JPS5930208A - magnetic recording and reproducing device - Google Patents
magnetic recording and reproducing deviceInfo
- Publication number
- JPS5930208A JPS5930208A JP57140545A JP14054582A JPS5930208A JP S5930208 A JPS5930208 A JP S5930208A JP 57140545 A JP57140545 A JP 57140545A JP 14054582 A JP14054582 A JP 14054582A JP S5930208 A JPS5930208 A JP S5930208A
- Authority
- JP
- Japan
- Prior art keywords
- recording
- head
- reproducing
- signal
- magnetic
- 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.)
- Granted
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
本発明は短波長磁気記録に通ずるトランスベース記録方
式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 a magnetic recording/reproducing apparatus using a trans-based recording method that leads to short wavelength magnetic recording.
従来例の構成とそのjl」照点
従来、ビデオテープレコーダなどの磁気記録再生装置に
おいては、磁気記録媒体として磁気テープ、を用い、磁
気ヘッドあるいは磁気テープを上記ヘッドの幅方向に対
し、はぼ直角あるいは数度のアジマス角をもって走行さ
せることにより、パピ録またii再再生行なっている。Conventional configuration and its points of interest Conventionally, in magnetic recording and reproducing devices such as video tape recorders, a magnetic tape is used as a magnetic recording medium, and the magnetic head or magnetic tape is moved roughly in the width direction of the head. By running it at a right angle or at an azimuth angle of several degrees, papi recordings and replays are performed.
このような媒体の運動方向に磁化する磁化方式は長手方
向磁化と抑場れ、ビデオテープレコーダなどVC丸−い
ては記録波長1μm程度のところから記録減磁が増加し
、これ以上の短波長記録の実用化は困難であった。Such a magnetization method that magnetizes the medium in the direction of motion is suppressed by longitudinal magnetization, and in VC machines such as video tape recorders, recording demagnetization increases from a recording wavelength of about 1 μm, and shorter wavelength recording It was difficult to put it into practical use.
一方、これ以上の短波長記録を目的とした垂直磁化方式
が検討され、実用化への提案が数多くきれているが、記
録再生に主磁極と補助a極が必要であり、また記録媒体
としても垂直磁化膜と水平磁化膜のJmJ1g構造が必
要であるなど構成が複雑になる欠点がある。On the other hand, perpendicular magnetization methods have been studied for the purpose of recording at even shorter wavelengths, and many proposals for practical use have been made. There is a drawback that the configuration is complicated, such as the need for a JmJ1g structure of a vertically magnetized film and a horizontally magnetized film.
また、磁気ヘッドのヘッド1隔方向と磁気テープの走行
方向をほぼ同一にする、いわゆるトランスバース目己録
(Transverse記録)も提案されているが、従
来は、長手方向磁化のギャップ幅に相当するヘッド幅よ
り長い波長(実際には、3倍程度以上)しか記録再生は
できないと考えられており、大幅な短波長記録の実5J
tにはならなかった。In addition, so-called transverse recording has been proposed, in which the head direction of the magnetic head is made almost the same as the running direction of the magnetic tape. It is believed that only wavelengths longer than the head width (actually, about 3 times or more) can be recorded and reproduced, and the actual 5J wavelength recording is significantly shorter than the width of the head.
It didn't reach t.
発明の目的
本発明は上述し/こ従来の欠点を除去し、大幅な短波長
記録を口J能にする磁気記録再生装置を提供することを
目的とするものである。OBJECTS OF THE INVENTION It is an object of the present invention to provide a magnetic recording and reproducing apparatus which eliminates the above-mentioned drawbacks of the prior art and makes recording at significantly shorter wavelengths possible.
