JPH0210504A - Magnetic recording method for angle modulating signal - Google Patents
Magnetic recording method for angle modulating signalInfo
- Publication number
- JPH0210504A JPH0210504A JP63160058A JP16005888A JPH0210504A JP H0210504 A JPH0210504 A JP H0210504A JP 63160058 A JP63160058 A JP 63160058A JP 16005888 A JP16005888 A JP 16005888A JP H0210504 A JPH0210504 A JP H0210504A
- Authority
- JP
- Japan
- Prior art keywords
- signal
- period
- frequency
- recording
- supplied
- 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.)
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Abstract
Description
【発明の詳細な説明】
産業上の利用分野
本発明は角度変調信号を磁気記録媒体上に記録する際の
記録方法に関するもので、特に映像信号を周波数変調し
て記録するビデオテープレコーダ及び磁気ディスク等の
装置に適した記録方法に関する。Detailed Description of the Invention Field of the Invention The present invention relates to a recording method for recording angle modulated signals on a magnetic recording medium, and in particular to a video tape recorder and a magnetic disk that frequency modulate and record video signals. This document relates to a recording method suitable for such devices.
従来の技術
映像信号を周波数を変調して記録、再生するビデオテー
プレコーダなどでは、再生信号中に不要成分が混入し、
画面上にモワレ現象が起る場合がある。この主な要因と
しては、(1)記録される周波数変調信号中に下側帯波
がゼロ周波数で折シ返って不要スプリアスとなシ使用帯
域内に混入する場合、(2)周波数変調器がマルチバイ
ブレータなどの方形波発振器であシ、搬送波の第3高調
波からの下側帯波が使用帯域内に混入する場合、((9
)電磁変換系の非直線歪により不要成分が発生し使用帯
域内に混入する場合、(4) F M復調器がパルスカ
ウント形2逓倍復調器であシ、周波数変調信号の2逓倍
波の有する下側帯波が復調帯域内に混入する場合などが
知られている。Conventional technology: In video tape recorders and other devices that record and play back video signals by frequency modulating them, unnecessary components are mixed into the playback signal.
A moiré phenomenon may occur on the screen. The main reasons for this are (1) when lower sideband waves are folded back at zero frequency in the recorded frequency modulated signal and mixed into the used band as unnecessary spurious signals; (2) when the frequency modulator is With a square wave oscillator such as a vibrator, if the lower sideband from the third harmonic of the carrier wave mixes into the used band, ((9
) If unnecessary components are generated due to non-linear distortion in the electromagnetic conversion system and mixed into the used band, (4) The FM demodulator is a pulse count type doubler demodulator, and the frequency modulation signal has a double wave. It is known that lower sideband waves mix into the demodulation band.
本発明はこれらの主なモワレ発生要因のうち2と3に関
するものであるため、これらについてさらに詳しく説明
する。まず搬送波が方形波の場合の不要スプリアスの発
生について説明する。搬送波が方形波の場合、第3高調
波成分の振幅は基本波成分に対し3分の1であるが第3
高調波成分も周波数変調され、その変調指数は基本波の
変調指数の3倍となるため側帯波の振幅は比較的大きく
なる。−例として、搬送波周波数fCを6 、sMHz
変調信号周波数f。を3 、OMHz、変調指数を0.
7とした場合の主な周波数スペクトルを第6図に示す。Since the present invention relates to 2 and 3 of these main causes of moiré, these will be explained in more detail. First, the occurrence of unnecessary spurious when the carrier wave is a square wave will be explained. When the carrier wave is a square wave, the amplitude of the third harmonic component is one-third that of the fundamental wave component, but
The harmonic components are also frequency modulated, and the modulation index is three times the modulation index of the fundamental wave, so the amplitude of the sideband is relatively large. - As an example, if the carrier frequency fC is 6, sMHz
Modulating signal frequency f. 3, OMHz, modulation index 0.
7 shows the main frequency spectrum in FIG.
O〜4.5MHzの映像信号を記録する場合第5図から
れかるように使用帯域に混入する不要成分は、第3高調
波の下側帯波である3fC−3frn成分と3 fo−
4fm成分、及び基本波の下側帯波がゼロ周波数で折返
ったfC−3fm成分である。When recording a video signal of 0 to 4.5 MHz, as shown in Figure 5, the unnecessary components that mix into the used band are the 3fC-3frn component, which is the lower sideband of the third harmonic, and the 3fo-
4fm component and the fC-3fm component in which the lower sideband wave of the fundamental wave is folded back at zero frequency.
