Deprecated: The each() function is deprecated. This message will be suppressed on further calls in /home/zhenxiangba/zhenxiangba.com/public_html/phproxy-improved-master/index.php on line 456
JPS6158428B2 - - Google Patents
[go: Go Back, main page]

JPS6158428B2 - - Google Patents

Info

Publication number
JPS6158428B2
JPS6158428B2 JP58075245A JP7524583A JPS6158428B2 JP S6158428 B2 JPS6158428 B2 JP S6158428B2 JP 58075245 A JP58075245 A JP 58075245A JP 7524583 A JP7524583 A JP 7524583A JP S6158428 B2 JPS6158428 B2 JP S6158428B2
Authority
JP
Japan
Prior art keywords
tio
magnetic
bao
zro
voids
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
JP58075245A
Other languages
Japanese (ja)
Other versions
JPS59203771A (en
Inventor
Mitsuo Tamura
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.)
Tokin Corp
Original Assignee
Tohoku Metal Industries 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 Tohoku Metal Industries Ltd filed Critical Tohoku Metal Industries Ltd
Priority to JP58075245A priority Critical patent/JPS59203771A/en
Publication of JPS59203771A publication Critical patent/JPS59203771A/en
Publication of JPS6158428B2 publication Critical patent/JPS6158428B2/ja
Granted legal-status Critical Current

Links

Landscapes

  • Magnetic Heads (AREA)
  • Compositions Of Oxide Ceramics (AREA)

Description

【発明の詳細な説明】[Detailed description of the invention]

