JPH03257387A - Driving circuit of magnetoresistance element - Google Patents

Driving circuit of magnetoresistance element

Info

Publication number
JPH03257387A
JPH03257387A JP2057153A JP5715390A JPH03257387A JP H03257387 A JPH03257387 A JP H03257387A JP 2057153 A JP2057153 A JP 2057153A JP 5715390 A JP5715390 A JP 5715390A JP H03257387 A JPH03257387 A JP H03257387A
Authority
JP
Japan
Prior art keywords
resistor
magnetoresistance element
wave
capacitor
circuits
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
JP2057153A
Other languages
Japanese (ja)
Inventor
Hiroshi Shimamura
嶋村 寛
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial 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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP2057153A priority Critical patent/JPH03257387A/en
Publication of JPH03257387A publication Critical patent/JPH03257387A/en
Pending legal-status Critical Current

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  • Measuring Magnetic Variables (AREA)
  • Recording Or Reproducing By Magnetic Means (AREA)
  • Hall/Mr Elements (AREA)

Abstract

PURPOSE:To lessen a consumed current and also to obtain an output having a high midpoint fluctuation potential by a method wherein a magnetoresistance element is driven by a rectangular wave voltage and an output signal of the magnetoresistance element is subjected to wave-shaping by an integrating circuit and taken out. CONSTITUTION:A driving circuit of a magnetoresistance element is constructed of a power source Vcc 1 for IC, a semiconductor circuit component, etc., a comparator 2, a reference signal 3 of a triangular wave or a sine wave and a resistor 4 formed of the magnetoresistance element (MR element) made of a thin film. Integrating circuits 5 and 6 are composed of a resistor R1 and a capacitor C1 and a resistor R2 and a capacitor C2 respectively. An amplifier 7 receives outputs of the circuits 5 and 6 as inputs and is provided with resistors R5 to R7. Resistors R3 and R4 and a capacitor C3 are connected to the comparator 2. Construction is made so that a rectangular wave voltage is impressed on the MR element and that an output signal of the MR element is subjected to wave-shaping by the circuits 5 and 6 and taken out. According to this constitution, a consumed current can be lessened even when the MR element of low resistance is employed.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は薄膜型の磁気抵抗素子(以下、MR素子という
)の駆動回路に関するものである。
DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application The present invention relates to a drive circuit for a thin film type magnetoresistive element (hereinafter referred to as an MR element).

従来の技術 この種のMR素子を用いた水量計、ガス流量計等Gこお
いて、ハンテリによる駆動を可能にするためには、MR
素子に供給する電流を微少電流にすることが必要である
が、このためにDC供給電圧を低くするか、またはMR
素子と直列に抵抗を接続j7、電流を低く制限するか、
またはMR素子自身の抵抗値を高く設定し、電流を低く
制限する等のDC電圧による直流駆動によるものである
2. Prior Art In order to enable driving by a hunter, water meters, gas flow meters, etc. using this type of MR element are required.
It is necessary to reduce the current supplied to the element to a minute current, but for this purpose, the DC supply voltage must be lowered or the MR
Connect a resistor in series with the element j7 to limit the current to a low level, or
Alternatively, the resistance value of the MR element itself may be set high and the current may be limited to a low level by direct current driving using a DC voltage.

発明が解決しようとする課題 しかしながら、MR素子自身の抵抗値が低いときは自己
発熱による特性変動があり、これを避けるため、供給D
C電圧を低く設定する必要がある。
Problems to be Solved by the Invention However, when the resistance value of the MR element itself is low, characteristics change due to self-heating, and to avoid this, the supply D
It is necessary to set the C voltage low.

このため、半導体素子(IC)、半導体回路部品と同一
の供給電圧を使えないという欠点があった。
For this reason, there is a drawback that the same supply voltage cannot be used for semiconductor elements (ICs) and semiconductor circuit components.

