JPS6120051B2 - - Google Patents

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Publication number
JPS6120051B2
JPS6120051B2 JP9369477A JP9369477A JPS6120051B2 JP S6120051 B2 JPS6120051 B2 JP S6120051B2 JP 9369477 A JP9369477 A JP 9369477A JP 9369477 A JP9369477 A JP 9369477A JP S6120051 B2 JPS6120051 B2 JP S6120051B2
Authority
JP
Japan
Prior art keywords
current
coil
output
voltage
circuit
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
JP9369477A
Other languages
Japanese (ja)
Other versions
JPS5428108A (en
Inventor
Hiroshi Totsutori
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric Corp
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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP9369477A priority Critical patent/JPS5428108A/en
Publication of JPS5428108A publication Critical patent/JPS5428108A/en
Publication of JPS6120051B2 publication Critical patent/JPS6120051B2/ja
Granted legal-status Critical Current

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  • Recording Or Reproducing By Magnetic Means (AREA)

Description

【発明の詳細な説明】 この発明は、磁気抵抗効果素子(以下MR素子
と称す)を用いた磁気記録再生装置の改良に関す
るものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an improvement of a magnetic recording/reproducing device using a magnetoresistive element (hereinafter referred to as an MR element).

MR素子は出力電圧が大きいことが特徴である
が、入力信号磁界に対して出力が比例しない。し
がつて、MR素子を磁気記録再生装置に用いる
と、元信号に対して再生信号が歪む欠点を有す
る。
MR elements are characterized by a large output voltage, but the output is not proportional to the input signal magnetic field. However, when an MR element is used in a magnetic recording/reproducing device, it has the disadvantage that the reproduced signal is distorted with respect to the original signal.

この欠点を除去した磁気記録再生装置が考えら
れており、その装置を第1図に示す。この図にお
いて、1はMR素子、2はMR素子1とで磁気ヘ
ツドを構成するコイル、3は直流電源、4は電流
制限抵抗、5は増幅器、6は差動増幅器、7は基
準電圧発生器、8はコイル電流源、9はコイル電
流制御回路、10は電流・電圧変換回路、11は
出力端子である。
A magnetic recording/reproducing device which eliminates this drawback has been considered, and this device is shown in FIG. In this figure, 1 is an MR element, 2 is a coil that constitutes a magnetic head with MR element 1, 3 is a DC power supply, 4 is a current limiting resistor, 5 is an amplifier, 6 is a differential amplifier, and 7 is a reference voltage generator. , 8 is a coil current source, 9 is a coil current control circuit, 10 is a current/voltage conversion circuit, and 11 is an output terminal.

