JPH0366722B2 - - Google Patents

Info

Publication number
JPH0366722B2
JPH0366722B2 JP56211716A JP21171681A JPH0366722B2 JP H0366722 B2 JPH0366722 B2 JP H0366722B2 JP 56211716 A JP56211716 A JP 56211716A JP 21171681 A JP21171681 A JP 21171681A JP H0366722 B2 JPH0366722 B2 JP H0366722B2
Authority
JP
Japan
Prior art keywords
magnetic
magnetic head
head
gap length
magnetic recording
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 - Lifetime
Application number
JP56211716A
Other languages
Japanese (ja)
Other versions
JPS58114319A (en
Inventor
Shigemitsu Hamazaki
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.)
Fujitsu Ltd
Original Assignee
Fujitsu 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 Fujitsu Ltd filed Critical Fujitsu Ltd
Priority to JP21171681A priority Critical patent/JPS58114319A/en
Publication of JPS58114319A publication Critical patent/JPS58114319A/en
Publication of JPH0366722B2 publication Critical patent/JPH0366722B2/ja
Granted 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
    • G11B5/012Recording on, or reproducing or erasing from, magnetic disks

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は磁気デイスク装置の記録/再生に用い
られる磁気ヘツドに関わり、特に、磁気デイスク
の内周部と外周部に夫々専用のものとして用意さ
れる磁気ヘツドに関わる。
[Detailed Description of the Invention] [Field of Industrial Application] The present invention relates to a magnetic head used for recording/reproducing in a magnetic disk device, and in particular, a magnetic head provided exclusively for the inner and outer circumferential portions of a magnetic disk. related to magnetic heads.

電算機システムを構成する大容量記憶装置の一
つに磁気デイスク装置がある。該装置は磁気デイ
スクの直径を大にし、或いは同一回転軸に取りつ
けられるデイスク数を増すことによつて、記憶容
量を増加させることが可能で、大型電算機システ
ムの記憶媒体として多用されている。
A magnetic disk device is one of the mass storage devices that constitute a computer system. This device can increase the storage capacity by increasing the diameter of the magnetic disk or by increasing the number of disks attached to the same rotating shaft, and is often used as a storage medium in large computer systems.

〔従来技術と発明が解決すべき課題〕[Prior art and issues to be solved by the invention]

磁気デイスク記録領域には回転軸を中心とする
同心円状のトラツクが設定され、各トラツクには
円周方向に記録ビツトが並ぶ形で磁気記録が行わ
れる。デイスクの回転速度は一定であるから、ビ
ツト密度は外周になるほど疎となり、記録される
波長は長くなる。
Concentric tracks centered around the rotation axis are set in the magnetic disk recording area, and magnetic recording is performed on each track with recording bits arranged circumferentially. Since the rotational speed of the disk is constant, the bit density becomes sparser toward the outer periphery, and the recorded wavelength becomes longer.

磁気ヘツドのコアのギヤツプ(以下、ギヤツプ
と略称)は、記録すべき最短波長のデータに対し
て十分に狭く且つ十分な分解能を備えることが必
要である。即ち、磁気デイスクの最内周トラツク
に対してもこの条件を満たすことが必要である
が、このように定めたギヤツプ長を持つ単一のヘ
ツドでデイスク全域をカバーしようとすると、最
外周に近い辺りでは、記録波長に対してギヤツプ
長が狭くなりすぎる。
The gap in the core of the magnetic head (hereinafter abbreviated as gap) must be sufficiently narrow and have sufficient resolution for the shortest wavelength data to be recorded. In other words, it is necessary to satisfy this condition even for the innermost track of a magnetic disk, but if you try to cover the entire disk area with a single head with the gap length determined in this way, it is necessary to satisfy this condition for the track near the outermost track. Around this point, the gap length becomes too narrow relative to the recording wavelength.

ギヤツプ長が狭すぎると磁気記録媒体を十分に
磁化することができないため、前歴特性が低下す
るばかりでなく、比較的疎なビツト密度に対して
は分解能がよくなりすぎ、取り扱う信号に対しラ
イトコンペ等の復調回路系が適切でなくなるた
め、ビツトエラーが生ずることになる。
If the gap length is too narrow, the magnetic recording medium cannot be sufficiently magnetized, which not only deteriorates the antecedent characteristics, but also makes the resolution too good for relatively sparse bit densities, making it difficult to write competitively with the signals being handled. Since the demodulation circuit system is no longer appropriate, bit errors will occur.

