JPS6348604A - Erasing method for magnetic record - Google Patents
Erasing method for magnetic recordInfo
- Publication number
- JPS6348604A JPS6348604A JP19060986A JP19060986A JPS6348604A JP S6348604 A JPS6348604 A JP S6348604A JP 19060986 A JP19060986 A JP 19060986A JP 19060986 A JP19060986 A JP 19060986A JP S6348604 A JPS6348604 A JP S6348604A
- Authority
- JP
- Japan
- Prior art keywords
- erasure
- signal
- current
- magnetic head
- level
- 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
- 238000000034 method Methods 0.000 title claims description 17
- 230000007423 decrease Effects 0.000 claims abstract description 9
- 229920006395 saturated elastomer Polymers 0.000 abstract description 2
- 238000010586 diagram Methods 0.000 description 7
- 230000010355 oscillation Effects 0.000 description 6
- 238000001228 spectrum Methods 0.000 description 4
- 230000000694 effects Effects 0.000 description 2
- 230000003247 decreasing effect Effects 0.000 description 1
- 239000010410 layer Substances 0.000 description 1
- 239000004576 sand Substances 0.000 description 1
- 239000002344 surface layer Substances 0.000 description 1
Landscapes
- Digital Magnetic Recording (AREA)
Abstract
Description
【発明の詳細な説明】
〈産業上の利用分野〉
本発明は磁気記録における消去方7人に関し、映像信号
の周波数帯域内に消去信号が残留することがなく良好な
消去をなくし得るよう工夫したものである。[Detailed Description of the Invention] <Industrial Application Field> The present invention relates to seven methods of erasing in magnetic recording, and is devised to eliminate good erasure without leaving any erasure signal within the frequency band of the video signal. It is something.
〈従来の技術〉
映像信号のiH磁気記録特に電rスチルカメラシステム
てのフロッピーディスクを磁気記録媒体とする磁気記録
における1トラツク消去方法としては、従来より種々の
技i41か提案されている。これら一方法としてスイー
プ消去方法と呼称されるものかある。スイープ消去方法
とは、最初に、映像信号の帯域内の周波数(例えば6M
1lz)の消去信号を、既に映像信号が書き込まれてい
る磁気記録媒体、例えば−気ディスクのトラックに、外
き込み、この消去信号の周波数を連続的に上げなから同
様の書き込みを、繰り返し・、最終的に消去13号の周
波数を映像信号の帯域外にもっていくというものである
。このスィーブ7肖去方法により、トラックに古き込ま
わた消去(2r渇の周波数は、最終的には、映像イ、j
号の帯域外のものとなるため、再生時にフィルタて容鴇
にカットすることかでき、必要な映像44 ”jのみを
再生することができる。即ち、周波数の異なる多くの消
去信号を、元の映像信号を書き込んだトラックに重ねδ
きすることにより実質的に元の映像信号を消去している
。このとき磁気記録媒体の深層は相対的に低周波数の消
去信号で、また表層は相対的に高周波数の消去信号で夫
々消去される。<Prior Art> Various techniques have been proposed in the past as methods for erasing one track in iH magnetic recording of video signals, particularly in magnetic recording using a floppy disk as a magnetic recording medium in an electric still camera system. One of these methods is called a sweep erase method. The sweep cancellation method is to first erase a frequency within the video signal band (for example, 6M
1lz) is written onto a track of a magnetic recording medium on which a video signal has already been written, such as a magnetic disk, and the frequency of this erasing signal is increased continuously, and the same writing is repeated. , the frequency of erasure No. 13 is finally brought out of the band of the video signal. By this sweep method, the track is erased (the frequency of 2r
Since it is out of the signal band, it can be cut by a filter during playback, and only the necessary video can be played back.In other words, many erasing signals with different frequencies can be removed from the original signal. Overlap the track on which the video signal is written δ
By doing so, the original video signal is essentially erased. At this time, the deep layer of the magnetic recording medium is erased with a relatively low frequency erase signal, and the surface layer is erased with a relatively high frequency erase signal.
〈発明か解決しようとする問題点〉
ところが、上記従来技術に係るスィーブ消去方法では、
消去時間を短かくした場合(例えば2秒以下)、映像信
号の周波数帯域内にも消去17号そのものが大きなレベ
ルで残留するとともに、バルク・イレーザで消去したも
のよりノイズレベルか大きいという問題があった。<Problem to be solved by the invention> However, in the sweep erasing method according to the above-mentioned prior art,
When the erasing time is shortened (for example, 2 seconds or less), there is a problem that the erasure No. 17 itself remains at a large level within the frequency band of the video signal, and the noise level is higher than that erased by the bulk eraser. Ta.
