JPS6329308A - Magnetic head - Google Patents

Magnetic head

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Publication number
JPS6329308A
JPS6329308A JP61171394A JP17139486A JPS6329308A JP S6329308 A JPS6329308 A JP S6329308A JP 61171394 A JP61171394 A JP 61171394A JP 17139486 A JP17139486 A JP 17139486A JP S6329308 A JPS6329308 A JP S6329308A
Authority
JP
Japan
Prior art keywords
magnetic head
frequency
recording
gap width
luminance signal
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
Application number
JP61171394A
Other languages
Japanese (ja)
Other versions
JPH0758526B2 (en
Inventor
Kunihide Sakai
酒井 邦英
Hiroyuki Hayashi
博之 林
Hiroshi Minami
南 寛
Katsushi Tagami
勝詞 田上
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.)
Victor Company of Japan Ltd
Original Assignee
Victor Company of Japan Ltd
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 Victor Company of Japan Ltd filed Critical Victor Company of Japan Ltd
Priority to JP61171394A priority Critical patent/JPH0758526B2/en
Publication of JPS6329308A publication Critical patent/JPS6329308A/en
Publication of JPH0758526B2 publication Critical patent/JPH0758526B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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  • Magnetic Heads (AREA)

Abstract

PURPOSE:To improve S/N and the color picture quality of a reproduced picture by selecting the gap width of a magnetic head so as to satisfy specified relations relative to the recording wavelength of a low frequency conversion carrier chrominance signals and the recording wavelength of a luminance signal to be frequency-modulated. CONSTITUTION:A magnetic head selects a gap width (g) to the value to satisfy both inequalitis lambdac/g<=42 and lambdaw/g>=2 to a recording wavelength lambdac of low frequency conversion carrier chrominance signals and the recording wavelength lambdaw of a luminance signal to be frequency-modulated in a white peak clip level. Both inequalities are obtained by an experiment, etc., the gap width of a magnetic head is selected to the value to satisfy both inequalities and in both bands of the low frequency conversion carrier chrominance signals and an FM luminance signal, a recording loss, a magnetic flux reduction at the time of reproduction and a gap loss are respectively decreased. Thus, a common magnetic head is used and a satisfactory S/N video signal can be obtained.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は磁気ヘッドに係り、特に低域変換搬送色信号及
び被周波数変調輝度信号を磁気記録媒体に記録及び再生
する磁気ヘッドに関する。
DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to a magnetic head, and more particularly to a magnetic head for recording and reproducing a low frequency converted carrier chrominance signal and a frequency modulated luminance signal on a magnetic recording medium.

従来の技術 VTRでは磁気ヘッドを用いて映像信号を磁気テープに
記録し、またこれを再生している。この場合、VTRの
小型軽値高密度化を図るため、あるいは、水平@像度を
^めて高品位高画質化を図るため、被周波数変調輝度信
号(FM輝度信号)のキャリア周波数を高く設定した水
平解像度の高い高品位型VTRがある。かかる高品位型
VTRでは、映像信号の最小記録波長をλminとする
と、高いS/Nを得、かつ、ヘッド再生出力を最大とす
るために、磁気ヘッドのギャップ幅を例えばλminの
略1/3に設定していた。
In conventional VTRs, a magnetic head is used to record video signals on a magnetic tape and to reproduce the video signals. In this case, the carrier frequency of the frequency-modulated luminance signal (FM luminance signal) is set high in order to make the VTR compact, light, and high-density, or to increase the horizontal resolution and improve the image quality. There are high-definition VTRs with high horizontal resolution. In such a high-quality VTR, assuming that the minimum recording wavelength of a video signal is λmin, the gap width of the magnetic head is set to approximately 1/3 of λmin, for example, in order to obtain a high S/N and maximize the head reproduction output. It was set to .

ここで、従来型VTRにおける周波数スペクトラムは例
えば第6図(A)に足す如くであり、低域変換搬送色信
号1への低域変換色副搬送波周波数は629kH2、F
M輝度信号IIAのシンクデツプレベル、ホワイトピー
クレベル及びホワイトピーククリップレベルのキャリア
周波数は夫々34MHz 、  4.4M)−1z及び
5.4Mf(zである。一方、高品位型V’TRにおけ
る周波数スペクトラムは]シ11えば第5図(B)に示
す如くであり、低域変換搬送色信号IBの低域変換色n
1搬送波周波数は629kH7、FMi度信号■8のシ
ンクチップレベル、ホワイトピークレベル及びホワイト
ピーククリップレベルのキャリア周波数は夫々5〜IH
7゜7 M l−1z及び9MHzに設定されている。
Here, the frequency spectrum in a conventional VTR is, for example, as shown in FIG.
The carrier frequencies of the sync depth level, white peak level, and white peak clip level of the M luminance signal IIA are 34MHz, 4.4M)-1z, and 5.4Mf(z, respectively.On the other hand, the frequency spectrum in the high-quality V'TR For example, as shown in FIG. 5(B), the low-frequency conversion color n of the low-frequency conversion carrier color signal IB is
1 carrier frequency is 629kHz7, carrier frequency of FMi degree signal ■8 sync chip level, white peak level, and white peak clip level is 5 to IH, respectively.
It is set at 7°7M l-1z and 9MHz.

