JPS5848208A - Sound recording method to magnetic tape - Google Patents

Sound recording method to magnetic tape

Info

Publication number
JPS5848208A
JPS5848208A JP14592781A JP14592781A JPS5848208A JP S5848208 A JPS5848208 A JP S5848208A JP 14592781 A JP14592781 A JP 14592781A JP 14592781 A JP14592781 A JP 14592781A JP S5848208 A JPS5848208 A JP S5848208A
Authority
JP
Japan
Prior art keywords
magnetic tape
iron cores
iron core
recording
frequency
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
Application number
JP14592781A
Other languages
Japanese (ja)
Inventor
Hidekazu Hata
秦 秀和
Hirotaka Kurata
倉田 裕隆
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.)
TRIO KENWOOD CORP
Trio KK
Kenwood KK
Original Assignee
TRIO KENWOOD CORP
Trio KK
Kenwood KK
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 TRIO KENWOOD CORP, Trio KK, Kenwood KK filed Critical TRIO KENWOOD CORP
Priority to JP14592781A priority Critical patent/JPS5848208A/en
Publication of JPS5848208A publication Critical patent/JPS5848208A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B5/00Recording by magnetisation or demagnetisation of a record carrier; Reproducing by magnetic means; Record carriers therefor
    • G11B5/02Recording, reproducing, or erasing methods; Read, write or erase circuits therefor
    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B5/00Recording by magnetisation or demagnetisation of a record carrier; Reproducing by magnetic means; Record carriers therefor
    • G11B5/008Recording on, or reproducing or erasing from, magnetic tapes, sheets, e.g. cards, or wires
    • G11B5/00813Recording on, or reproducing or erasing from, magnetic tapes, sheets, e.g. cards, or wires magnetic tapes

Landscapes

  • Magnetic Heads (AREA)

Abstract

PURPOSE:To execute recording with good quality, by dividing a frequency band of an input sound signal, opposing an iron core of a magnetic head in 1 track width of a magnetic tape, setting air-gap length and air-gap depth of the iron core, and a sound recording bias current, and recording them in parallel. CONSTITUTION:To a track 5 of a magnetic tape 1, iron cores 7, 8 of a magnetic head are opposed, and to a track 6, iron cores 9, 10 are opposed and placed. Air-gap length of the iron cores 7, 10 is set longer than air-gap length of the iron cores 8, 9, and also air-gap depth of the iron cores 7, 10 is set shorter than air-gap depth of the iron cores 8, 9. To input terminals Ti1, Ti2 of a recording amplifier 11, signals of the tracks 5, 6 are applied, respectively, and a frequency- divided signal is applied to coils of the iron cores 7-9 together with a bias current given by a sound recording bias oscillator 12. In this way, distortion and a frequency characteristic can be improved as a whole. Also, drop of a reproducing level can be reduced by selecting the width of the iron cores 7-9.

Description

【発明の詳細な説明】 不発明線音声信号を磁気テープに記帰する機器に利用で
きる磁気テープへの鈴音方法に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method for recording a ringing sound on a magnetic tape that can be used in a device that records an uninvented line audio signal on a magnetic tape.

従来のカセットテープレコーダ、オープンリールテープ
レコーダ、マイク四カセットテープレコーダ等、磁気テ
ープに音声信号を記録する鈴音機における磁気テープ六
磁気ヘッドの鉄心との関係は第1図に示す如く、磁気テ
ープlの1トラツクに対してfi埋1トラック幅の幅を
有する鉄心2を並置した磁気ヘッド3を用いて、各トラ
ックに全帯域記録を行なっている。トラック配置はテー
プレコーダの形式によって異なるが、第1図にかいては
4トラツク2チヤンネルステレオ碌音の場合の例を示し
ておシ、4拡磁気ヘツド3の鉄心2の空隙である。
The relationship between the magnetic tape 6 magnetic heads and the iron core in Suzune machines that record audio signals on magnetic tape, such as conventional cassette tape recorders, open reel tape recorders, and 4-microphone cassette tape recorders, is as shown in Figure 1. Full-band recording is performed on each track using a magnetic head 3 in which iron cores 2 having a width equal to one track width filled with fi are juxtaposed. The track arrangement varies depending on the type of tape recorder, but FIG. 1 shows an example of a four-track, two-channel stereo sound system, in which the gaps between the iron cores 2 of the four magnetic expansion heads 3 are used.

