JPH0441446Y2 - - Google Patents
Info
- Publication number
- JPH0441446Y2 JPH0441446Y2 JP16791985U JP16791985U JPH0441446Y2 JP H0441446 Y2 JPH0441446 Y2 JP H0441446Y2 JP 16791985 U JP16791985 U JP 16791985U JP 16791985 U JP16791985 U JP 16791985U JP H0441446 Y2 JPH0441446 Y2 JP H0441446Y2
- Authority
- JP
- Japan
- Prior art keywords
- operational amplifier
- resistor
- current
- magnetoresistive element
- input terminal
- 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
Links
Landscapes
- Magnetic Heads (AREA)
- Recording Or Reproducing By Magnetic Means (AREA)
Description
【考案の詳細な説明】
(イ) 産業上の利用分野
本考案は磁気抵抗効果型磁気ヘツド(以下MR
ヘツドと称する)の反転増幅回路に関し、特に
MRヘツドを保護することを目的としたものであ
る。[Detailed explanation of the invention] (a) Industrial application field This invention is a magnetoresistive magnetic head (hereinafter referred to as MR).
Regarding inverting amplifier circuits (referred to as heads),
The purpose is to protect the MR head.
(ロ) 従来の技術
MRヘツドの信号増幅器としては、従来第2図
に示すように演算増幅器を使用した反転増幅回路
が用いられている。(例えばAES東京コンフアレ
ンス′85予稿集P170参照)
即ち、定電流源1より磁気抵抗素子2に検出電
流を流し、抵抗変化を電圧に変換した後演算増幅
器3の反転入力端子に入力し、出力端子より電圧
増幅された信号出力を得るようになつている。
尚、結合コンデンサ4は磁気抵抗素子2の交流変
化分を取り出すもので、5は演算増幅器3の帰還
抵抗器である。(b) Prior Art As a signal amplifier for an MR head, an inverting amplifier circuit using an operational amplifier as shown in FIG. 2 has conventionally been used. (For example, see AES Tokyo Conference '85 Proceedings P170.) In other words, a detection current is passed through the magnetoresistive element 2 from the constant current source 1, and after converting the resistance change into voltage, it is input to the inverting input terminal of the operational amplifier 3, and then the output terminal It is designed to obtain a signal output with a higher voltage amplification.
Incidentally, the coupling capacitor 4 is used to take out the alternating current variation of the magnetoresistive element 2, and the reference numeral 5 is a feedback resistor of the operational amplifier 3.
ところで、演算増幅器には反転入力端子と非反
転入力端子との間に一対の保護ダイオードを逆並
列に接続したタイプのものがある。 By the way, some types of operational amplifiers have a pair of protection diodes connected in antiparallel between an inverting input terminal and a non-inverting input terminal.
従つてこのタイプの演算増幅器をMRヘツドの
信号増幅器として使用した場合、第3図に示すよ
うに構成されることとなる。 Therefore, when this type of operational amplifier is used as a signal amplifier for an MR head, it will be constructed as shown in FIG.
(ハ) 考案が解決しようとする問題点
即ち、斯る第3図においてMRヘツドの磁気抵
抗素子2はコネクタ6,7を介して演算増幅器に
対して接続されるが、該コネクタ6,7よりMR
ヘツドを取り外した場合、第4図Aに示すように
保護ダイオード8,9のうち定電流源1に対して
順方向のダイオード8とコンデンサ4の直列回路
が構成され、定電流源1によりその駆動電圧+V
まで充電される。この状態でMRヘツドの磁気抵
抗素子2が接続された場合、第4図Bに示すよう
に保護ダイオード9とコンデンサ4の直列回路に
より磁気抵抗素子2に放電電流iが流れる。(c) Problems to be solved by the invention Namely, in FIG. 3, the magnetoresistive element 2 of the MR head is connected to the operational amplifier via the connectors 6 and 7; MR
When the head is removed, as shown in Fig. 4A, a series circuit is formed of the diode 8 and the capacitor 4 in the forward direction with respect to the constant current source 1 among the protective diodes 8 and 9, and the constant current source 1 drives the diode 8 and the capacitor 4. Voltage +V
will be charged up to. When the magnetoresistive element 2 of the MR head is connected in this state, a discharge current i flows through the magnetoresistive element 2 due to the series circuit of the protection diode 9 and the capacitor 4, as shown in FIG. 4B.
