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JP3105929B2 - Magnetostrictive material - Google Patents
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JP3105929B2 - Magnetostrictive material - Google Patents

Magnetostrictive material

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Publication number
JP3105929B2
JP3105929B2 JP03009305A JP930591A JP3105929B2 JP 3105929 B2 JP3105929 B2 JP 3105929B2 JP 03009305 A JP03009305 A JP 03009305A JP 930591 A JP930591 A JP 930591A JP 3105929 B2 JP3105929 B2 JP 3105929B2
Authority
JP
Japan
Prior art keywords
magnetostrictive
magnetic field
magnetostriction
alloy
powder
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 - Fee Related
Application number
JP03009305A
Other languages
Japanese (ja)
Other versions
JPH04246150A (en
Inventor
勲 酒井
忠彦 小林
知己 船山
政司 佐橋
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.)
Toshiba Corp
Original Assignee
Toshiba Corp
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 Toshiba Corp filed Critical Toshiba Corp
Priority to JP03009305A priority Critical patent/JP3105929B2/en
Publication of JPH04246150A publication Critical patent/JPH04246150A/en
Application granted granted Critical
Publication of JP3105929B2 publication Critical patent/JP3105929B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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  • Powder Metallurgy (AREA)
  • Hard Magnetic Materials (AREA)

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】〔発明の目的〕[Object of the invention]

【0002】[0002]

【産業上の利用分野】本発明は、磁歪量と印加磁界応答
性の両磁歪特性に優れ、かつ機械的強度も高い自己バイ
アス磁界型の磁歪材料に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a self-biased magnetic field type magnetostrictive material which is excellent in both magnetostriction and response of an applied magnetic field and has high mechanical strength.

【0003】[0003]

【従来の技術】磁性体は外部から磁場を印加すると磁歪
によって変形するため、この磁歪を応用して以下のよう
な磁気−機械変位変換デバイス(以下「デバイス」とい
う)が開発された。すなわち、振動分野では磁歪振動子
としてスピーカ、ソナー、パーツフィーダ、超音波遅延
線、超音波加工機、モータの除振・防振機構などへ応用
でき、機械応用分野では変位制御アクチュエータとして
精密位置決め機構、バルブ制御弁、機械スイッチ、マイ
クロポンプ、プリンタヘッドなどへ応用できる。また磁
歪センサとして、圧力センサ、ノックセンサ、音圧セン
サなどに使用可能であり、さらには表面弾性波応用素子
への応用など工業上極めて有用な材料となる。
2. Description of the Related Art Since a magnetic substance is deformed by magnetostriction when a magnetic field is applied from the outside, the following magneto-mechanical displacement conversion device (hereinafter referred to as "device") has been developed by applying this magnetostriction. In other words, in the field of vibration, it can be applied to speakers, sonars, parts feeders, ultrasonic delay lines, ultrasonic processing machines, vibration isolation / vibration prevention mechanisms for motors, etc. in magnetostrictive transducers, and in precision positioning mechanisms as displacement control actuators in mechanical applications It can be applied to valve control valves, mechanical switches, micro pumps, printer heads, etc. Further, it can be used as a magnetostrictive sensor for a pressure sensor, a knock sensor, a sound pressure sensor, and the like, and is a very industrially useful material for application to a surface acoustic wave application element.

【0004】そして、これらデバイスに用いられる磁歪
材料としては、従来からNi基合金、Fe−Co合金、
フェライト系材料などが知られていたが、最近ではこれ
らの磁歪材料より磁歪の絶対量(磁歪量)においてはる
かに優れた(飽和磁歪λが1000×10-6以上)希
土類−鉄系のラーベス型金属間化合物(一般式AB
で、MgCu(立方晶系)またはMgZn,Mg
Ni(いずれも六方晶系)の結晶構造をもつ合金相
で、磁歪を示す)が報告されている(特公昭61−33
892号など)。
As magnetostrictive materials used for these devices, Ni-based alloys, Fe-Co alloys,
Although such a ferrite-based material has been known, much better (saturation magnetostriction lambda s is 1000 × 10 -6 or higher) in the absolute amount of magnetostriction than these magnetostrictive materials recently (magnetostriction) rare earth - Laves ferrous Type intermetallic compound (general formula AB
2 , MgCu 2 (cubic system) or MgZn 2 , Mg
An alloy phase having a crystal structure of Ni 2 (both hexagonal systems and exhibiting magnetostriction) has been reported (JP-B-61-33).
No. 892).

【0005】[0005]

【発明が解決しようとする課題】ところが、上記の希土
類−鉄系の巨大磁歪合金は、機械的強度が弱くて非常に
脆いために、割れや欠けが生じやすく、形状の任意性に
乏しい(限られた形状のものしか成形できない)という
欠点があった。
However, the above rare earth-iron giant magnetostrictive alloy has a low mechanical strength and is very brittle, so that it is liable to be cracked or chipped and has a poor shape arbitrarily. However, it is possible to mold only those having a given shape).