本発明は、各種磁気ヘツド特にフロツピーデイ
スクヘツドを構成する非磁性構造材料に関するも
のである。 従来より磁気ヘツド用非磁性構造材料としては
アルミナ、フオルステライト、ステアタイト磁器
等が用いられていた。しかしながらこれらの欠点
は、磁性材料のフエライトの組成が磁気ヘツドの
仕様の違いにより多少異なるため、それに応じて
熱膨張係数が変り、フエライトと非磁性材料の熱
膨張係数が一致せず、ガラスボンデイング工程で
いずれかに割れが生じ歩留りを低下させることで
あつた。 この磁気ヘツド用の非磁性材料は、常にフエラ
イトと同時に高速でフロツピーデイスク面を摺動
しながら移動する。従つて、その耐摩耗性がフエ
ライトと同程度でない場合、フエライト部と非磁
性材料との間にすき間を生じ、磁気ヘツドの機能
を低下させる。また材質の表面に30μ以上のボイ
ドがある場合、ボイド部から微少なカケを生じて
磁気記憶媒体の表面にキズをつける原因になる。
さらに、これらの構成部品は、精密な加工工程を
経て磁気ヘツドに加工するので、機械加工に際し
て適度の加工性の良さを要求される。 アルミナ、フオルステライト、ステアタイト等
はこれらの要求に対して満足できるものではな
く、最近になり、Ni―Znフエライトを用いるヘ
ツドに対しては、マイクロ波誘電体材料として既
知の材料であるBaO―TiO2―ZrO2系の磁器が用
いられるのが一般的になつている。これは、BaO
―TiO2―ZrO2系磁器が適度の加工性と耐摩耗性
を備え、かつ組成比の調整により機械的性質を損
うことなく90〜100×10-7/℃の範囲で熱膨張係
数を自由に変えることができることが見い出され
たことによる。 しかしながら、近年フロツピーデイスク装置の
高性能化がはかられるにつれて、磁気ヘツド材料
に対する要求も次第に激しくなり、研摩面のボイ
ドに対する要求値も5μ以下が標準となりつつあ
る。この要求に対してBaO―TiO2―ZrO2系磁器
は通常の製法では対応できなくなり、ホツトプレ
スや熱間静水圧プレス(HIP)が用いられてい
る。これらの高密度化の手法により研摩面のボイ
ドは一応要求性能を満足できるようになつたが価
格が高く巾広い普及がはばまれている。 本発明の目的は、通常の焼結手法ながら研摩面
のボイドが5μ以下で、熱膨張係数が90〜100×
10-7/℃のBaO―TiO2―ZrO2系の磁気ヘツド用
非磁性磁器組成物を提供するものである。 本発明は、TiO280〜91.0mol%、BaO6〜
16.0mol%、ZrO20.5〜3.0mol%、Al2O30.05〜
1.0mol%、Y2O30.05〜1.0mol%の成分範囲よりな
り合計が100mol%になる組成で熱膨張係数が90
×10-7/℃〜100×10-7/℃の範囲となることを
特徴とする磁気ヘツド用非磁性磁器組成物であ
る。 BaO―TiO2系においてTiO2のmol比が80モル%
以上の組成域ではBaT4O9の結晶相とTiO2の2つ
の結晶相から成ることが通常の相平衡状態図から
予想できるが、マイクロ波誘電体に関する詳細な
研究から第3の結晶相としてBa2Ti9O20が存在す
ることが確認され、さらにこの結晶相が含まれる
量が多い程磁器としての強度が向上することが知
られている。仮焼条件、焼結条件によりこの
Ba2Ti9O20の結晶相の生成量は異なるが、添加物
としてZrO2、SnO2、を含むと、Ba2Ti9O20の結晶
相の生成を促進できることが認められ、またこれ
により誘電特性が向上することから、BaO―
TiO2―ZrO2系磁器がマイクロ波の誘電体として
用いられていた。 磁気ヘツドの構造材用磁器としてBaO―TiO2
―ZrO2の磁器をみた場合、Ba2Ti9O20の生成によ
り機械的強度が増したことは応用上好都合であ
る。またBaOとTiO2の比率を変えることにより
Ba2Ti9O20の結晶相とTiO2の結晶相の比率をコン
トロールでき、双方の体積比で熱膨張係数をコン
トロールできるという長所がある。これらのこと
から、BaO―TiO2―ZrO2系の磁器が磁気ヘツド
用の構造材料として一般的に用いられるようにな
つた。 本発明におけるTiO2及びBaOの配合比率は熱
膨張係数を90×10-7/℃から100×10-7/℃の間
でコントロールするために必須のものである。 ZrO2は、上記説明のようにBa2Ti9O20の結晶相
の生成を促進させるためのものである。ZrO2
量が、0.5mol%未満では、この効果が認められ
ず、3mol%を越えると焼結過程で焼結体の内部
が還元しやすくなる。 焼結体の研磨面のボイドの大きさ及び量は仮焼
粉の粉砕後の粒径に反比例する。即ち粉砕が進行
するにつれて、焼結密度は向上し、研磨面のボイ
ドは小さくなりかつ数量も減る。ボイドの小さい
焼結体を得るためには、いかに効率の良い仮焼後
の粉砕を行うかがポイントである。一つの対策と
しては、なるべく仮焼温度を下げて軟い粉末にし
て粉砕すれば良いが、あまり低い温度で仮焼した
場合、原料の炭酸バリウム(BaCO3)が充分分解
しないことがあり、焼結体の内部に発生するガス
(CO2)のため巨大ボイドが生じて逆効果となる。 発明者はBaO―TiO2―ZrO2系に種々の添加物
を試みた結果、Al2O3、Y2O3の添加が仮焼時の反
応を抑制し、BaCO3が充分分解する仮焼条件下
でも軟い仮焼粉が得られることを見い出した。さ
らに、これを湿式再粉砕して得た粉末を成形、焼
結して得られた磁器の研磨面のボイドは、従来の
BaO―TiO2―ZrO2系で同一仮焼、粉砕、焼結し
て得られた磁器に比して、著しく小さくかつ数が
減少することを見い出した。 Al2O3、Y2O3の添加量を、いずれも0.05から1.0
に限定した理由は、添加量をこれ以下にしたら効
果が失われること、またこれ以上にすると磁器の
内部が焼結過程で環元しやすくなることまた材質
が硬くなり加工性が劣化することが認められたか
らである。 以下実施例をもつて本発明を詳細に説明する。
TiO2、BaCO3、ZrO2は純度99%以上の試薬を用
い、また、添加物としてのAl2O3及びY2O3も純度
99%以上の試薬を用いた。表の組成になるように
原料を配合し、ボールミルで湿式混合した。乾燥
後粉砕し、1100℃から1200℃の間で3時間仮焼し
た。仮焼粉は樹脂製のボールミルを用いて20時間
以上粉砕した。次に乾燥後、バインダーを混合
し、1.0〜2.0t/cm2の圧力で成形した。焼結は
1280℃〜1360℃の間で大気中で行つた。得られた
試料の密度及び熱膨張係数を測定し更に研磨面の
ボイドを金属顕微鏡を用いて観察した。その結果
を表に示す。
The present invention relates to non-magnetic structural materials constituting various magnetic heads, particularly floppy disk heads. Conventionally, alumina, forsterite, steatite porcelain, etc. have been used as non-magnetic structural materials for magnetic heads. However, these drawbacks are that the composition of the magnetic material ferrite differs slightly depending on the specifications of the magnetic head, so the thermal expansion coefficient changes accordingly, and the thermal expansion coefficients of ferrite and non-magnetic material do not match, making it difficult to process the glass bonding process. This resulted in cracks occurring in one of the parts, resulting in a decrease in yield. This non-magnetic material for the magnetic head always slides along the floppy disk surface at high speed simultaneously with the ferrite. Therefore, if its wear resistance is not comparable to that of ferrite, a gap will be created between the ferrite portion and the non-magnetic material, reducing the functionality of the magnetic head. Furthermore, if there are voids of 30 microns or more on the surface of the material, minute chips may occur from the voids, causing scratches on the surface of the magnetic storage medium.