第1図は磁気デイスクの2分割された磁気記録
面を示す図であつて、1は磁気デイスク、2はア
クセスアーム、2a,2bは磁気ヘツド、3は内
周部、4は外周部である。磁気デイスクの回転速
度が一定であれば記録ビツト5の1ビツト当たり
の中心角は内外とも同じであり、1ビツトの長さ
は外周ほど大となることは図から明らかである。
FIG. 1 is a diagram showing the magnetic recording surface of a magnetic disk divided into two parts, where 1 is the magnetic disk, 2 is an access arm, 2a and 2b are magnetic heads, 3 is an inner circumferential portion, and 4 is an outer circumferential portion. . It is clear from the figure that if the rotational speed of the magnetic disk is constant, the central angle per one recording bit 5 is the same inside and outside, and the length of one bit increases as the outer circumference approaches.

本発明の目的は、磁気ヘツドが備える分解能、
前歴特性等の電磁変換特性に於いて、内周部/外
周部の差を極力減少させた磁気ヘツドを提供する
ことである。
The object of the present invention is to improve the resolution of a magnetic head;
It is an object of the present invention to provide a magnetic head in which the difference between the inner circumferential portion and the outer circumferential portion in electromagnetic conversion characteristics such as antecedent characteristics is reduced as much as possible.

〔課題を解決するための手段〕[Means to solve the problem]

本発明では上記の問題を解決するため本発明の
磁気ヘツドは、 内周部及び外周部に夫々専用の磁気ヘツドを用
意し、 個々のヘツドが担当する磁気記録領域の最短記
録波長λと磁気ヘツドのコアのギヤツプ長gとの
間にg=λ/ηが成立する常数ηを想定し、 内周部の磁気ヘツドの該常数η0と外周部の該常
数η〓は |η〓−η0|≦1 なる関数を満たすようにg〓及びg0が設定されたも
のである。
In order to solve the above problem, the magnetic head of the present invention has dedicated magnetic heads for the inner circumference and the outer circumference, and the shortest recording wavelength λ of the magnetic recording area handled by each head and the magnetic head Assuming a constant η such that g = λ/η holds between the gap length g of the core, the constant η 0 of the magnetic head in the inner circumference and the constant η〓 of the outer circumference are |η〓−η 0 g〓 and g 0 are set so as to satisfy the function |≦1.

〔作用〕[Effect]

ビツト長が大である領域に対しては磁気ヘツド
のギヤツプを大にすれば良いわけであるが、恣意
的にこれを設定してもよいわけではない。本発明
の如く、最短記録波長λと磁気ヘツドのコアのギ
ヤツプ長gとの関係をほゞ一定に保ちつつギヤツ
プ長を変化させれば、分解能を過度に上昇させる
ことが避けられるのみならず、内周部及び外周部
夫々に於ける磁気記録の読み取り出力を、最高周
波数と最低周波数で近似したものとすることがで
き、ピークシフトに対する回路的補正が容易なも
のとなる。
For regions where the bit length is large, it is sufficient to increase the gap of the magnetic head, but this does not mean that it can be set arbitrarily. By varying the gap length while keeping the relationship between the shortest recording wavelength λ and the gap length g of the core of the magnetic head approximately constant as in the present invention, it is possible not only to avoid an excessive increase in resolution, but also to The readout output of the magnetic recording in the inner circumferential portion and the outer circumferential portion can be approximated by the highest frequency and the lowest frequency, and circuit correction for peak shift becomes easy.

本発明の作用・効果は実地に即して説明するの
が適当であるから、その詳細な説明は次項の実施
例の説明に含めて行うことにする。
Since it is appropriate to explain the functions and effects of the present invention based on actual conditions, the detailed explanation will be included in the description of the embodiments in the next section.

〔実施例〕〔Example〕

第1図は実施例の磁気記録装置の磁気記録面を
示す図である。のデイスク装置に於いて、内周部
13の最内周トラツクの直径201mm、最外周トラ
ツクの直径265mmであり、外周部の最内周トラツ
クの直径275mm、最外周トラツクの直径339mmであ
る。これを回転速度3600rpm、周波数5MHzで使
用すると、内周部の最内周トラツクのビツト長は
8μm、外周部の最内周トラツクのビツト長は
10.8μmとなる。
FIG. 1 is a diagram showing a magnetic recording surface of a magnetic recording device according to an embodiment. In this disk device, the diameter of the innermost track of the inner circumference part 13 is 201 mm, the diameter of the outermost track is 265 mm, the diameter of the innermost track of the outer circumferential part is 275 mm, and the diameter of the outermost track is 339 mm. When this is used at a rotation speed of 3600 rpm and a frequency of 5 MHz, the bit length of the innermost track on the inner circumference is
8μm, the bit length of the innermost track on the outer periphery is
It becomes 10.8μm.