【0006】また、前述の希土類−鉄系磁歪合金は、図
2に示すような磁歪特性を有するため、ゼロ磁界付近で
の印加磁界応答性がよくない(一定量の磁界を印加した
ときの磁歪の変化量が少ない)。さらに正の磁界におい
ても負の磁界においても正の磁歪を生じて印加磁界応答
性が単調増加または単調減少でない。
Further, since the rare earth-iron based magnetostrictive alloy has magnetostrictive characteristics as shown in FIG. 2, the applied magnetic field response near zero magnetic field is poor (magnetostriction when a fixed amount of magnetic field is applied). Is small). Further, positive magnetostriction occurs in both the positive magnetic field and the negative magnetic field, and the response of the applied magnetic field is not monotonically increasing or monotonically decreasing.

【0007】したがって、通常考えられるように、磁界
を何ら加えないときの磁歪量がゼロとなるように印加磁
場を変化させたのでは、所望の磁歪量が得られず、また
磁界の印加による磁歪量の制御も難しい。このため、上
述の磁気−機械変位変換デバイスに用いる際には、磁歪
量制御のための磁界とは別に外部からバイアス磁界をか
けて、図中の破線で示すように、制御のため変化させる
磁界の範囲をゼロの近傍を含まず、例えば正の領域だけ
となるようにずらし、変化させる磁界の範囲では磁歪の
印加磁界応答性が高く、磁歪量も印加磁界量に対して単
調に変化するようにしていた。
Therefore, if the applied magnetic field is changed so that the amount of magnetostriction when no magnetic field is applied becomes zero as expected, a desired amount of magnetostriction cannot be obtained, and the magnetostriction caused by the application of a magnetic field cannot be obtained. It is difficult to control the amount. For this reason, when used in the above-described magneto-mechanical displacement conversion device, a bias magnetic field is applied from the outside in addition to the magnetic field for controlling the magnetostriction, and the magnetic field is changed for control as shown by the broken line in the figure. Is shifted so as to include only the positive region, for example, without including the vicinity of zero.In the range of the magnetic field to be changed, the applied magnetic field response of magnetostriction is high, and the amount of magnetostriction changes monotonically with respect to the amount of applied magnetic field. I was

【0008】しかし、このためには、図3に示すよう
に、この磁歪合金を利用するデバイス1において、矢印
の方向に磁歪・伸縮する磁歪合金片1と、磁歪合金片1
の磁歪量を制御する磁界を印加する電磁石2の他に、外
部バイアス磁界を形成するための永久磁石3を含む磁気
回路等を設置しなければならず、コスト高およびデバイ
スの大型化が避けられなかった。
However, for this purpose, as shown in FIG. 3, in a device 1 using this magnetostrictive alloy, a magnetostrictive alloy piece 1 that expands and contracts in the direction of an arrow and a magnetostrictive alloy piece 1
In addition to the electromagnet 2 for applying a magnetic field for controlling the amount of magnetostriction, a magnetic circuit or the like including a permanent magnet 3 for forming an external bias magnetic field must be installed, so that high cost and large-sized device can be avoided. Did not.

【0009】本発明は上記事情に鑑みてなされたもの
で、機械的強度に優れ、かつ磁歪特性の良好な磁歪材料
を提供することを目的とする。 〔発明の構成〕
The present invention has been made in view of the above circumstances, and has as its object to provide a magnetostrictive material having excellent mechanical strength and good magnetostriction characteristics. [Configuration of the invention]

【0010】[0010]

【課題を解決するための手段および作用】本発明は上記
課題を解決するために、例えばRFe(Rは少なくと
も1種の希土類元素、1.5≦x≦4)磁歪合金粉末と
永久磁石粉末の混合粉末を一体化したことを特徴とする
磁歪材料を提供する。
Means and operation for solving the problems The present invention in order to solve the above problems, for example, RFe x (R is at least one rare earth element, 1.5 ≦ x ≦ 4) magnetostrictive alloy powder and permanent magnet powder A magnetostrictive material characterized by integrating a mixed powder of

