JPS6037521B2 - magnetic recording and reproducing device - Google Patents

magnetic recording and reproducing device

Info

Publication number
JPS6037521B2
JPS6037521B2 JP10008279A JP10008279A JPS6037521B2 JP S6037521 B2 JPS6037521 B2 JP S6037521B2 JP 10008279 A JP10008279 A JP 10008279A JP 10008279 A JP10008279 A JP 10008279A JP S6037521 B2 JPS6037521 B2 JP S6037521B2
Authority
JP
Japan
Prior art keywords
signal
magnetic
circuit
simulated
core
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
JP10008279A
Other languages
Japanese (ja)
Other versions
JPS5625213A (en
Inventor
敏朗 中村
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.)
ERUKU KK
Original Assignee
ERUKU KK
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 ERUKU KK filed Critical ERUKU KK
Priority to JP10008279A priority Critical patent/JPS6037521B2/en
Publication of JPS5625213A publication Critical patent/JPS5625213A/en
Publication of JPS6037521B2 publication Critical patent/JPS6037521B2/en
Expired legal-status Critical Current

Links

Description

【発明の詳細な説明】 この発明は例えばテープレコーダ或いは磁気ディスク装
置等の磁気記録再生装置に関し、特に磁気媒体のヒステ
リシスに基ずく波形歪を除去しようとするものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a magnetic recording/reproducing device such as a tape recorder or a magnetic disk device, and is particularly intended to eliminate waveform distortion based on hysteresis of a magnetic medium.

磁気記録再生装置ではその再生信号は磁気媒体の磁気的
ヒステリシスにより波形歪が起きる欠点がある。つまり
磁気へッド‘こよって磁気媒体に記録する場合、磁気ヘ
ッドから発生する磁界は磁気ギャップを中心に或る広が
りを持つ。このため信号と信号の継目においては磁気的
な加減算が行なわれていると考えられる。このため磁気
媒体が例えば第1図に示すようなヒステリシスを持って
いると、再生波形は第2図aに示すような波形歪を受け
る。尚第2図bは正常な正弦波形を示す。こ)で特に波
形の始まりの半サイクルに要する時間T.は第1図に示
すヒステリシス特性の初期曲線Dを通るためそれ以後の
各半サイクルに要する時情け2より長くなってしまう。
このため音楽再生の場合その頭の部分の立上りが悪いと
か或いはアタックが悪いという表現が使われている。こ
の発明の目的は磁気媒体のヒステリシスによって再生す
る歪を除去し、且つ立上りの半サイクルに要する時間が
正常な長さで得られる磁気記録再生菱贋を提供するにあ
る。この発明では磁気記録再生装置において、記録又は
再生系の何れかに磁気媒体の磁気的なヒステリシスに基
ずく波形歪を模似的に発生させる模似回路と、この模似
回路から出力される歪信号とこの榛似回路に供給される
元信号との差を演算する減算回路とを挿入するものであ
る。
A magnetic recording/reproducing device has a disadvantage in that the reproduced signal suffers waveform distortion due to the magnetic hysteresis of the magnetic medium. In other words, when recording on a magnetic medium using a magnetic head, the magnetic field generated by the magnetic head has a certain spread around the magnetic gap. For this reason, it is thought that magnetic addition and subtraction is performed at the joint between signals. Therefore, if the magnetic medium has hysteresis as shown in FIG. 1, the reproduced waveform will be subjected to waveform distortion as shown in FIG. 2a. Note that FIG. 2b shows a normal sine waveform. In particular, the time required for the first half cycle of the waveform T. Since it passes through the initial curve D of the hysteresis characteristic shown in FIG. 1, it becomes longer than the time interval 2 required for each subsequent half cycle.
For this reason, when playing music, expressions such as the beginning of a song having a bad rise or attack are used. It is an object of the present invention to provide a magnetic recording/reproduction disk which eliminates reproduction distortion due to hysteresis of a magnetic medium and allows the time required for a half cycle of rise to be a normal length. The present invention provides a magnetic recording/reproducing device including a simulating circuit that simulates waveform distortion based on magnetic hysteresis of a magnetic medium in either the recording or reproducing system, and a distortion output from the simulating circuit. A subtraction circuit is inserted to calculate the difference between the signal and the original signal supplied to the Harini circuit.

以下にこの発明の一実施例を第3図を用いて詳細に説明
する。第3図において1は例えば再生信号源を示す。
An embodiment of the present invention will be described in detail below with reference to FIG. In FIG. 3, 1 indicates, for example, a reproduced signal source.