つる明の構成
上dピ目的を達成するために本発明は、磁気ヘッドと前
記磁気ヘッド幅方向に相対的に移動する記録媒体を有す
るトランスバース記録方式の磁気記録再生装置であって
、ヘッド幅りを有する記録再生ヘッドまたは記録ヘッド
とヘッド幅りを有する再生ヘッドを具備し、前記記録再
生ヘッドまたは記録ヘッドにより、記録媒体上を相対的
に多くとも距離り移動する区間だけ信号を記録し、次に
前記記録再生ヘッドまたは記録ヘッドが前記記録媒体上
を相対的に少なくとも距離り移動する区間は記録を停止
するように構成したものである。In order to achieve the object of d-pi due to the structure of the Tsurume, the present invention provides a transverse recording type magnetic recording/reproducing apparatus having a magnetic head and a recording medium that moves relatively in the width direction of the magnetic head, a recording/reproducing head or a recording head having a head width and a reproducing head having a head width, the recording/reproducing head or recording head recording a signal only in a section in which the recording head or the recording head relatively moves at most a distance on the recording medium; Next, recording is stopped during a section in which the recording/reproducing head or the recording head moves relatively at least a distance on the recording medium.
さらに、本発明は、ヘッド幅りを有する再生ヘッドを具
備し、多くとも距離りの区間だけ記録され、次の少なく
とも距離、Lの区間は記録されてぃな、い記録媒体を前
記再生ヘッドにょシ再生して再生、信号を得るように構
成したものである。Furthermore, the present invention includes a reproducing head having a head width, and the reproducing head uses a recording medium in which at most an interval of L is recorded, and the next interval of at least L is unrecorded. This device is configured to reproduce signals by reproducing signals.
実施例の説明
以下本発明の一実施例を図面に基づいて説明する。第1
図(ILIはトランスバース記録の記録ヘッド(1)、
記録波形(2)、磁気テープ(3)、コイル(4)、テ
ープ走行方向(イ)、記録ヘッド幅L、ギャップ幅Gを
示したもの、(b)はその裏面図を示したもので、磁気
テープ(3)は記録ヘッド(1)の幅方向に移動する。DESCRIPTION OF EMBODIMENTS An embodiment of the present invention will be described below with reference to the drawings. 1st
Figure (ILI is a recording head (1) for transverse recording,
The recording waveform (2), the magnetic tape (3), the coil (4), the tape running direction (A), the recording head width L, and the gap width G are shown, and (b) shows the back view. The magnetic tape (3) moves in the width direction of the recording head (1).
ここで、記録波形(2)は磁気テープ(3)が記録ヘッ
ド(1)の終端g1+g2間のギャップを通る時に加わ
る記録信号により決足されると考えてよく、記録信号の
波長λは記録ヘッド幅りと何ら関係しない。すなわち、
記録ヘッド幅りよりも短い波長をもつ信号の記録が可能
であることがわかる。これは従来の長手方向磁化方式で
は記録減磁により実現が困難であった。Here, the recording waveform (2) can be considered to be determined by the recording signal applied when the magnetic tape (3) passes through the gap between the ends g1 and g2 of the recording head (1), and the wavelength λ of the recording signal is It has nothing to do with width. That is,
It can be seen that it is possible to record a signal with a wavelength shorter than the width of the recording head. This was difficult to achieve with the conventional longitudinal magnetization method due to recording demagnetization.
次に、このように記録された信号を再生する時の例を第
2図に示す。第2図(&)はヘッド幅りの中に半波長大
る信号が示されており、この時再生出力は最大となる。Next, FIG. 2 shows an example of reproducing a signal recorded in this manner. FIG. 2 (&) shows a signal that is half a wavelength larger within the width of the head, and at this time the reproduction output is at its maximum.
これは、再生出力はへッドコア内を辿る磁束の変化と考
えると、再生信号の波長λがヘッドlll1jLとλ=
2Lの関係の時磁束の変化量が最大になることから明ら
かである。This means that if we consider that the reproduced output is a change in the magnetic flux that follows inside the head core, then the wavelength λ of the reproduced signal is equal to the head lll1jL and λ=
This is clear from the fact that the amount of change in magnetic flux is maximum when the relationship is 2L.
仄に、第2図(1))にヘッド幅りに1波長が入る信号
をボす。この時再生ヘッドが移動してもコア内に磁束の
変化は発生せず再生出力は0となる。つまり再生信号の
波長λ=−(nは自然数)を満だ一ノ一時、再生出力は
Oとなり、これは従来の長手方向記録におけるギャップ
ロスに相当すると考えられる。In other words, a signal with one wavelength included in the width of the head shown in FIG. 2 (1)) is dropped. At this time, even if the reproducing head moves, no change in magnetic flux occurs within the core, and the reproducing output becomes zero. In other words, once the wavelength λ=-(n is a natural number) of the reproduced signal is satisfied, the reproduced output becomes O, which is considered to correspond to the gap loss in conventional longitudinal recording.