次に、このように構成された磁気記録再生装置
の動作について説明する。MR素子1はいわゆる
“磁気抵抗効果”によつて、図示ない記録媒体か
ら信号磁界を受けるとその電気抵抗値が磁界に対
して特殊な関係で変化する。直流電源3は電流制
限抵抗4を介してMR素子1に直流電流を流すこ
とにより、その抵抗値を電圧信号に変換して検知
するもので、この電圧信号は増幅器5によつて増
幅され、差動増幅器6の一つの入力となる。一
方、基準電圧発生器7は、MR素子1の入力磁界
の変動に対しそ抵抗値の変化が最も大きい領域に
あらかじめ入力磁界を定め、この磁界における増
幅後の出力電圧に等しい電圧を記憶し、この電圧
を基準電圧として差動増幅器6の今一つの入力に
対して発生する。そして、差動増幅器6は上記基
準電圧と実際の出力電圧の差を増幅し、コイル電
流制御回路9の入力とする。他方、コイル2には
コイル電流源8から電流・電圧変換回路10およ
びコイル電流制御回路9を介してコイル電流が流
れており、記録媒体からの信号磁界と同様にMR
素子1に磁界を印加する。この場合、コイル磁界
とコイル電流との間には良い比例関係があり、こ
のコイル電流を、上記基準電圧と実際の出力電圧
が一致する向きに、差動増幅器6の出力に基づい
てコイル電流制御回路9により制御する。すなわ
ち、この種の磁気記録再生装置は、記録媒体から
の信号磁界を打消して常にMR素子1の出力電圧
が一定になるようにコイル磁界を印加し、この時
に生じるコイル電流の変化が信号磁界の変化に一
致するのを利用し、このコイル電流を電流・電圧
変換回路10によつて電圧信号に変換し出力端子
11に出力する。この場合、MR素子1はその出
力電圧がほぼ一定電圧になるように入力磁界が調
節される。したがつて、MR素子1の入力磁界と
出力電圧(抵抗値)との間の非直線性に基づく再
生出力の歪みは全く除去される。
Next, the operation of the magnetic recording/reproducing apparatus configured as described above will be explained. Due to the so-called "magnetoresistive effect," when the MR element 1 receives a signal magnetic field from a recording medium (not shown), its electrical resistance value changes in a special relationship with respect to the magnetic field. The DC power supply 3 converts the resistance value into a voltage signal and detects it by passing a DC current through the MR element 1 via the current limiting resistor 4. This voltage signal is amplified by the amplifier 5 and the difference is It becomes one input of the dynamic amplifier 6. On the other hand, the reference voltage generator 7 determines in advance an input magnetic field in a region where the change in resistance value is the largest with respect to fluctuations in the input magnetic field of the MR element 1, and stores a voltage equal to the output voltage after amplification in this magnetic field, This voltage is used as a reference voltage and is generated for the other input of the differential amplifier 6. Then, the differential amplifier 6 amplifies the difference between the reference voltage and the actual output voltage and inputs it to the coil current control circuit 9. On the other hand, a coil current flows through the coil 2 from a coil current source 8 via a current/voltage conversion circuit 10 and a coil current control circuit 9, and the MR as well as the signal magnetic field from the recording medium
A magnetic field is applied to element 1. In this case, there is a good proportional relationship between the coil magnetic field and the coil current, and the coil current is controlled based on the output of the differential amplifier 6 so that the above reference voltage matches the actual output voltage. Controlled by circuit 9. That is, in this type of magnetic recording/reproducing device, a coil magnetic field is applied so that the signal magnetic field from the recording medium is canceled and the output voltage of the MR element 1 is always constant, and the change in the coil current that occurs at this time is the signal magnetic field. This coil current is converted into a voltage signal by the current/voltage conversion circuit 10 and outputted to the output terminal 11 by utilizing the fact that the current corresponds to the change in the voltage. In this case, the input magnetic field of the MR element 1 is adjusted so that its output voltage becomes a substantially constant voltage. Therefore, distortion of the reproduced output due to nonlinearity between the input magnetic field and the output voltage (resistance value) of the MR element 1 is completely eliminated.

しかるに、上記のような磁気記録再生装置で
は、MR素子1の温度変化に基づく再生出力の減
少あるいは出力の消滅が生じる欠点を有する。す
なわち、入力磁界によるMR素子1の抵抗値変化
率は最大で素子自身の抵抗値の2%程度である。
これに対して、MR素子1の温度変化による抵抗
値の変化率は0.6%/℃程度である。それゆえ、
基準電圧を設定した時点の温度からMR素子1の
温度が数℃変化すると、MR素子1の抵抗値は入
力磁界では基準電圧に等しい出力電圧を出力する
状態にはなり得ないことにになり、使用できなく
なる。また、この状態に達するまでには入力磁界
の変動に対して出力電圧の変化が小さい領域を通
過するので、この時点で再生出力が小さくなる。
However, the magnetic recording/reproducing apparatus as described above has a drawback that the reproduction output decreases or disappears due to temperature changes of the MR element 1. That is, the rate of change in the resistance value of the MR element 1 due to the input magnetic field is at most about 2% of the resistance value of the element itself.
On the other hand, the rate of change in resistance value due to temperature change of the MR element 1 is about 0.6%/°C. therefore,
If the temperature of MR element 1 changes by several degrees from the temperature at the time the reference voltage was set, the resistance value of MR element 1 will not be able to output an output voltage equal to the reference voltage under the input magnetic field. It becomes unusable. Furthermore, by the time this state is reached, the output voltage has passed through a region where the change in the output voltage is small relative to the change in the input magnetic field, so the reproduction output becomes small at this point.