上記第6図(A)に示す周波数スペクトラムの信号を記
録再生する従来型VTRにおいて、低域変換搬送色信号
IAの記録波長は922μm、ホワイトピーククリップ
レベルでのFM輝度信号Isの記録波長は11μlであ
る。従って、従来型V T Rに用いるビデオ用記録再
生ヘッドのギャップ幅は最小記録波長11μmの略1/
3の0.35μlm〜0.40μlに設定されていた。
In a conventional VTR that records and reproduces signals with the frequency spectrum shown in FIG. 6(A) above, the recording wavelength of the low frequency conversion carrier color signal IA is 922 μm, and the recording wavelength of the FM luminance signal Is at the white peak clip level is 11 μl. It is. Therefore, the gap width of the video recording/reproducing head used in conventional VTRs is approximately 1/1 of the minimum recording wavelength of 11 μm.
3 was set at 0.35 μlm to 0.40 μl.

一方、第6図(B)に示り°周波数スペクトラムの信号
を記録再生する高品位型VTRにおいては、低域変換搬
送色信号Isの記録波長λcは約922μm、ホワイト
ピーククリップレベルでのFM輝度信号IIeの記録波
長(すなわち、最小記録波長)λwは約0.64μ醜で
ある。従って、前記の如く、高品位型VTRに用いるビ
デオ用記録再生ヘッドのギャップ幅はλwの略1/3で
ある0、2μm1.:設定される。
On the other hand, in a high-quality VTR that records and reproduces signals with a frequency spectrum as shown in FIG. The recording wavelength (ie, the minimum recording wavelength) λw of the signal IIe is about 0.64μ. Therefore, as mentioned above, the gap width of the video recording/reproducing head used in high-quality VTRs is approximately 1/3 of λw, which is 0.2 μm1. : Set.

ここで、高品位型VTRで高保持力〈例えば800Q 
c〜9000c )の高品位型テープに前記第6図(B
)に示す如き周波数スペクトラムの映像信号を記録再生
する場合において、磁気ヘッドとして前記ギャップ幅0
,35μ11−0.40μ−の従来型ヘッドを用いた場
合とギャップ幅02μlの高品位型ヘッドを用いた場合
とを比較覆ると、高品位型ヘッドを用いた場合の方がホ
ワイトピーククリップレベルでのFM輝度信号のキャリ
ア周波数98H2において約4」〜19dBも再生出力
が改善され、また水平解像度も400TV本以」−実現
される。
Here, use a high-quality VTR with high holding power (for example, 800Q).
The above-mentioned figure 6 (B
) When recording and reproducing a video signal having a frequency spectrum as shown in FIG.
, 35μ11-0.40μ- and a high-quality head with a gap width of 02μl, the white peak clip level is higher when using the high-quality head. At the carrier frequency of 98H2 of the FM luminance signal, the reproduction output is improved by about 4'' to 19 dB, and the horizontal resolution is also achieved at 400 TV lines or more.

上記高品位型ヘッドを従来型VTRに用いて低保持力(
例えば、60008〜7000e)の従来型テープに前
記第6図(A)に示す如き周波数スペクトラムの映像信
号を記録再生する場合においても、FM輝度信号帯域の
再す出力は従来型VTRの規格を満たしている。
The above high-quality heads can be used in conventional VTRs with low holding force (
For example, even when recording and reproducing a video signal with a frequency spectrum as shown in FIG. 6(A) on a conventional tape (60008 to 7000e), the re-output of the FM luminance signal band does not meet the standards of the conventional VTR. ing.

従って、従来型VTRと高品位型VTRとの間に、FM
輝度信号帯域においてはギャップ幅0.2μmの高品位
型ヘッドを用いても互いに互換性を有している。
Therefore, there is an FM difference between the conventional VTR and the high-quality VTR.
In the luminance signal band, they are compatible with each other even if a high quality head with a gap width of 0.2 μm is used.