そこで、次に第2図(b)において、1波長のみ記録さ
れていた場合の再生出力を考えてみる。第3図(t、)
は記録信号の先端S、が再生ヘッドの先端り。Next, let us consider the reproduced output when only one wavelength is recorded in FIG. 2(b). Figure 3 (t,)
The leading edge S of the recording signal is the leading edge of the playback head.
と一致し再生されはじめる瞬間を示した図、(t2)は
ヘッドIIILの中に1波長人っている状態の図、(t
5)は再生が終った瞬間の図をボしている。ここで再生
ヘッドはギャップ部のみを示している。上目己(tl)
の状態から(t2)の状態を経て(t3)の状態まdφ
4、図に示す。ここで了「は再生出力を示している。(t2) is a diagram showing the moment when the head IIIL is occupied by one wavelength person.
5) shows the image at the moment the playback ends. Here, only the gap portion of the reproducing head is shown. Kimi Kamime (tl)
From the state of (t2) to the state of (t3), dφ4, as shown in the figure. Here, "" indicates the playback output.
ここで、再生途中において第3図に示すヘッド先端部分
り、とヘッド後端部分h2の間を通過している信号はヘ
ッドのコアを通る磁束φの変化には(”Jら寄与しない
(袈、=0)ため、再生出力には現dφ
われてこない。つまり第4図の丹生出カーcltにおい
て、t1〜t2区間はヘッド先端h1での再生波形と考
えられ、t2〜t3区間はヘッド後端h2でp再生波形
と考えられる。Here, during reproduction, the signal passing between the head end portion h2 and the head rear end portion h2 shown in FIG. 3 does not contribute to the change in magnetic flux φ passing through the head core. , = 0), the current dφ is not reflected in the playback output.In other words, in the Nyu output car clt in Fig. 4, the period t1 to t2 is considered to be the playback waveform at the head tip h1, and the period t2 to t3 is the waveform after the head. The end h2 is considered to be a p-regeneration waveform.
このように、′波長λ=L/n(LHヘッド幅、n:自
然数)であ本信号の再生において、第2図(b)に示し
たように連続波では再生出力は得られないが、第3図の
如くバースト状に記録することによって再生が可能とな
る。In this way, when reproducing this signal at wavelength λ=L/n (LH head width, n: natural number), as shown in FIG. 2(b), no reproduction output can be obtained with continuous waves; Reproduction is possible by recording in bursts as shown in FIG.
再生出力として、第4図のt、〜t2間IC4られる波
形を用いてもよく、t2〜t3間に得られる波形金柑い
てもよく、また両方の波形を合成して得ることもできる
。この合成方法の一例を簡単Vこ述べS0第5図(a)
は再生波形、(b)はヘッド先端で再生された信号波形
、(0)は(b)を再生ヘッドがテープ上を相対的に距
離り移動する時間T1だけ遅延させた波形、(d−1は
(C)の位相を反転させた波形、モして(e)f″i再
生波形と(d)の波形を重ねあわせたことにより得らl
しる波形を示しており、明らかにSハ比が6dB向上す
る。As the reproduced output, the waveform obtained by IC4 between t and t2 in FIG. 4 may be used, the waveform obtained between t2 and t3 may be used, or both waveforms may be synthesized. An example of this synthesis method is briefly described below in Figure 5 (a).
is a reproduced waveform, (b) is a signal waveform reproduced at the tip of the head, (0) is a waveform obtained by delaying (b) by a time T1 during which the reproduction head moves a relative distance on the tape, (d-1 is a waveform obtained by inverting the phase of (C), and is obtained by superimposing (e) f″i reproduced waveform and (d) waveform.
It is clear that the S/C ratio is improved by 6 dB.