本発明は、上記従来技術の欠点に鑑み、映像信号の周波
数帯域内には消去信号は残留させないようにするととも
に、消去後の全帯域に■るノイズ・レベルをバルク・イ
レーズ消去程度にまで下げることができる磁気記録にお
ける消去方法を提供することを目的とする。In view of the above drawbacks of the prior art, the present invention prevents the erased signal from remaining within the frequency band of the video signal, and lowers the noise level in the entire band after erasing to the level of bulk erase erase. The purpose of the present invention is to provide an erasing method in magnetic recording that can be performed.
〈間逆点を解決するだめの手段〉
上記目的を達成する本発明の構成は、回転磁気記録媒体
のトラックに磁気ヘッドにより書き込まれた映像信号を
消去する方法であって、
消去すべきトラック上を前記磁気ヘッドて走査させると
ともに、周波数が前記映像信号の記録帯域周波数よりも
高く日、つ振幅レベルが磁気ヘッドの最適記録電流レベ
ルよりも大きい初期振幅レベルからa減していく消去電
流を、前記磁気ヘッドに流すことを特徴とする。<Means to Solve the Interval Reversal> The structure of the present invention that achieves the above object is a method for erasing a video signal written by a magnetic head on a track of a rotating magnetic recording medium, which comprises: is scanned by the magnetic head, and an erase current whose frequency is higher than the recording band frequency of the video signal and whose amplitude level is higher than the optimum recording current level of the magnetic head decreases from an initial amplitude level, It is characterized in that it is caused to flow through the magnetic head.
〈作 用〉
映像信号は消去信号により消去され、また消去信号自身
は、映像45号の記録帯域外でほとんど消滅する。<Operation> The video signal is erased by the erasure signal, and the erasure signal itself almost disappears outside the recording band of Video No. 45.
く実 施 例〉
以下本発明の実施例を図面に基づき詳細に説明する。第
1図は本発明の実施例を実現する711去装置を示すブ
ロック図である。Embodiments Hereinafter, embodiments of the present invention will be described in detail based on the drawings. FIG. 1 is a block diagram illustrating a 711 apparatus implementing an embodiment of the present invention.
同図において、1は発振器、2は減衰回路、3は記録ア
ンプ、4は磁気ヘッド、5は磁気記録媒体であるフロッ
ピーディスク、6は制御回路である。このうち発振器1
は、制御回路6から発振制御信号S、を受けると発振し
、正弦波である発振信号S2を出力する。この発振信号
S2の周波数は、映像信号の記録帯域周波数(約0〜1
2Mtlz)よりも高く、具体的には 14MHzにし
ている。減衰回路2は前記発振信号S2をI!l減させ
て′a減発派信号S3を得る。この場合、Wk減全発振
信号S3レベルが充分小さくなる迄の時間、即ち減衰時
間はフロッピーディスク5の回転数との関係において定
めれば良く、1760秒で1回転するスチルカメラシス
テムのフロッピーディスク5では、60回回転度が適切
である。記録アンプ3は、制御回路6の記録制御信号S
4により作動し、漸バ発振信号S3を増幅して消去電流
Iを得る。この消去電流Iの初期振幅レベルは磁気ヘッ
ド4の最適記録電流よりも大きくしている。本例では消
去電流Iの初期振幅レベルを100mA p−pに設定
して、磁気ヘッド4の最適記録電流値80mA P−P
の25%増にしている。なお最適記録電流とは、電子ス
チルカメラ用磁気ディスクの場合では、その規、格に定
められているように、記録される信号のスペクトルが7
MHz近傍をピークとして分布しているので、実用的
には7 MHzの周波数で記録したときにその再生出力
が最大となるような値の記録電流をいう。結局、周波数
か映像信号の記録帯域周波数よりも高く、且つ、振幅が
磁気ヘッド4の最適記録電流レベルよりも大きい初期振
幅レベルから漸減していく消去電流Iを、磁気ヘッド4
に流す。In the figure, 1 is an oscillator, 2 is an attenuation circuit, 3 is a recording amplifier, 4 is a magnetic head, 5 is a floppy disk which is a magnetic recording medium, and 6 is a control circuit. Of these, oscillator 1
receives the oscillation control signal S from the control circuit 6, oscillates, and outputs an oscillation signal S2 which is a sine wave. The frequency of this oscillation signal S2 is the recording band frequency of the video signal (approximately 0 to 1
2Mtlz), specifically 14MHz. The attenuation circuit 2 converts the oscillation signal S2 into I! l is decreased to obtain 'a reduction signal S3. In this case, the time required for the level of the Wk reduced total oscillation signal S3 to become sufficiently small, that is, the decay time, may be determined in relation to the rotational speed of the floppy disk 5. In this case, 60 degrees of rotation is appropriate. The recording amplifier 3 receives the recording control signal S from the control circuit 6.