この発明は上記のような従来のものの欠点を除
去するためになされたもので、コイルに、一定値
の直流電流とMR素子出力の交流成分に基づいて
制御された交流電流とを重畳して流すことによ
り、MR素子の磁界変動に対する抵抗値変化の大
きい領域に、MR素子の温度変化に関係なくその
出力電圧を設定すると同時に、映像や音声などの
交流信号に対しては従来と同様に歪みのない再生
出力を発生することのできる磁気記録再生装置を
提供することを目的とする。
This invention was made in order to eliminate the drawbacks of the conventional ones as described above, and involves superimposing a fixed value of DC current and an AC current controlled based on the AC component of the MR element output to flow through the coil. By doing this, the output voltage can be set in the region where the resistance value changes greatly due to magnetic field fluctuations of the MR element, regardless of the temperature change of the MR element, and at the same time, distortion can be maintained for AC signals such as video and audio as before. It is an object of the present invention to provide a magnetic recording and reproducing device that can generate a reproduction output that is unique.

以下この発明の一実施例を図面を参照して説明
する。第2図は一実施例による磁気記録再生装置
を示し、この図において、1はMR素子、2は
MR素子1とで磁気ヘツドを構成するコイル、3
は直流電源、4は電流制限抵抗、5は増幅器、8
はコイル電流源、9はコイル電流制御回路、10
は電流・電圧変換回路、11は出力端子、21は
増幅器5の入力に接続されたコンデンサ、22は
電流規制抵抗である。そして、この場合はコイル
電流源8より、一つは電流規制抵抗22を介して
一定の直流電流がコイル2に流され、さらにこの
電流規制抵抗22とは並列に電流・電圧変換回路
10およびコイル電流制御回路9を介してコイル
2に電流が流される。また、コイル電流制御回路
9を通る電流は、増幅器5によつて増幅された
MR素子1出力の交流成分の信号によつて、この
出力を打消す向きにコイル電流制御回路9により
制御される。さらに、電流・電圧変換回路10は
上記制御された電流を電圧に変換し出力端子11
に出力するもので、直流電源3に関しては従来と
同様である。
An embodiment of the present invention will be described below with reference to the drawings. FIG. 2 shows a magnetic recording/reproducing device according to one embodiment, and in this figure, 1 is an MR element, and 2 is an MR element.
A coil 3 that constitutes a magnetic head with the MR element 1
is a DC power supply, 4 is a current limiting resistor, 5 is an amplifier, 8
9 is a coil current source, 9 is a coil current control circuit, and 10 is a coil current source.
1 is a current/voltage conversion circuit, 11 is an output terminal, 21 is a capacitor connected to the input of the amplifier 5, and 22 is a current regulating resistor. In this case, a constant DC current is passed through the coil 2 from the coil current source 8 through the current regulating resistor 22, and the current/voltage conversion circuit 10 and the coil are connected in parallel with the current regulating resistor 22. A current is passed through the coil 2 via the current control circuit 9. Further, the current passing through the coil current control circuit 9 is amplified by the amplifier 5.
The coil current control circuit 9 is controlled by the AC component signal of the output of the MR element 1 to cancel this output. Further, the current/voltage conversion circuit 10 converts the controlled current into a voltage and outputs it to the output terminal 11.
The DC power supply 3 is the same as the conventional one.

