JPS60261004A - Magnetic recording and reproducing device - Google Patents
Magnetic recording and reproducing deviceInfo
- Publication number
- JPS60261004A JPS60261004A JP11698384A JP11698384A JPS60261004A JP S60261004 A JPS60261004 A JP S60261004A JP 11698384 A JP11698384 A JP 11698384A JP 11698384 A JP11698384 A JP 11698384A JP S60261004 A JPS60261004 A JP S60261004A
- Authority
- JP
- Japan
- Prior art keywords
- winding
- windings
- magnetic
- magnetic head
- reproducing
- 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
Links
Classifications
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B5/00—Recording by magnetisation or demagnetisation of a record carrier; Reproducing by magnetic means; Record carriers therefor
- G11B5/02—Recording, reproducing, or erasing methods; Read, write or erase circuits therefor
Landscapes
- Recording Or Reproducing By Magnetic Means (AREA)
Abstract
Description
【発明の詳細な説明】
産業上の利用分野
本発明は、固定磁気ディスク装置やフレキシブル磁気デ
ィスク駆動装置や磁気テープ装置などの磁気記録再生装
置に関するものである。DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application The present invention relates to magnetic recording and reproducing devices such as fixed magnetic disk drives, flexible magnetic disk drives, and magnetic tape devices.
従来例の構成とその問題点
第1図は、従来の磁気記録再生装置を示している。以下
に、この従来例の構成について第1図とともに説明する
。Structure of a conventional example and its problems FIG. 1 shows a conventional magnetic recording/reproducing apparatus. The configuration of this conventional example will be explained below with reference to FIG. 1.
第1図において、1は磁気ヘッドであシ、この磁気ヘッ
ド1は磁気記録媒体の磁束変化を検出する。2は上記磁
気へ゛ラド1の再生電圧を増幅する増幅器であり、該増
幅器2の出力を信号処理回路3に導いて復調を行ない、
目的とする信号を得る。In FIG. 1, 1 is a magnetic head, and this magnetic head 1 detects changes in magnetic flux of a magnetic recording medium. Reference numeral 2 denotes an amplifier for amplifying the reproduction voltage of the magnetic helad 1, and the output of the amplifier 2 is guided to a signal processing circuit 3 for demodulation.
Obtain the desired signal.
一方、磁気ヘッド1には書き込み回路4も接続され必要
に応じて上記磁気ヘッド1に書き込み電流を印加する。On the other hand, a write circuit 4 is also connected to the magnetic head 1 and applies a write current to the magnetic head 1 as required.
次に、1記従来例の動作について説明する。Next, the operation of the conventional example No. 1 will be explained.
磁気へノド1が検出する再生電圧EPは該磁気ヘッド1
の巻線(巻線数N)が鎖交する磁気回路中の磁束ψに対
して、
Bp =N * (& ψ/” ) ・−−−・・(t
)なる巻線数に比例する時間微分形で与えられる。The reproduction voltage EP detected by the magnetic head 1 is
For the magnetic flux ψ in the magnetic circuit interlinked with the windings (number of turns N), Bp = N * (& ψ/”) ・----・(t
) is given in a time differential form proportional to the number of windings.
一方、磁気ヘッド1の巻線はインダクタンスLを有して
おシ、該インダクタンスは巻線数Nに対して、
L −N2 ・・・・・・・・・・・(2)なる関係を
有する。更に、上記インダクタンスは浮遊容量Cのため
に共振系を形成するが、該共振系の共振周波数f。は、
fo=1/2πvLで− ・・・・・・・・・・・(3
)と表わされる。磁気ヘッド1の動作領域は、上記(3
)式で与えられるf。以下の周波数領域に限定される。On the other hand, the winding of the magnetic head 1 has an inductance L, and the inductance has the relationship L - N2 (2) with respect to the number of windings N. . Furthermore, the inductance forms a resonant system due to the stray capacitance C, and the resonant frequency f of the resonant system. is, fo = 1/2πvL - ・・・・・・・・・・・・(3
). The operating area of the magnetic head 1 is the above (3)
) is given by the formula. Limited to the following frequency ranges.
