JPH03134514A - Magnetoresistance effect element - Google Patents

Magnetoresistance effect element

Info

Publication number
JPH03134514A
JPH03134514A JP1272826A JP27282689A JPH03134514A JP H03134514 A JPH03134514 A JP H03134514A JP 1272826 A JP1272826 A JP 1272826A JP 27282689 A JP27282689 A JP 27282689A JP H03134514 A JPH03134514 A JP H03134514A
Authority
JP
Japan
Prior art keywords
voltage
transistor
zener diode
zener
base
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
JP1272826A
Other languages
Japanese (ja)
Inventor
Kazunari Kawabe
川邊 一成
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 JP1272826A priority Critical patent/JPH03134514A/en
Publication of JPH03134514A publication Critical patent/JPH03134514A/en
Pending legal-status Critical Current

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  • Transmission And Conversion Of Sensor Element Output (AREA)
  • Measuring Magnetic Variables (AREA)

Abstract

PURPOSE:To stabilize signal detecting operation by providing an overvoltage- application preventing circuit in a power source line. CONSTITUTION:An overvoltage-application preventing circuit is a constant- voltage circuit using a Zener diode ZD. The Zener diode ZD is provided between the base and the ground of a transistor Tr. An input terminal is provided at the side of the collector, and an output terminal is provided at the side of the emitter. The value of a resistor R is determined by an input voltage Vin, an output voltage Vout, a base current IB of the transistor Tr and a Zener diode current IZ. The output voltage Vout is obtained by using a resistance rz of the Zener diode and a Zener voltage VZ. At this time, the Zener voltage VZ of the Zener diode AD is set at a value which is obtained by adding the rated voltage of a magnetoresistance effect element to a base-emitter voltage VBE of the transistor Tr. Even if an overvoltage is applied to the input terminal Vin, the base voltage of the transistor Tr is kept constant by the Zener effect. The rated voltage is always applied to the magnetoresistance effect element.

Description

【発明の詳細な説明】 産業上の利用分野 本発明はモータの回転制御2位置制御に使用される磁気
式エンコーダの磁気抵抗効果素子(磁気センサ)に関す
るものである。
DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to a magnetoresistive element (magnetic sensor) of a magnetic encoder used for two-position rotational control of a motor.

従来の技術 磁気式エンコーダは、第3図に示すようにモータ3のシ
ャフトに固定された円筒形の磁気ドラム1と、この磁気
ドラム1と所定のギャップを隔てて対向配置された磁気
抵抗効果素子2とによシ構成されている。
As shown in FIG. 3, a conventional magnetic encoder includes a cylindrical magnetic drum 1 fixed to the shaft of a motor 3, and a magnetoresistive element placed opposite the magnetic drum 1 with a predetermined gap therebetween. It is composed of two parts.

磁気ドラム1には、磁気抵抗効果素子2と対向する円軌
道に沿って磁化パターン(図示せず)が多極着磁されて
いる。モータ3により磁気ドラム1が回転することで、
磁気抵抗効果素子2に対向する磁極(磁化パターン)が
変化し、それに伴い磁気抵抗効果素子2の抵抗値が変化
する。この原理をもとに磁気抵抗効果素子は信号検出を
行う。
The magnetic drum 1 is magnetized with a multipolar magnetization pattern (not shown) along a circular orbit facing the magnetoresistive element 2 . When the magnetic drum 1 is rotated by the motor 3,
The magnetic pole (magnetization pattern) facing the magnetoresistive element 2 changes, and the resistance value of the magnetoresistive element 2 changes accordingly. Based on this principle, the magnetoresistive element performs signal detection.

磁気抵抗効果素子2で検出された信号(第5図+IL)
〜(C))は、そのまま第4図に示すような電子回路に
とりかこまれ、波形増幅が行われた後に波形整形回路を
通してデジタル信号(第6図(!L)〜(f))に変換
される(第5図(IL)〜(Q)はそれぞれ((ml−
(f)に対応している)。
Signal detected by magnetoresistive element 2 (Fig. 5 + IL)
- (C)) are directly surrounded by an electronic circuit as shown in Figure 4, and after waveform amplification, are converted into digital signals (Figure 6 (!L) - (f)) through a waveform shaping circuit. (Figure 5 (IL) to (Q) are respectively ((ml-
(corresponds to (f)).