その磁気デイスクの記録/再生用磁気ヘツドの
ギヤツプ長を、内周用1.4μm、外周用1.9μmに設
定する。この場合には前記常数ηは内周部で
5.71、外周部で5.68となり、両者はほゞ近似して
いる。
The gap length of the recording/reproducing magnetic head of the magnetic disk is set to 1.4 μm for the inner circumference and 1.9 μm for the outer circumference. In this case, the constant η is at the inner circumference.
5.71, and 5.68 at the outer periphery, and the two are almost similar.

第3図及び第4図は上記磁気デイスク装置に於
ける周波数特性及び前歴特性である。先ず、第3
図について説明する。
FIGS. 3 and 4 show the frequency characteristics and antecedent characteristics of the magnetic disk device. First, the third
The diagram will be explained.

同図は前記のようにηが設定された磁気ヘツド
に於ける、ビツト密度とヘツド出力の関係を示し
ており、実線15は内周部の磁気ヘツドに関わる
もの、破線17はこれと同じギヤツプ長のヘツド
を外周部に用いた場合に関わるものである。更
に、実線16は本発明によりギヤツプ長を定めた
ヘツドを外周部に用いた場合である。
The figure shows the relationship between bit density and head output in a magnetic head with η set as described above, where the solid line 15 relates to the magnetic head at the inner circumference, and the broken line 17 relates to the same gap. This is relevant when a long head is used on the outer periphery. Further, a solid line 16 shows a case where a head with a defined gap length according to the present invention is used at the outer periphery.

図の横軸は単位長当たりのビツト数であるか
ら、同じ最高周波数と最低周波数に対応する範囲
は、内周部では図の右寄りにあつて広い幅の領域
となるのに対し、外周部では左寄りにあつてより
狭い幅の領域となる。そのため、破線17の当該
範囲における最大出力/最小出力の比率は、実線
15に於ける当該範囲の同種比率よりも小であ
る。
Since the horizontal axis of the diagram is the number of bits per unit length, the range corresponding to the same highest and lowest frequencies is a wide area toward the right of the diagram at the inner periphery, while at the outer periphery. The area is closer to the left and has a narrower width. Therefore, the maximum output/minimum output ratio in the range indicated by the broken line 17 is smaller than the same ratio in the range indicated by the solid line 15.

ところが、外周部の磁気ヘツドのギヤツプ長を
拡げることにより、この磁気ヘツド出力が実線1
6で示されるようなものになれば、当該範囲にお
ける最大出力/最少出力の比率は増加し、実線1
5に於ける当該周波数範囲の最大出力/最少出力
の比率に近いものとなる。
However, by widening the gap length of the magnetic head on the outer periphery, the output of this magnetic head changes to the solid line 1.
6, the ratio of maximum output/minimum output in the range increases, and the solid line 1
The ratio is close to the maximum output/minimum output ratio in the frequency range in No. 5.

このように夫々の磁気ヘツドにおける出力の周
波数依存度を近似させておけば、信号位置のずれ
(ピークシフト)を回路的に補正することが容易
となる。
By approximating the frequency dependence of the output of each magnetic head in this way, it becomes easy to correct the signal position shift (peak shift) using a circuit.

次に第4図を説明する。前歴特性は、当業者に
周知の如く、或るデータを記録したトラツクに異
なるデータを上書きした時に旧データがどれだけ
減衰するかを示すものと見做してよく、当然のこ
とながらこの減衰量は大きいほど優れている。
Next, FIG. 4 will be explained. As is well known to those skilled in the art, the prior history characteristic can be regarded as indicating how much old data is attenuated when a track on which certain data is recorded is overwritten with different data, and naturally, this attenuation amount is The larger the value, the better.

図の実線18は内周部に於ける前歴特性、実線
19は本発明による外周部の前歴特性であつて、
外周部のヘツドを内周部と同じにした場合の前歴
特性である破線20に比べ、実線19は旧データ
がより大幅に減衰することを示している。なお図
の横軸の単位はアンペア・ターンである。
The solid line 18 in the figure is the antecedent characteristic at the inner circumference, and the solid line 19 is the antecedent characteristic at the outer circumference according to the present invention.
Compared to the dashed line 20, which is the previous history characteristic when the head of the outer circumference is the same as the inner circumference, the solid line 19 indicates that the old data is more significantly attenuated. The unit of the horizontal axis in the figure is ampere-turn.

本発明の実施に当たつて、前記常数ηは両磁気
ヘツドで等しいことが望ましいが、若干のずれが
あつても同じ効果を得ることができる。通常の磁
気ヘツドではこのηの値が3より小に設定される
ことは殆どなく、両磁気ヘツドのηが異なる時の
許容範囲は±1程度とみることができる。
In implementing the present invention, it is desirable that the constant .eta. be equal for both magnetic heads; however, even if there is a slight deviation, the same effect can be obtained. In a normal magnetic head, the value of η is almost never set to less than 3, and when the η of the two magnetic heads are different, the allowable range can be considered to be approximately ±1.