しかるに1鉄心を磁気テープの1トラツクに対応さ、せ
下、1トラツクに全帯域記録する場合には鈴音バイアス
電流を400 Hs+ 1えは315 Hzの基準レベ
ル信号で歪が最低になる値に設定すると、数KH,以上
の信号に対してはオーバーバイアスとなり、周波数特性
の劣化を招く問題があった。このため周波数特性を重視
した場合、歪が最低となる最適鈴音バイアスを無視して
所定の歪内で可能な限り周波数特性の幅が広くなるよう
な鈴音バイアス電流値に設定している場合が多い。この
様に鈴音バイアス電流値を設定すると当然妊域における
歪は悪化する。
However, if one iron core corresponds to one track of a magnetic tape, and the entire band is to be recorded on one track, the bell bias current should be set to a value that minimizes distortion with a reference level signal of 400 Hs + 1, or 315 Hz. As a result, there is a problem in that overbiasing occurs for signals of several kilohertz or more, leading to deterioration of frequency characteristics. For this reason, when emphasis is placed on frequency characteristics, the optimum bell sound bias that produces the lowest distortion is often ignored, and the sound bias current value is often set so that the width of the frequency response is as wide as possible within a predetermined distortion. . If the bell bias current value is set in this way, the distortion in the pregnant region will naturally worsen.

上記の如く、従来の場合、歪から決まる最適鈴音バイア
ス電流値と、周波数特性を広げる九めのQ音バイアス電
流値とは一致せず、歪を最低にすることと、周波数特性
を広げることとを同時に満足させる仁とはできない欠点
があった。
As mentioned above, in the conventional case, the optimal bell tone bias current value determined from distortion and the ninth Q tone bias current value that widens the frequency characteristics do not match, and it is important to minimize distortion and widen the frequency characteristics. There was a drawback that it was impossible to satisfy both Jin and Jin at the same time.

まえ、磁気ヘッドの鉄心の空隙長さを記録信号の短波長
の方に合せであるため、信号電流が大きくかつ長波長の
信号を記録すると歪は増大する欠点があった。
Previously, since the length of the air gap in the iron core of the magnetic head was adjusted to the short wavelength of the recording signal, there was a drawback that distortion increased when the signal current was large and a long wavelength signal was recorded.

本発明は上記にかんがみなされたもので、上記の欠点を
解消した磁気テープへの鈴音方法を提供する仁とを目的
とするものである。
The present invention has been made in view of the above, and an object of the present invention is to provide a method for attaching bells to a magnetic tape, which eliminates the above-mentioned drawbacks.

以下、本発明を実施例によシ説明する。The present invention will be explained below using examples.

第2図および第4図は本発明方法を適用し7’? 一実
施例の磁気ヘッドの鉄心と磁気テープとの関係図および
鈴音・再生回路のブロック図であり1本実施例は周波数
帯竣を2分割した場合の例を示している。
FIGS. 2 and 4 show 7'? after applying the method of the present invention. 1 is a diagram showing the relationship between the iron core and the magnetic tape of a magnetic head and a block diagram of a chime/playback circuit according to an embodiment, and this embodiment shows an example in which the frequency band end is divided into two.

本実施例においては磁気テープ1の1トラック幅内に磁
気テープ幅方向に磁気ヘッドの独立した2個の鉄心を磁
気テープ1に対向して配設する。
In this embodiment, two independent iron cores of a magnetic head are disposed within one track width of the magnetic tape 1 in the width direction of the magnetic tape, facing the magnetic tape 1.

第2図は゛4トラック2チャンネ゛ルの場合の例を示し
ており、第1のトラック5に対しては磁気ヘッドの第1
の鉄心7と第2の鉄心8とを対向させ、第2のトラック
6に対しては磁気ヘッドの第3の鉄心9と第4の鉄心1
0とを対向させて配置する。
FIG. 2 shows an example of a 4-track 2-channel system, in which the first track 5 of the magnetic head is
The iron core 7 and the second iron core 8 of the magnetic head are opposed to each other, and the third iron core 9 and the fourth iron core 1 of the magnetic head are placed opposite to each other with respect to the second track 6.
0 and are placed facing each other.

また第1の鉄心フと第4の鉄心10は低域周波数用であ
って、第2の鉄心8と第3の鉄心9は高域周波数用であ
る。
Further, the first iron core 10 and the fourth iron core 10 are used for low frequencies, and the second iron core 8 and the third iron core 9 are used for high frequencies.