また、第3高調波の下側帯波成分が折返し成分よシ振輻
が大きくなっている。Further, the lower sideband component of the third harmonic has a larger vibration than the folded component.
次に電磁変換系で発生する歪と不要スプリアスについて
説明する。記録信号波形と残留磁化波形との関係は、基
本的には「磁気記録技術筒3券P177日本工業技術セ
ンター昭和56年6月3o日発行」などの文献に記載さ
れているようにS字形の初期磁化曲線に類似したものに
なると考えられているので、正弦波と方形波とを飽和記
録した場合の残留磁化波形は第6図と第7図に示すよう
にほぼ等しくどちらも方形波状の残留磁化波形となる。Next, distortion and unnecessary spurious generated in the electromagnetic conversion system will be explained. The relationship between the recording signal waveform and the residual magnetization waveform is basically an S-shaped one, as described in documents such as "Magnetic Recording Technology Tube 3, P177, Japan Industrial Technology Center, published June 3, 1982." Since it is thought that the initial magnetization curve will be similar to the initial magnetization curve, the residual magnetization waveforms when saturated recording of a sine wave and a square wave are almost equal, as shown in Figures 6 and 7, and both have square wave-like residuals. It becomes a magnetization waveform.
したがって飽和記録を行うビデオテープレコーダなどで
は、周波数変調信号の搬送波が正弦波であっても搬送波
が方形波の周波数変調信号を記録したこととほぼ等しく
第3高調波の下側帯波が使用帯域内に混入して記録され
、また再生されることになる。Therefore, in a video tape recorder that performs saturation recording, even if the carrier wave of the frequency modulated signal is a sine wave, the lower side band of the third harmonic is within the used band, which is almost equivalent to recording a frequency modulated signal whose carrier wave is a square wave. It will be recorded and played back again.
発明が解決しようとする課題
以上のように、FM信号は飽和記録されるため、搬送波
が正弦波であっても方形波を記録したものと同様になシ
、3次高調波からのモワレが使用帯域内に混入する。Problems to be Solved by the Invention As mentioned above, since FM signals are recorded in saturation, even if the carrier wave is a sine wave, it is the same as recording a square wave, and moiré from the third harmonic is used. mixed into the band.
本発明は上記モワレの発生要因のうち周波数変調器及び
電磁変換系で発生する周波数変調信号の第3高調波の下
側波成分が使用帯域内に混入して起るものについて、こ
の不要成分の発生を軽減することを目的とする。The present invention deals with the cause of moiré caused by the lower side wave component of the third harmonic of the frequency modulation signal generated in the frequency modulator and electromagnetic conversion system mixed into the usage band. The aim is to reduce the occurrence of
課題を解決するための手段
期間のレベルがo、旦T−T期間のレベルが−Aとなる
信号を搬送波とし、この搬送波を入力信号で角度変調し
て磁気記録媒体上に記録するものである。Means for Solving the Problem A signal whose level is o during the period and -A during the T-T period is used as a carrier wave, and this carrier wave is angularly modulated by an input signal and recorded on a magnetic recording medium. .
作 用
したがって、本発明における記録される周波数変調信号
の搬送波波形は第1図に示されるものであり、この波形
y (t)を、フーリエ展開して各周波数成分に分解し
式で表わすと(1)式となる。Function Therefore, the carrier waveform of the frequency modulated signal recorded in the present invention is shown in FIG. 1) Equation becomes.
Aは振幅、ωは角周波数である。A is the amplitude and ω is the angular frequency.
つまり、従来方法において問題となる第3高調波成分が
含まれないものであり、よってこれを搬送波とする周波
数変調信号中には第3高調波とその側帯波成分は含まれ
ない。In other words, the third harmonic component, which is a problem in the conventional method, is not included, and therefore, the frequency modulated signal using this as a carrier wave does not include the third harmonic and its sideband components.