すなわち、MR素子1は温度変化によつて抵抗
値が変化するが、磁気的特性の変化は一般の使用
温度範囲では比較的少ない。したがつて、上記装
置では、電流規制抵抗22を調整して無信号時の
コイル磁界をMR素子1の入力磁界変化に対する
抵抗値変化の大きい領域に設定するもので、この
ようにするとこの磁界の中心に信号磁界が重畳さ
れることになり、温度が変化しても抵抗値変化の
大きい領域からずれることがなくなる。この点が
従来の装置と上記装置との大きな相違で、従来は
基準電圧すなわち温度による変化を受け易いMR
素子1の抵抗値を基準にしたが、上記装置では
MR素子1への入力磁界において基準を定めた。
一方、再生出力の歪みについては、従来のものと
同様にMR素子1の出力を一定に保つようにコイ
ル電流が制御されてコイル電流から出力が再生さ
れ、コイル電流とコイルの発生磁界との間の非常
に良い比例関係を利用できるので原理的にはなく
なる。
That is, although the resistance value of the MR element 1 changes with temperature changes, the change in magnetic characteristics is relatively small in the general operating temperature range. Therefore, in the above device, the current regulating resistor 22 is adjusted to set the coil magnetic field when there is no signal in a region where the resistance value changes greatly in response to changes in the input magnetic field of the MR element 1. Since the signal magnetic field is superimposed at the center, even if the temperature changes, the resistance value will not deviate from the region where the change is large. This point is a major difference between conventional devices and the above devices. Conventionally, MR
Although the resistance value of element 1 was used as the standard, in the above device,
A reference was established for the input magnetic field to the MR element 1.
On the other hand, regarding the distortion of the reproduced output, the coil current is controlled to keep the output of MR element 1 constant as in the conventional case, and the output is reproduced from the coil current. Since we can take advantage of the very good proportionality of

第3図は上記装置の具体的回路図であり、この
図において、1はMR素子、2はコイル、11は
出力端子、31〜36は抵抗、41〜44はコン
デンサ、51はトランジスタ、52は電源、53
はアースである。そして、抵抗31とコンデンサ
41はMR素子1に直流電流を流すための安定化
回路を形成しており、抵抗332はMR素子1へ
の電流を制限するための抵抗である。この素子用
直流電流は電源52から抵抗31,32および
MR素子1を通つてアース53に流れる。記録媒
体からの信号磁界に基づく電圧変化はコンデンサ
42を介して交流成分のみトランジスタ51のベ
ース電極に印加される。一方、コイル電流は、電
源52より抵抗33、コイル2およびトランジス
タ51のコレクタ電極からエミツタ電極を通つて
アース53に流れる。抵抗34,35,36とコ
ンデンサ44はコイル電流の増減に対して逆の極
性に非常にゆつくりと追従する電圧を作るもの
で、この電圧はコイル2に流れる直流電流成分の
電流量を規制するトランジスタ51のベース電流
量を決める。トランジスタ51のベース電極には
この直流成分のベース電極とコンデンサ42を介
して印加されるMR素子1出力に基づく交流成分
が同時に加わり、これらの信号がトランジスタ5
1により電流増幅されてコイル2の電流となる。
また、この回路においては、出力がコンデンサ4
3を介して出力端子11に導出される。
FIG. 3 is a specific circuit diagram of the above device. In this figure, 1 is an MR element, 2 is a coil, 11 is an output terminal, 31 to 36 are resistors, 41 to 44 are capacitors, 51 is a transistor, and 52 is a power supply, 53
is earth. The resistor 31 and the capacitor 41 form a stabilizing circuit for flowing direct current to the MR element 1, and the resistor 332 is a resistor for limiting the current to the MR element 1. This element direct current is supplied from the power supply 52 to the resistors 31, 32 and
It flows through the MR element 1 to the ground 53. Only the alternating current component of the voltage change based on the signal magnetic field from the recording medium is applied to the base electrode of the transistor 51 via the capacitor 42 . On the other hand, the coil current flows from the power source 52 through the resistor 33, the coil 2, the collector electrode of the transistor 51, and the emitter electrode to the ground 53. The resistors 34, 35, and 36 and the capacitor 44 create a voltage that very slowly follows the opposite polarity as the coil current increases and decreases, and this voltage regulates the amount of DC current component flowing through the coil 2. The amount of base current of transistor 51 is determined. An AC component based on the output of the MR element 1 applied via the base electrode of the DC component and the capacitor 42 is simultaneously applied to the base electrode of the transistor 51, and these signals are applied to the base electrode of the transistor 51.
The current is amplified by 1 and becomes the current of coil 2.
Also, in this circuit, the output is capacitor 4
3 to the output terminal 11.