4, the erase current I is obtained by amplifying the gradual oscillation signal S3. The initial amplitude level of this erase current I is set larger than the optimum recording current of the magnetic head 4. In this example, the initial amplitude level of the erase current I is set to 100 mA p-p, and the optimum recording current value of the magnetic head 4 is 80 mA p-p.
This is an increase of 25%. In the case of magnetic disks for electronic still cameras, the optimum recording current means that the spectrum of the recorded signal is 7.
Since it is distributed with a peak near MHz, in practical terms it refers to the recording current of a value that maximizes the reproduction output when recording at a frequency of 7 MHz. As a result, the erasing current I, which gradually decreases from an initial amplitude level whose frequency is higher than the recording band frequency of the video signal and whose amplitude is larger than the optimum recording current level of the magnetic head 4, is applied to the magnetic head 4.
flow to.
次に、かかる装置を用いた本発明方法を説明する。例え
ば、フロッピーディスク5のトラック5aに磁気ヘッド
4により記録した映像信号を消去するには、フロッピー
ディスク5を回転させてトラック5a上を磁気ヘッド4
て走査させるとともに、磁気ヘッド4に消去電流Iを流
′4−5そうすると、711去′1コ流■の初期振幅レ
ベルか大きいので消去′π流Iによりトラック5aか磁
気飽和し、映像信号が消されてその残留レベルはバルク
・イレーズ消去と同程度までtがる。また、消去電流I
の振幅は漸減していくためトラック5aにおける、消去
電流Iによる消去信号の残留レベルも漸減する。減衰時
間Tを1秒以上にすれば消去信号の残留レベルは更に低
下して問題にならないレベルになる。更に消去信号が残
留したとしても、その周波数は映像信号の記録帯域周波
数よりも高いので、通常は再書込した信号により新しい
スペクトルに書き換えられてしまうので問題はない。Next, a method of the present invention using such an apparatus will be explained. For example, in order to erase a video signal recorded by the magnetic head 4 on the track 5a of the floppy disk 5, the floppy disk 5 is rotated and the magnetic head 4 moves over the track 5a.
At the same time, the erasing current I is applied to the magnetic head 4. Since the initial amplitude level of 711 is large, the track 5a is magnetically saturated by the erasing current I, and the video signal is After erasing, the residual level drops to the same level as bulk erase. Also, the erase current I
Since the amplitude of the erase signal gradually decreases, the residual level of the erase signal caused by the erase current I in the track 5a also gradually decreases. If the decay time T is set to 1 second or more, the residual level of the erased signal is further reduced to a level that does not pose a problem. Furthermore, even if the erased signal remains, since its frequency is higher than the recording band frequency of the video signal, it is normally rewritten to a new spectrum by the rewritten signal, so there is no problem.
次に第1図に示す装置により行なった各種実験のデータ
を示す。なお、消去すべきトラック5aには、80mA
I)−pで7M11zの単一周波数及びこの信号レベ
ルに対し一17dBレベルの1.25MIIzの単一周
波数の信″−′i電流を流して、消去率′、qの評価実
りに使うための模擬的映像イ言号か記録されている。Next, data of various experiments conducted using the apparatus shown in FIG. 1 will be shown. Note that the track 5a to be erased has a power of 80 mA.
I) A single frequency signal of 7M11z at -p and a single frequency signal of 1.25MIIz at a level of -17 dB with respect to this signal level '-'i is applied to evaluate the erasure rate', q. A simulated video of the words was recorded.
第2図、第3図及び第4図は、消去率:A Iのイ直か
60+n八p−p、 80mA p−p、 !00mA
p−pであるときに消去電流■の減Q時間を15秒。Figures 2, 3, and 4 show the erasure rate: AI 60+n8p-p, 80mA p-p, ! 00mA
When p-p, the reduction Q time of the erase current (■) is 15 seconds.