【0011】本発明の磁歪材料において、まず磁歪合金
は、上記の如くRFeの超磁歪合金が挙げられるが、
これを構成するR元素が1種の元素である場合は、L
a、Ce、Pr、Nd、Pm、Sm、Eu、Gd、T
b、Dy、Ho、Er、Tm、Yb、Luなどの希土類元
素とすることができる。またR元素とすることができ2
種以上の希土類元素の組み合わせである場合は、Tb−
Dy、Tb−Ho、Tb−Pr、Sm−Yb、Tb−D
y−Ho、Tb−Dy−Pr、Tb−Pr−Hoなどの
組み合わせが考えられる。
[0011] In the magnetostrictive material of the present invention, first magnetostrictive alloy is super magnetostrictive alloy of the as RFe x and the like,
When the R element constituting this is one kind of element, L
a, Ce, Pr, Nd, Pm, Sm, Eu, Gd, T
Rare earth elements such as b, Dy, Ho, Er, Tm, Yb, and Lu can be used. In addition, it can be R element,
When a combination of at least one kind of rare earth element is used, Tb-
Dy, Tb-Ho, Tb-Pr, Sm-Yb, Tb-D
Combinations of y-Ho, Tb-Dy-Pr, Tb-Pr-Ho and the like are conceivable.

【0012】一方、磁歪合金を構成する他の元素はFe
であるが、耐蝕性改善のためFeの一部をCoで置換す
ることが可能である。ただし、あまり置換量が多くなる
と磁歪特性の低下(磁歪量の縮小と印加磁界応答性の減
少)を招くため、CoによるFeの置換量は95at%
(95原子%)以下とする。
On the other hand, the other element constituting the magnetostrictive alloy is Fe
However, it is possible to partially replace Fe with Co for improving corrosion resistance. However, if the substitution amount is too large, the magnetostriction characteristics are reduced (the magnetostriction amount is reduced and the response to the applied magnetic field is reduced). Therefore, the substitution amount of Fe by Co is 95 at%.
(95 atomic%) or less.

【0013】また、必要に応じてFeの一部を、さらに
Mnで置換してもよい。R−Fe系の磁歪合金は、Mn
を含有させると、希土類原子の磁気異方性が変化し、高
磁界のみならず低磁界においても優れた磁歪特性が得ら
れる。MnによるFeの置換量の上限は50at%であ
り、この上限値を越えるとキュリー温度が低下し、磁歪
特性が劣化する。
Further, if necessary, a part of Fe may be further substituted with Mn. The R-Fe magnetostrictive alloy is Mn.
When the element is contained, the magnetic anisotropy of the rare earth element changes, and excellent magnetostriction characteristics can be obtained not only in a high magnetic field but also in a low magnetic field. The upper limit of the amount of Fe replaced by Mn is 50 at%. If the upper limit is exceeded, the Curie temperature decreases, and the magnetostriction characteristics deteriorate.

【0014】この他、Feは、磁歪材料の機械的強度、
耐蝕性、飽和磁歪などの向上を目的としてNi、Mg、
Al、Ga、Zn、V、Zr、Hf、Ti、Nb、C
u、Ag、Sn、Mo、Cr、Ta、Pd、In、S
b、Ir、Pt、Au、Pb、W、Si、Bなどでさら
に置換してもよい。ただし、これら置換元素の量は、M
nによる置換量も含めて、Feの50at%程度までが限
度であり、これを超えると磁歪量が減少する。
In addition, Fe is the mechanical strength of the magnetostrictive material,
For the purpose of improving corrosion resistance and saturation magnetostriction, Ni, Mg,
Al, Ga, Zn, V, Zr, Hf, Ti, Nb, C
u, Ag, Sn, Mo, Cr, Ta, Pd, In, S
It may be further substituted with b, Ir, Pt, Au, Pb, W, Si, B or the like. However, the amount of these substitution elements is M
The limit is up to about 50 at% of Fe, including the amount of substitution by n. If it exceeds this, the amount of magnetostriction decreases.

【0015】なお、R元素とFeの原子比xは、1.5
≦x≦4としたが、これは1.5未満だと十分な磁歪特
性が得られず、他方4を超えると、靭性が著しく低下し
て脆くなるためである。
The atomic ratio x between the R element and Fe is 1.5
When x is less than 1.5, sufficient magnetostriction characteristics cannot be obtained, and when x is more than 4, toughness is significantly reduced and the film becomes brittle.

【0016】一方永久磁石粉末としては、フェライト磁
石、Sm−Co系磁石、Nd−Fe−B系磁石等の粉末
を使用することができるが、少量の粉末で十分な磁界を
得るためにはSm−Co系およびNd−Fe−B系磁石
の粉末が好ましい。
On the other hand, as the permanent magnet powder, powders such as ferrite magnets, Sm-Co magnets, and Nd-Fe-B magnets can be used. -Co and Nd-Fe-B magnet powders are preferred.