第1、第2゛、第3および第4の鉄心7.8.9517
 、”8 、暑9およびaleとし、第1の鉄心7と第
2の鉄心8との磁気テープ幅方向における間隙および第
3の鉄心9と第4の鉄心10との磁気テープ幅方向にお
ける間隙をす、第2の鉄心8と第3の鉄心9との磁気テ
ープ幅方内における間隙をCとし九とき、第1図に示す
鉄心20幅を為、鉄心2間の磁気テープ幅方向の間隙を
Cとの間に祉、l’==117+Jl−1−b=’a@
−)11@−)bSC’=:Cとなるように第1、第2
、第3、第4の鉄心7.8.9および100幅a?、畠
S、a・、麿1Gおよびそれらの間隙bScが設定しで
ある。また間隙すはb=c/2G−C1509度が望ま
しい。
First, second, third and fourth cores 7.8.9517
, "8, heat 9 and ale, and the gap between the first iron core 7 and the second iron core 8 in the magnetic tape width direction and the gap between the third iron core 9 and the fourth iron core 10 in the magnetic tape width direction. If the gap between the second core 8 and the third core 9 in the width direction of the magnetic tape is C, then the width of the core 20 shown in FIG. Between C and l'==117+Jl-1-b='a@
-)11@-)bSC'=:C.
, third and fourth cores 7.8.9 and 100 width a? , Hatake S, a., Maro 1G and the gap bSc between them are set. Further, the gap is preferably b=c/2G-C1509 degrees.

従って本実施例によるときは、従来の方式による場合と
機械的に互換性がある。
Therefore, this embodiment is mechanically compatible with the conventional system.

つぎに第1〜第4の鉄心7〜9の空隙長さについて説明
する。第3図(麿)および−)祉第2、第3の鉄心8.
9の一部の平面図および第1、第4の鉄心7.10の一
部の平面図である。第1および第4の鉄心の空隙長さL
t、LIOと、第2および第3の鉄心の空隙長さL8、
L9とは異なり、たとえばLt”Llo>Ls=L・ 
に設定しである。また第1および第4の鉄心の空隙課さ
”I、’10  と、第2および第3の鉄心の空隙課さ
dll、’llとは異なシ、九とえばdy = dto
< da = ds K’一定してあシ、空隙長さを短
かくした方の鉄心は空隙深さを深く、空隙長さを長くし
た方の鉄心は空隙深さを浅くする。
Next, the gap lengths of the first to fourth cores 7 to 9 will be explained. Figure 3 (Maro) and -) Second and third iron cores 8.
9 and a plan view of a portion of the first and fourth iron cores 7.10. FIG. Gap length L of the first and fourth cores
t, LIO and the gap length L8 of the second and third iron cores,
Unlike L9, for example, Lt”Llo>Ls=L・
It is set to . Also, the air gap imposition of the first and fourth cores ``I, '10'' is different from the air gap imposition dll, 'll of the second and third iron cores, for example, dy = dto.
< da = ds K' Constantly, the core with shorter void length has a deeper void depth, and the core with longer void length has a shallower void depth.

なお、ことにおいて、第1〜第4の鉄心7−10で1個
の磁気ヘッドを構成してもよく、各電l〜第4−の鉄心
?、8.9および1oでそれぞれ独立した磁気ヘッドを
構成してもよく、壕大第1の鉄心7と第2の鉄心8とで
1つの磁気ヘッドを構成し第3の鉄心9と第4の鉄心1
0とで他の1つの磁気ヘッドを構成してもよい。
Incidentally, one magnetic head may be constituted by the first to fourth iron cores 7-10, and each of the first to fourth iron cores 7-10 may constitute one magnetic head. . Iron core 1
0 may constitute another magnetic head.

つぎに、第1〜第4の鉄心7〜10を用いえ場合の鈴音
・再生について説明する。
Next, the bell sound and reproduction when the first to fourth iron cores 7 to 10 are not used will be explained.

第4図社本発明方法を適用した一実施例における鈴音・
再生回路のプセック図である。
Figure 4: Suzune in an example of applying the method of the present invention.
FIG. 3 is a psek diagram of a reproducing circuit.

11は―前増幅器を、12は鈴音バイアス発振器を、1
3a鈴音/1番生の切替スイッチを、14は再生増幅器
をそれぞれ示している。
11 - pre-amplifier, 12 - Suzune bias oscillator, 1
3a indicates a Suzune/No. 1 student selector switch, and 14 indicates a regenerative amplifier.