Furthermore, since these components are processed into magnetic heads through precise processing steps, appropriate machinability is required during machining. Alumina, forsterite, steatite, etc. cannot satisfy these requirements, and recently, for heads using Ni--Zn ferrite, BaO--, which is a known microwave dielectric material, has been used. It has become common to use TiO 2 -ZrO 2 based porcelain. This is BaO
―TiO 2 ―ZrO 2 -based porcelain has appropriate workability and wear resistance, and by adjusting the composition ratio, it has a thermal expansion coefficient in the range of 90 to 100 × 10 -7 /℃ without impairing mechanical properties. This is because it was discovered that it can be changed freely. However, as the performance of floppy disk devices has improved in recent years, the requirements for magnetic head materials have become increasingly severe, and a requirement for voids on the polished surface of 5 microns or less is becoming the standard. To meet this demand, BaO-TiO 2 -ZrO 2- based porcelain cannot be manufactured using normal manufacturing methods, and hot pressing and hot isostatic pressing (HIP) are now used. These high-density techniques have made it possible to reduce the voids on the polished surface to a certain extent to meet the required performance, but their high cost has prevented their widespread use. The purpose of the present invention is to reduce voids on the polished surface to 5μ or less and to have a coefficient of thermal expansion of 90 to 100×, even though it is a normal sintering method.
The present invention provides a BaO-TiO 2 -ZrO 2 -based non-magnetic ceramic composition for magnetic heads with a temperature of 10 -7 /°C. The present invention uses TiO2 80~91.0mol%, BaO6~
16.0mol%, ZrO2 0.5~3.0mol%, Al2O3 0.05 ~
1.0 mol%, Y 2 O 3 0.05 to 1.0 mol%, and the total composition is 100 mol%, and the thermal expansion coefficient is 90.
This is a non-magnetic ceramic composition for a magnetic head, characterized in that the magnetic flux is in the range of ×10 -7 /°C to 100 × 10 -7 /°C. In the BaO-TiO 2 system, the mol ratio of TiO 2 is 80 mol%
In the above composition range, it can be predicted from the normal phase equilibrium diagram that the crystalline phase consists of two crystalline phases: BaT 4 O 9 and TiO 2 , but detailed research on microwave dielectrics suggests that the third crystalline phase is formed as a third crystalline phase. It has been confirmed that Ba 2 Ti 9 O 20 exists, and it is also known that the greater the amount of this crystalline phase contained, the higher the strength of the porcelain. This depends on the calcination and sintering conditions.
Although the amount of Ba 2 Ti 9 O 20 crystal phase produced differs, it has been recognized that including ZrO 2 and SnO 2 as additives can promote the formation of Ba 2 Ti 9 O 20 crystal phase, and this Due to its improved dielectric properties, BaO−
TiO 2 -ZrO 2 ceramics were used as microwave dielectrics. BaO-TiO 2 as a structural material for magnetic heads
- When looking at ZrO 2 porcelain, the increased mechanical strength due to the formation of Ba 2 Ti 9 O 20 is advantageous for applications. Also, by changing the ratio of BaO and TiO 2