【0017】そして永久磁石粉末の混合比は、磁歪合金
粉末に対して5〜50重量%とするのが好ましい。5重
量%未満では永久磁石粉末を着磁しても十分な自己バイ
アス磁界を得ることが難しく、また50重量%を超える
と磁歪合金について十分な磁歪量を得ることが難しくな
るからである。この混合比は、さらに好ましくは10〜
30重量%である。
The mixing ratio of the permanent magnet powder is preferably 5 to 50% by weight based on the magnetostrictive alloy powder. If the content is less than 5% by weight, it is difficult to obtain a sufficient self-bias magnetic field even when the permanent magnet powder is magnetized, and if it exceeds 50% by weight, it is difficult to obtain a sufficient magnetostriction for the magnetostrictive alloy. This mixing ratio is more preferably 10 to
30% by weight.

【0018】なお磁歪合金粉末および永久磁石粉末の粒
径は、1〜800μmが好ましい。1μm未満だと粉末
全体の表面積が大きくなりすぎて酸化による磁歪特性お
よび磁石特性の劣化を招きやすくなり、他方800μm
を超えると磁歪材料の機械的強度が低下し、また超薄片
に成形するのが困難になるなど、形状の任意性が劣化す
る。
The particle size of the magnetostrictive alloy powder and the permanent magnet powder is preferably from 1 to 800 μm. If it is less than 1 μm, the surface area of the whole powder becomes too large, which tends to cause deterioration of the magnetostriction characteristics and magnet characteristics due to oxidation, and 800 μm
If it exceeds, the mechanical strength of the magnetostrictive material is reduced, and it is difficult to mold the material into ultra-thin flakes.

【0019】つぎに、本発明の磁歪材料の製造方法を説
明する。
Next, a method for producing the magnetostrictive material of the present invention will be described.

【0020】まず、所定原子比のR元素およびFe、さ
らに必要に応じて上述のCo、Mnなどを調製してアー
ク溶解などにより溶湯とした後、超急冷法、水素吸蔵法
などによって磁歪合金粉末を得る。超急冷法は、一般に
非晶質合金を製造する際に使用される単ロール法、双ロ
ール法、ガスアトマイズ法、RDP(Rotating Disk Pr
ocess;回転円盤上に溶湯金属を噴出させる方法)などに
より、合金の溶湯を超急冷して粉末化する方法である。
なお超急冷は酸化防止の観点から、Ar、Heなどの不
活性ガス雰囲気中で行うことが好ましい。
First, an R element and Fe having a predetermined atomic ratio and, if necessary, the above-mentioned Co, Mn, etc. are prepared and melted by arc melting or the like, and then a magnetostrictive alloy powder is obtained by a super-quenching method, a hydrogen absorbing method or the like. Get. The rapid quenching method is a single-roll method, a twin-roll method, a gas atomizing method, a RDP (Rotating Disk Pr
ocess; a method in which a molten metal is jetted onto a rotating disk) to rapidly quench the molten alloy to form a powder.
It is preferable that the super-quenching is performed in an atmosphere of an inert gas such as Ar or He from the viewpoint of preventing oxidation.

【0021】また、磁歪合金の溶湯を冷却して一旦、ボ
ールミル、ブラウンミル、スタンプミルなどの機械的手
段で粉砕可能な形状の合金インゴットにした後、この合
金インゴットを上述の機械的粉砕手段で粉砕しても磁歪
合金粉末を得ることができる。
Further, after cooling the melt of the magnetostrictive alloy into an alloy ingot having a shape that can be pulverized by a mechanical means such as a ball mill, a brown mill, a stamp mill, and the like, the alloy ingot is subjected to the mechanical pulverization means described above. Even if it is pulverized, a magnetostrictive alloy powder can be obtained.

【0022】なお、合金インゴットから粉砕する場合
は、粉砕の前後に300℃ないし超磁歪合金の融点の温
度範囲で0.1〜500時間程度熱処理を施すと、磁歪
特性の向上を図ることができる。
In the case of pulverizing from an alloy ingot, the magnetostrictive properties can be improved by performing a heat treatment before and after the pulverization at 300 ° C. or a temperature range of the melting point of the giant magnetostrictive alloy for about 0.1 to 500 hours. .

【0023】さて、こうして磁歪合金の粉末が得られた
ら、つぎは同様にして永久磁石の粉末を得、両粉末を混
合する。そして、この混合粉末を例えば所望形状の金型
に挿入後、ホットプレスやHIP(熱間静水圧プレス)
等により一体化し磁歪材料を得る。本発明で一体化した
混合粉末とは、磁歪合金粉末と永久磁石粉末が互いに粉
末の形状を保ったまま高密度で凝集したものをいう。
After the powder of the magnetostrictive alloy is obtained, the powder of the permanent magnet is obtained in the same manner, and the two powders are mixed. Then, after inserting the mixed powder into a mold having a desired shape, for example, hot pressing or HIP (hot isostatic pressing) is performed.
To obtain a magnetostrictive material. The mixed powder integrated in the present invention refers to a powder in which the magnetostrictive alloy powder and the permanent magnet powder are aggregated at a high density while maintaining the powder shape with each other.