この放電電流のヒーク値は、MRヘツドの磁気
抵抗素子の値をRとすると、i=V/Rであり、
通常Vは電源電圧にほぼ等しく+12V程度、磁気
抵抗素子の抵抗値Rは100Ω前後であるため、
100mA以上のピーク電流値となる。一方、磁気
抵抗素子の検出電流の許容値は、高々10mA程度
であるため、前記過大電流によつて破壊又は磁気
特性の劣化(極端な感度低下)が起る。前記過大
電流は、増幅器側電源を切つた後にコネクタを取
り外す場合には発生しないが、コネクタの接触不
良によつて等価的に発生する場合があり、従つて
MRヘツドのように検出電流を必要とする増幅回
路では問題である。 The heak value of this discharge current is i=V/R, where R is the value of the magnetoresistive element of the MR head.
Normally, V is approximately equal to the power supply voltage, about +12V, and the resistance value R of the magnetoresistive element is around 100Ω, so
The peak current value is 100mA or more. On the other hand, since the permissible value of the detection current of the magnetoresistive element is about 10 mA at most, the excessive current causes destruction or deterioration of the magnetic properties (extreme decrease in sensitivity). The above-mentioned excessive current will not occur if the connector is removed after the amplifier side power is turned off, but it may equivalently occur due to poor contact of the connector, and therefore
This is a problem in amplifier circuits that require a detection current, such as MR heads.
そこで、第5図に示すように、抵抗器10を直
列に挿入する方法が考えられるが、この場合には
増幅率が低下するため、その分帰還抵抗器の値を
大きくしなければならず、演算増幅器のバイアス
電流による出力端での直流オフセツト電圧、更に
信号源インピーダンスの増大による熱雑音の発生
が問題となる。 Therefore, a method of inserting a resistor 10 in series as shown in FIG. 5 can be considered, but in this case, the amplification factor decreases, so the value of the feedback resistor must be increased accordingly. Problems include a direct current offset voltage at the output end due to the bias current of the operational amplifier, and the generation of thermal noise due to an increase in signal source impedance.
(ニ) 問題点を解決するための手段
本考案は上記の問題点に鑑み、第3図で説明し
たような演算増幅器によつて構成される反転増幅
回路において、磁気抵抗素子からの信号出力の交
流分を取り出す結合コンデンサと直列に電流制限
抵抗器を接続し、該抵抗器を演算増幅器の反転入
力端子に接続し、該演算増幅器の出力より信号を
帰還させる帰還抵抗器を前記コンデンサと電流制
限抵抗器の接続点に接続した回路構成を提供する
ものである。(d) Means for Solving the Problems In view of the above problems, the present invention has been developed to solve the problems described above. A current limiting resistor is connected in series with a coupling capacitor that takes out the alternating current, the resistor is connected to the inverting input terminal of an operational amplifier, and a feedback resistor that feeds back the signal from the output of the operational amplifier is connected to the capacitor and the current limiting resistor. It provides a circuit configuration connected to the connection point of the resistor.
(ホ) 作用
本考案の回路構成により、保護ダイオードを介
した結合コンデンサの放電電流を磁気抵抗素子の
許容値に制限し、且つ信号源インピーダンスの増
加とならないため直流オフセツト電圧の増加、雑
音の増加の問題を解決し得る。(e) Effect The circuit configuration of the present invention limits the discharge current of the coupling capacitor via the protection diode to the permissible value of the magnetoresistive element, and does not increase the signal source impedance, thereby increasing the DC offset voltage and noise. can solve the problem.
(ヘ) 実施例
以下第1図に示す本考案回路の実施例について
説明する。(F) Embodiment An embodiment of the circuit of the present invention shown in FIG. 1 will be described below.
第1図において、第3図と同一部品には同一の
附号を付している。本考案においては結合コンデ
ンサ4と演算増幅器3の反転入力端子との間に電
流制限抵抗器11を接続し、帰還抵抗器5をコン
デンサ4と抵抗器11の接続点に接続している。 In FIG. 1, parts that are the same as those in FIG. 3 are given the same numbers. In the present invention, a current limiting resistor 11 is connected between the coupling capacitor 4 and the inverting input terminal of the operational amplifier 3, and a feedback resistor 5 is connected to the connection point between the capacitor 4 and the resistor 11.
従つて、斯る本考案の回路構成に依れば、第6
図に示すように演算増幅器3のダイオード9を介
したコンデンサ4の放電路に、直列に電流制限抵
抗器11が接続されるため、該抵抗器11を適当
な値(例えば1KΩ〜2KΩ)に設定することによ
り、放電電流を磁気抵抗素子2の許容値に制限す
ることが出来る。 Therefore, according to the circuit configuration of the present invention, the sixth
As shown in the figure, a current limiting resistor 11 is connected in series to the discharge path of the capacitor 4 via the diode 9 of the operational amplifier 3, so the resistor 11 is set to an appropriate value (for example, 1KΩ to 2KΩ). By doing so, the discharge current can be limited to the permissible value of the magnetoresistive element 2.
