JPH0114992Y2 - - Google Patents

Info

Publication number
JPH0114992Y2
JPH0114992Y2 JP9027981U JP9027981U JPH0114992Y2 JP H0114992 Y2 JPH0114992 Y2 JP H0114992Y2 JP 9027981 U JP9027981 U JP 9027981U JP 9027981 U JP9027981 U JP 9027981U JP H0114992 Y2 JPH0114992 Y2 JP H0114992Y2
Authority
JP
Japan
Prior art keywords
magnetic head
core
external radio
core half
turns
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.)
Expired
Application number
JP9027981U
Other languages
Japanese (ja)
Other versions
JPS57201611U (en
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 filed Critical
Priority to JP9027981U priority Critical patent/JPH0114992Y2/ja
Publication of JPS57201611U publication Critical patent/JPS57201611U/ja
Application granted granted Critical
Publication of JPH0114992Y2 publication Critical patent/JPH0114992Y2/ja
Expired legal-status Critical Current

Links

Landscapes

  • Magnetic Heads (AREA)

Description

【考案の詳細な説明】 本考案は、ビデオテープレコーダ等の磁気記録
再生装置に用いられる磁気ヘツドに関し、特にラ
ジオ放送の中波AM放送電波等の外部電波の飛び
込みによつて生ずるビート等の発生の改善を図る
ようにしたものである。
[Detailed Description of the Invention] The present invention relates to a magnetic head used in magnetic recording and reproducing devices such as video tape recorders, and is particularly concerned with the generation of beats and the like caused by the intrusion of external radio waves such as medium-wave AM broadcast radio waves. The aim is to improve this.

従来、ビデオテープレコーダ等の磁気記録再生
装置に用いられる磁気ヘツド1は、第1図に示す
ように、一方のコア半体2とコイル挿通孔を構成
する切欠き凹部3を形成した他方のコア半体4と
をギヤツプ面5を突合せて形成したヘツドチツプ
6の各コア半体2,4にギヤツプ面5を介してそ
れぞれコイル7,7の巻き数を同数にしたいわゆ
るバランス巻きによる巻線方法によつて構成され
ている。
Conventionally, a magnetic head 1 used in a magnetic recording/reproducing device such as a video tape recorder, as shown in FIG. A winding method using so-called balance winding in which coils 7, 7 are wound with the same number of turns on each core half 2, 4 of a head chip 6 formed by abutting the half body 4 with the gap surface 5 through the gap surface 5, respectively. It is structured accordingly.

このように構成された磁気ヘツド1の外部電波
の飛び込み特性を第2図に示すように構成した測
定系により測定したところ、上記磁気ヘツド1の
外部電波の飛び込み特性としてのヘツド固定時の
指向特性は第3図中実線イで示すような方向依存
性をもつものとなる。
When the external radio wave intrusion characteristics of the magnetic head 1 configured as described above were measured using a measurement system configured as shown in FIG. has a directional dependence as shown by the solid line A in FIG.

上記外部電波の飛び込み特性の測定系は、モー
タ8によつて回転駆動されるビデオテープレコー
ダ用の回転ドラム9に被測定用の磁気ヘツド1を
取付ける。この磁気ヘツド1から距離rを略56cm
離間して直径1mmの銅線を9回巻きした送信アン
テナ10を設置し、このアンテナ10を介して発
信器11から周波数693KHzの外部電波を発信す
る。そして、上記磁気ヘツド1を回転させながら
この磁気ヘツド1に飛び込む上記外部電波をアン
プ12を通じてスペクトラムアナライザ13で測
定する。
In the system for measuring the characteristics of external radio waves, a magnetic head 1 to be measured is attached to a rotating drum 9 for a video tape recorder which is rotationally driven by a motor 8. The distance r from this magnetic head 1 is approximately 56 cm.
A transmitting antenna 10 made of a copper wire wound nine times with a diameter of 1 mm is installed at a distance, and an external radio wave with a frequency of 693 KHz is transmitted from a transmitter 11 via this antenna 10. Then, while the magnetic head 1 is being rotated, the external radio wave that enters the magnetic head 1 is measured by a spectrum analyzer 13 through an amplifier 12.