また、直列抵抗を入れることにより、MR素子自身に印
加される供給電圧を低くすると、MR素子の出力が低下
するという欠点があった。更に、MR素子自身の抵抗値
を高く設定するには、MR膜の面積を大きくしなiJれ
ばなあないとか、膜厚、膜111を小さくすることによ
る外形寸法の小型化傾向に伴なう工法上の問題という欠
点があった。
Furthermore, if the supply voltage applied to the MR element itself is lowered by inserting a series resistor, there is a drawback that the output of the MR element decreases. Furthermore, in order to set the resistance value of the MR element itself high, it is necessary to increase the area of the MR film, and with the trend toward smaller external dimensions by reducing the film thickness and film 111. There was a drawback due to problems with the construction method.

本発明はこのような課題に鑑メ、MR素子駆動部のパワ
ーロスを小さくし、MR素子の、特に低抵抗値の出力特
性を改善することを目的とする。
In view of these problems, it is an object of the present invention to reduce the power loss of the MR element drive section and improve the output characteristics of the MR element, especially for low resistance values.

課題を解決するための手段 この課題を解決するために本発明は、MR素子を矩形波
電流による駆動を行ない、ON−〇FF時間を適当に設
定することにより、任意の微少電流を流すようにしたも
のである。
Means for Solving the Problem In order to solve this problem, the present invention drives the MR element with a rectangular wave current, and by appropriately setting the ON-FF time, an arbitrary minute current can be caused to flow. This is what I did.

デユーティD=Ton/ (Ton−+−Tof f)
とすれば、Dを小さくずればする程微少電流による駆動
が可能となる。
Duty D=Ton/(Ton-+-Tof f)
If this is the case, the smaller D is shifted, the more it becomes possible to drive with a minute current.

作用 この構成により、IC1半導体回路部品等の駆動電圧と
ほぼ同程度の電圧で、低抵抗のMR素子を駆動ずろこと
ができることにより、MR素子の抵抗値の選択可能範囲
が拡大されろ。また、Mrl素子自身の膜パターンの大
きさが小さくなり、作用磁界に対して有効に作用する。
Effect: With this configuration, the low resistance MR element can be driven with a voltage approximately equal to the driving voltage of the IC1 semiconductor circuit components, etc., thereby expanding the selectable range of the resistance value of the MR element. Furthermore, the size of the film pattern of the Mrl element itself is reduced, and it acts effectively on the applied magnetic field.

実施例 以下本発明実施例について、第1図〜第4図を用いて説
明する。
Examples Examples of the present invention will be described below with reference to FIGS. 1 to 4.

第1図に本発明の一実施例による磁気抵抗素子の駆動回
路を示す図で、第1図において、1はIC1半導体回路
部品等の電源Vcc、2はコンパレータ、3はコンパレ
ータ2に人力する三角波又は正弦波の基準信号、4はM
R素子による抵抗体で、ブリノン回路を構成している。
FIG. 1 is a diagram showing a drive circuit for a magnetoresistive element according to an embodiment of the present invention. In FIG. or a sine wave reference signal, 4 is M
A resistor composed of an R element constitutes a Brinon circuit.

5,6は抵抗R1とコンチン+JC1、抵抗R2とコン
デンサC2による積分回路(ローパスフ1ルター)、7
はこの積分回路5,6の出力が入力される増「11器で
ある。また、R3,R4,R5,R6R7は抵抗、C3
はコンデンサである。
5 and 6 are integration circuits (low-pass filter 1) consisting of resistor R1, contin + JC1, resistor R2 and capacitor C2, 7
is an integrator 11 to which the outputs of the integrating circuits 5 and 6 are input. Also, R3, R4, R5, R6 and R7 are resistors, and C3
is a capacitor.

第2図はコンパレータ2の一方の入力信弓と、MR素子
に供給される電圧波形を示しており、PWM波形の矩形
波電圧がMR素子に印加される。
FIG. 2 shows one input signal of the comparator 2 and the voltage waveform supplied to the MR element, and a rectangular wave voltage of PWM waveform is applied to the MR element.

デユーティDはコンパレータ2の入力電圧を抵抗R3,
R4の比を変えることここより変えることができる。
Duty D connects the input voltage of comparator 2 to resistor R3,
You can change the ratio of R4 from here.

第3図にMR素子に外部磁界が印加された時の中点電位
波形9を示している。また、第4図に増巾器7によって
増巾された出力波形lOに示している。
FIG. 3 shows a midpoint potential waveform 9 when an external magnetic field is applied to the MR element. Further, FIG. 4 shows an output waveform IO amplified by the amplifier 7.