この再生信号源1は再生ヘッド単体でもよく、また再生
増幅器を含むものと考えてもよい。再生信号源1の出力
信号は必要に応じてバッファ増幅器2を通じて磁気媒体
のヒステリシスに基ずく波形歪と等価な歪を模似的に与
える漠似回路3に供給される。この模似回路3はバッフ
ァ増幅器2の出力側に接続された磁界発生手段4と、こ
の磁界発生手段4の磁界を検出する磁電変換素子5と、
この磁電変換素子5の電気出力を増幅する増幅器6とに
より構成される。磁電変換素子5は例えばホール素子或
いはその他の感磁性素子を用いるとができる。図の例で
はホール素子を用いた場合を示し、9はホール素子の電
流端子間に一定電流を流すための直流電源を示す。磁界
発生手段4はコアとこれに者装したコイルによって構成
され、コイルにバッファ増幅器2の出力電流を与える。
コアは環状コアが用いられその環状コアの一部に磁気ギ
ャップを設け、この磁気ギャップ内に磁軍変換素子5を
挿入し、磁界発生手段4と磁電変換素子5とを密に結合
する。こ)で磁界発生手段4を構成するコァの磁気的ヒ
ステリシス特性を磁気記録媒体のそれとほゞ等しくなる
ようにコアの材質を選定すれば磁界発生手段−磁電変換
素子5を通る過程において信号は磁気記録媒体で発生す
る歪とほゞ等価な歪を受ける。よって元信号が磁気媒体
のヒステリシスに基ずく歪を受けているものとすると、
模似回路3の出力はその約2倍の歪を受けて出力される
。模似回路3の出力は減算回路7の一方の入力端子に供
給する。減算回路7の他方の入力端子には再生信号源1
の出力を直接供給する。減算回路7の減算出力は加算回
路8に供V給され、加算回路8にて再生信号に加算する
。 このように構成することによって加算回路8の出力
には歪が徐去された再生信号を得ることができる。以下
にその説明を行なう。磁界発生手段4の磁気コアにも先
に説明したようにヒステリシスが存在する。このため磁
電変換素子5の出力信号は磁界発生手段4を構成する磁
気コァの磁気的なヒステリシスによる歪を受ける。この
結果増幅器6から出力される信号は再生信号源1から出
力される信号a第2図の立上りより更に遅れて立上る波
形となる。第4図にその詳細を示す。第4図においてa
は再生信号源1の再生信号、cは増幅器6の出力信号を
示す。再生信号aから増幅器6の出力信号を減算回路7
によって減算すると、第4図に示すような第2高調波成
分を持つ補正信号dが得られる。この補正信号dは磁気
媒体のヒステリシスに基ずく歪波と、その倍の歪波の差
であり、これは正弦波と再生信号aの差には)、近似す
ることができる。よってこの補正信号dを加算回路8に
て再生信号aに加算することにより立上りが正常な、つ
まり立上りの半サイクルに要する時間とそれ以後の半サ
イクルに要する時間が等しく、且つ歪が除去された第4
図に示すような正弦波bを得ることができる。以上説明
したようにこの発明によれば磁気記録再生装置において
磁気媒体が持つヒステリシスによって発生する再生信号
の歪を除去することができ、且つ再生波の頭部の半サイ
クルがそれ以後の各半サイクルに要する時間より長くな
るのも補正され、正常なアタックを持つ信号を再生する
ことができる。
The reproduction signal source 1 may be a single reproduction head, or may include a reproduction amplifier. The output signal of the reproduced signal source 1 is supplied via a buffer amplifier 2 as necessary to an approximate circuit 3 which gives a simulated distortion equivalent to the waveform distortion based on the hysteresis of the magnetic medium. This simulated circuit 3 includes a magnetic field generating means 4 connected to the output side of the buffer amplifier 2, a magnetoelectric conversion element 5 that detects the magnetic field of the magnetic field generating means 4,
It is constituted by an amplifier 6 that amplifies the electrical output of this magnetoelectric conversion element 5. For example, a Hall element or other magnetically sensitive element can be used as the magnetoelectric conversion element 5. The example shown in the figure shows a case where a Hall element is used, and 9 indicates a DC power supply for flowing a constant current between the current terminals of the Hall element. The magnetic field generating means 4 is constituted by a core and a coil attached to the core, and supplies the output current of the buffer amplifier 2 to the coil.
An annular core is used as the core, a magnetic gap is provided in a part of the annular core, a magnetic force conversion element 5 is inserted into this magnetic gap, and the magnetic field generating means 4 and the magnetoelectric conversion element 5 are tightly coupled. In this case, if the material of the core is selected so that the magnetic hysteresis characteristic of the core constituting the magnetic field generating means 4 is almost equal to that of the magnetic recording medium, the signal will not become magnetic in the process of passing between the magnetic field generating means and the magnetoelectric transducer 5. It receives distortion that is almost equivalent to the distortion that occurs in the recording medium. Therefore, assuming that the original signal is subject to distortion due to the hysteresis of the magnetic medium,
The output of the simulated circuit 3 is subjected to distortion approximately twice that amount. The output of the simulating circuit 3 is supplied to one input terminal of the subtraction circuit 7. The other input terminal of the subtraction circuit 7 is connected to the reproduction signal source 1.
directly supplies the output of The subtraction output of the subtraction circuit 7 is supplied to an addition circuit 8, where it is added to the reproduced signal. With this configuration, it is possible to obtain a reproduced signal from which distortion has been removed at the output of the adder circuit 8. The explanation will be given below. The magnetic core of the magnetic field generating means 4 also has hysteresis as described above. Therefore, the output signal of the magnetoelectric transducer 5 is subjected to distortion due to the magnetic hysteresis of the magnetic core constituting the magnetic field generating means 4. As a result, the signal output from the amplifier 6 has a waveform that rises later than the rise of the signal a output from the reproduced signal source 1 as shown in FIG. Figure 4 shows the details. In Figure 4 a
indicates the reproduced signal of the reproduced signal source 1, and c indicates the output signal of the amplifier 6. A circuit 7 that subtracts the output signal of the amplifier 6 from the reproduced signal a.
By subtracting , a correction signal d having a second harmonic component as shown in FIG. 4 is obtained. This correction signal d is the difference between a distorted wave based on the hysteresis of the magnetic medium and a distorted wave twice that amount, and can be approximated to the difference between the sine wave and the reproduced signal a. Therefore, by adding this correction signal d to the reproduced signal a in the adding circuit 8, the rise is normal, that is, the time required for a half cycle of the rise is equal to the time required for the subsequent half cycle, and distortion is removed. Fourth
A sine wave b as shown in the figure can be obtained. As explained above, according to the present invention, it is possible to remove the distortion of the reproduced signal caused by the hysteresis of the magnetic medium in a magnetic recording/reproducing device, and the head half cycle of the reproduced wave is changed from each subsequent half cycle. It is also possible to correct the fact that the time is longer than the time required for the attack, and it is possible to reproduce a signal with a normal attack.