上述のような測定系によつて測定される従来用
いられている磁気ヘツド1の外部電波の飛び込み
特性は、第3図から明らかなように、各コア半体
2,4の突き合せ面を基準線としたとき、切欠き
凹部3を形成した他方のコア半体4側45度方向か
ら飛び込む外部電波の入力レベルは一方のコア半
体2側45度方向から飛び込む外部電波の入力レベ
ルに対し10dbも悪くなり、外部電波の入力方向
により著しい差を生ずる。このように、従来の磁
気ヘツド1は、外部電波の入力方向に対して著し
い方向依存性を有している。
As is clear from FIG. 3, the intrusion characteristics of external radio waves of the conventionally used magnetic head 1 measured by the measurement system described above are based on the abutting surfaces of the core halves 2 and 4. When it is a line, the input level of the external radio wave coming in from the 45 degree direction on the other core half 4 side where the notch recess 3 is formed is 10 db compared to the input level of the external radio wave coming in from the 45 degree direction on the one core half 2 side. This also causes significant differences depending on the input direction of external radio waves. As described above, the conventional magnetic head 1 has a significant directional dependence on the input direction of external radio waves.

そして、ビデオテープレコーダに磁気ヘツドを
実装し、該ビデオテープレコーダによりビデオ信
号を上記磁気ヘツドから再生するとき、この磁気
ヘツドに外部電波が飛び込むとこの外部電波の周
波数f1と低減変換クロマ周波数f2の差f1−f2がビ
ートとなつて再生画像を防害する作用をするが、
上記従来の磁気ヘツド1における他方のコア半体
4側45度方向から飛び込む外部電波の入力レベル
は、再生画像上明らかにビートとなつて現出させ
るレベルであり画質評価を著しく悪化させてい
る。
When a magnetic head is mounted on a video tape recorder and the video tape recorder reproduces a video signal from the magnetic head, when an external radio wave jumps into the magnetic head, the frequency f 1 of the external radio wave and the reduced converted chroma frequency f The difference f 1 − f 2 between 2 becomes a beat and acts to prevent damage to the reproduced image, but
In the conventional magnetic head 1, the input level of the external radio wave coming in from the 45-degree direction on the other core half 4 side is at a level that clearly appears as a beat on the reproduced image, significantly deteriorating the image quality evaluation.

そこで、本考案は外部電波飛び込み特性の方向
依存性をなくし、外部電波飛び込みレベルの最大
値を低くおさえるようにし、ビデオテープレコー
ダ等の磁気記録再生装置に実装したとき良好な再
生画像を得られる磁気ヘツドを提供しようとする
ものである。
Therefore, the present invention eliminates the directional dependence of the external radio wave drop-in characteristics, suppresses the maximum value of the external radio wave drop-in level to a low value, and provides a magnetic field that provides good playback images when implemented in a magnetic recording/playback device such as a video tape recorder. It is intended to provide a head.

本考案によつて構成される磁気ヘツド21は、
一対のコア半体22,23のギヤツプ面24を突
き合せてヘツドチツプ25を形成し、上記各コア
半体22,23のそれぞれにギヤツプ面24を介
してコイル26,27を巻線して構成してなるも
のである。
The magnetic head 21 constructed according to the present invention is
A head chip 25 is formed by abutting the gap surfaces 24 of the pair of core halves 22 and 23, and coils 26 and 27 are wound around each of the core halves 22 and 23 via the gap surfaces 24. This is what happens.

このように構成される磁気ヘツド21におい
て、上記一対のコア半体22,23のうちの一方
のコア半体22の巻線部28の断面積は他方のコ
ア半体23の巻線部29の断面積より大きく形成
されている。すなわち、他方のコア半体23の巻
線部29には、各コア半体22,23に巻装され
るコイル26,27が挿通する巻線穴を構成する
ように切欠き凹部30が形成され、この切欠き凹
部30を形成することにより、この一方のコア半
体22の巻線部28の断面積は他方のコア半体2
3の巻線部29より大きいものとされる。
In the magnetic head 21 configured in this manner, the cross-sectional area of the winding portion 28 of one of the pair of core halves 22 and 23 is equal to that of the winding portion 29 of the other core half 23. It is formed larger than the cross-sectional area. That is, a notch recess 30 is formed in the winding portion 29 of the other core half 23 so as to constitute a winding hole through which the coils 26 and 27 wound around the respective core halves 22 and 23 are inserted. , by forming this notch recess 30, the cross-sectional area of the winding portion 28 of this one core half 22 is made smaller than that of the other core half 22.
The winding portion 29 of No. 3 is larger than the winding portion 29 of No. 3.