発明が解決しようとする課題 ところで、磁気抵抗効果素子2の電源ラインには定格電
圧を印加しておくことが必要で、定格以上の電圧がかけ
られた場合、磁気抵抗効果素子2そのものが破壊されて
しまったり、過負荷による発熱で磁気抵抗効果素子の抵
抗変化率が変化し、信号検出能力の低下という問題があ
る。
Problem to be Solved by the Invention By the way, it is necessary to apply a rated voltage to the power supply line of the magnetoresistive element 2, and if a voltage higher than the rated voltage is applied, the magnetoresistive element 2 itself will be destroyed. There is a problem in that the resistance change rate of the magnetoresistive element changes due to heat generation due to overload, and the signal detection ability deteriorates.

本発明の目的は、磁気抵抗効果素子2の電源ラインに定
格以上の電圧が印加されたときでも、磁気抵抗効果素子
2が正常な動作を行えるようにすることである。
An object of the present invention is to enable the magnetoresistive element 2 to operate normally even when a voltage higher than the rated voltage is applied to the power supply line of the magnetoresistive element 2.

課題を解決するための手段 上記目的を達成するために本発明の磁気抵抗効果素子は
、電源ラインに過電圧印加防止回路を備えたものである
Means for Solving the Problems In order to achieve the above object, the magnetoresistive element of the present invention is provided with an overvoltage application prevention circuit in the power supply line.

作用 上記した構成により、磁気抵抗効果素子の信号検出動作
が安定したものになる。
Effect: With the above-described configuration, the signal detection operation of the magnetoresistive element becomes stable.

実施例 以下、図面に示す実施例に基づいて本発明の詳細な説明
する。
EXAMPLES Hereinafter, the present invention will be explained in detail based on examples shown in the drawings.

第1図は本発明における磁気抵抗効果素子の電源ライン
用過電圧印加防止回路を示したもので、第2図は第1図
の回路を用いたとき、電源電圧と磁気抵抗効果素子に印
加される電圧との関係を示した特性図である。
Figure 1 shows an overvoltage application prevention circuit for the power line of the magnetoresistive element in the present invention, and Figure 2 shows the power supply voltage and the voltage applied to the magnetoresistive element when the circuit of Figure 1 is used. FIG. 3 is a characteristic diagram showing the relationship with voltage.

第1図に示す過電圧印加防止回路はツェナー・ダイオー
ドを使用した定電圧回路で、トランジスタのベースとグ
ランドの間にツェナー・ダイオードを配置し、コレクタ
側に入力端子、エミッタ側に出力端子をそれぞれもって
いる。抵抗Rは入力電圧Winと出力電圧VOut、ト
ランジスタのペース電流工、および、ツェナー・ダイオ
ード電流Xzできまり、 R=(Win −vout )/(I B+I z )
となる。
The overvoltage application prevention circuit shown in Figure 1 is a constant voltage circuit using a Zener diode.The Zener diode is placed between the base of the transistor and the ground, and the input terminal is on the collector side and the output terminal is on the emitter side. There is. The resistance R is determined by the input voltage Win, the output voltage VOut, the transistor pace current, and the Zener diode current Xz, R = (Win - vout ) / (I B + I z )
becomes.

そして出力電圧Voutは、ツェナー・ダイオードの抵
抗rg、ツェナー電圧vzを用いて、Vout =(W
in−r、−1−vz−R)/rz+Rとなる。しかし
ながら、実際の出力電圧はこれからトランジスタのベー
ス・エミッタ電圧V□を差し引いた値(vout  ’
ax)となる。
Then, the output voltage Vout is calculated using the resistance rg of the Zener diode and the Zener voltage vz, as follows: Vout = (W
in-r, -1-vz-R)/rz+R. However, the actual output voltage is the value obtained by subtracting the transistor base-emitter voltage V□ (vout '
ax).

したがって出力電圧はツェナー・ダイオードのツェナー
電圧vzで決まることになる。ツェナーダイオードには
逆方向印加電圧が増加すると、ある電圧値から急激に逆
方向電流が流れだしてプレクダウンを起こすツェナー効
果という現象がある。
Therefore, the output voltage is determined by the Zener voltage vz of the Zener diode. Zener diodes have a phenomenon called the Zener effect, in which when the reverse applied voltage increases, a reverse current suddenly starts flowing from a certain voltage value, causing pre-kdown.