【0024】一体化の際ホットプレスを行う場合は、ホ
ットプレス温度は、600〜1200℃が好ましく、ま
たプレス圧は1t/cm2 以上とするのが好ましい。60
0℃未満では液相が生じにくく高密度化が困難になり、
機械的強度の低下を招く。他方1200℃を超えると磁
歪合金と永久磁石は粉末の形状を保てず固溶化するが、
この固溶化した材料は永久磁石の保磁力および磁歪合金
の磁歪特性が劣化するためである。また、プレス圧が1
t/cm2 未満の場合も高密度が難しい。さらに、ホット
プレスを行う場合は、磁歪合金粉末が酸化して磁歪特性
が劣化しないように、Ar、Heなどの不活性ガス雰囲
気中で行うのが好ましい。
When hot pressing is performed at the time of integration, the hot pressing temperature is preferably 600 to 1200 ° C., and the pressing pressure is preferably 1 t / cm 2 or more. 60
If the temperature is lower than 0 ° C., it is difficult to generate a liquid phase, and it is difficult to increase the density.
This leads to a decrease in mechanical strength. On the other hand, when the temperature exceeds 1200 ° C., the magnetostrictive alloy and the permanent magnet do not maintain the shape of the powder and are solidified.
This is because the co-solved material deteriorates the coercive force of the permanent magnet and the magnetostrictive characteristics of the magnetostrictive alloy. Also, if the pressing pressure is 1
Even when it is less than t / cm 2, high density is difficult. Further, when hot pressing is performed, it is preferable to perform hot pressing in an atmosphere of an inert gas such as Ar or He so that the magnetostrictive alloy powder is not oxidized and the magnetostriction characteristics are not deteriorated.

【0025】このように、磁歪合金を一旦粉末化した後
にホットプレスで成形一体化すると、結晶粒径が均一化
されるとともに、組成の偏析なども防止されるため、良
好な磁歪特性が安定して得られ、かつ機械的強度も向上
する。また粉末成形のため、形状の任意性にも優れる。
As described above, if the magnetostrictive alloy is once powdered and then molded and integrated by hot pressing, the crystal grain size is made uniform and the segregation of the composition is prevented, so that good magnetostrictive characteristics are stabilized. And the mechanical strength is also improved. In addition, since the powder is molded, it is excellent in arbitrary shape.

【0026】ところで、もしR元素が2種以上の元素を
含む場合、例えばR1p R21-p Fe(R1とR2は互いに
異なる希土類元素で、0<p<1)の場合には、上述の
合金インゴットを粉砕する方法に倣って、まずR1
x1とR21-p Fex2(x1+x2=x)の組成の合金イン
ゴットからそれぞれ合金粉末を製造し、この一体化の段
階で両粉末を混合すると、ホットプレス時の粒成長によ
って所望の組成の磁歪合金粉末を得ながら、磁歪材料を
形成することができる。
By the way, if R element comprises two or more elements, e.g. R1 p R2 1-p Fe x (R1 and R2 mutually different rare earth elements, 0 <p <1) in the case of the above to follow the alloy ingot to a method of grinding, first R1 p F
An alloy powder is manufactured from an alloy ingot having a composition of e x1 and R2 1-p Fe x2 (x1 + x2 = x). When the two powders are mixed at the stage of the integration, the desired composition is obtained by grain growth during hot pressing. The magnetostrictive material can be formed while obtaining the magnetostrictive alloy powder.

【0027】またホットプレス成形の際には、磁場を印
加して磁歪合金の磁化容易軸方向に磁気的に異方性化す
ると磁歪特性の向上が図れる。R元素が2種以上の元素
を含み、かつ個々のR元素含有合金がそれぞれ磁気異方
性方向を異にする場合は、上述のように所望の組成とな
るように2種以上の希土類−鉄系の合金粉末を混合し、
この混合粉末を磁場成形(磁場中で成形体をつくる)し
てそれぞれの合金について磁気異方性化を達成した後、
ホットプレスを施せば、全体として磁気異方性方向を同
じくする磁歪合金が得られ、磁歪特性に富む磁歪材料を
形成できる。
In hot press molding, when a magnetic field is applied to make the magnetostrictive alloy magnetically anisotropic in the direction of the axis of easy magnetization, the magnetostriction characteristics can be improved. In the case where the R element contains two or more elements and the alloys containing each R element have different magnetic anisotropy directions, two or more rare earth-iron alloys are formed so as to have a desired composition as described above. System alloy powder,
After magnetically forming this mixed powder (forming a compact in a magnetic field) and achieving magnetic anisotropy for each alloy,
When hot pressing is performed, a magnetostrictive alloy having the same magnetic anisotropy direction can be obtained as a whole, and a magnetostrictive material having excellent magnetostrictive properties can be formed.