第5図はこの発明の他の実施例を示す。FIG. 5 shows another embodiment of the invention.

この例では磁界発生手段4を励磁する増幅器2に差動増
幅器を用い、この差敷増幅器2によって減算回路7を兼
用するように構成した場合を示す。従ってこの場合には
差動増幅器2の出力側には差信号dが出力されており、
この差信号を加算回路8にて再生信号に加算することに
より第3図の場合と同様に歪を持つ再生信号を正弦波に
補正することができる。尚、上述では磁気媒体のヒステ
リシスによって生じる歪の逆極性の歪を持つ補正信号を
得る襟似回路3を再生信号系に挿入した場合を説明した
が必ずしもその必要はな、例えば記録系に挿入し予め逆
極性の歪を与えた状態で記録しておくことにより、再生
信号は正常な波形で得ることができる。
In this example, a differential amplifier is used as the amplifier 2 that excites the magnetic field generating means 4, and this differential amplifier 2 is configured to also serve as the subtraction circuit 7. Therefore, in this case, the difference signal d is output to the output side of the differential amplifier 2,
By adding this difference signal to the reproduced signal in the adding circuit 8, it is possible to correct the distorted reproduced signal to a sine wave as in the case of FIG. In the above description, a case has been described in which the analog circuit 3 for obtaining a correction signal having a distortion of the opposite polarity to the distortion caused by the hysteresis of the magnetic medium is inserted into the reproduction signal system, but it is not necessarily necessary to do so; for example, it may be inserted into the recording system. By recording in advance with reverse polarity distortion, a reproduced signal can be obtained with a normal waveform.

また上述では減算結果を加算器8に供聯合したが減算器
7に供9台する元信号のレベルを2倍に設定し、2倍の
レベルを持つ元信号から差信号を減算するように構成す
ることもできる。
In addition, in the above, the subtraction result is combined with the adder 8, but the level of the original signal fed into the subtracter 7 is set to double, and the difference signal is subtracted from the original signal having twice the level. You can also.