このときの電圧をツェナー電圧と呼ぶ。このため、ツェ
ナー・ダイオードzDのツェナー電圧v2を磁気抵抗効
果素子の定格電圧(第2図において5V )、!−ト;
>ンジスタのベース・エミッタ電圧VBIを加えた値(
第2図においてs、eV)に設定しておけば、第2図に
示すように入力端子vinに過電圧(s、eV以上)が
印加されても、ツェナー効果によりトランジスタのベー
ス電圧バ一定に保たれ、磁気抵抗効果素子には常に定格
の電圧(6v)が印加されるようになる。
The voltage at this time is called Zener voltage. Therefore, the Zener voltage v2 of the Zener diode zD is set to the rated voltage of the magnetoresistive element (5V in FIG. 2), ! -t;
>The sum of the resistor's base-emitter voltage VBI (
If the voltage is set to s, eV in Figure 2, even if an overvoltage (more than s, eV) is applied to the input terminal vin as shown in Figure 2, the Zener effect will keep the base voltage of the transistor constant. As a result, the rated voltage (6V) is always applied to the magnetoresistive element.

発明の効果 以上のように本発明は、電源ラインに過電圧印加防止回
路を備えることで、磁気抵抗効果素子の破壊を防ぐこと
ができ、また、発熱による磁気抵抗効果素子の抵抗変化
率の変化を無くし、信号検出動作を安定なものにする仁
とになる。
Effects of the Invention As described above, the present invention can prevent destruction of the magnetoresistive element by providing an overvoltage application prevention circuit in the power supply line, and can also prevent changes in the resistance change rate of the magnetoresistive element due to heat generation. This is the key to making the signal detection operation stable.

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

第1図は本発明における磁気抵抗効果素子の電源ライン
に備える過電圧印加防止回路の回路図、第2図は第1図
における入力電圧Winと磁気抵抗効果素子の電源ライ
ンに印加される電圧V outとの関係を表した特性図
、第3図は従来の磁気式エンコーダの構成例を示す模式
図、第4図は磁気抵抗効果素子から信号を取り出すため
に用いる電子回路の1例を示す回路図、第5図は第4図
に示す電子回路に入力する信号と、それを波形整形した
信号の波形図である。 ZD・・・・・・ツェナー・ダイオード、Tr・・・・
・・トランジスタ、MR・・・・・・磁気抵抗効果素子
Fig. 1 is a circuit diagram of an overvoltage application prevention circuit provided in the power supply line of the magnetoresistive element according to the present invention, and Fig. 2 shows the input voltage Win in Fig. 1 and the voltage V out applied to the power supply line of the magnetoresistive element. Figure 3 is a schematic diagram showing a configuration example of a conventional magnetic encoder, Figure 4 is a circuit diagram showing an example of an electronic circuit used to extract signals from a magnetoresistive element. , FIG. 5 is a waveform diagram of a signal input to the electronic circuit shown in FIG. 4 and a signal obtained by shaping the signal. ZD... Zener diode, Tr...
...Transistor, MR... Magnetoresistive element.

Claims (2)

【特許請求の範囲】[Claims] (1)電源ラインに過電圧印加防止回路を備えたことを
特徴とする磁気抵抗効果素子。
(1) A magnetoresistive element characterized in that a power supply line is equipped with an overvoltage application prevention circuit.
(2)過電圧印加防止回路は、トランジスタのベースと
グランドの間にツェナー・ダイオードを配置し、トラン
ジスタのコレクタ側に入力端子、エミッタ側に出力端子
をもっていることを特徴とする請求項1記載の磁気抵抗
効果素子。
(2) The overvoltage application prevention circuit has a Zener diode placed between the base of the transistor and the ground, and has an input terminal on the collector side of the transistor and an output terminal on the emitter side. Resistance effect element.
JP1272826A 1989-10-19 1989-10-19 Magnetoresistance effect element Pending JPH03134514A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1272826A JPH03134514A (en) 1989-10-19 1989-10-19 Magnetoresistance effect element

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1272826A JPH03134514A (en) 1989-10-19 1989-10-19 Magnetoresistance effect element

Publications (1)

Publication Number Publication Date
JPH03134514A true JPH03134514A (en) 1991-06-07

Family

ID=17519306

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1272826A Pending JPH03134514A (en) 1989-10-19 1989-10-19 Magnetoresistance effect element

Country Status (1)

Country Link
JP (1) JPH03134514A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0575686U (en) * 1992-02-17 1993-10-15 旭化成工業株式会社 Temperature correction circuit

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0575686U (en) * 1992-02-17 1993-10-15 旭化成工業株式会社 Temperature correction circuit

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