録音増幅器11は入力端子TixおよびTi2に各別に
入力された各チャンネルの信号をそれぞれ増幅する増幅
器151および152からまる入力増幅器群15と、増
幅器151の出力信号の周波数帯域を分割する四−パス
フィルタ16’lとバイパスフィルタ162および増幅
器152の出力信号の周波数帯域を分割するローパス7
−イルタ163とバイパスフィルタ164からなる周波
数帯域分割フィルタ群16と、田−パスフィルタ161
とバイパスフィルタ162のりpスオーバー周波数付近
の再生時における周波数特性を平坦にするためのイコラ
イザ171.172およびローパスフィルタ163とバ
イパスフィルタ164のりpスオーバー周波数付近の再
生時における周波数特性を平坦にするためのイブライf
l?3.174からなるイブライず群17と、イ′:1
ライザ1フl〜174の出力信号をそれぞれ各□別に入
力する録音イーライブを有しかつバイアストラップを通
して各録音イコライザ6躊、力をそれぞれ各別に入力し
て第1〜第4の鉄心7〜10のコイルを切替スイッチ1
3と介して駆動する駆動回路1′81〜184からまる
駆動回路群18とから壜、つている。
The recording amplifier 11 includes an input amplifier group 15 consisting of amplifiers 151 and 152 that amplify the signals of each channel input separately to the input terminals Tix and Ti2, and a four-pass filter 16 that divides the frequency band of the output signal of the amplifier 151. 'l and a low pass 7 that divides the frequency band of the output signal of the bypass filter 162 and the amplifier 152.
- frequency band division filter group 16 consisting of filter 163 and bypass filter 164;
Equalizers 171 and 172 for flattening the frequency characteristics during reproduction near the p-over frequency, and the bypass filter 162 and the low-pass filter 163 and bypass filter 164 flatten the frequency characteristics during reproduction near the p-over frequency. Evely f for
l? 3. Evelyz group 17 consisting of 174 and I′:1
It has a recording equalizer into which the output signals of the risers 1 to 174 are separately input, and inputs the output signals of the risers 1 to 174 separately through the bias traps to the respective recording equalizers 6 and 174 to input the output signals to the first to fourth iron cores 7 to 10. Switch 1 to change the coil of
3 and a drive circuit group 18 consisting of drive circuits 1'81 to 184, which are driven through the drive circuits 1'81 to 184.

一方、録音バイアス発振器12は、その出力信号を分枝
して、コンデンサ19と抵抗23、コンデンサ20と抵
抗24、コンデン゛す21と抵抗25、=ンデンサ22
と抵抗26とのそれぞれの直列回路を通して出力し、そ
れぞれ対応する駆動回路181〜184の出力信号と重
畳して切替スイッチ13′を介して第1〜第4の鉄心7
〜10のコイルにそれぞれ各別に印加する。なお;ンデ
ンサ19〜22と抵抗23〜26とからなるそれぞれの
直列回路線対応するそれぞれの第1〜第4の鉄心7〜1
0に対して最適録音バイアス電流値になるように設定し
である。
On the other hand, the recording bias oscillator 12 branches its output signal and connects the capacitor 19 and resistor 23, the capacitor 20 and resistor 24, the capacitor 21 and resistor 25, and the capacitor 22.
and the resistor 26, and are superimposed on the output signals of the corresponding drive circuits 181 to 184 and sent to the first to fourth iron cores 7 via the changeover switch 13'.
~10 coils each separately. Note that each of the first to fourth iron cores 7 to 1 corresponding to each series circuit line consisting of capacitors 19 to 22 and resistors 23 to 26
The recording bias current value is set to be the optimum value for 0.

以上の如く構成し九本実施例において、入力端子Ti1
に第1のチャンネルの音声信号が印加1れ、入力端子T
I2に紘第′20チャンネルの音声信号が印加される。
In the nine embodiments configured as described above, the input terminal Ti1
The audio signal of the first channel is applied to the input terminal T.
The audio signal of the '20th channel is applied to I2.

第1のチャンネルの音声信号は増幅器151によって増
幅され、ローパスフィルタ161および162に印加さ
れる。
The first channel audio signal is amplified by amplifier 151 and applied to low pass filters 161 and 162.

′イルタ162.164の振幅特性線第5図の実線で示
す如く設定してあって、田−パスフィルタ161とハイ
パスフ1イルタ162によシ増幅器151の出力信号は
その周波数帯域が間隙を生ずることなく2分割されて、
低域側は−p−パスフィルタ161から出力され、高域
側は11イパスフイルタ162から出力される。
'The amplitude characteristic lines of the filters 162 and 164 are set as shown by the solid lines in FIG. It was divided into two parts,
The low frequency side is output from the -p-pass filter 161, and the high frequency side is output from the 11-pass filter 162.