なお、このような具体的回路と第2図との相間
について説明すると、第2図の直流電源3は抵抗
31とコンデンサ41の安定化回路に相当する。
この場合、抵抗31はコイルに置替えてもよい。
また、電流制限抵抗4は抵抗32に相当し、増幅
器5とコイル電流制御回路9の両方の働きはトラ
ンジスタ51が行う。コイル電流源8は電源52
であり、電流・電圧変換回路10は抵抗33によ
り電圧ドロツプを検知することによつて行つてい
る。また、コンデンサ21がコンデンサ42であ
り、規制抵抗22は抵抗34,35,36が相当
する働きをし、コンデンサ44とともに自動的に
適正な直流のコイル電流が流れるようになつてい
る。なお、第3図において、MR素子1の出力が
小さい場合、MR素子1とコンデンサ42との間
に増幅回路を挿入することは有効である。
In addition, to explain the phase between such a specific circuit and FIG. 2, the DC power supply 3 in FIG. 2 corresponds to a stabilizing circuit including a resistor 31 and a capacitor 41.
In this case, the resistor 31 may be replaced with a coil.
Further, the current limiting resistor 4 corresponds to the resistor 32, and the transistor 51 functions as both the amplifier 5 and the coil current control circuit 9. Coil current source 8 is connected to power source 52
The current/voltage conversion circuit 10 performs this by detecting the voltage drop using the resistor 33. Further, the capacitor 21 is a capacitor 42, and the regulating resistor 22 has a function corresponding to that of the resistors 34, 35, and 36, so that an appropriate DC coil current automatically flows together with the capacitor 44. Note that in FIG. 3, when the output of the MR element 1 is small, it is effective to insert an amplifier circuit between the MR element 1 and the capacitor 42.

以上のように、この発明による磁気記録再生装
置によれば、従来の基準電圧設定法から基準コイ
ル磁界設定法になるように構成したので、使用温
度範囲が広くなり、しかも再生出力の歪みの少な
いものが得られる効果を有する。
As described above, according to the magnetic recording and reproducing apparatus according to the present invention, since the conventional reference voltage setting method is changed to the reference coil magnetic field setting method, the operating temperature range is widened, and the distortion of the reproduced output is reduced. It has the effect of obtaining something.

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

第1図は従来の磁気記録再生装置を示すブロツ
ク図、第2図はこの発明による磁気記録再生装置
の一実施例を示すブロツク図、第3図はこの発明
による装置の具体的回路図である。 1…MR素子、2…コイル、3…直流電源、4
…電流制限抵抗、5…増幅器、8…コイル電流
源、9…コイル電流制御回路、10…電流電圧変
換回路、11…出力端子、21…コンデンサ、2
2…規制抵抗、31〜36…抵抗、41〜44…
コンデンサ、51…トランジスタ、52…電極。
なお、図中同一符号は同一または相当部分を示
す。
FIG. 1 is a block diagram showing a conventional magnetic recording/reproducing device, FIG. 2 is a block diagram showing an embodiment of the magnetic recording/reproducing device according to the present invention, and FIG. 3 is a specific circuit diagram of the device according to the present invention. . 1...MR element, 2...coil, 3...DC power supply, 4
...Current limiting resistor, 5...Amplifier, 8...Coil current source, 9...Coil current control circuit, 10...Current voltage conversion circuit, 11...Output terminal, 21...Capacitor, 2
2... Regulatory resistance, 31-36... Resistance, 41-44...
Capacitor, 51...transistor, 52...electrode.
Note that the same reference numerals in the figures indicate the same or corresponding parts.