発明が解決しようとする問題点 しかるに、上記高品位型ヘッドは水平解像度を高めるた
めに高周波特性の改良を強調した狭ギヤツプ幅を有して
いるため、この高品位型ヘッドを従来型VTRに用いて
従来型テープに映像信号の記録再生を行なった場合、狭
ギャップ化により低周波領域、特に低域変換色副搬送波
周波数629 k +−I Zにおける記録損失が大き
くなり、また再生時の磁束効率が低下し、ざらにギヤツ
ブn失が大きくなってしまうという問題点があった。
Problems to be Solved by the Invention However, since the above-mentioned high-quality head has a narrow gap width that emphasizes improvement of high-frequency characteristics in order to increase horizontal resolution, it is difficult to use this high-quality head in a conventional VTR. When recording and reproducing video signals on a conventional tape, the narrowing of the gap increases the recording loss in the low frequency region, especially in the low conversion color subcarrier frequency 629k+-IZ, and the magnetic flux efficiency during reproduction increases. There was a problem in that the gear wheel loss would decrease and the gear loss would become large.

この場合、低域変換搬送色信号の再外出力レベルが、従
来型ヘッドを用いた場合に比べて、約−4,B〜−5+
f3低下し、そのS/Nも低下してしまう。このような
傾向は高品位型ヘッド及び高品位型テープを用いた高品
位型VTRシステムにおいても現われ、揮度信号周波数
特竹等の高域特性は大幅に改善され、水平W?象度ち4
00T V本以上となり輝度信号S/Nら従来型ヘッド
及び従来型テープを用いた従来型VTRシステムと同等
以上になる反面、低域変換色シ1搬送波周波数629k
Hzでの再生出力レベルが−5出低下し、そのS/Nも
低下し、よって再生画面のカラー画質が低下してしまう
答の問題点があった。
In this case, the external output level of the low-pass conversion carrier color signal is approximately -4,B to -5+ compared to when using the conventional head.
f3 decreases, and its S/N also decreases. This trend also appears in high-quality VTR systems that use high-quality heads and high-quality tapes, and high-frequency characteristics such as volatile signal frequency characteristics have been greatly improved, and horizontal W? Zodochi 4
The brightness signal S/N is equivalent to or higher than a conventional VTR system using a conventional head and a conventional tape, but the low frequency conversion color signal 1 carrier frequency is 629k.
There was a problem in that the reproduction output level at Hz decreased by -5 outputs, the S/N ratio also decreased, and the color image quality of the reproduction screen deteriorated.

そこで、本発明は磁気ヘッドのギャップ幅を低域変換搬
送色信号及びF〜1輝度信号の両帯域において所要レベ
ル以上の再生出力が得られるような値に選定することに
より、上記問題点を解決した磁気ヘッドを提供すること
を目的とする。
Therefore, the present invention solves the above problem by selecting the gap width of the magnetic head to a value that allows reproduction output at a required level or higher to be obtained in both bands of the low frequency conversion carrier chrominance signal and the F~1 luminance signal. The purpose of the present invention is to provide a magnetic head with improved characteristics.

問題点を解決するための手段 本発明になる磁気ヘッドは、そのギャップ幅Qを、低域
変換搬送色信号の記録波長λcとホワイトピーククリッ
プレベルにおける被周波数変調に411信号の記録波長
λwとに対して、 λc / Q≦42.2w / Q≧2の山王等式を満
足するような値に選定して構成される。
Means for Solving the Problems The magnetic head according to the present invention sets its gap width Q to the recording wavelength λc of the low-pass conversion carrier color signal and the recording wavelength λw of the 411 signal for frequency modulation at the white peak clip level. On the other hand, it is constructed by selecting a value that satisfies the Sanno equation of λc/Q≦42.2w/Q≧2.

作用 上記の両不等式は、後述する如く、実験等により得られ
たものであり、この両不等式を満足するような値に磁気
ヘッドのギャップ幅を選定することにより、低域変換搬
送色信号及びFM輝度信号の両帯域において、記録損失
、再生時の磁束効率低下分及びギャップ損失は夫々低減
される。
Effect The above two inequalities have been obtained through experiments, etc., as described later. By selecting the gap width of the magnetic head to a value that satisfies these two inequalities, the low frequency conversion carrier color signal and the FM In both bands of the luminance signal, recording loss, reduction in magnetic flux efficiency during reproduction, and gap loss are reduced.