一一パスフィルタ161からの出力信号およびバイパス
フィルタ162からの出力信号はそれぞ1.172に各
別に入力されて 、磁気テープ10銀音内容を再生したときにおいてクロ
スオーバ周波数付近の周波数特性を平坦にするようにイ
ブライズされて、・駆動回路1811182に各別に入
力される。駆動回路181.1820入力信号は駆動回
路181.182においてそれぞれレベル調整されたう
え、それぞれ帰音儒に設定された録音/再生の切替スイ
ッチを介して第2の鉄心7のコイルおよび第2の鉄心8
のコイルに印加される。同時に第1の鉄心7のフィルに
はコンデンサ19と抵抗23の直列回路により最適値に
設定された録音バイアス電流が流され、また第2の鉄心
8の;イルには=ンデンサ20と抵抗24の直列回路に
よシ最適値に設定された録音バイアス電流が流される。
The output signal from the pass filter 161 and the output signal from the bypass filter 162 are inputted separately to 1.172, respectively, to flatten the frequency characteristics near the crossover frequency when the contents of the magnetic tape 10 are played back. 1811182, and are individually input to the drive circuit 1811182. The input signals of the drive circuits 181 and 1820 are level-adjusted in the drive circuits 181 and 182, respectively, and sent to the coil of the second iron core 7 and the second iron core via the recording/playback switch set to ``return''. 8
is applied to the coil. At the same time, a recording bias current set to an optimal value is passed through the fill of the first iron core 7 by a series circuit of a capacitor 19 and a resistor 23, and a recording bias current set to an optimum value is passed through the fill of the second iron core 8. A recording bias current set to an optimal value is passed through the series circuit.

従って第1のチャンネルの音声信号は周波数帯域が分割
運れて、高域側音声信号は第2の鉄心8によシ、低域側
音声信号杜第1の鉄心7により磁気テープ1の第1のト
ラック上に磁気テープ10幅方向に低域側音声信号と高
域側音声信号とが並列に記録される仁とになる。この鳩
舎において、第1のチャンネルの音声信号の周波数帯域
を低域側と高域側とに分割し、さらに録音バイアス電流
線コンデンサ19と抵抗23との直列回路およびコンデ
にす20と抵抗24との直列回路によシそれぞれ独立し
て設定できるために、低域側は低域側に最適の録音バイ
アス電流値によシ、高域側は高域側に最適の録音バイア
ス電流値によシそれぞれ磁気テープlの第1のトラック
5上に低域側音声信号および高域側音声信号が記−され
ることになる。
Therefore, the frequency band of the audio signal of the first channel is divided and carried, and the high-frequency audio signal is transmitted to the second iron core 8, and the low-frequency audio signal is transmitted to the first iron core 7 of the magnetic tape 1. A low-frequency audio signal and a high-frequency audio signal are recorded in parallel on the track in the width direction of the magnetic tape 10. In this pigeon house, the frequency band of the audio signal of the first channel is divided into a low frequency side and a high frequency side, and a series circuit of a recording bias current line capacitor 19 and a resistor 23, and a series circuit of a condenser 20 and a resistor 24 are used. Because they can be set independently by the series circuit of A low-frequency audio signal and a high-frequency audio signal are respectively recorded on the first track 5 of the magnetic tape 1.

また入力端子Titに印加された第2のチャyネ′ルの
音声信号も同様にして、磁気テープ1の第2のトラック
6上に低域側音声信号と高域側音−信号とに分割されて
、それぞれ独立した最適の録音バイアス電流が加えられ
て並列に記録されることになる。
Similarly, the audio signal of the second channel applied to the input terminal Tit is divided into a low-frequency audio signal and a high-frequency sidetone signal on the second track 6 of the magnetic tape 1. Then, independent optimal recording bias currents are applied to each, and recording is performed in parallel.