さらに、この搬送波を記録した場合の残留磁化波形は記
録減磁損失及び自己減磁損失がないとすると第2図に示
すととくなジ飽和記録をしても形状は変化せず、したが
って電磁変換系においても搬送波の第3高調波の側帯波
が使用帯域内に混入しにくいものである。Furthermore, when this carrier wave is recorded, the shape of the residual magnetization waveform does not change even if saturated recording is performed, as shown in Figure 2, assuming that there is no recording demagnetization loss or self-demagnetization loss, and therefore the shape does not change due to electromagnetic conversion. In the system as well, sideband waves of the third harmonic of the carrier wave are difficult to mix into the used band.
実施例
以下本発明をビデオテープレコーダに実施した場合の実
施例について説明する。第3図はその映像信号処理部の
ブロック図、第4図は信号波形図である。記録時には、
端子1から入力された映像信号が周波数変調器2へ供給
されて周波数変調され、その出力信号イは1/6分周回
路3へ供給される。1/6分周回路では周波数変調信号
を1/6の周波数に分周し信号口とハに示す互いにco
度位相の異なる2つの方形信号が出力される。これらの
2つの出力信号は加算器4へ供給され振幅比1対1で加
算される。したがって加算器4の出力信号は信号二に示
すように、無変調時の搬送波のベルがA、−〜−丁期間
であるt 期間のレベルがo、−T−T期間であるt
期間のレベルが−八となシすでに説明したように第3高
周波とその側帯波を含まない周波数変調信号となる。加
算器4の出力信号は記録増幅器5へ供給されて増幅され
記録用磁気ヘッド6を介して磁気テープ7に飽和記録さ
れる。Embodiments Hereinafter, embodiments in which the present invention is implemented in a video tape recorder will be described. FIG. 3 is a block diagram of the video signal processing section, and FIG. 4 is a signal waveform diagram. When recording,
A video signal input from a terminal 1 is supplied to a frequency modulator 2 where it is frequency modulated, and its output signal A is supplied to a 1/6 frequency divider circuit 3. In the 1/6 frequency divider circuit, the frequency modulation signal is divided into 1/6 frequency and the signal port and the co
Two square signals having different degrees and phases are output. These two output signals are supplied to an adder 4 and added in an amplitude ratio of 1:1. Therefore, as shown in signal 2, the output signal of the adder 4 is as follows: t when the level of the carrier wave during non-modulation is A, -~-d period, o, and t when the level of the period is o, and -T-T period.
When the level of the period is -8, the frequency modulated signal becomes a frequency modulated signal that does not include the third high frequency and its sideband waves, as described above. The output signal of the adder 4 is supplied to a recording amplifier 5, amplified, and recorded in saturation on a magnetic tape 7 via a recording magnetic head 6.
再生時には磁気テープ7から再生用磁気ヘッド8により
周波数変調信号が再生され、再生増幅器9へ供給されて
増幅される。再生増幅器9の出力信号は再生等価h10
へ供給され再生時の電磁変換による周波数対振幅特性が
補正される。再生等側型1oの出力信号は周波数変換器
11へ供給され、よシ高い周波数変換される。周波数変
換器の出力信号は、リミッタ12へ供給され、振幅変動
が除去されてFM復調器13へ供給されて復調される。During reproduction, a frequency modulated signal is reproduced from the magnetic tape 7 by the reproduction magnetic head 8, and is supplied to the reproduction amplifier 9 and amplified. The output signal of the regenerative amplifier 9 is the regenerative equivalent h10
The frequency versus amplitude characteristics due to electromagnetic conversion during playback are corrected. The output signal of the reproducing isolateral type 1o is supplied to a frequency converter 11, where it is converted to a higher frequency. The output signal of the frequency converter is supplied to a limiter 12, amplitude fluctuations are removed, and the output signal is supplied to an FM demodulator 13 for demodulation.
よって端子14には再生された映像信号が出力される。Therefore, the reproduced video signal is output to the terminal 14.
したがって第3図に示す構成とした場合、加算器4の出
力信号中には搬送波の第3高調波とその調帯波が含まれ
ず、また、記録時の電磁変換系においても第2図を用い
′て説明したように記録信号の波形が保たれてテープ上
に磁化されるため第3高調波とその側帯波の発生が少な
い。よって、磁気ヘッド8によシ再生される周波数変調
信号中にも第3高調波とその側帯波成分は少なく、この
不要成分の少ない周波数変調信号を復調することにより
不要成分の混入が少ない映像信号が再生できる。Therefore, when the configuration shown in FIG. 3 is used, the output signal of the adder 4 does not include the third harmonic of the carrier wave and its harmonic wave, and the electromagnetic conversion system shown in FIG. As explained above, since the waveform of the recording signal is maintained and magnetized on the tape, third harmonics and their sidebands are less likely to occur. Therefore, the third harmonic and its sideband components are also small in the frequency modulated signal reproduced by the magnetic head 8, and by demodulating the frequency modulated signal with fewer unnecessary components, a video signal with less unnecessary components mixed in can be obtained. can be played.