It has the advantage that the ratio of the Ba 2 Ti 9 O 20 crystal phase to the TiO 2 crystal phase can be controlled, and the coefficient of thermal expansion can be controlled by the volume ratio of both. For these reasons, BaO--TiO 2 -ZrO 2- based porcelain has come to be commonly used as a structural material for magnetic heads. The blending ratio of TiO 2 and BaO in the present invention is essential in order to control the thermal expansion coefficient between 90×10 -7 /°C and 100×10 -7 /°C. ZrO 2 is for promoting the formation of the Ba 2 Ti 9 O 20 crystal phase as explained above. If the amount of ZrO 2 is less than 0.5 mol%, this effect will not be observed, and if it exceeds 3 mol%, the inside of the sintered body will be easily reduced during the sintering process. The size and amount of voids on the polished surface of the sintered body are inversely proportional to the particle size of the calcined powder after pulverization. That is, as the grinding progresses, the sintered density increases and the voids on the polished surface become smaller and less numerous. In order to obtain a sintered body with small voids, the key is how efficiently the pulverization after calcination can be carried out. One countermeasure is to lower the calcination temperature as much as possible and pulverize it into a soft powder, but if calcination is performed at too low a temperature, the raw material barium carbonate (BaCO 3 ) may not decompose sufficiently, and Due to the gas (CO 2 ) generated inside the solid, huge voids are created and have the opposite effect. As a result of trying various additives to the BaO-TiO 2 -ZrO 2 system, the inventor found that the addition of Al 2 O 3 and Y 2 O 3 suppressed the reaction during calcination, and that BaCO 3 was sufficiently decomposed during calcination. It has been found that soft calcined powder can be obtained even under these conditions. Furthermore, the voids in the polished surface of the porcelain obtained by wet re-grinding, molding and sintering the powder obtained are as follows:
It has been found that the porcelain is significantly smaller and the number of particles is reduced compared to the BaO-TiO 2 -ZrO 2- based porcelain obtained by the same calcining, crushing, and sintering process. The amounts of Al 2 O 3 and Y 2 O 3 added are both from 0.05 to 1.0.
The reason for limiting the amount is that if the amount added is less than this, the effect will be lost, and if it is more than this, the inside of the porcelain will be prone to ring formation during the sintering process, and the material will become hard and workability will deteriorate. Because it was recognized. The present invention will be explained in detail below with reference to Examples.
TiO 2 , BaCO 3 , and ZrO 2 use reagents with a purity of 99% or higher, and the additives Al 2 O 3 and Y 2 O 3 also have high purity.
More than 99% of reagents were used. The raw materials were blended to have the composition shown in the table and wet mixed in a ball mill. After drying, it was crushed and calcined at between 1100°C and 1200°C for 3 hours. The calcined powder was ground for over 20 hours using a resin ball mill. Next, after drying, a binder was mixed and molded at a pressure of 1.0 to 2.0 t/cm 2 . Sintering is
It was carried out in air between 1280°C and 1360°C. The density and coefficient of thermal expansion of the obtained sample were measured, and voids on the polished surface were observed using a metallurgical microscope. The results are shown in the table.