つぎに記録内容を再生する場合社鈴音/再生の切替スイ
ッチ13を再生側に切替えて、第1〜第4の鉄心7〜1
0のコイルに誘起した電圧が再生増幅器14に入力され
る。再生増幅器14において第1および第2の鉄心7お
よび8のコイルに誘起された電圧はそれぞれ所定のレベ
ルで混合された後、再生標準のイブライザを通して所定
のレベルにまで増幅されて、出力端子TOIかも第1の
チャンネルの音声信号が得れ、第3および第4の鉄心9
および10のコイルに誘起された電圧も同様に処理され
て、出力端子’I’ozから第2のチャンネルの音声信
号が得られる。
Next, when reproducing the recorded content, switch the chime/reproduction selector switch 13 to the reproduction side, and select the first to fourth cores 7 to 1.
The voltage induced in the zero coil is input to the regenerative amplifier 14. In the regenerative amplifier 14, the voltages induced in the coils of the first and second iron cores 7 and 8 are mixed at a predetermined level, and then amplified to a predetermined level through a regenerative standard equalizer and output to the output terminal TOI. The audio signal of the first channel is obtained, and the third and fourth iron cores 9
The voltages induced in the coils 1 and 10 are similarly processed to obtain the second channel audio signal from the output terminal 'I'oz.

一方、一般に鉄心の空隙長さおよび空隙深さは歪に関係
し、空隙長さは再生時の一起電圧をも考直して記録信号
波長の172以下に設定されるのが普通であるが、空隙
長さが狭いと記録時において歪が増加し、空隙長さが同
一ならば空隙深さが浅い程、歪が増加する。
On the other hand, the gap length and gap depth in the iron core are generally related to strain, and the gap length is usually set to 172 or less of the recorded signal wavelength, taking into consideration the instantaneous electromotive force during reproduction. If the length is narrow, distortion increases during recording, and if the gap length is the same, the shallower the gap depth, the more distortion increases.

しかるに本実施例においては前記した如く第1の鉄心ツ
ーと第2の鉄心8、第3の鉄心9と第4の鉄心10によ
りそれぞれのチャンネルの音声信号の周波数帯域を分割
して磁気テープ1−に並列に記録するのみではなく、第
11第4の鉄心7.10の空隙長さL7、LIG  と
、第2、第3の鉄心8.9の空隙長15Ls 、Le 
 とを異ならしめ、また第1、第4の鉄心7.10の空
隙探さd7、dlo  と、第2、第3の鉄心8.9の
空隙深さ’lI、’会とを異ならしめている。、この空
隙長さL?(LIO)とLm(Le)は帯域分割した各
々の録音信号の波長に対応して設定し、かつ空隙長さに
対応して最適な空隙深さdt (dlo )・ds (
ds )を設定することkよシ゛綜合的に査あ周波数特
性の゛改善を図ることができる。
However, in this embodiment, as described above, the frequency band of the audio signal of each channel is divided by the first iron core 2, the second iron core 8, the third iron core 9, and the fourth iron core 10, and the magnetic tape 1- In addition to recording in parallel, the gap length L7, LIG of the eleventh and fourth cores 7.10 and the gap lengths 15Ls, Le of the second and third cores 8.9 are recorded in parallel.
In addition, the gap depths d7,dlo of the first and fourth cores 7.10 and the gap depths 'lI,' of the second and third cores 8.9 are made different. , this gap length L? (LIO) and Lm (Le) are set corresponding to the wavelength of each band-divided recording signal, and the optimum gap depth dt (dlo)・ds (
By setting ds), it is possible to improve the frequency characteristics of the scan more comprehensively than k.

またさらに、録音バイアス電流値拡それぞれの帯域に対
応し九鉄心7 (10)、8(9)K対゛して竜適値に
設定し得るために、周波数特iおよび飽和特性を改善す
゛ることかでき為。
Furthermore, the frequency characteristics and saturation characteristics are improved so that recording bias current values can be set at appropriate values for nine iron cores 7 (10) and 8 (9) K in response to each expanded band. Because of Kadeki.

また、母音バイアス電流に基づく録音信号レベルの増加
があるために1この増加の分だけ鉄心の□#、L?4、
。じ46カ、84,7.1って低域側を受持つ鉄心7お
よび1bの幅幻 およびatOを広くミ高域側を受□持
つ鉄心8および9の幅a8 およびms を狭くするこ
とが可能であシ、鉄心7 (10)の幅at(ato)
>鉄心8(9)の幅ms (11G)として磁気テープ
10幅方向分割に基づく再生レベルの低下を軽減するこ
とができる。
Also, since there is an increase in the recording signal level based on the vowel bias current, the iron core □ #, L? 4,
. 46, 84, 7.1, the widths a8 and ms of cores 7 and 1b, which handle the low frequency side, are widened, and the widths a8 and ms of cores 8 and 9, which handle the high frequency side, can be made narrower. Possible, width at (ato) of iron core 7 (10)
>The width of the iron core 8 (9) ms (11G) can reduce the reduction in the reproduction level due to the division of the magnetic tape 10 in the width direction.