【0028】さらに、ホットプレスは、磁歪合金粉末に
例えばAlなどの低融点金属もしくは合金を添加または
粉末表面に被覆した後に行うと、ホットプレス温度を低
下させることができ、ホットプレスに係るコストを節約
できる。また、ホットプレス後に、300℃〜磁歪合金
の融点の温度で熱処理をすると上記合金インゴット粉砕
後の熱処理と同様、磁歪特性の向上を図れる。
Further, when hot pressing is performed after adding a low melting point metal or alloy such as Al to the magnetostrictive alloy powder or coating the powder surface, the hot pressing temperature can be lowered, and the cost associated with hot pressing can be reduced. Can save. In addition, when the heat treatment is performed at a temperature of 300 ° C. to the melting point of the magnetostrictive alloy after the hot pressing, the magnetostriction characteristics can be improved, similarly to the heat treatment after the alloy ingot pulverization.

【0029】本発明の磁歪材料は、上記一体化の後、デ
バイス化前に磁歪材料に磁場を印加して永久磁石粉末を
着磁することにより、磁歪材料中にバイアス磁界を有す
る自己バイアス磁界型磁歪材料とすることができる。自
己バイアス磁界、およびこの自己バイアス磁界による当
初磁歪量(例えば図3の電磁石2などにより適宜磁歪量
を変化させる以前の磁歪量)は、永久磁石粉末量を調整
することにより調節することができる。
The magnetostrictive material of the present invention comprises a self-biased magnetic field type having a bias magnetic field in the magnetostrictive material by applying a magnetic field to the magnetostrictive material and magnetizing the permanent magnet powder before device formation after the integration. It can be a magnetostrictive material. The self-biased magnetic field and the initial magnetostriction due to the self-biased magnetic field (for example, the magnetostriction before the magnetostriction is appropriately changed by the electromagnet 2 in FIG. 3) can be adjusted by adjusting the amount of the permanent magnet powder.

【0030】なお本発明の磁歪材料は、表面にNiメッ
キなどの金属コーティングまたはエポキシ樹脂などで樹
脂コーティングすることにより、さび防止等耐候性の改
善を図るのが望ましい。
The magnetostrictive material of the present invention is desirably improved in weather resistance such as rust prevention by coating the surface with a metal coating such as Ni plating or resin coating with an epoxy resin or the like.

【0031】本発明の磁歪材料においては、磁歪合金粉
末と永久磁石粉末との混合粉末をホットプレス等により
一体化するため、デバイスに組込む前に磁歪材料に磁界
を印加すれば磁歪材料中の永久磁石粉末を着磁し、バイ
アス磁界として作用させることができる。したがって、
本発明の磁歪材料を用いるデバイスにおいては、外部か
らバイアス磁界を加えるための永久磁石等は不要にな
る。
In the magnetostrictive material of the present invention, the mixed powder of the magnetostrictive alloy powder and the permanent magnet powder is integrated by hot pressing or the like. The magnet powder can be magnetized and act as a bias magnetic field. Therefore,
In the device using the magnetostrictive material of the present invention, a permanent magnet or the like for applying a bias magnetic field from the outside is unnecessary.

【0032】[0032]

【実施例】以下図1を参照して本発明の実施例を説明す
る。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS An embodiment of the present invention will be described below with reference to FIG.

【0033】〈実施例1〉まず原子比でTb0.35Dy
0.65(Fe0.85Mn0.152 となるように、各原子を調
製した後Ar雰囲気下で水冷銅ボート中においてアーク
溶解を行い、上記組成の合金インゴットを得た。つい
で、この合金インゴットをブラウンミルで平均粒径30
μmまで粉砕し、磁歪合金粉末を得た。そして、この磁
歪合金粉末に対して、20重量%のNd−Fe−B系永
久磁石粉末(平均粒径100μm)を混合した。
Example 1 First, Tb 0.35 Dy in atomic ratio
After preparing each atom so as to be 0.65 (Fe 0.85 Mn 0.15 ) 2 , arc melting was performed in a water-cooled copper boat under an Ar atmosphere to obtain an alloy ingot having the above composition. Then, the alloy ingot was brown-milled to have an average particle size of 30.
It was pulverized to μm to obtain a magnetostrictive alloy powder. Then, 20% by weight of an Nd—Fe—B-based permanent magnet powder (average particle diameter: 100 μm) was mixed with the magnetostrictive alloy powder.