この合成方法を実玩するための回路ブロック図を第6図
に示す。回路はアンプ(8)、アナログスイッチ(SW
’l ) (SW2 )、遅延回路(5)、位相反転回
路(6)、ミックス回路(7)から構成されている。第
4図で示したt1〜t2間はスイッチ(EIW2)がO
NL、t2〜t5間はスイッチ(SWI )がONする
。スイッチ(SW2)を通った信号すなわちヘッド先端
部で検出きれた信号は前記遅延回路(5)で前記時間T
、遅延させられ、位相反転回路(6)で位相反転した後
ミックス回路(7)へ送られる。このミックス回路(7
)では、上記信号とスイッチ(SWI )を通った信号
は同波形になっており、加算することによりEl/Nを
6dB向上することができる。A circuit block diagram for experimenting with this synthesis method is shown in FIG. The circuit consists of an amplifier (8), an analog switch (SW
'l) (SW2), a delay circuit (5), a phase inversion circuit (6), and a mix circuit (7). Between t1 and t2 shown in Fig. 4, the switch (EIW2) is turned off.
NL, the switch (SWI) is turned on between t2 and t5. The signal that has passed through the switch (SW2), that is, the signal that has been detected at the tip of the head, is sent to the delay circuit (5) for the time T.
, is delayed, phase inverted by a phase inversion circuit (6), and then sent to a mix circuit (7). This mix circuit (7
), the above signal and the signal passing through the switch (SWI) have the same waveform, and by adding them together, El/N can be improved by 6 dB.
ここで、上記記録再生方式では、従来長手方向における
記録減磁、再生時におけるギャップロスが発生しないた
め、短波長記録再生が可能となる。Here, in the above-mentioned recording and reproducing method, recording demagnetization in the longitudinal direction and gap loss during reproduction do not occur conventionally, so short wavelength recording and reproduction is possible.
、そこで、次に短波長記録再生の一例を示す。第7図は
、ヘッド幅L=5μとして、波長1μのdピ録再生の例
を示したものである。(a)は記録時の状態、(1))
は慶生状態、(C)は再生波形、(d)は前記ミックス
回路を用いてS/IJを向上きせた場合の出力波形を示
している。すなわち、バースト状に記録することにより
ヘッド幅に関係なく、短波長記録再生が可能であること
がわかる。, Therefore, next, an example of short wavelength recording and reproduction will be shown. FIG. 7 shows an example of d-pi recording and reproduction at a wavelength of 1 μm with a head width L=5 μm. (a) is the state at the time of recording, (1))
(C) shows the reproduced waveform, and (d) shows the output waveform when the S/IJ is improved using the mix circuit. In other words, it can be seen that by recording in bursts, short wavelength recording and reproduction is possible regardless of the head width.
ここで、記録する区間は再生ヘッド幅りによって決定賂
れ、記録ヘッド幅には何ら関係しないため、記録ヘッド
幅がLである必要はない。まだヘッド幅りを有する記録
再生ヘッドを使用するようにしてもよい。Here, the recording section is determined by the reproduction head width and has no relation to the recording head width, so the recording head width does not need to be L. It is also possible to use a recording/reproducing head having a wider head width.
このように、従来のトランスバース記録において、再生
ヘッド幅りとするとλ−=L/n (nは自然数)なる
波長をもつ信号は再生できなかったが、以上述べてきた
ように、記録ヘッドが記録媒体上を多くとも距離L(再
生ヘッドIIQiI)を移動する間だけ記録し、次の少
なくとも距離り移動する間記録を停止する、いわゆるバ
ースト状に記録することVCより、再生時においてギャ
ップロスを発生せず、短波長記録帰生が”J曲となる。In this way, in conventional transverse recording, it was not possible to reproduce a signal with a wavelength of λ-=L/n (n is a natural number) when the width of the reproducing head was taken. Recording is performed only while moving at most a distance L (playback head IIQiI) on the recording medium, and then recording is stopped while moving for at least the next distance, so-called burst recording. VC is used to reduce gap loss during playback. This does not occur, and the short wavelength recording returns to "J".