上記従来例においては、上記(1)式に基づいて再生電
圧を増加させるために巻線数Nを増加すれば上記(21
,(31式から明らかなように共振周波数几の低下を招
き、使用可能な周波数領域の上限が低下する欠点を有し
ていた。即ち、磁気ヘッド1の使用可能な周波数領域を
確保するためには、巻線数はある値以下としなくてはな
らず、従って、再生電圧の上限も定まってしまっていた
。なお、(3)式より浮遊容量Cの低下は共振周波数の
増加に有効であるが、該浮遊容量は現実的には低下させ
ることは必ずしも容易でない。In the above conventional example, if the number of windings N is increased in order to increase the reproduction voltage based on the above equation (1), the above (21
, (as is clear from Equation 31, the resonant frequency was lowered and the upper limit of the usable frequency range was lowered. In other words, in order to secure the usable frequency range of the magnetic head 1, In this case, the number of windings must be kept below a certain value, and therefore, the upper limit of the reproduction voltage has also been determined.From equation (3), reducing the stray capacitance C is effective in increasing the resonant frequency. However, it is not necessarily easy to reduce the stray capacitance in reality.
発明の目的
本発明は、上記従来例の欠点を除去するものであり、磁
気ヘッドとしての使用可能な周波数領域を低下させるこ
となく、巻線数を増加せしめて再生電圧を増加させるこ
とを目的とするものである。Purpose of the Invention The present invention eliminates the drawbacks of the conventional example described above, and aims to increase the number of windings and increase the reproduction voltage without reducing the usable frequency range as a magnetic head. It is something to do.
発明の構成
本発明は、上記目的を達成するために、磁気ヘッドの同
一の磁気回路中に設けられた複数の巻線と該巻線群の各
々一つの増幅器を接続するように構成された複数の再生
増幅器群とを具備するもので、磁気ヘッドの共振周波数
を一定に確保しつつ再生電圧を増加する効果を得るもの
である。Structure of the Invention In order to achieve the above object, the present invention provides a plurality of windings provided in the same magnetic circuit of a magnetic head and a plurality of windings configured to connect each of the winding groups to one amplifier. It is equipped with a group of regenerative amplifiers, and has the effect of increasing the reproducing voltage while keeping the resonant frequency of the magnetic head constant.
実施例の説明
以下に本発明の一実施例の構成について、図面とともに
説明する。DESCRIPTION OF EMBODIMENTS The configuration of an embodiment of the present invention will be described below with reference to the drawings.
第2図において、10は磁気ヘッドの磁路を成すコアで
あシ、該コア10中に流入する磁束と鎖交するように複
数の巻線11.12が設けられている。上記巻線11.
12は各々が再生増幅器13.14にリード線15.1
6によ多接続される。上記再生増幅器群は加算器17に
接続され、最終的に単一の再生出力を得る。■8は書き
込み回路である。In FIG. 2, reference numeral 10 denotes a core forming a magnetic path of the magnetic head, and a plurality of windings 11 and 12 are provided so as to interlink with the magnetic flux flowing into the core 10. The above winding 11.
12 are each connected to a lead wire 15.1 to a regenerative amplifier 13.14.
6. The regenerative amplifier group is connected to an adder 17 to finally obtain a single regenerative output. (2) 8 is a write circuit.
なお、本実施例では簡単のため、2つの巻線と再生増幅
器を例示したが、2つに限定されるものではない。又、
上記実施例では記録時には上記複数の巻線のうちの1つ
を用いて行なっているが、複数の巻線を用いることもで
きる。更に、巻線の構成法として、必ずしも独立した複
数の巻線を形成する必要はなく、中間タップを設けて等
測的に複数の巻線として動作させることも可能である。Note that in this embodiment, for simplicity, two windings and a regenerative amplifier are illustrated, but the number is not limited to two. or,
In the above embodiment, recording is performed using one of the plurality of windings, but a plurality of windings may also be used. Furthermore, as a method of configuring the windings, it is not necessarily necessary to form a plurality of independent windings, and it is also possible to provide an intermediate tap and operate the windings equimetrically as a plurality of windings.
次に上記従来例の動作について説明する。Next, the operation of the above conventional example will be explained.
第2図において、個々の巻線の巻線数をNとする。磁気
へラドコアの再生磁束に対して、(1)式にて示した再
生電圧が巻線に発生するが、本実施例においては同一の
磁気回路に複数の巻線11.12と再生増幅器13.1
4を具備してなるため、最終的な再生出力E、 tot
alは、
E、 total = N ”’ + N” ’−13
t δを
−(N+N)−9−
t
と全巻線数に対応する電圧を得ることが可能である。一
方、磁気ヘッドとしての使用可能帯域を決定する共振周
波数は個々の巻線のインダクタンスと浮遊容量の積に依
存する。このため、複数の巻線群を有していても、その
共振周波数は単一の巻線の場合と同じである。In FIG. 2, the number of turns of each winding is N. In response to the reproducing magnetic flux of the magnetic helad core, a reproducing voltage expressed by equation (1) is generated in the winding, but in this embodiment, the same magnetic circuit includes a plurality of windings 11, 12 and regenerative amplifiers 13. 1
4, the final playback output E, tot
al is E, total = N"' + N"'-13
It is possible to set t δ to −(N+N)−9− t and obtain a voltage corresponding to the total number of turns. On the other hand, the resonant frequency that determines the usable band as a magnetic head depends on the product of the inductance and stray capacitance of each individual winding. Therefore, even if it has a plurality of winding groups, its resonant frequency is the same as in the case of a single winding.