【0034】つぎに、上記混合粉末を金型に充填後、ア
ルゴン雰囲気中で900℃、1.5t/cm2 の条件でホ
ットプレスを行い、直径6mm、長さ30mmの円柱状の磁
歪合金ロッドを得た。最後に、この磁歪合金ロッドに3
0kOeの磁界を印加して含有する永久磁石を着磁し、
磁歪合金ロッドを自己バイアス磁界型磁歪材料とした。
Next, after filling the above mixed powder into a mold, hot pressing was performed in an argon atmosphere at 900 ° C. and 1.5 t / cm 2 to obtain a cylindrical magnetostrictive alloy rod having a diameter of 6 mm and a length of 30 mm. I got Finally, add 3 to this magnetostrictive alloy rod.
Applying a magnetic field of 0 kOe to magnetize the contained permanent magnet,
The magnetostrictive alloy rod was a self-biased magnetic field type magnetostrictive material.

【0035】この磁歪合金ロッドについて、室温下で対
向磁極型電磁石により、±300Oeの範囲で印加磁界
を変化させ、歪みゲージを用いて磁歪特性を評価した。
その結果を図1に示す。図1から明らかなように、この
磁歪材料は−300Oe〜+300Oeの印加磁界範囲
においてゼロ磁界(自己バイアス磁界は存在する)付近
をも含めてほぼ線形で約120〜130ppm/kOeの印
加磁界応答性を示し、かつこの印加磁界範囲における磁
歪量も約−400ppmないし+400ppm と、合計して
約800ppm 近い大きなものになる。したがって、本実
施例に係る磁歪合金ロッドは優れた磁歪特性を有するも
のであり、かつ印加磁界範囲全般において印加磁界応答
性がよいため、新たに永久磁石等によるバイアス磁界を
設ける必要がない。
With respect to this magnetostrictive alloy rod, the applied magnetic field was changed within a range of ± 300 Oe by a facing magnetic pole type electromagnet at room temperature, and the magnetostriction characteristics were evaluated using a strain gauge.
The result is shown in FIG. As is clear from FIG. 1, this magnetostrictive material is almost linear in the applied magnetic field range of -300 Oe to +300 Oe, including near the zero magnetic field (there is a self-biased magnetic field), and has an applied magnetic field response of about 120 to 130 ppm / kOe. And the magnetostriction in this applied magnetic field range is about -400 ppm to +400 ppm, which is a large value close to about 800 ppm in total. Therefore, the magnetostrictive alloy rod according to the present embodiment has excellent magnetostrictive characteristics and has good response to the applied magnetic field over the entire range of the applied magnetic field, so that there is no need to newly provide a bias magnetic field using a permanent magnet or the like.

【0036】また、上述の方法で本実施例の磁歪材料か
ら製造した10本の磁歪合金ロッドについて、10kO
e印加磁界中の磁歪量(λ10kOe )を測定したところ、
1200±20ppm とばらつきが少なく、かつ絶対的な
値としても良好な値が得られた。
Further, for 10 magnetostrictive alloy rods manufactured from the magnetostrictive material of the present embodiment by the above-described method, 10 kO
eWhen the magnetostriction (λ 10kOe ) in the applied magnetic field was measured,
The dispersion was small at 1200 ± 20 ppm, and a good value was obtained as an absolute value.

【0037】さらに、本実施例で得られた磁歪合金ロッ
ドは、所望の形状についての寸法精度がよいため後加工
を施す必要がなかった。そして、3点曲げ試験で機械的
強度を測定したところ、17kg/mm2 と良好な値が得ら
れた。
Further, since the magnetostrictive alloy rod obtained in this embodiment has high dimensional accuracy in a desired shape, it is not necessary to perform post-processing. When the mechanical strength was measured by a three-point bending test, a good value of 17 kg / mm 2 was obtained.

【0038】〈実施例2−15〉まず、実施例1と同様
の方法によって、下記表1に示す組成の各合金のインゴ
ットを製造し、ついで各合金インゴットを溶融して得ら
れた各合金の混合溶湯について、Ar雰囲気中で直径3
00mm、ロール速度25m/sec のCuロールによる単
ロール法で超急冷を行い、平均粒径100μmの磁歪合
金粉末を得た。
<Example 2-15> First, ingots of the respective alloys having the compositions shown in Table 1 below were produced in the same manner as in Example 1, and then the ingots of the respective alloys obtained by melting the respective alloy ingots were prepared. The mixed molten metal has a diameter of 3 in an Ar atmosphere.
Ultra-quenching was performed by a single roll method using a Cu roll having a thickness of 00 mm and a roll speed of 25 m / sec to obtain a magnetostrictive alloy powder having an average particle diameter of 100 μm.

