幣Mの移動方向と平行に磁気抵抗素子M1,M
2が内設されている。磁気抵抗素子M1,M2は直列接
続され、その直列回路は電源Vcc−Gnd間に接続さ
れている。そして、磁気抵抗素子M1,M2の接続点の
電圧Vaは、バッファBに入力される。そのバッファB
の出力電圧Vbは、コンデンサCと入力抵抗Riを介し
て反転増幅器A1の反転入力端子に入力される。その反
転増幅器A1の反転入力端子と出力端子の間には帰還抵
抗Rfが接続され、また、反転増幅器A1の非反転入力
端子には基準電圧Vrが入力されている。そして、反転
増幅器A1の出力端子から検出電圧Voが出力される。
First Embodiment FIG. 1 shows a magnetic sensor device according to a first embodiment of the present invention, which is used in a bill validator. In this magnetic sensor device 1, in the vicinity of the bill insertion slit in the socket S, the magnetic resistance elements M1 and M are arranged parallel to the moving direction of the bill M.
2 is installed internally. The magnetoresistive elements M1 and M2 are connected in series, and the series circuit is connected between the power supply Vcc and Gnd. Then, the voltage Va at the connection point between the magnetoresistive elements M1 and M2 is input to the buffer B. Its buffer B
Output voltage Vb is input to the inverting input terminal of the inverting amplifier A1 via the capacitor C and the input resistor Ri. A feedback resistor Rf is connected between the inverting input terminal and the output terminal of the inverting amplifier A1, and the reference voltage Vr is input to the non-inverting input terminal of the inverting amplifier A1. Then, the detection voltage Vo is output from the output terminal of the inverting amplifier A1.

【0009】次に、この磁気センサ装置1の動作を説明
する。紙幣が挿入されるとき、接続点の電圧Vaの電圧
Vaは図2の(a)に示す波形となる。但し、Viは中
性電圧を示す。そこで、バッファBからの出力電圧Vb
は、図2の(b)に示す波形となる。反転増幅器A1か
らの出力される検出電圧Voは、 Vo=(−Rf/Ri)・Vb …(2) なので、図2の(c)に示す波形となる。
Next, the operation of the magnetic sensor device 1 will be described. When a bill is inserted, the voltage Va of the connection point voltage Va has a waveform shown in FIG. However, Vi shows a neutral voltage. Therefore, the output voltage Vb from the buffer B
Has the waveform shown in FIG. The detection voltage Vo output from the inverting amplifier A1 is Vo = (− Rf / Ri) · Vb (2), and thus has the waveform shown in (c) of FIG.

【0010】(2)式から判るように、反転増幅器A1の
増幅度は入力抵抗Riと帰還抵抗Rfのみに依存し、磁
気抵抗素子M1,M2に依存しない。すなわち、増幅度
は、磁気抵抗素子M1,M2のバラツキや温度特性の差
異の影響を受けなくなる。このため、磁気抵抗素子M
1,M2の特性を揃える必要がなくなり、歩留りを向上
できる。
As can be seen from the equation (2), the amplification degree of the inverting amplifier A1 depends only on the input resistance Ri and the feedback resistance Rf, and does not depend on the magnetoresistive elements M1 and M2. That is, the amplification degree is not affected by variations in the magnetoresistive elements M1 and M2 and differences in temperature characteristics. Therefore, the magnetoresistive element M
It is not necessary to match the characteristics of 1 and M2, and the yield can be improved.

【0011】−第2実施例− この発明の第2実施例の磁気センサ装置であって、紙幣
識別機に用いられているものを、図3に示す。この磁気
センサ装置21では、ソケットS内の紙幣挿入スリット
付近に、紙幣Mの移動方向と平行に磁気抵抗素子M1,
M2が内設されている。磁気抵抗素子M1,M2は直列
接続され、その直列回路は電源Vcc−Gnd間に接続
されている。そして、磁気抵抗素子M1,M2の接続点
の電圧Vpは、非反転増幅器A2の非反転入力端子に入
力される。その非反転増幅器A2の反転入力端子と出力
端子の間には帰還抵抗Rbが接続され、また、非反転増
幅器A2の反転入力端子は接地抵抗Raと接地コンデン
サC1を介して接地されている。そして、非反転増幅器
A2の出力電圧Vqは、コンデンサC2を介して、抵抗
R1と抵抗R2とにより基準電圧Vrに調整された分圧
点に入力され、その分圧点の電圧が検出電圧Voとして
出力される。
-Second Embodiment- FIG. 3 shows a magnetic sensor device according to a second embodiment of the present invention, which is used in a bill validator. In this magnetic sensor device 21, in the vicinity of the bill insertion slit in the socket S, the magnetic resistance elements M1 and M1 are arranged parallel to the moving direction of the bill M.
M2 is installed internally. The magnetoresistive elements M1 and M2 are connected in series, and the series circuit is connected between the power supply Vcc and Gnd. The voltage Vp at the connection point between the magnetoresistive elements M1 and M2 is input to the non-inverting input terminal of the non-inverting amplifier A2. A feedback resistor Rb is connected between the inverting input terminal and the output terminal of the non-inverting amplifier A2, and the inverting input terminal of the non-inverting amplifier A2 is grounded via a grounding resistor Ra and a grounding capacitor C1. The output voltage Vq of the non-inverting amplifier A2 is input via the capacitor C2 to the voltage dividing point adjusted to the reference voltage Vr by the resistors R1 and R2, and the voltage at the voltage dividing point is used as the detection voltage Vo. Is output.