次に信号源インピーダンスの増加問題について
は、第7図に示すように演算増幅器を用いた反転
増幅回路においては、磁気抵抗素子2の抵抗値と
帰還抵抗器5の値の比によつてのみ決まるため、
第5図のように抵抗器10による直列素子のイン
ピーダンス変化はない。尚、第7図においてコン
デンサはインピーダンスが充分低いものとして省
略している。 Next, regarding the problem of increase in signal source impedance, in an inverting amplifier circuit using an operational amplifier as shown in FIG. For,
As shown in FIG. 5, there is no change in the impedance of the series element due to the resistor 10. Incidentally, in FIG. 7, the capacitor is omitted because the impedance is sufficiently low.
(ト) 考案の効果
以上のように本考案に依れば、演算増幅器の保
護ダイオードを介した結合コンデンサの放電電流
を、信号源インピーダンスを増加させることなく
許容電流値に制限するとが出来るものである。(g) Effects of the invention As described above, according to the invention, the discharge current of the coupling capacitor via the operational amplifier's protection diode can be limited to the permissible current value without increasing the signal source impedance. be.
従つてMRヘツド等のように検出電流を必要と
し、そのため結合コンデンサが増幅器との間に接
続され、且つ、低ノイズ特性が要求される反転増
幅回路に用いて有益なものであある。 Therefore, it is useful for use in an inverting amplifier circuit such as an MR head that requires a detection current, a coupling capacitor is connected between it and the amplifier, and low noise characteristics are required.
第1図は本考案回路の実施例、第2図は従来の
MRヘツド増幅回路、第3図はMRヘツドの増幅
回路に入力保護用のダイオードを接続した演算増
幅器を用いた場合の回路例、第4図A,Bは入力
保護用ダイオードにより磁気抵抗素子に過大電流
が流れることを説明する等価回路、第5図は過大
電流を防止するため通常使用される回路例、第6
図及び第7図は本考案の動作を説明する図であ
る。
1……定電流源、2……磁気抵抗素子、3……
演算増幅器、4結合コンデンサ、5……帰還抵抗
器、8,9……ダイオード、11……電流制限抵
抗器。
Figure 1 shows an example of the circuit of the present invention, and Figure 2 shows a conventional circuit.
MR head amplifier circuit. Figure 3 is an example of a circuit using an operational amplifier with an input protection diode connected to the MR head amplifier circuit. Figures 4A and B show an input protection diode that prevents excessive damage to the magnetoresistive element. An equivalent circuit explaining the flow of current, Figure 5 is an example of a circuit normally used to prevent excessive current, and Figure 6 is an equivalent circuit that explains the flow of current.
7 and 7 are diagrams for explaining the operation of the present invention. 1... Constant current source, 2... Magnetoresistive element, 3...
Operational amplifier, 4 coupling capacitors, 5... feedback resistors, 8, 9... diodes, 11... current limiting resistors.
Claims (1)
素子と、該磁気抵抗素子からの信号出力の交流分
を取り出す結合コンデンサと、該コンデンサと直
列に接続された電流制限抵抗器と、該抵抗器が反
転入力端子に接続された演算増幅器と、該演算増
幅器の反転入力端子と非反転入力端子間に逆並列
接続された一対のダイオードと、前記演算増幅器
の出力より信号を帰還させる帰還抵抗器とより成
り、前記演算増器の出力信号を前記結合コンデン
サと電流制限抵抗器の接続点に帰還させることを
特徴とする磁気抵抗効果型磁気ヘツドの反転増幅
回路。 A constant current source, a magnetoresistive element to which the constant current source is supplied, a coupling capacitor for taking out an alternating current component of a signal output from the magnetoresistive element, a current limiting resistor connected in series with the capacitor, an operational amplifier having an inverting input terminal connected to a resistor; a pair of diodes connected in antiparallel between the inverting input terminal and the non-inverting input terminal of the operational amplifier; and a feedback resistor for feeding back a signal from the output of the operational amplifier. 1. An inverting amplifier circuit for a magnetoresistive head, characterized in that the output signal of the operational amplifier is fed back to a connection point between the coupling capacitor and the current limiting resistor.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP16791985U JPH0441446Y2 (en) | 1985-10-31 | 1985-10-31 |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP16791985U JPH0441446Y2 (en) | 1985-10-31 | 1985-10-31 |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6277401U JPS6277401U (en) | 1987-05-18 |
| JPH0441446Y2 true JPH0441446Y2 (en) | 1992-09-29 |
Family
ID=31100305
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP16791985U Expired JPH0441446Y2 (en) | 1985-10-31 | 1985-10-31 |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0441446Y2 (en) |
-
1985
- 1985-10-31 JP JP16791985U patent/JPH0441446Y2/ja not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS6277401U (en) | 1987-05-18 |
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