【0039】そして、この超磁歪合金粉末を実施例1と
同様な方法で表1に示す種類・混合比の永久磁石粉末と
ホットプレスにより一体化して磁歪材料のロッドを成形
し、実施例1と同様の方法により30kOeの自己バイ
アス磁界を印加した後、±0.3kOeの磁界中におい
て磁歪の測定を行った。その結果を表1に併せて示す。
Then, this giant magnetostrictive alloy powder was integrated with a permanent magnet powder having the type and mixing ratio shown in Table 1 by hot pressing in the same manner as in Example 1 to form a rod of a magnetostrictive material. After applying a self-biased magnetic field of 30 kOe by the same method, the magnetostriction was measured in a magnetic field of ± 0.3 kOe. The results are shown in Table 1.

【0040】[0040]

【表1】 [Table 1]

【0041】表1から明らかなように、本実施例の磁歪
材料は、いずれも±0.3kOeの磁界範囲においてゼ
ロ磁界を中心に対称な磁歪量(絶対値が同じで正負の符
号が反対)を示してほぼ線形の印加磁界応答性をもち、
磁歪の絶対量も大きい。よって、実施例2〜15の磁歪
材料も良好な磁歪特性を有することが確認された。
As is clear from Table 1, the magnetostrictive materials of the present embodiment all have a symmetric magnetostriction centered on a zero magnetic field in the magnetic field range of ± 0.3 kOe (the absolute value is the same and the positive and negative signs are opposite). Has a substantially linear applied magnetic field response,
The absolute amount of magnetostriction is also large. Therefore, it was confirmed that the magnetostrictive materials of Examples 2 to 15 also had good magnetostrictive characteristics.

【0042】[0042]

【発明の効果】以上説明したように、本発明の磁歪材料
は、自己バイアス磁界を有し、磁歪量と印加磁界応答性
の両面において優れた磁歪特性を発揮する。そして本発
明の磁歪材料は外部バイアス磁界が不要のため、デバイ
ス構造を簡略化できる。
As described above, the magnetostrictive material of the present invention has a self-biased magnetic field, and exhibits excellent magnetostriction characteristics in both the amount of magnetostriction and the response of the applied magnetic field. Since the magnetostrictive material of the present invention does not require an external bias magnetic field, the device structure can be simplified.

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

【図1】本発明の一実施例に係る磁歪材料でできたロッ
ドの磁歪特性図。
FIG. 1 is a diagram showing magnetostriction characteristics of a rod made of a magnetostrictive material according to one embodiment of the present invention.

【図2】従来の磁歪材料の磁歪特性図。FIG. 2 is a diagram showing magnetostriction characteristics of a conventional magnetostrictive material.

【図3】従来の磁気−機械変位変換デバイスの模式断面
図。
FIG. 3 is a schematic sectional view of a conventional magnetic-mechanical displacement conversion device.

【符号の説明】[Explanation of symbols]

1 磁歪合金片 2 電磁石 3 永久磁石 1 Magnetostrictive alloy piece 2 Electromagnet 3 Permanent magnet

───────────────────────────────────────────────────── フロントページの続き (72)発明者 佐橋 政司 神奈川県川崎市幸区小向東芝町1番地 株式会社東芝 総合研究所内 (58)調査した分野(Int.Cl.7,DB名) C22C 33/02 C22C 38/00 303 ──────────────────────────────────────────────────続 き Continuing from the front page (72) Inventor Masashi Sabashi 1 Koga Toshiba-cho, Saiwai-ku, Kawasaki-shi, Kanagawa Prefecture Toshiba Research Institute, Inc. (58) Field surveyed (Int. Cl. 7 , DB name) C22C 33 / 02 C22C 38/00 303

Claims (1)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】 磁歪合金粉末と永久磁石粉末の混合粉末
を一体化したことを特徴とする磁歪材料。
1. A magnetostrictive material wherein a mixed powder of a magnetostrictive alloy powder and a permanent magnet powder is integrated.
JP03009305A 1991-01-29 1991-01-29 Magnetostrictive material Expired - Fee Related JP3105929B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP03009305A JP3105929B2 (en) 1991-01-29 1991-01-29 Magnetostrictive material

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP03009305A JP3105929B2 (en) 1991-01-29 1991-01-29 Magnetostrictive material

Publications (2)

Publication Number Publication Date
JPH04246150A JPH04246150A (en) 1992-09-02
JP3105929B2 true JP3105929B2 (en) 2000-11-06

Family

ID=11716757

Family Applications (1)

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Country Link
JP (1) JP3105929B2 (en)

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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP5120710B2 (en) * 2008-06-13 2013-01-16 日立金属株式会社 RL-RH-T-Mn-B sintered magnet
JP5823783B2 (en) * 2011-09-09 2015-11-25 公益財団法人鉄道総合技術研究所 Mechanical permanent current switch using giant magnetostrictive element
JP2026048319A (en) * 2024-09-05 2026-03-17 住友金属鉱山株式会社 Magnetostrictive member and method for manufacturing a magnetostrictive member

Also Published As

Publication number Publication date
JPH04246150A (en) 1992-09-02

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