また再生出力としては、再生ヘッド先端部分による再生
信号、つまり信号が書生きれ始めてから門生ヘッドが記
録媒体上を相対的に多くとも距離り移動する間に得られ
た情報を用いてもよく、また再生ヘッド後端部分による
再生信号、つまり信号が再生ぜれ始めてから再生ヘッド
が記録媒体上を相対的に距離り移動した後より得られる
情報を用いてもよく、また上記両方の情報を用いてもよ
い○
ま、化上記説明では、アナログ1ぎ号の記録再生の例を
示したが、本発明は原理的にディジタル記録丹生vc適
しており、その場合ディジタル信号2ビツト長が本H9
e明で述べた1波長に相当すると考えてよい。Further, as the reproduction output, a reproduction signal from the tip of the reproduction head, that is, information obtained while the reproduction head moves relatively at most a distance on the recording medium after the signal begins to be written may be used. It is also possible to use the reproduction signal from the rear end of the reproduction head, that is, the information obtained after the reproduction head has moved a relative distance on the recording medium after the signal begins to be reproduced, or the information obtained from both of the above information may be used. In the above explanation, an example of analog 1-digit recording and reproduction was shown, but the present invention is in principle suitable for digital recording, and in that case, the 2-bit length of the digital signal is
It can be considered that this corresponds to one wavelength mentioned in section e.
発明の効果
以上の説明で明らかなように本発明によれば、トランス
バース記録であるので、記録の際に記録幅値が発生せず
、また再生においてもギャップロスを発生しないため、
記録再生密度は飛躍的に向上する大きな利点を廟する。Effects of the Invention As is clear from the above explanation, according to the present invention, since transverse recording is performed, no recording width value occurs during recording, and no gap loss occurs during reproduction.
It has the great advantage of dramatically increasing recording and reproducing density.
第1図はトランスバース記録の概念全示す概略斜視図と
裏面図、8g2図はトランスバース再生の概略構成図、
第3図は本発明での再生を示した波形図、第4図は本発
明の再生におけるコア内の磁束と再生出力を示した波形
図、第5図は本発明の再生方法を説明するための図、第
6図は再生方法の一例を示すブロック図、第7図は高密
度記録、再生を示した波形図である。
(1)・・・磁気ヘッド、(2)・・・記録波形、(3
)・・・磁気テープ、(4)・・・コイル、(5)・・
・遅延回路、(6)・・・反転回路、(7)・・・ミッ
クス回路
代理人 森 本 幌 私
用1図
第8図
fL→
Z、 7゜
第4図
第5図
第4図
第7図
(4ン
−(
νλFigure 1 is a schematic perspective view and back view showing the entire concept of transverse recording, Figure 8g2 is a schematic configuration diagram of transverse playback,
Fig. 3 is a waveform diagram showing reproduction in the present invention, Fig. 4 is a waveform diagram showing magnetic flux in the core and reproduction output in reproduction according to the invention, and Fig. 5 is for explaining the reproduction method of the present invention. FIG. 6 is a block diagram showing an example of a reproduction method, and FIG. 7 is a waveform diagram showing high-density recording and reproduction. (1)...Magnetic head, (2)...Recording waveform, (3
)...Magnetic tape, (4)...Coil, (5)...
・Delay circuit, (6)...Inverting circuit, (7)...Mix circuit agent Horo Morimoto Private use 1 Figure 8 fL → Z, 7° Figure 4 Figure 5 Figure 4 Figure 7 Figure (4)
−(
νλ
Claims (1)
する記録媒体を有するトランスバース記録方式の磁気記
録再生装置であって、ヘッド幅りを有する記録再生ヘッ
ドまたは記録ヘッドとヘッド幅りを有する再生ヘッドを
具備し、前記記録再生ヘッドまたは記録ヘッドにより、
記録媒体上を相対的に多くとも距離り移動する区間だけ
信号を記録し、次に前記記録再生ヘッドまたは記録ヘッ
ドが前記記録媒体上を相対的に少なくとも距1@!L移
動する区伺は記録を停止するようVごしたことを特徴と
する磁気記録再生装置。 2、 配録信号の波長は前記記録再生ヘッドまたは再生
ヘッドのヘッド幅りよりも短い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。 へ −磁気ヘッドと、前記磁気ヘッド幅方向に相対的に
移動する記録媒体を有するトランスバース記録方式の磁
気記録再生装置であって、ヘッド幅りを有する再生ヘッ
ドを具備し、多くとも距離りの区間だけ記録され、次の
少なくとも距離りの区間は記録されていない記録媒体を
、前記再生ヘッドにより再生して外生信号を得るように
したことを特徴とする磁気記録再生装置。 4 再生信号は、再生ヘッドが記録媒体上に記録された
信号を再生し始めてから、前記記録媒体上を相対的に多
くとも距離り移動する区間に得られた再生ヘッド出力か
らのみ得ることt特徴とする特?ff請求の範囲第3項
記載の磁気記録再生装置。 5 再生信号は、再生ヘッドがl己録媒体上に記録され
た信号を再生し始めてから、前記記録媒体上を相対的に
距離り移動した地点よりざらに相対的に距#IL移動し
た地点までの区間に得られた再生ヘッド出力からのみ得
ることを特徴とする時計1肯求の範囲第3項記載の磁気
目[シ録丹生装亘。 G 再生18号は、再生ヘッドが記録媒体上に記録さ扛
た信号を再生し始めてから、前記記録媒体上を相対的に
距離り移動する区間に得られた881の信号と、その後
さらに相対的に距離り移動する区間に得られた第2信号
を情報とし1.前記第1の信号を所定時間遅延した後、
前記第2信号S2と合成することにより得ることを特徴
とする特杵請求の範囲第3項記載の磁気記録再生装置。[Scope of Claims] L A transverse recording type magnetic recording/reproducing device having a magnetic head and a recording medium that moves relatively in the width direction of the magnetic head, the recording/reproducing head having a head width or a recording head. A reproducing head having a head width is provided, and the recording/reproducing head or the recording head allows