10秒、0.5秒と変えるとともに消去?:L流Iの周
波数を変えた場合における輝度イ5写fYの消去率を示
す。これらの図から、ハ衰時間が長く、周波数か高く、
消去電流値が太きいぼと消去率が大きく、特に消去電流
値が消去率に大きく影Δを与えることか理解される。Change it to 10 seconds or 0.5 seconds and delete it? : Shows the erasure rate of luminance A5 fY when the frequency of L flow I is changed. From these figures, it can be seen that the decay time is long, the frequency is high,
It is understood that the erase rate is large for warts with a thick erase current value, and that the erase current value in particular has a large influence Δ on the erase rate.
即ち、消去電流値が60mA p−pでは消失率か−3
0dB前後であるが80mA p−p以上にすると−5
0dl]以−Lの消去性能か得られる。また100mA
p−pて 目Mllzにするとほぼバルク・・rレー
ズレベル(−60dB)になる。That is, when the erase current value is 60 mA p-p, the erasure rate is -3
It's around 0dB, but when it's over 80mA p-p -5
0dl] or more -L erasing performance can be obtained. Also 100mA
If you set it to Mllz from pp to m, it becomes almost the bulk...r laser level (-60dB).
′f25図、第6図及び第7図は、消去電流Iのイ直か
50mA p−p、 80ffl八p−p、 100m
A p−pであるときに消失電流Iの減衰時間を 1.
5秒。Figures 'f25, 6 and 7 show the erase current I of 50mA p-p, 80ffl8p-p, 100m
The decay time of the dissipation current I when A pp is 1.
5 seconds.
1.0秒、0.5砂と変えるとともに消去電流■の周波
数を変えた場合における色信号f、、の消去率を示す。The erasing rate of the color signal f is shown when changing the frequency of the erasing current (2) to 1.0 seconds, 0.5 sand, and changing the frequency of the erasing current (2).
これらの図から、上記輝度信号の消去と同様に、消去電
流値の影響が最大であることか理解される。即ち、消去
電流値が60m八pへpテは一10dBii7r?、4
.80m八pへpテハー20〜−25d[l程度、l0
0iA 1pでは一40dBH*となる。From these figures, it can be seen that the effect of the erase current value is the greatest, similar to the above-mentioned erasure of the luminance signal. That is, the erase current value is 60m8p and pte is -10dBii7r? , 4
.. 80m 8p to p Teher 20~-25d [about l, l0
At 0iA 1p, it becomes -40dBH*.
第8図、第9図及び第1o図は単一スペクトル以外の残
留レベルを示す。こゎらの図がら次のことかわかる。つ
まり、電流依存性については、60[11A p−p″
Cは残留レベルは小ざくならないか、80mΔp−p、
+00+nA p−p テハP]シ、J−うな傾向を
示して残留レベルが小さくなる。Figures 8, 9 and 1o show residual levels other than a single spectrum. From these diagrams, you can understand the following. In other words, the current dependence is 60[11A p-p''
C: Does the residual level become small? 80mΔp-p,
+00+nA p-p TEHAP] し、J- The residual level becomes smaller.
周波数依存性は周波数が高くなるほど残留レベルは小さ
くなる。減衰時間依荏性は0.5秒 くでは残留レベル
が大きく、 1.0秒、1.5秒では残留レベルか小さ
くなる。Regarding frequency dependence, the higher the frequency, the lower the residual level. The dependence on the decay time is that the residual level is large at 0.5 seconds, and becomes small at 1.0 seconds and 1.5 seconds.
次にS/N比についてバルク・イレーズと本発明方法と
を次表に比較して示す。本発明方法では 14MHz、
+00mA p−p 、の消去”j+ r<iを1.
0秒減衰させた。Next, the following table shows a comparison of the S/N ratio between bulk erase and the method of the present invention. In the method of the present invention, 14MHz,
+00mA p-p, erasure of "j+ r<i 1.
Decayed for 0 seconds.
表 (S/N比、単位dB)
以上より、本発明方法によれば、バルク・イレーズなみ
の消去かできることが確認できた。Table (S/N ratio, unit dB) From the above, it was confirmed that according to the method of the present invention, erasing comparable to bulk erasing can be achieved.