発明の効果
本発明はモワレ成分を低減できるものであるから、ビデ
オテープレコーダに適用すれば不要成分の少ない高品質
の画像が再生できる。また、モワレ成分は変調指数が大
きいほど大きくなるため、本発明の方法を用いれば従来
方法よシ変調指数を大きくしてもよいことになるのでS
/N比を改善できる。Effects of the Invention Since the present invention can reduce moire components, when applied to a video tape recorder, high quality images with less unnecessary components can be reproduced. Furthermore, since the moiré component increases as the modulation index increases, the method of the present invention allows the modulation index to be increased compared to the conventional method.
/N ratio can be improved.
第1図は本発明の磁気記録方法に用いる角度変調信号の
搬送波波形図、第2図は同磁気記録方法における記録信
号波形と残留磁化波形との関係図、第3図は同磁気記録
方法を施したビデオテープレコーダの映像信号処理を示
すブロック図、第4図は第3図における各部の波形図、
第6図は搬送波が方形波である周波数変調信号のスペク
トル、第6図は記録信号が正弦波の場合の残留磁化の説
明図、第7図は記録信号が方形波の場合の残留磁化の説
明図である。
代理人の氏名 弁理士 中 尾 敏 男 ほか1名第1
図
第2図
第
図
第
図
11 浪敗(MHXIFig. 1 is a carrier wave waveform diagram of an angle modulation signal used in the magnetic recording method of the present invention, Fig. 2 is a relationship diagram between the recording signal waveform and residual magnetization waveform in the magnetic recording method, and Fig. 3 is a diagram showing the relationship between the recording signal waveform and the residual magnetization waveform in the magnetic recording method. A block diagram showing the video signal processing of the video tape recorder that has been applied, FIG. 4 is a waveform diagram of each part in FIG. 3,
Figure 6 is a spectrum of a frequency modulated signal whose carrier wave is a square wave. Figure 6 is an illustration of residual magnetization when the recording signal is a sine wave. Figure 7 is an illustration of residual magnetization when the recording signal is a square wave. It is a diagram. Name of agent: Patent attorney Toshio Nakao and 1 other person No. 1
Figure 2 Figure 11 Lost (MHXI)
Claims (1)
T/6〜T/2期間のレベルがA、T/2〜(2/3)
T期間のレベルがO、(2/3)T〜T期間のレベルが
−Aとなる信号を搬送波とし、この搬送波を入力信号で
角度変調して磁気記録媒体上に記録することを特徴とし
た角度変調信号の磁気記録方法。When one period is T, the level from O to T/6 period is O,
Level of T/6 to T/2 period is A, T/2 to (2/3)
The carrier wave is a signal whose level is O during the T period and -A during the (2/3)T to T period, and this carrier wave is angularly modulated by an input signal and recorded on a magnetic recording medium. Magnetic recording method for angle modulated signals.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP63160058A JPH0210504A (en) | 1988-06-28 | 1988-06-28 | Magnetic recording method for angle modulating signal |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP63160058A JPH0210504A (en) | 1988-06-28 | 1988-06-28 | Magnetic recording method for angle modulating signal |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH0210504A true JPH0210504A (en) | 1990-01-16 |
Family
ID=15706995
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP63160058A Pending JPH0210504A (en) | 1988-06-28 | 1988-06-28 | Magnetic recording method for angle modulating signal |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0210504A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN102583728A (en) * | 2012-01-18 | 2012-07-18 | 上海泓济环保工程有限公司 | Rotary type pulse water distributor with corrugated guide rail |
-
1988
- 1988-06-28 JP JP63160058A patent/JPH0210504A/en active Pending
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN102583728A (en) * | 2012-01-18 | 2012-07-18 | 上海泓济环保工程有限公司 | Rotary type pulse water distributor with corrugated guide rail |
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