このようにMR素子に矩形波電圧を印加し、そしてMR
素子の出力信号を積分回路5,6によって波形整形し、
取り出す構成としており、低抵抗のMR素子を使用した
場合でも、消費電流を少なくすることができ、中点変動
電位を高くすることができる。
In this way, a rectangular wave voltage is applied to the MR element, and the MR
The output signal of the element is waveform-shaped by integrating circuits 5 and 6,
Even if a low-resistance MR element is used, current consumption can be reduced and the midpoint fluctuation potential can be increased.

発明の効果 以上のように本発明によれば、低抵抗のMR素子であっ
ても矩形波の供給電圧をMR素子に印加することにより
、消費電流を少なくでき、しかも中点変動電位の高い出
力が得られる。また高抵抗のMR素子においては更に少
ない消費電流が可能である。このように消費電流を少な
くすることにより、抵抗体の発熱が抑えられ、良好なM
R特性が得られる。
Effects of the Invention As described above, according to the present invention, even if the MR element has a low resistance, by applying a rectangular wave supply voltage to the MR element, current consumption can be reduced, and an output with a high midpoint fluctuation potential can be achieved. is obtained. Further, in a high-resistance MR element, even lower current consumption is possible. By reducing the current consumption in this way, the heat generation of the resistor is suppressed and a good M
R characteristics can be obtained.

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

第1図は本発明の一実施例による磁気抵抗素子の駆動回
路の回路構成図、第2図はMR素子の駆動電圧の波形図
、第3図はMR素子の中点電圧の波形図、第4図は第1
図の回路構成による出力波形図である。 2・・・・・・コンパレータ、4・・・・・・MR素子
の抵抗体、5.6・・・・・積分回路。
FIG. 1 is a circuit configuration diagram of a drive circuit for a magnetoresistive element according to an embodiment of the present invention, FIG. 2 is a waveform diagram of the driving voltage of the MR element, FIG. 3 is a waveform diagram of the midpoint voltage of the MR element, and FIG. Figure 4 is the first
FIG. 3 is an output waveform diagram of the circuit configuration shown in the figure. 2...Comparator, 4...Resistor of MR element, 5.6...Integrator circuit.

Claims (1)

【特許請求の範囲】[Claims] 磁気抵抗素子を矩形波電圧で駆動しその磁気抵抗素子の
出力信号を積分回路によって波形整形し取り出すように
構成したこと特徴とする磁気抵抗素子の駆動回路。
1. A drive circuit for a magnetoresistive element, characterized in that the magnetoresistive element is driven by a rectangular wave voltage, and the output signal of the magnetoresistive element is waveform-shaped and extracted by an integrating circuit.
JP2057153A 1990-03-08 1990-03-08 Driving circuit of magnetoresistance element Pending JPH03257387A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2057153A JPH03257387A (en) 1990-03-08 1990-03-08 Driving circuit of magnetoresistance element

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2057153A JPH03257387A (en) 1990-03-08 1990-03-08 Driving circuit of magnetoresistance element

Publications (1)

Publication Number Publication Date
JPH03257387A true JPH03257387A (en) 1991-11-15

Family

ID=13047621

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2057153A Pending JPH03257387A (en) 1990-03-08 1990-03-08 Driving circuit of magnetoresistance element

Country Status (1)

Country Link
JP (1) JPH03257387A (en)

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5233508A (en) * 1975-09-08 1977-03-14 Ibm Magnetic converter
JPS54143177A (en) * 1978-04-18 1979-11-08 Nec Corp Magnetic field detector
JPS5856980B2 (en) * 1978-06-29 1983-12-17 エヌ・ベ−・フイリツプス・フル−イランペンフアブリケン integrated circuit

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5233508A (en) * 1975-09-08 1977-03-14 Ibm Magnetic converter
JPS54143177A (en) * 1978-04-18 1979-11-08 Nec Corp Magnetic field detector
JPS5856980B2 (en) * 1978-06-29 1983-12-17 エヌ・ベ−・フイリツプス・フル−イランペンフアブリケン integrated circuit

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