また、第1および第2の鉄心7および8、第3および第
4の鉄心9およびlOによシ周波数分割して音声信号を
記録した磁゛気テープにおいてそのトラック上の情報線
従来の場−合と同一であシ、かつ第1および第2の鉄心
7および8、第3および第4の鉄心9および10を有す
る磁気λラドと第1図に示した如〈従来の鉄心2を有す
る従来の磁気ヘッドとはトラックに対して機械的に互換
性があるために、本実施例によシ鈴音した磁気量−プを
従来の磁気ヘッドによシ再生しても正常に音声信号出力
を得′ることかでき、従来の録音方法と互換性がある。
In addition, in a magnetic tape on which an audio signal is recorded by dividing the frequency by the first and second iron cores 7 and 8 and the third and fourth iron cores 9 and 1O, the information line on the track is As shown in FIG. Since the track is mechanically compatible with the magnetic head of the present invention, it is possible to normally obtain audio signal output even if the magnetic head that generates the sound of this embodiment is reproduced by a conventional magnetic head. It is compatible with traditional recording methods.

        ゛ なお、以上説明した一実施例は入力音声信号の周波数1
域を2分割するとともにミ鉄心の空隙長もかつ空W*さ
もそれぞれ低域側と高域”側とに対応して設定した場谷
の例であるが、鉄心の空隙長さまたは空隙深さの何れか
一方を設定してもほぼ同様の効果を得る仁とができる。
゛In addition, in the embodiment described above, the frequency 1 of the input audio signal is
This is an example of a case where the area is divided into two, and the gap length of the iron core is also set corresponding to the low-frequency side and the high-frequency side, respectively. Almost the same effect can be obtained by setting either one of them.

また、以上説明した一実施例は入力音声信号のができる
Furthermore, the embodiment described above can handle input audio signals.

また、磁気ヘッドは録音パ再生兼用として説明したが、
鈴音用と再生用とがそれぞれ専用の場合にも本発明を適
用することができる。
Also, the magnetic head was explained as being used for both recording and playback purposes, but
The present invention can also be applied to a case where bell sounds and playback are respectively dedicated.

以上説明した如く本発明によれば、入力音声信号の周波
数帯域を分割し、この分割数に対応して磁気テープの1
トラック幅内に磁気ヘッドの鉄心を対向させ、鉄心の空
隙長さ、または/および鉄心の空隙深さを帯域分割した
各々の録音信号の波長に対応して最適に設定することに
よシ、綜合的に歪と周波数特性を改善することができ、
かつそれぞれの鉄心に対して録音バイアス電流を最適に
設定することによって周波数特性および飽和特性を改善
するζ、とができる。
As explained above, according to the present invention, the frequency band of an input audio signal is divided, and one part of the magnetic tape is divided corresponding to the number of divisions.
This is achieved by arranging the iron cores of the magnetic heads to face each other within the track width and optimally setting the gap length and/or the gap depth of the iron cores in accordance with the wavelength of each band-divided recording signal. can improve distortion and frequency characteristics,
Furthermore, by optimally setting the recording bias current for each core, it is possible to improve the frequency characteristics and saturation characteristics.

ま九、鉄心の幅を選定すると七によって、再生レベルの
低下を軽減することができる。
(9) By selecting the width of the iron core, it is possible to reduce the decrease in the regeneration level.

また従来の鈴音方法との互換性も有している。It is also compatible with the conventional Suzune method.