実施例 第1図及び第2図は夫々本発明になる磁気ヘッドの一実
施例の平面図及び側面図を示す。両図中、磁気ヘッド1
は酸化物系強磁性体であるフェライトよりなる磁気ヘッ
ド半休2a、2b及びガラス系接着剤3a、3b、4.
5 (図中、梨地で示す)等より構成される。磁気ヘッ
ド半休2a、2bにはギャップ部Aが形成されている。
Embodiment FIGS. 1 and 2 show a plan view and a side view, respectively, of an embodiment of a magnetic head according to the present invention. In both figures, magnetic head 1
are magnetic head half-holes 2a, 2b made of ferrite, which is an oxide-based ferromagnetic material, and glass-based adhesives 3a, 3b, 4.
5 (shown in matte finish in the figure), etc. A gap portion A is formed between the magnetic head half-rests 2a and 2b.

また、6.7及び8は夫々コイル巻回用溝を示す。Further, 6.7 and 8 indicate coil winding grooves, respectively.

ところで、一般に水平解像度は、FMti度信号の白5
0%に相当する周波数から低域変換搬送色信号の上側サ
イドバンドまでの利用できる最高周波数帯域幅に比例す
る。この場合、第3図に示す如く、複合映像信号の同期
信号部分と映像信号部分とのレベルの比は40:100
であるので、前記第6図(A)に示す如き従来型VTR
の周波数スペクトラムにおいて、白50%に相当するF
M搬送波周波数は、 となる。ここで、低域変換搬送色信号IAの上側サイド
バンドの周波数は、 629+500”=1130 (kHz)であるため、
記録可能な最高周波数帯域は、4.04−1.13=2
.91 (MHz)となる。よって、従来型VTRの水
平解像度は、輝度信号の1MHzが約80TV本に相当
するので、 2.91X80紐233 (TV本) となる。これと同様にして、前記第6図(B)に示す如
き周波数スペクトラムの高品位型V T Rの水平解像
度を求めると、約410T V本となる。
By the way, the horizontal resolution is generally the white 5 of the FMti degree signal.
It is proportional to the highest available frequency bandwidth from the frequency corresponding to 0% to the upper sideband of the low-pass transform carrier color signal. In this case, as shown in FIG. 3, the level ratio of the synchronization signal part and the video signal part of the composite video signal is 40:100.
Therefore, the conventional VTR as shown in FIG. 6(A)
In the frequency spectrum of , F corresponding to 50% white
The M carrier frequency is as follows. Here, the frequency of the upper sideband of the low-pass conversion carrier color signal IA is 629+500''=1130 (kHz), so
The highest frequency band that can be recorded is 4.04-1.13=2
.. 91 (MHz). Therefore, the horizontal resolution of the conventional VTR is 2.91×80 strings 233 (TV lines), since 1 MHz of the luminance signal corresponds to about 80 TV lines. Similarly, when the horizontal resolution of a high quality VTR with a frequency spectrum as shown in FIG. 6(B) is determined, it is approximately 410 TV lines.

第4図は前記従来型VTR及び高品位型VTRにおける
一例の規格化再生出力対周波数特性を示す。この特性図
は、テープヘッド相対速度を5.8i /secとし、
従来型VTRに低保持力(700Qe )の磁気テープ
を用い、また高品位型VTRに高保持力(8500e 
)の磁気テープを用いた場合のVTRの記録再生実験結
果よりも得られたものである。ここで、実線で示す特性
LA及びLsは高品位型VTRにいて磁気ヘッドのギ1
?ツブ幅qを夫々0.20μl及び025μmとしたと
きの特性曲線を示し、破線で示す特性Lc及びLoは従
来型VTRにおいて磁気ヘッドのギャップ幅9を夫々0
.35μm及び040LtIIlとしたときの特性曲線
示す。
FIG. 4 shows the normalized playback output versus frequency characteristics of an example of the conventional VTR and high-quality VTR. This characteristic diagram assumes that the tape head relative speed is 5.8i/sec,
A magnetic tape with a low holding force (700Qe) is used for conventional VTRs, and a magnetic tape with high holding force (8500Qe) is used for high-quality VTRs.
) was obtained from the results of a VTR recording and reproducing experiment using a magnetic tape. Here, the characteristics LA and Ls shown by solid lines are the characteristics of the magnetic head gear 1 in a high-quality VTR.
? The characteristic curves are shown when the knob width q is 0.20 μl and 0.25 μm, respectively, and the characteristics Lc and Lo shown by broken lines are obtained when the gap width 9 of the magnetic head is 0.
.. The characteristic curve when it is 35 μm and 040LtIIl is shown.