〔効果〕〔effect〕

以上説明した如く、内周部の磁気ヘツドのギヤ
ツプ長と外周部の磁気ヘツドのギヤツプ長を、η
を共有するように設定することによつて、分解能
特性及び前歴特性を、復調回路に於いて処理容易
な範囲に収めることができ、信頼性の高い磁気デ
イスク装置が実現することになる。
As explained above, the gap length of the magnetic head on the inner circumference and the gap length of the magnetic head on the outer circumference are expressed as η
By setting the data to be shared, the resolution characteristics and antecedent characteristics can be kept within a range that can be easily processed by the demodulation circuit, and a highly reliable magnetic disk device can be realized.

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

第1図は磁気デイスクの2分割された磁気記録
面を示す図、第2図は実施例の磁気記録装置の磁
気記録面を示す図、第3図は実施例に於けるビツ
ト密度とヘツド出力の関係を示す図、第4図は実
施例に於ける前歴特性を示す図、であつて、 1は磁気デイクス、2はアクセスアーム、2
a,2bは磁気ヘツド、3,13は内周部、4,
14は外周部、5は記録ビツト、15〜17はヘ
ツド出力特性線、16〜18は前歴特性線であ
る。
Fig. 1 is a diagram showing the magnetic recording surface divided into two parts of a magnetic disk, Fig. 2 is a diagram showing the magnetic recording surface of the magnetic recording device of the embodiment, and Fig. 3 is a diagram showing the bit density and head output in the embodiment. FIG. 4 is a diagram showing the antecedent characteristics in the embodiment, in which 1 is a magnetic disk, 2 is an access arm, 2 is a diagram showing the relationship between
a, 2b are magnetic heads, 3, 13 are inner peripheral parts, 4,
Reference numeral 14 indicates the outer circumference, 5 indicates recording bits, 15 to 17 indicate head output characteristic lines, and 16 to 18 indicate previous history characteristic lines.

Claims (1)

【特許請求の範囲】 1 中心軸周りに回転するデイスクの表面に磁気
記録領域が設けられ、該磁気記録領域の内周部及
び外周部は別個の磁気ヘツドによつて記録/再生
されるように構成された磁気記録装置に用いられ
る磁気ヘツドであつて、 前記磁気記録領域の内周部に於いて、最短記録
波長λ〓と前記磁気ヘツドのコアのギヤツプ長g〓
の関係はg〓=λ〓/η〓であり、 前記磁気記録領域の外周部に於いて、最短記録
波長λ0と前記磁気ヘツドのコアのギヤツプ長g0
関係はg0=λ0/η0であるとした時に、 |η〓−η0|≦1 なる関係を満たして該コアのギヤツプg〓及びg0
設定されていることを特徴とする磁気ヘツド。
[Claims] 1. A magnetic recording area is provided on the surface of a disk that rotates around a central axis, and the inner and outer peripheries of the magnetic recording area are recorded/reproduced by separate magnetic heads. In the magnetic head used in the magnetic recording device configured, in the inner peripheral part of the magnetic recording area, the shortest recording wavelength λ〓 and the gap length g〓 of the core of the magnetic head
The relationship between the shortest recording wavelength λ 0 and the gap length g 0 of the core of the magnetic head at the outer periphery of the magnetic recording area is g 0 = λ 0 / 1. A magnetic head characterized in that the gap g and g 0 of the core are set to satisfy the following relationship: |η〓−η 0 |≦1 when η 0 .
JP21171681A 1981-12-25 1981-12-25 Magnetic head Granted JPS58114319A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP21171681A JPS58114319A (en) 1981-12-25 1981-12-25 Magnetic head

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP21171681A JPS58114319A (en) 1981-12-25 1981-12-25 Magnetic head

Publications (2)

Publication Number Publication Date
JPS58114319A JPS58114319A (en) 1983-07-07
JPH0366722B2 true JPH0366722B2 (en) 1991-10-18

Family

ID=16610410

Family Applications (1)

Application Number Title Priority Date Filing Date
JP21171681A Granted JPS58114319A (en) 1981-12-25 1981-12-25 Magnetic head

Country Status (1)

Country Link
JP (1) JPS58114319A (en)

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS55135315A (en) * 1979-03-30 1980-10-22 Basf Ag Data memory system and magnetic disc for same

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS55135315A (en) * 1979-03-30 1980-10-22 Basf Ag Data memory system and magnetic disc for same

Also Published As

Publication number Publication date
JPS58114319A (en) 1983-07-07

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