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

第1図は従来の録音方法によるときの磁気ヘッドの鉄心
と磁気テープとの位置関係を示す関係図。 第2図は本発明方法を適用した一実施例における磁気ヘ
ッドの鉄心と磁気テープとの位置関係を示す関係図。 第3図(1)および(b)は第2図における鉄心の平面
図。 第一4図は本発明方法を適用した一実施例における場合
の鈴音・再生回路のブロック図〇第5図は第4図におけ
るp−パスフィルタとバイパスフィルタの振幅特性図。 l・・・・・・磁気テープ、5および6・・・・・・ト
ラック、7.8.9および10・・・・・・磁気ヘッド
の第1、第2、第3および第4の鉄心、11・・・・・
・録音増幅器、12・・・・・・鈴音バイアス発振器、
13・・・・・・鐘音/再生の切替スイッチ、14・・
・・・・再生増幅器、161および163・・・・・・
−一バスフィルタ、163お!び164・・・・・・バ
イパスフィルタ、171〜174・・・・・・イコライ
ず、181〜184・・・・・・駆動回路。 特許出願人 トリオ株式会社
FIG. 1 is a relationship diagram showing the positional relationship between the core of the magnetic head and the magnetic tape when using a conventional recording method. FIG. 2 is a relationship diagram showing the positional relationship between the core of the magnetic head and the magnetic tape in an embodiment to which the method of the present invention is applied. FIGS. 3(1) and 3(b) are plan views of the iron core in FIG. 2. FIG. 14 is a block diagram of a bell sound reproduction circuit in one embodiment to which the method of the present invention is applied; FIG. 5 is an amplitude characteristic diagram of the p-pass filter and bypass filter in FIG. 4. l...magnetic tape, 5 and 6...track, 7.8.9 and 10...first, second, third and fourth iron cores of magnetic head , 11...
・Recording amplifier, 12...Suzune bias oscillator,
13...Bell tone/playback switch, 14...
...Regenerative amplifier, 161 and 163...
-One bus filter, 163! 164...Bypass filter, 171-174...Equalization, 181-184...Drive circuit. Patent applicant: Trio Co., Ltd.

Claims (3)

【特許請求の範囲】[Claims] (1)  被記録信号としての入力信号の周波数帯域を
複数の周波数帯域に分割し、分割し九それぞれの周波数
帯域に対応して空隙長さと空隙深さとの少なくとも何れ
か一方を変えた磁気ヘッドの鉄心を設け、磁気テープの
幅方向に前記鉄心を前記磁気テープの1トラツク幅内に
位置するように配置し、前記鉄心に巻回されたコイルの
それぞれに帯域分割され九備考電流と周波数帯域に応じ
た最適のバイアス電流とを流して、前記1トラツク幅内
に周波数帯域を分割された各信号を並列に記帰するヒと
を特徴とする磁気テープへの鈴音方法。
(1) A magnetic head in which the frequency band of an input signal as a recorded signal is divided into a plurality of frequency bands, and at least one of the gap length and the gap depth is changed in accordance with each frequency band. An iron core is provided, and the iron core is arranged in the width direction of the magnetic tape so that it is located within one track width of the magnetic tape, and the band is divided into each of the coils wound around the iron core. 1. A method for producing bells on a magnetic tape, characterized in that each signal having a frequency band divided within the one track width is recorded in parallel by flowing an optimum bias current corresponding to the track width.
(2)  磁気ヘッドの鉄心の幅線周波数帯域に応じて
異なっていることを特徴とする特許請求の範囲第1項記
載の磁気テープへの鈴音方法。
(2) The method for producing bells on a magnetic tape according to claim 1, wherein the method differs depending on the width line frequency band of the iron core of the magnetic head.
(3)  磁気ヘッドの鉄心の幅は同一であることを特
徴とする特許請求の範囲第1項記載の磁気テープへの鈴
音方法。
(3) The method for producing bells on a magnetic tape according to claim 1, wherein the widths of the cores of the magnetic heads are the same.
JP14592781A 1981-09-16 1981-09-16 Sound recording method to magnetic tape Pending JPS5848208A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP14592781A JPS5848208A (en) 1981-09-16 1981-09-16 Sound recording method to magnetic tape

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP14592781A JPS5848208A (en) 1981-09-16 1981-09-16 Sound recording method to magnetic tape

Publications (1)

Publication Number Publication Date
JPS5848208A true JPS5848208A (en) 1983-03-22

Family

ID=15396289

Family Applications (1)

Application Number Title Priority Date Filing Date
JP14592781A Pending JPS5848208A (en) 1981-09-16 1981-09-16 Sound recording method to magnetic tape

Country Status (1)

Country Link
JP (1) JPS5848208A (en)

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5282207A (en) * 1975-12-27 1977-07-09 Kenzou Inoue Magnetic recorder
JPS52121307A (en) * 1976-04-05 1977-10-12 Toshiba Corp Magnetic recording and reproducing system
JPS5680808A (en) * 1979-12-07 1981-07-02 Victor Co Of Japan Ltd Signal recording system

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5282207A (en) * 1975-12-27 1977-07-09 Kenzou Inoue Magnetic recorder
JPS52121307A (en) * 1976-04-05 1977-10-12 Toshiba Corp Magnetic recording and reproducing system
JPS5680808A (en) * 1979-12-07 1981-07-02 Victor Co Of Japan Ltd Signal recording system

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