【表】【table】

【表】 実験試料No.1〜27はそれぞれTiO2とBaOの比
が一定の配合に対してZnO2、Al2O3、Y2O3の配
合量が異なる試料群である。 熱膨張係数はほぼTiO2とBaOの比率で決る。
Ni―Znフエライトを用いる磁気ヘツド用非磁性
磁器としては熱膨張係数が90〜100×10-7/℃の
値が要求される。これを満足できる試料はNo.1〜
25で、これらのTiO2とBaOの配合比はそれぞれ
80〜91.0mol%、6〜16.0mol%であることがわか
る。 ZrO2の効果は磁器の焼結性を改善し、機械的
強度が改善される。また還元を防止する効果があ
り、少くとも0.5mol%まではこの効果が認められ
た。またZnO2量が3mol%を越えると逆に還元し
やすくなりまた研磨面のボイドが大きくなる。試
料No.1、11、16、21はZrO2が過剰のため磁器の
機械的強度が弱くまた研磨面のボイドが大きく好
ましくなり、5、10、15、20、25はZrO2を含ま
ない場合であり焼結体の内部が部分的に還元し、
灰色となり実用上好しくない。 Al2O3は焼結体時の粒の成長を阻止し緻密な焼
結体を得るために有効である。その効果は
0.05mol%以上で認められた。が、1.0mol%を越
えると磁器が硬くまたもろくなり加工性が劣る。
またBaOとTiO2の比によつては還元しやすくな
る。 Y2O3は仮焼時の反応を抑制し仮焼粉の粉砕を
容易に焼結体のボイドを細くする効果がある。そ
の効果は0.05mol%以上で認められた。一方Y2O3
の含有量が増大して1.0mol%を越えると、Al2O3
と同様に材質を硬くし加工性を劣化させる。4、
9、14、19、24はAl2O3、Y2O3のいずれかが過剰
になつた例で加工性の劣るものである。 上記実施例の説明から明らかなように、本発明
によれば、熱膨張係数が、90〜100×10-7/℃の
範囲にあり、ボイドが少なく、機械的強度の大き
な非磁性磁器組成物を得ることができ、これは、
磁気ヘツドの非磁性構造材料として適している。
[Table] Experimental samples Nos. 1 to 27 are a group of samples in which the ratio of TiO 2 to BaO is constant, but the amounts of ZnO 2 , Al 2 O 3 , and Y 2 O 3 are different. The coefficient of thermal expansion is determined approximately by the ratio of TiO 2 and BaO.
Non-magnetic porcelain for magnetic heads using Ni--Zn ferrite is required to have a coefficient of thermal expansion of 90 to 100 x 10 -7 /°C. Samples that can satisfy this are No. 1~
25, and the mixing ratios of these TiO 2 and BaO are respectively
It can be seen that they are 80 to 91.0 mol% and 6 to 16.0 mol%. The effect of ZrO2 improves the sinterability of porcelain, and the mechanical strength is improved. It also had the effect of preventing reduction, and this effect was observed at least up to 0.5 mol%. On the other hand, if the amount of ZnO2 exceeds 3 mol%, reduction tends to occur and voids on the polished surface become larger. Samples No. 1, 11, 16, and 21 have excessive ZrO 2 , so the mechanical strength of the porcelain is weak and the voids on the polished surface are large, which is preferable, and samples 5, 10, 15, 20, and 25 do not contain ZrO 2 . and the inside of the sintered body is partially reduced,
The color turns gray, which is not practical. Al 2 O 3 is effective in inhibiting grain growth during sintering and obtaining a dense sintered body. The effect is
It was observed at 0.05 mol% or more. However, if it exceeds 1.0 mol%, the porcelain becomes hard and brittle, resulting in poor workability.
Also, depending on the ratio of BaO and TiO 2 , reduction becomes easier. Y 2 O 3 has the effect of suppressing the reaction during calcination, facilitating the pulverization of the calcined powder, and narrowing the voids in the sintered body. The effect was observed at 0.05 mol% or more. On the other hand Y 2 O 3
When the content of Al 2 O 3 increases and exceeds 1.0 mol%,
Similarly, it hardens the material and deteriorates workability. 4,
Samples Nos. 9, 14, 19, and 24 are examples in which either Al 2 O 3 or Y 2 O 3 was present in excess, and the processability was poor. As is clear from the description of the above examples, the present invention provides a non-magnetic porcelain composition having a coefficient of thermal expansion in the range of 90 to 100×10 -7 /°C, having few voids, and having high mechanical strength. You can get this, which is
Suitable as a non-magnetic structural material for magnetic heads.