そして、巻線部28の断面積の大きな一方のコ
ア半体22には、巻線部29の断面積の小さな他
方のコア半体23に巻回されるコイル27の巻き
数に対し1.5〜3倍の巻き数をもつてコイル26
が巻回されている。
The number of turns of the coil 27 wound around the other core half 23 of the winding part 29 having a small cross-sectional area is 1.5 to 3 turns on one core half 22 having a large cross-sectional area of the winding part 28. Coil 26 with double the number of turns
is wound.

ここで、ギヤツプ面24を介して一方及び他方
のコア半体22,23に巻回される各コイル2
6,27の巻き数の比を変化させた場合における
磁気ヘツド21の外部電波飛び込み特性を前述し
た第2図に示したような測定系により測定する
と、各巻き数を変化させた場合の外部電波飛び込
み特性の最大レベル点をとつて比較すると第5図
に示すようになる。このとき、一方のコア半体2
2及び他方のコア半体23に巻回されるコイル2
6,27の巻き数の比が、従来のバランス巻きの
磁気ヘツド1と略等しい8:9の場合を0dbとし
て比較すると各コア半体22,23に巻回される
コイルの巻き数の比が2:1の比をもつて巻回し
た場合を最底レベルにして第5図に示すように変
化する。そして、一方のコア半体22に巻回され
たコイル26の巻き数を他方のコア半体23に巻
回されたコイル27の巻き数に対し1.5〜3倍と
すると、最大レベル点において2〜3db外部電波
飛び込み特性が改善される。
Here, each coil 2 is wound around one core half body 22 and the other core half body 23 through a gap surface 24.
When the external radio wave penetration characteristics of the magnetic head 21 are measured by changing the ratio of the number of turns 6 and 27 using the measurement system shown in Fig. 2, the external radio waves when the number of turns is changed are Fig. 5 shows a comparison of the maximum level points of the diving characteristics. At this time, one core half 2
2 and the coil 2 wound around the other core half 23
When comparing the case where the ratio of the number of turns of the coils 6 and 27 is 8:9, which is almost the same as that of the conventional balanced winding magnetic head 1, and assuming 0 db, the ratio of the number of turns of the coils wound around each core half 22 and 23 is The lowest level is the case where the windings are wound at a ratio of 2:1, and changes as shown in FIG. If the number of turns of the coil 26 wound around one core half 22 is set to 1.5 to 3 times the number of turns of the coil 27 wound around the other core half 23, then at the maximum level point 2~ 3db external radio wave jump characteristics are improved.

そして、一方のコア半体22のコイル26の巻
き数を他方のコア半体23のコイル27の巻き数
に対し1.5〜3倍とすると、磁気ヘツド21の各
方向からの外部電波飛び込み特性は、第3図中破
線ロで示す如く全体に方向依存性がなくなり、且
つ各点における入力レベルが低く押えられる。
If the number of turns of the coil 26 of one core half 22 is set to 1.5 to 3 times the number of turns of the coil 27 of the other core half 23, the external radio wave penetration characteristics from each direction of the magnetic head 21 are as follows. As shown by the broken line B in FIG. 3, there is no directional dependence as a whole, and the input level at each point is kept low.

上述したような本考案によれば、たとえ外部電
波がビデオテープレコーダ等の磁気記録再生装置
に実装された磁気ヘツドに入力されても、再生画
像の画質に実質的に影響を与えない範囲の入力レ
ベルとすることができ、再生画像の画質の向上を
図ることができる。
According to the present invention as described above, even if external radio waves are input to a magnetic head installed in a magnetic recording/reproducing device such as a video tape recorder, the input is within a range that does not substantially affect the quality of the reproduced image. level, and the quality of the reproduced image can be improved.