第4図から解るように、従来型VTRにおけるFMi度
信号のホワイトピークレベル付近でのヤシリア周波数5
MHzにおける規格化再生出力く再生感度)と高品位型
VTRにおけるFM輝度信号のホワイトピークレベルで
のキャリア周波数7 M Hzにおtプる再生感度とが
略同−レベルにある。また、この場合、高品位型VTR
では、例えばFM輝度信z3のシンクチップレベルから
ホワイトピークレベルまでの周波数偏移は従来型VTR
の2倍の2 M l−1zなので、輝度信号のS/Nが
約6cE向上し、また前記の如く、水平解像度も400
TV本以上が達成される。
As can be seen from Figure 4, the Yasiri frequency 5 near the white peak level of the FMi degree signal in the conventional VTR
The normalized reproduction output (reproduction sensitivity) at MHz and the reproduction sensitivity at the carrier frequency of 7 MHz at the white peak level of the FM luminance signal in a high-quality VTR are approximately at the same level. In addition, in this case, a high-quality VTR
For example, the frequency deviation from the sync tip level to the white peak level of the FM luminance signal z3 is
Since it is 2 M l-1z, which is twice that of
More than a TV book can be achieved.

しかし、高品位型VTRにおいてギャップ幅が02μm
の磁気ヘッドを用いると、狭ギャップ化による再生時の
磁束効率の低下、ギャップ10失、更にはテープの高保
持力化による低周波領域でのヘッド飽和による記録jO
失も加わって、従来型VTRに比べて、低域変換色i?
IIw1送彼周波数629kH2に近い周波数500k
H2において再生出力レベルが約−4,9cEム低下し
、S / N t)(l(下していた。
However, in high-quality VTRs, the gap width is 0.2 μm.
When using a magnetic head of
In addition to the loss, compared to conventional VTRs, the low frequency conversion color i?
IIw1 sending frequency 629kHz frequency 500k close to H2
In H2, the playback output level decreased by about -4.9 cEm, and the S/Nt)(l) decreased.

ところで、前記の如く、磁気ヘッドのギャップ幅を設定
する場合、最小記録波長λwの約1/3〜1/4に設定
すること(すなわら、λw / Q =3〜4に設定す
ること〉が一般的て−あった。しかし、上記の如くギャ
ップ幅を設定すると、低域変換搬送色信号帯域において
再生出力レベルが低下してしまう。
By the way, as mentioned above, when setting the gap width of the magnetic head, it should be set to about 1/3 to 1/4 of the minimum recording wavelength λw (that is, set to λw / Q = 3 to 4). However, if the gap width is set as described above, the reproduced output level will decrease in the low frequency conversion carrier color signal band.

そこで、本発明は、低域変換搬送色信号に対応する記録
波長λc,ホワイトピーククリップレベルでのFM輝度
信号に対応する記録波長(最小記録波長)λw及び磁気
ヘッドのギャップ幅Qの3つの値に着目して実験を行な
い、再生出力レベルの低下が最小となるような関係式を
求めた点に特徴を有している。
Therefore, the present invention provides three values: a recording wavelength λc corresponding to a low-band conversion carrier color signal, a recording wavelength (minimum recording wavelength) λw corresponding to an FM luminance signal at a white peak clip level, and a gap width Q of a magnetic head. This method is characterized by conducting experiments focusing on , and finding a relational expression that minimizes the decrease in the playback output level.

ここで、λc= 9.22μm、λw=0.64μmと
し、ギャップ幅Qを0.2μm−0,4μlまで変化さ
せたときの周波数500kH2,5MHz及び9MH2
における再生出力レベルの実験測定結果を下表に示す。
Here, when λc = 9.22 μm and λw = 0.64 μm, and the gap width Q is changed from 0.2 μm to 0.4 μl, the frequencies are 500 kHz, 5 MHz, and 9 MH2.
The table below shows the experimental measurement results of the playback output level.

幅04μm、すなわちλc / G = 23.05及
びλw10=1.61の磁気ヘッドを用いた従来型VT
Rで従来型テープの記録再生を行なった場合の各周波数
における再生出力(すなわち、従来型VTRシステムの
最大再生出力レベル)を基準v <−iなりら、0ct
3)として、この基準値からの変位列を示している。
Conventional VT using a magnetic head with a width of 04 μm, i.e. λc/G = 23.05 and λw10 = 1.61
The playback output at each frequency when recording and playing back a conventional tape with R (i.e., the maximum playback output level of the conventional VTR system) is the standard v < -i, 0ct
3) shows a sequence of displacements from this reference value.