この場合には加算回路8は必要なく、よって加算回路8
はこの発明の構成要素から外されること容易に理解でき
よう。以上説明したようにこの発明によれば磁気記録再
生装置の磁気媒体のヒステリシスによって発生する再生
信号の歪を除去でき、またアタックが正常な再生信号を
得ることができその効果は実用に供して頗る大である。
In this case, the adder circuit 8 is not necessary, so the adder circuit 8
It is easy to understand that these are excluded from the constituent elements of this invention. As explained above, according to the present invention, it is possible to remove the distortion of the reproduced signal caused by the hysteresis of the magnetic medium of the magnetic recording and reproducing device, and it is also possible to obtain a reproduced signal with a normal attack. It's large.

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

第1図は磁気媒体のヒステリシス特性の一例を示すグラ
フ、第2図はそのヒステリシスによって発生する再生信
号の歪を説明するための波形図、第3図はこの発明の一
実施例を示す系統図、第4図はこの発明の動作の説明に
供する波形図、第5図はこの発明の他の実施例を示す系
統図である。 1:再生信号源、2:増幅器、3:模似回路。 第1図共2図 ※3図 第4 図 券 5 図
Fig. 1 is a graph showing an example of the hysteresis characteristic of a magnetic medium, Fig. 2 is a waveform diagram to explain the distortion of the reproduced signal caused by the hysteresis, and Fig. 3 is a system diagram showing one embodiment of the present invention. , FIG. 4 is a waveform diagram for explaining the operation of the present invention, and FIG. 5 is a system diagram showing another embodiment of the present invention. 1: reproduction signal source, 2: amplifier, 3: imitation circuit. Figures 1 and 2 *3 Figure 4 Ticket 5 Figure

Claims (1)

【特許請求の範囲】[Claims] 1 コア及びこのコアに巻設されるコイルよりなる磁界
発生手段及びこの磁界発生手段に電磁的に結合して配さ
れる磁電変換素子とを有する模似回路と、この模似回路
で作成される歪信号と前記模似回路の入力信号との差を
演算する減算回路とが記録系又は再生系に挿入され、前
記入力信号として磁気媒体の磁気的なヒステリシスに基
づく波形歪を有する元信号が前記模似回路に入力され、
前記コアは磁気的ヒステリシス特性が前記磁気媒体の磁
気的ヒステリシス特性にほぼ等しくなるようにその材質
が選定され、前記模似回路では前記波形歪を模似的に発
生して前記元信号に重畳して前記歪信号が作成され、こ
の歪信号と前記元信号との差が前記減算回路で演算され
、、前記元信号から前記波形歪が除去された信号が得ら
れるように構成されてなる磁気記録再生装置。
1. A simulated circuit having a core, a magnetic field generating means consisting of a coil wound around the core, and a magnetoelectric transducer arranged electromagnetically coupled to the magnetic field generating means, and a simulated circuit created using this simulated circuit. A subtraction circuit that calculates the difference between the distorted signal and the input signal of the simulated circuit is inserted into the recording system or the reproduction system, and the original signal having waveform distortion based on the magnetic hysteresis of the magnetic medium is used as the input signal. input into the simulated circuit,
The material of the core is selected so that its magnetic hysteresis characteristic is approximately equal to the magnetic hysteresis characteristic of the magnetic medium, and the simulated circuit generates the waveform distortion in a simulated manner and superimposes it on the original signal. the distorted signal is created, the difference between the distorted signal and the original signal is calculated by the subtraction circuit, and a signal from which the waveform distortion is removed is obtained from the original signal. playback device.
JP10008279A 1979-08-06 1979-08-06 magnetic recording and reproducing device Expired JPS6037521B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP10008279A JPS6037521B2 (en) 1979-08-06 1979-08-06 magnetic recording and reproducing device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP10008279A JPS6037521B2 (en) 1979-08-06 1979-08-06 magnetic recording and reproducing device

Publications (2)

Publication Number Publication Date
JPS5625213A JPS5625213A (en) 1981-03-11
JPS6037521B2 true JPS6037521B2 (en) 1985-08-27

Family

ID=14264511

Family Applications (1)

Application Number Title Priority Date Filing Date
JP10008279A Expired JPS6037521B2 (en) 1979-08-06 1979-08-06 magnetic recording and reproducing device

Country Status (1)

Country Link
JP (1) JPS6037521B2 (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0420756B1 (en) * 1989-09-29 1994-12-14 Ube Industries, Ltd. Process for catalytically producing monoalkylether of dihydric phenol compound
US5817886A (en) * 1995-12-28 1998-10-06 Nippon Shokubai Co., Ltd. Process for production of alkyl ether of phenol and catalyst used therein

Also Published As

Publication number Publication date
JPS5625213A (en) 1981-03-11

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