Claims (1)

【特許請求の範囲】 1 磁気抵抗効果素子およびこの素子に磁界を印
加するコイルからなる磁気ヘツドと、上記磁気抵
抗効果素子の出力の交流成分を検知する回路と、
上記コイルに電流を流す電源を有し、かつコイル
電流に関して、一定の直流電流および上流磁気抵
抗効果素子の出力に基づいて制御した電流とを重
畳し得る回路と、上記制御された電流量を電圧値
に変換する回路とを具備してなる磁気記録再生装
置。 2 直流電源、コンデンサおよび増幅器を有し、
直流電源から磁気抵抗効果素子に直流電流を流す
とともに、この素子の両端において発生する出力
電圧をコンデンサを通して交流成分だけ増幅し、
かつ抵抗とコイル電流制御回路を有し、コイル電
流を流す電源からコイルまでの電流路の間に、こ
の抵抗とコイル電流制御回路を挿入し、上記増幅
された交流成分の出力信号に基づいて上記コイル
電流制御回路によりコイル電流を制御することを
特徴とする特許請求の範囲第1項記載の磁気記録
再生装置。 3 増幅器としてトランジスタを有し、そのベー
ス電流に対してコンデンサと抵抗群を用いて出力
電圧を平滑し、しかも電流を調節したコイル電流
の直流成分に当る制御電流と磁気抵抗効果素子の
出力信号を重畳して印加し、コイルをこのトラン
ジスタのコレクタ電極に接続することによつてト
ランジスタに出力増幅とコイル電流の制御の両機
能をもたせたことを特徴とする特許請求の範囲第
1項または第2項記載の磁気記録再生装置。
[Scope of Claims] 1. A magnetic head consisting of a magnetoresistive element and a coil that applies a magnetic field to the element, a circuit that detects an alternating current component of the output of the magnetoresistive element,
A circuit that has a power source that allows current to flow through the coil and can superimpose a constant DC current and a current controlled based on the output of the upstream magnetoresistive element with respect to the coil current, and a circuit that can convert the controlled current amount into a voltage. A magnetic recording/reproducing device comprising a circuit for converting into a value. 2 Has a DC power supply, a capacitor and an amplifier,
Direct current is passed from a DC power supply to the magnetoresistive element, and the output voltage generated at both ends of this element is amplified by the AC component through a capacitor.
The resistor and the coil current control circuit are inserted between the current path from the power supply to the coil to cause the coil current to flow, and based on the output signal of the amplified alternating current component, the above-mentioned 2. The magnetic recording and reproducing apparatus according to claim 1, wherein the coil current is controlled by a coil current control circuit. 3 It has a transistor as an amplifier, uses a capacitor and a group of resistors to smooth the output voltage for its base current, and also uses a control current corresponding to the DC component of the coil current that has been adjusted and the output signal of the magnetoresistive element. Claims 1 or 2, characterized in that the transistor has both the functions of output amplification and control of the coil current by applying the voltage in a superimposed manner and connecting the coil to the collector electrode of the transistor. The magnetic recording and reproducing device described in .
JP9369477A 1977-08-03 1977-08-03 Magnetic recorder-reproducer Granted JPS5428108A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP9369477A JPS5428108A (en) 1977-08-03 1977-08-03 Magnetic recorder-reproducer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP9369477A JPS5428108A (en) 1977-08-03 1977-08-03 Magnetic recorder-reproducer

Publications (2)

Publication Number Publication Date
JPS5428108A JPS5428108A (en) 1979-03-02
JPS6120051B2 true JPS6120051B2 (en) 1986-05-20

Family

ID=14089497

Family Applications (1)

Application Number Title Priority Date Filing Date
JP9369477A Granted JPS5428108A (en) 1977-08-03 1977-08-03 Magnetic recorder-reproducer

Country Status (1)

Country Link
JP (1) JPS5428108A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63155648A (en) * 1986-12-18 1988-06-28 Toshiba Corp Ceramic package for solid-state image sensor

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB2100470A (en) * 1981-04-25 1982-12-22 British Aluminium Co Ltd Working strip material
JP2706404B2 (en) * 1992-03-30 1998-01-28 ティーディーケイ株式会社 Screen stretching machine

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63155648A (en) * 1986-12-18 1988-06-28 Toshiba Corp Ceramic package for solid-state image sensor

Also Published As

Publication number Publication date
JPS5428108A (en) 1979-03-02

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