ここで、前記第4図及び上記表より、ギャップ幅が0.
25μm、すなわらλc / Q = 36.88及び
λw/Q=2.58の磁気ヘッドでは、従来型VTRで
従来型テープを記録再生した場合でも、また高品位型V
TRで高品位型テープを記録再生した場合でも周波数5
00kH2での規格化再生出力レベルの低下が約−2c
B以内になり、実用上何ら差しつかえなく十分な色信号
S/Nを確保できる。
Here, from the above-mentioned FIG. 4 and the above-mentioned table, the gap width is 0.
With a magnetic head of 25 μm, that is, λc/Q = 36.88 and λw/Q = 2.58, even when recording and reproducing conventional tapes with a conventional VTR, it is possible to record and play back a conventional tape with a high-quality VTR.
Even when recording and playing back high-quality tape with TR, the frequency is 5.
The normalized playback output level decreases by approximately -2c at 00kHz2.
B or less, and it is possible to secure a color signal S/N that is sufficient for practical purposes.

一方、上記ギャップ幅025μmの磁気ヘッドを用いて
へ品位型VTRrH品佼型テープを記録再生した場合は
、ギt・ツブ幅が020μm、すなわちλc/Q=46
.10及び2w / q= 3.22の磁気ヘッドを用
いた場合に比べて、周波数9M)−1zの規格化再生出
力レベルにおいて約2J3の低下がみられる。しかし、
これはヘッドの先鋭度Qで充分補える範囲(約4 、f
3)である。まlζ、上記の場合において、高品位型V
TRの周波数7 M Hzにおける再生出力レベルも従
来型VTRの周波数7 M Hzにおける再生出力レベ
ルより約2dBの低下がみられる。しかし、この場合に
は、高品位型VTRのFM輝度信号の周波数偏移幅が従
来型VTRの2倍の2M)−1zであるため、前記の如
く、高品位VTRにおいても従来型VTRと同等以上の
輝度信号S/Nを確保できる。
On the other hand, when a magnetic head with a gap width of 025 μm is used to record and reproduce a high quality VTRrH high quality tape, the gap width is 020 μm, that is, λc/Q=46
.. Compared to the case of using a magnetic head of 10 and 2w/q=3.22, there is a decrease of about 2J3 in the normalized reproduction output level of frequency 9M)-1z. but,
This can be fully compensated for by the sharpness Q of the head (approximately 4, f
3). In the above case, high-quality type V
The reproduction output level of the TR at a frequency of 7 MHz is also approximately 2 dB lower than the reproduction output level of a conventional VTR at a frequency of 7 MHz. However, in this case, the frequency deviation width of the FM luminance signal of the high-definition VTR is 2M)-1z, which is twice that of the conventional VTR, so as mentioned above, even the high-definition VTR is equivalent to the conventional VTR. The above luminance signal S/N can be ensured.

次に、磁気ヘッドのギャップ幅を最適とするための関係
式(不等式)について説明する。この関係式を求めるに
あたっては、前記表において、0周波数500k)−1
2における再生出力レベルの出力低下が−2,f3以内
であること、及び■周波数9MH2における再生出力レ
ベルの出力低下が、ギャップ幅02μm1すなわちλc
 / CJ =46.10及びλw/C1=3.22の
磁気ヘッドを用いて高品位型テープの記録再生を行なっ
た場合の値(+ 19.5.E )から−3dB以内で
あること、の2点を条件とした。
Next, a relational expression (inequality) for optimizing the gap width of the magnetic head will be explained. To find this relational expression, in the table above, 0 frequency 500k)-1
2. The output decrease in the reproduction output level at frequency 9MH2 is within -2, f3, and
/ CJ = 46.10 and λw / C1 = 3.22, the value when recording and reproducing a high-quality tape (+19.5.E) using a magnetic head is within -3 dB. Two points were required.

この場合、上記条件■を満足する関係式は、前記表から 298≧λw / Q 、 41.91≧λc / Q
   ・・・(1)となり、条件■を満足する関係式は
、 322≧λw / Q≧2.38 。
In this case, the relational expressions that satisfy the above condition (■) are as follows from the above table: 298≧λw/Q, 41.91≧λc/Q
...(1), and the relational expression that satisfies condition (■) is 322≧λw/Q≧2.38.

46、10≧λc / Q≧34.15       
・・・■となる。
46, 10≧λc / Q≧34.15
... becomes ■.

従って、上記(1)式及び(2)式を両方共満足する関
係式は、 293≧λw / CJ≧2.38゜ 4191≧λc / Q≧34.15       ・
・・■となる。
Therefore, the relational expression that satisfies both equations (1) and (2) above is: 293≧λw / CJ≧2.38° 4191≧λc / Q≧34.15 ・
... becomes ■.

上記(3)式において、実験測定結果の誤差及びテープ
走行速度の変化等を考慮すると、(3)式は大略(4)
式のように店き直せる。
In equation (3) above, if we take into account errors in experimental measurement results and changes in tape running speed, equation (3) can be roughly transformed into equation (4).
You can renovate your store like a ceremony.