〈発明の効果〉
以上実施例とともに具体的に説明したように、本発明に
よりば映像信潟の周波数帯域内の信号をバルク・イレー
ズを行なった場合と同程度に良好に消去しく11る。<Effects of the Invention> As specifically explained above in conjunction with the embodiments, according to the present invention, signals within the video signal frequency band can be erased as well as when bulk erasing is performed.
第1図は本発明の方光を実現する装置を示すブロック図
、第2図〜第4図は輝度(iE号の消去率を示すデータ
図、第5〜第7図は色信号の消去ヰ(を示すデータ図、
第8図〜第10し1は中−−−スペクトル以外の残留レ
ベルを示すテータ図である。
図面中、
1ば発振器、
2は舐衰回路、
3は記録アじブ、
4は磁気ヘッド、
5はフロッピーディスク、
6は制御回路、
1は1肖去電流である。Figure 1 is a block diagram showing a device for realizing the direction lighting of the present invention, Figures 2 to 4 are data diagrams showing the erasure rate of luminance (iE), and Figures 5 to 7 are data diagrams showing the erasure rate of color signals. (data diagram showing
FIGS. 8 to 10-1 are theta diagrams showing residual levels other than the middle spectrum. In the drawing, 1 is an oscillator, 2 is a decay circuit, 3 is a recording head, 4 is a magnetic head, 5 is a floppy disk, 6 is a control circuit, and 1 is a decay current.
Claims (1)
まれた映像信号を消去する方法であって、 消去すべきトラック上を前記磁気ヘッドで走査させると
ともに、周波数が前記映像信号の記録帯域周波数よりも
高く且つ振幅レベルが磁気ヘッドの最適記録電流レベル
よりも大きい初期振幅レベルから漸減していく消去電流
を、前記磁気ヘッドに流すことを特徴とする磁気記録に
おける消去方法。[Claims] A method for erasing a video signal written by a magnetic head on a track of a rotating magnetic recording medium, comprising: scanning the track to be erased with the magnetic head, and adjusting the frequency of the recording of the video signal. An erasing method in magnetic recording, characterized in that an erasing current that gradually decreases from an initial amplitude level higher than a band frequency and larger than an optimum recording current level of the magnetic head is passed through the magnetic head.
Priority Applications (2)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP19060986A JPS6348604A (en) | 1986-08-15 | 1986-08-15 | Erasing method for magnetic record |
| US07/085,648 US4851936A (en) | 1986-08-15 | 1987-08-14 | Erasing method for erasing information corrected on a magnetic recording medium |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP19060986A JPS6348604A (en) | 1986-08-15 | 1986-08-15 | Erasing method for magnetic record |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPS6348604A true JPS6348604A (en) | 1988-03-01 |
Family
ID=16260916
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP19060986A Pending JPS6348604A (en) | 1986-08-15 | 1986-08-15 | Erasing method for magnetic record |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6348604A (en) |
-
1986
- 1986-08-15 JP JP19060986A patent/JPS6348604A/en active Pending
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| JPH0441406B2 (en) | ||
| JPS6113404A (en) | Magnetic recording green reproducing device | |
| US4851936A (en) | Erasing method for erasing information corrected on a magnetic recording medium | |
| JP2508884B2 (en) | Magnetic recording / reproducing device | |
| JPS62243101A (en) | Erasing system in magnetic recording | |
| JPS6320703A (en) | Erasion system for magnetic recording | |
| JP3203155B2 (en) | Magnetic recording / reproducing device | |
| JPS6040505A (en) | Magnetic recording and reproducing device | |
| JPS62243102A (en) | Erasing system in magnetic recording | |
| JPS6338765B2 (en) | ||
| JPS60185207A (en) | Video signal erasing device | |
| JPH03157802A (en) | Magnetic recording system | |
| JP3013828B2 (en) | Digital signal recording method | |
| JPS6139784A (en) | Magnetic recording and reproducing method | |
| JP2559457B2 (en) | Digital recording / playback device | |
| JPH0425601B2 (en) | ||
| JPS61902A (en) | Erasing system of magnetic disk | |
| JPH0731776B2 (en) | Digital signal recording method | |
| JPS6025006A (en) | Magnetic recording erasure system | |
| JPS62243103A (en) | Erasing system in magnetic recording | |
| JPS6083203A (en) | Erasing device for magnetic recording information | |
| JPH052701A (en) | Magnetic recording and reproducing device | |
| JPS59142706A (en) | Record erasing method and device | |
| JPH0743808B2 (en) | Erasing method in magnetic recording | |
| JPS61192002A (en) | magnetic recording and reproducing device |