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

第1図は従来例を示す模式図である。第2図は
外部電波の飛び込み特性を測定する測定和を示す
概略図である。第3図は従来例と本考案における
各方向からの外部電波飛び込み特性を示す特性図
である。第4図は本考案の一実施例を示す模式図
である。第5図は一方及び他方のコア半体に巻回
されるコイルの巻き数比に応じた外部電波飛び込
み特性を示す比較図である。 21…磁気ヘツド、22…一方のコア半体、2
3…他方のコア半体、26,27…コイル、2
8,29…巻線部。
FIG. 1 is a schematic diagram showing a conventional example. FIG. 2 is a schematic diagram showing a measurement sum for measuring the intrusion characteristics of external radio waves. FIG. 3 is a characteristic diagram showing characteristics of external radio wave intrusion from various directions in the conventional example and the present invention. FIG. 4 is a schematic diagram showing an embodiment of the present invention. FIG. 5 is a comparison diagram showing external radio wave jump characteristics depending on the turn ratio of the coils wound around one and the other core halves. 21... Magnetic head, 22... One core half, 2
3...Other core half, 26, 27...Coil, 2
8, 29... Winding section.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] ギヤツプ面を介して一対のコア半体それぞれに
巻線を施した磁気ヘツドにおいて、上記コア半体
のうち一方のコア半体の巻線部のコア断面積が他
方のコア半体の巻線部の断面積より大であり、上
記一方のコア半体に巻回されたコイルの巻き数が
上記他方のコア半体に巻回されたコイルの巻き数
の1.5〜3倍であることを特徴とする磁気ヘツド。
In a magnetic head in which wires are wound on each of a pair of core halves through a gap plane, the core cross-sectional area of the winding portion of one of the core halves is the same as that of the winding portion of the other core half. , and the number of turns of the coil wound around the one core half is 1.5 to 3 times the number of turns of the coil wound around the other half of the core. magnetic head.
JP9027981U 1981-06-19 1981-06-19 Expired JPH0114992Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP9027981U JPH0114992Y2 (en) 1981-06-19 1981-06-19

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP9027981U JPH0114992Y2 (en) 1981-06-19 1981-06-19

Publications (2)

Publication Number Publication Date
JPS57201611U JPS57201611U (en) 1982-12-22
JPH0114992Y2 true JPH0114992Y2 (en) 1989-05-02

Family

ID=29885400

Family Applications (1)

Application Number Title Priority Date Filing Date
JP9027981U Expired JPH0114992Y2 (en) 1981-06-19 1981-06-19

Country Status (1)

Country Link
JP (1) JPH0114992Y2 (en)

Also Published As

Publication number Publication date
JPS57201611U (en) 1982-12-22

Similar Documents

Publication Publication Date Title
US4652955A (en) Multi-head transducer assembly for helical scan video tape recorders
JPH0114992Y2 (en)
EP0219222B1 (en) Multi-head transducer assembly for helical scan video tape recorders
US4497004A (en) Picture reproducing apparatus in a helical scanning video tape recorder
US4796114A (en) Rotary head assembly with rigid adhesive bonding pole tips
JPS63192212A (en) Rotary transformer for electromagnetic conversion
JPS61182207A (en) Magnetic recorder/reproducer
JPS6316016Y2 (en)
US5734529A (en) Head drum assembly for use in a video cassette recorder
JPS61224106A (en) Magnetic recording and reproducing device
JP2804586B2 (en) Magnetic head and magnetic reproducing apparatus using the magnetic head
JPH0423324B2 (en)
JPH02108208A (en) Magnetic head
SU1115096A2 (en) Contactless current collector for rotary magnetic heads of video tape recorder
RU1770984C (en) Device for reproducing and recording radio signals received in tape
JPH0416241Y2 (en)
JPS6355853B2 (en)
JPS58111120A (en) Composite magnetic head
JPH048482Y2 (en)
SU972572A1 (en) Playback magnetic head
JPH0423292Y2 (en)
JPH02214109A (en) Rotary transformer
JPS6113286B2 (en)
JPH0325283Y2 (en)
KR0119825Y1 (en) Rotary transformer