2w / g≧2.λc/g≦42     ・・・(
4)次に、第5図はギャップ幅0435μm(ずなわら
、λc / Q = 26.3,2w / Q = 1
.84)の磁気ヘッドaを用いた場合の各周波数におり
る配録及び再生レベルを基準値として、ギャップ幅02
5μl1l(すなわら、λc / Q = 36.88
 、λw/g= 2.58 )の磁気ヘッドbとギ1シ
ップ幅02μm(すなわらλc/g =46.1.−2
w / Q =322)の磁気ヘッドCとを用いた場合
の記録及び再生レベルを比較したグラフである。
2w/g≧2. λc/g≦42...(
4) Next, in Figure 5, the gap width is 0435 μm (Zunawara, λc / Q = 26.3, 2w / Q = 1
.. Using the recording and playback level at each frequency when using the magnetic head a of 84) as a reference value, the gap width is 02.
5μl1l (i.e., λc/Q = 36.88
, λw/g = 2.58) and a gear ship width of 02 μm (i.e., λc/g = 46.1.-2).
2 is a graph comparing the recording and reproducing levels when using a magnetic head C with w/Q = 322).

ここで、RA及びPAは夫々ギャップ幅0、25μmの
磁気ヘッドbを用いた場合の記録レベル及び再イト出力
レベルを示し、R8及びPaは夫々ギャップ幅0.20
μmの磁気ヘッドCを用いた場合の記録レベル及び再生
出力レベルを示す、1この場合、ギャップ幅025μl
の磁気ヘッドbは前記(4)式を満足する本発明になる
ヘッドであり、一方、ギャップ幅0.20μmの磁気ヘ
ッドCは(4)式を満足しない従来のヘッドである。
Here, RA and PA indicate the recording level and rewrite output level when using magnetic head b with a gap width of 0 and 25 μm, respectively, and R8 and Pa indicate a gap width of 0.20 μm, respectively.
Showing the recording level and reproduction output level when using a μm magnetic head C, 1 In this case, the gap width is 025 μl.
The magnetic head b is a head according to the present invention that satisfies the above formula (4), while the magnetic head C having a gap width of 0.20 μm is a conventional head that does not satisfy the formula (4).

第5図より、低域変換色副搬送波周波数629kl−1
2を合む周波数IMH2以下の領域では、磁気ヘッドC
は磁気ヘッドaに比べて一2出以上も記録損失があるが
、本発明になる磁気ヘッドbは記録損失が−2,13以
下となっている。また、再生においても、本発明になる
磁気ヘッドbが周波数1MHz付近でギャップ損失や再
生効率低下による再生損失がほぼ基準値に回復している
。一方FM輝度信号帯域では、周波数9MHzにおいて
磁気ヘッドCの方が磁気ヘッドbより再生出力レベルが
約1cE向上しているが、前記の理由により実用上影響
はない。
From Figure 5, low-pass conversion color subcarrier frequency 629kl-1
In the region below the frequency IMH2, which is the sum of 2, the magnetic head C
The magnetic head b has a recording loss of 12 times more than the magnetic head a, but the magnetic head b according to the present invention has a recording loss of -2.13 times or less. Also, in reproduction, the magnetic head b according to the present invention recovers reproduction loss due to gap loss and reduction in reproduction efficiency to almost the standard value at a frequency of around 1 MHz. On the other hand, in the FM luminance signal band, the reproduction output level of magnetic head C is about 1 cE higher than that of magnetic head B at a frequency of 9 MHz, but this has no practical effect for the above-mentioned reason.

発明の効果 上)ホの如く、本発明によれば、低域変換搬送色信号の
再生出力感度低下が実用上殆どなく、また広帯域化され
、かつ、キャリア周波数が高いFM輝度信号の再生出力
感度向上を実現でき、しかも、輝度信号S/Nも従来の
VTRと同等以上で、かつ、水平解像度400T V零
以上の高品位な再生画質を得ることができ、従来のVT
Rでもキャリア周波数の高いFM輝度信号を記録再生す
る高品位VTRでも、いずれも共通の磁気ヘッドを使用
して良好なS/Nの映像1g号が19られる記録再生が
できる等の特長を有する。
According to the present invention, there is virtually no reduction in the reproduction output sensitivity of the low frequency conversion carrier chrominance signal, and the reproduction output sensitivity of the FM luminance signal with a wide band and high carrier frequency is improved. In addition, the brightness signal S/N is equal to or higher than that of conventional VTRs, and high-quality playback image quality with horizontal resolution of 400TV or higher can be obtained, which is better than conventional VT
Both R and high-quality VTRs that record and reproduce FM luminance signals with high carrier frequencies have features such as being able to record and reproduce 1g video with a good S/N using a common magnetic head.