【0012】次に、この磁気センサ装置21の動作を説
明する。紙幣が挿入されるとき、接続点の電圧Vaの電
圧Vpは図4の(a)に示す波形となる。但し、Viは
中性電圧を示す。そこで、非反転増幅器A2からの出力
電圧Vqは、図2の(b)に示す波形となる。検出電圧
Voは、 Vo=(1+Rb/Ra)・Vp …(3) なので、図4の(c)に示す波形となる。
Next, the operation of the magnetic sensor device 21 will be described. When a bill is inserted, the voltage Vp of the voltage Va at the connection point has the waveform shown in FIG. However, Vi shows a neutral voltage. Therefore, the output voltage Vq from the non-inverting amplifier A2 has the waveform shown in FIG. Since the detected voltage Vo is Vo = (1 + Rb / Ra) · Vp (3), it has the waveform shown in FIG. 4 (c).

【0013】(2)式から判るように、非反転増幅器A2
の増幅度は帰還抵抗Rbと接地抵抗Raのみに依存し、
磁気抵抗素子M1,M2に依存しない。すなわち、増幅
度は、磁気抵抗素子M1,M2のバラツキや温度特性の
差異の影響を受けなくなる。このため、磁気抵抗素子M
1,M2の特性を揃える必要がなくなり、歩留りを向上
できる。
As can be seen from the equation (2), the non-inverting amplifier A2
The amplification degree of depends only on the feedback resistance Rb and the ground resistance Ra,
It does not depend on the magnetoresistive elements M1 and M2. That is, the amplification degree is not affected by variations in the magnetoresistive elements M1 and M2 and differences in temperature characteristics. Therefore, the magnetoresistive element M
It is not necessary to match the characteristics of 1 and M2, and the yield can be improved.

【0014】[0014]

【発明の効果】この発明の磁気センサ装置によれば、磁
気抵抗素子の特性のバラツキや温度−抵抗特性の差異が
あっても増幅度が変動しなくなる。そして、このため、
磁気抵抗素子の特性を揃える必要がなくなり、歩留りを
向上することが出来る。
According to the magnetic sensor device of the present invention, the amplification factor does not change even if there is a variation in the characteristics of the magnetoresistive element or a difference in temperature-resistance characteristics. And for this reason,
It is not necessary to match the characteristics of the magnetoresistive elements, and the yield can be improved.

【図面の簡単な説明】[Brief description of drawings]

【図1】この発明の磁気センサ装置の第1実施例を示す
回路図である。
FIG. 1 is a circuit diagram showing a first embodiment of a magnetic sensor device of the present invention.

【図2】図1の磁気センサ装置の各部の波形図である。FIG. 2 is a waveform diagram of each part of the magnetic sensor device of FIG.

【図3】この発明の磁気センサ装置の第2実施例を示す
回路図である。
FIG. 3 is a circuit diagram showing a second embodiment of the magnetic sensor device of the present invention.

【図4】図3の磁気センサ装置の各部の波形図である。FIG. 4 is a waveform diagram of each part of the magnetic sensor device of FIG.

【図5】従来の磁気センサ装置の一例を示す回路図であ
る。
FIG. 5 is a circuit diagram showing an example of a conventional magnetic sensor device.

【図6】図5の磁気センサ装置の各部の波形図である。6 is a waveform diagram of each part of the magnetic sensor device of FIG.

【符号の説明】[Explanation of symbols]

1 磁気センサ装置 21 磁気センサ装置 51 磁気センサ装置 M1 磁気抵抗素子 M2 磁気抵抗素子 A1 反転増幅器 A2 非反転増幅器 C コンデンサ C1 接地コンデンサ C2 コンデンサ Ra 接地抵抗 Rb 帰還抵抗 Rf 帰還抵抗 Ri 入力抵抗 R1 抵抗 R2 抵抗 Vo 検出電圧 1 magnetic sensor device 21 magnetic sensor device 51 magnetic sensor device M1 magnetic resistance element M2 magnetic resistance element A1 inverting amplifier A2 non-inverting amplifier C capacitor C1 grounding capacitor C2 capacitor Ra grounding resistance Rb feedback resistance Rf feedback resistance Ri input resistance R1 resistance R2 resistance Vo detection voltage

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】 2個の磁気抵抗素子の直列接続からなる
磁気センサを電源Vcc−Gnd間に接続し、前記2個
の磁気抵抗素子の接続点から信号電圧を取り出し、前記
信号電圧をバッファを介して増幅器に入力するか,また
は前記磁気センサに対して高入力インピーダンスの増幅
器に入力し、前記増幅器の出力を検出信号として取り出
すことを特徴とする磁気センサ装置。
1. A magnetic sensor comprising two magnetoresistive elements connected in series is connected between a power supply Vcc and Gnd, a signal voltage is taken out from a connection point of the two magnetoresistive elements, and the signal voltage is buffered. A magnetic sensor device, characterized in that it is inputted to an amplifier via an amplifier or is inputted to an amplifier having a high input impedance with respect to the magnetic sensor, and an output of the amplifier is taken out as a detection signal.
JP5000590A 1993-01-06 1993-01-06 Magnetic sensor device Pending JPH06201806A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP5000590A JPH06201806A (en) 1993-01-06 1993-01-06 Magnetic sensor device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP5000590A JPH06201806A (en) 1993-01-06 1993-01-06 Magnetic sensor device

Publications (1)

Publication Number Publication Date
JPH06201806A true JPH06201806A (en) 1994-07-22

Family

ID=11477950

Family Applications (1)

Application Number Title Priority Date Filing Date
JP5000590A Pending JPH06201806A (en) 1993-01-06 1993-01-06 Magnetic sensor device

Country Status (1)

Country Link
JP (1) JPH06201806A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0863783A (en) * 1994-08-26 1996-03-08 Nec Corp Information recording medium

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0863783A (en) * 1994-08-26 1996-03-08 Nec Corp Information recording medium

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