この結果、再生出力を全巻線数に対応する値に増加せし
める一方、共振周波数は分割した個々の巻線が有する高
い値に保つことが可能となる。As a result, while increasing the reproduction output to a value corresponding to the total number of windings, it is possible to maintain the resonant frequency at the high value of each divided winding.
更に、再生増幅器と加算器を差動増幅器として動作させ
ることで、同相雑音除去能力を、従来例の再生増幅器単
独の場合に比べて、再生増幅器と加算器の積とするとと
ができて改善可能である。Furthermore, by operating the regenerative amplifier and the adder as a differential amplifier, the common-mode noise removal ability can be improved by making it the product of the regenerative amplifier and the adder, compared to the conventional regenerative amplifier alone. It is.
なお、複数巻線では相互インダクタンスの影響が懸念さ
れるが、巻線が高インピーダンスで終端されるので、そ
の影響は小さい。Note that with multiple windings, there is a concern about the influence of mutual inductance, but since the windings are terminated with high impedance, this influence is small.
発明の効果
本発明は上記のような構成であシ、以下に示す効果が得
られるものである。Effects of the Invention The present invention has the above-described configuration, and provides the following effects.
(a) 共振周波数が高く、再生出力の大きい磁気ヘッ
ド系を提供できるので、再生信号のS/Nが向上する。(a) Since it is possible to provide a magnetic head system with a high resonance frequency and a large reproduction output, the S/N of the reproduction signal is improved.
(b) 磁気記録媒体及び磁気ヘッドの構造上の諸ノく
ラメータに依存せす、上記効果が得られるだめ、分解能
を劣化させることがない。(b) Since the above effects can be obtained depending on various structural parameters of the magnetic recording medium and the magnetic head, the resolution does not deteriorate.
第1図は従来の磁気記録再生装置のブロック図、第2図
は本発明の一実施例における磁気記録再生装置のプロ、
り図である。
10・・・コア、11.12・・・巻線、13.14・
再生増幅器、15.16・・リード線、17・・加算器
。
代理人の氏名 弁理士 中 尾 敏 男 ほか1名第1
図
第2図FIG. 1 is a block diagram of a conventional magnetic recording and reproducing device, and FIG. 2 is a block diagram of a magnetic recording and reproducing device according to an embodiment of the present invention.
This is a diagram. 10...Core, 11.12...Winding, 13.14.
Regenerative amplifier, 15.16... Lead wire, 17... Adder. Name of agent: Patent attorney Toshio Nakao and 1 other person No. 1
Figure 2
Claims (1)
この巻線の各々に接続される複数の再生増幅器と、上記
複数の再生増幅器の出力を加算する加算器とから成る磁
気記録再生装置。A plurality of windings interlinked with the same magnetic circuit in the magnetic head,
A magnetic recording/reproducing device comprising a plurality of reproducing amplifiers connected to each of the windings, and an adder for adding the outputs of the plurality of reproducing amplifiers.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP11698384A JPS60261004A (en) | 1984-06-07 | 1984-06-07 | Magnetic recording and reproducing device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP11698384A JPS60261004A (en) | 1984-06-07 | 1984-06-07 | Magnetic recording and reproducing device |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS60261004A true JPS60261004A (en) | 1985-12-24 |
Family
ID=14700583
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP11698384A Pending JPS60261004A (en) | 1984-06-07 | 1984-06-07 | Magnetic recording and reproducing device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS60261004A (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH01201802A (en) * | 1988-02-08 | 1989-08-14 | Canon Inc | Magnetic recording and reproducing device |
US5122916A (en) * | 1989-12-04 | 1992-06-16 | Archive Corporation | Electromagnetic head having interference compensation circuitry |
-
1984
- 1984-06-07 JP JP11698384A patent/JPS60261004A/en active Pending
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH01201802A (en) * | 1988-02-08 | 1989-08-14 | Canon Inc | Magnetic recording and reproducing device |
US5122916A (en) * | 1989-12-04 | 1992-06-16 | Archive Corporation | Electromagnetic head having interference compensation circuitry |
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