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

第1図及び第2図は夫々本発明になる磁気ヘッドの一実
施例を示す平面図及び側面図、第3図は映像信号のレベ
ルと周波数との関係を説明するための図、第4図は従来
型V T R及び高品位型VTRにおける一例の規格化
再生出力対周波数特性図、第5図は従来の磁気ヘッドと
本発明になる磁気ヘッドとの記録レベル及び再生レベル
を夫々示1図、第6図(A)及び(B)は夫々従来型V
TR及び高品位型VTRの一例の周波数スペクトラム図
である。 1・・・磁気ヘッド、2a、2b・・・磁気ヘッド半休
、3a、3b、4.5−・・ガラス系接着剤、6,7゜
8・・・コイル巻回用溝、A・・・ギャップ部。 特許出願人 日本ビクター株式会社 ・・ζ−゛、r> 同     弁理士  松  浦  兼  行゛、;゛
、−−−シ 第1図 第3図 周波@fMHXl− 第5図 「 第6r:M 喝坂数iMHzl−
1 and 2 are a plan view and a side view, respectively, showing an embodiment of the magnetic head according to the present invention, FIG. 3 is a diagram for explaining the relationship between the level and frequency of a video signal, and FIG. 4 FIG. 5 is a normalized playback output versus frequency characteristic diagram of an example of a conventional VTR and a high-quality VTR, and FIG. 5 shows the recording level and playback level of a conventional magnetic head and a magnetic head according to the present invention, respectively. , FIGS. 6(A) and (B) are respectively conventional V
FIG. 2 is a frequency spectrum diagram of an example of a TR and a high-quality VTR. 1...Magnetic head, 2a, 2b...Magnetic head half-closed, 3a, 3b, 4.5-...Glass adhesive, 6,7° 8...Coil winding groove, A... gap section. Patent applicant: Victor Company of Japan Co., Ltd. . Saka number iMHz-

Claims (1)

【特許請求の範囲】 低域変換搬送色信号及び被周波数変調輝度信号を磁気記
録媒体に記録及び再生する磁気ヘッドにおいて、該磁気
ヘッドのギャップ幅gを、該低域変換搬送色信号の記録
波長λ_cとホワイトピーククリップレベルにおける該
被周波数変調輝度信号の記録波長λ_wとに対して、 λ_c/g≦42、λ_w/g≧2 の両不等式を満足するような値に選定して構成したこと
を特徴とする磁気ヘッド。
[Scope of Claims] In a magnetic head for recording and reproducing a low-band conversion carrier color signal and a frequency-modulated luminance signal on a magnetic recording medium, the gap width g of the magnetic head is defined as the recording wavelength of the low-band conversion carrier color signal. For λ_c and the recording wavelength λ_w of the frequency modulated luminance signal at the white peak clip level, values are selected and configured to satisfy both the inequalities λ_c/g≦42 and λ_w/g≧2. Features a magnetic head.
JP61171394A 1986-07-21 1986-07-21 Video signal magnetic recording / reproducing method and video signal magnetic recording / reproducing apparatus Expired - Lifetime JPH0758526B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP61171394A JPH0758526B2 (en) 1986-07-21 1986-07-21 Video signal magnetic recording / reproducing method and video signal magnetic recording / reproducing apparatus

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61171394A JPH0758526B2 (en) 1986-07-21 1986-07-21 Video signal magnetic recording / reproducing method and video signal magnetic recording / reproducing apparatus

Publications (2)

Publication Number Publication Date
JPS6329308A true JPS6329308A (en) 1988-02-08
JPH0758526B2 JPH0758526B2 (en) 1995-06-21

Family

ID=15922343

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61171394A Expired - Lifetime JPH0758526B2 (en) 1986-07-21 1986-07-21 Video signal magnetic recording / reproducing method and video signal magnetic recording / reproducing apparatus

Country Status (1)

Country Link
JP (1) JPH0758526B2 (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6021884A (en) * 1996-12-12 2000-02-08 Asahi Seiko Co., Ltd. Coin selecting apparatus
US7100823B2 (en) 2003-06-30 2006-09-05 Asahi Seiko Kabushiki Kaisha Coin selector with a smart card charging function

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6021884A (en) * 1996-12-12 2000-02-08 Asahi Seiko Co., Ltd. Coin selecting apparatus
US7100823B2 (en) 2003-06-30 2006-09-05 Asahi Seiko Kabushiki Kaisha Coin selector with a smart card charging function

Also Published As

Publication number Publication date
JPH0758526B2 (en) 1995-06-21

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