Claims (1)

【特許請求の範囲】[Claims] 1 TiO280〜91.0mo%、BaO6〜16.0mo%、
ZrO20.5〜3.0mo%、A2O30.05〜1.0mo
%、Y2O30.05〜1.0mo%、の成分範囲よりなり
合計が100mo%になる組成物からなることを特
徴とする磁気ヘツド用非磁性磁器組成物。
1 TiO2 80~91.0mo%, BaO6~16.0mo%,
ZrO2 0.5~3.0mo%, A2O3 0.05 ~1.0mo
%, Y 2 O 3 0.05 to 1.0 mo%, and the total amount is 100 mo%.
JP58075245A 1983-04-28 1983-04-28 Non-magnetic ceramic composition for magnetic head Granted JPS59203771A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP58075245A JPS59203771A (en) 1983-04-28 1983-04-28 Non-magnetic ceramic composition for magnetic head

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP58075245A JPS59203771A (en) 1983-04-28 1983-04-28 Non-magnetic ceramic composition for magnetic head

Publications (2)

Publication Number Publication Date
JPS59203771A JPS59203771A (en) 1984-11-17
JPS6158428B2 true JPS6158428B2 (en) 1986-12-11

Family

ID=13570642

Family Applications (1)

Application Number Title Priority Date Filing Date
JP58075245A Granted JPS59203771A (en) 1983-04-28 1983-04-28 Non-magnetic ceramic composition for magnetic head

Country Status (1)

Country Link
JP (1) JPS59203771A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH09257287A (en) * 1996-03-19 1997-09-30 Seibu Electric Ind Co Ltd Air purifier at inlet port

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH09257287A (en) * 1996-03-19 1997-09-30 Seibu Electric Ind Co Ltd Air purifier at inlet port

Also Published As

Publication number Publication date
JPS59203771A (en) 1984-11-17

Similar Documents

Publication Publication Date Title
JPS6158428B2 (en)
JPS6021940B2 (en) Non-magnetic ceramics for magnetic heads
KR970004614B1 (en) Non-magnetic ceramic substrate material of magnetic head
JPH0335257B2 (en)
JP3460091B2 (en) Non-magnetic ceramics for magnetic heads
JPH0335258B2 (en)
JPS6232153B2 (en)
JPS6224386B2 (en)
JPS6029669B2 (en) Non-magnetic ceramics for magnetic heads
JPH0345024B2 (en)
JPS63134559A (en) Non-magnetic ceramics for magnetic head
JPH0712976B2 (en) Porcelain sintered body for magnetic head and manufacturing method thereof
JPS6251224B2 (en)
KR0137076B1 (en) Non-magnetic ceramic substrate for magnetic head
JP2917527B2 (en) Non-magnetic ceramic material and method of manufacturing the same
JPS6158429B2 (en)
JPS6048469B2 (en) Non-magnetic ceramics for magnetic heads
JPS6222946B2 (en)
JPS6152101B2 (en)
JPS6158427B2 (en)
JPS60103076A (en) Ceramic composition for magnetic head
JPS63170262A (en) Method for manufacturing ZrO↓2-TiC-SiC sintered body
JPS6359984B2 (en)
JPS6158426B2 (en)
JPS6339115A (en) Substrate material for thin film magnetic head