Signals are recorded over a distance that is relatively at most on the recording medium, and then the recording/reproducing head or the recording head moves on the recording medium relatively at a distance of at least 1@! A magnetic recording and reproducing device characterized in that the length of the L-moving section is V-shaped to stop recording. 2. The magnetic recording/reproducing apparatus according to claim 1, wherein the wavelength of the recording signal is shorter than the head width of the recording/reproducing head or the reproducing head. - A transverse recording type magnetic recording and reproducing device having a magnetic head and a recording medium that moves relatively in the width direction of the magnetic head, comprising a reproducing head having a width of the head and having a distance of at most 1. A magnetic recording and reproducing apparatus characterized in that the reproducing head reproduces a recording medium in which only one section is recorded and the next at least a distance is not recorded to obtain an external signal. 4. The reproduction signal is obtained only from the output of the reproduction head obtained during a period in which the reproduction head moves relatively at most a distance on the recording medium after the reproduction head starts reproducing the signal recorded on the recording medium. Special? ff A magnetic recording and reproducing device according to claim 3. 5. The playback signal is transmitted from the time when the playback head starts playing back the signal recorded on the recording medium to the point where the playback head has roughly moved a distance #IL from the point where the playback head has moved a relative distance on the recording medium. The magnetic eye according to item 3 of the range of the clock 1, characterized in that the magnetic eye is obtained only from the playback head output obtained in the interval. G Reproduction No. 18 refers to the signal 881 obtained during the period in which the reproduction head starts reproducing the signal recorded on the recording medium and moves a relative distance on the recording medium, and then further relatively The second signal obtained during the distance traveled is used as information 1. After delaying the first signal for a predetermined time,
4. The magnetic recording and reproducing apparatus according to claim 3, wherein the magnetic recording and reproducing apparatus is obtained by combining with the second signal S2.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP57140545A JPS5930208A (en) | 1982-08-12 | 1982-08-12 | magnetic recording and reproducing device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP57140545A JPS5930208A (en) | 1982-08-12 | 1982-08-12 | magnetic recording and reproducing device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5930208A true JPS5930208A (en) | 1984-02-17 |
| JPH0258682B2 JPH0258682B2 (en) | 1990-12-10 |
Family
ID=15271162
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP57140545A Granted JPS5930208A (en) | 1982-08-12 | 1982-08-12 | magnetic recording and reproducing device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5930208A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH01230605A (en) * | 1988-03-11 | 1989-09-14 | Hitachi Chem Co Ltd | Method and apparatus for production of coagulated resin |
-
1982
- 1982-08-12 JP JP57140545A patent/JPS5930208A/en active Granted
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH01230605A (en) * | 1988-03-11 | 1989-09-14 | Hitachi Chem Co Ltd | Method and apparatus for production of coagulated resin |
Also Published As
| Publication number | Publication date |
|---|---|
| JPH0258682B2 (en) | 1990-12-10 |
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