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JPH0317248A - Manufacturing method of magnetostrictive actuator - Google Patents
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JPH0317248A - Manufacturing method of magnetostrictive actuator - Google Patents

Manufacturing method of magnetostrictive actuator

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Publication number
JPH0317248A
JPH0317248A JP3221190A JP3221190A JPH0317248A JP H0317248 A JPH0317248 A JP H0317248A JP 3221190 A JP3221190 A JP 3221190A JP 3221190 A JP3221190 A JP 3221190A JP H0317248 A JPH0317248 A JP H0317248A
Authority
JP
Japan
Prior art keywords
magnetostriction
working
alloy
magnetostrictive
temp
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.)
Granted
Application number
JP3221190A
Other languages
Japanese (ja)
Other versions
JPH0645850B2 (en
Inventor
Ryo Masumoto
量 増本
Shizuo Kadowaki
門脇 静穂
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.)
Research Institute for Electromagnetic Materials
Original Assignee
Research Institute for Electromagnetic Materials
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 Research Institute for Electromagnetic Materials filed Critical Research Institute for Electromagnetic Materials
Priority to JP3221190A priority Critical patent/JPH0645850B2/en
Publication of JPH0317248A publication Critical patent/JPH0317248A/en
Publication of JPH0645850B2 publication Critical patent/JPH0645850B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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  • Soft Magnetic Materials (AREA)
  • Heat Treatment Of Steel (AREA)

Abstract

PURPOSE:To obtain the magnetostriction working body having high static magnetostriction by working a Pd-Co alloy having specified compsn. into a wire shape or a thin sheet shape by hot working and cold working and thereafter executing heat treatment under specified conditions. CONSTITUTION:An ingot of a Pd-Co alloy constituted of, by weight, 40 to 92% Pd and 60 to 8% Co is hot forged in the temp. range of 900 to 1400 deg.C and is successively cold rolled to work into a wire shape or a thin sheet shape, which is heated in the temp. range of 900 deg.C to the m.p. of the alloy for about 1min in the air, in an inert gas atmosphere or in vacuum and is thereafter slowly cooled to a room temp. at an arbitrary cooling rate. The magnetostriction working body having -40 to 170X10<-6> static magnetostriction and therefore suitable to structural body elements such as magnetostriction sensor elements and magnetostriction vibrator elements for ultrasonic generation can be obtd.

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は荷重計、圧力、張力等を測定する力計等に用い
られる磁気ひずみ式センサーの素子、超音波発生用の磁
歪振動体用素子あるいは磁歪バイメタル等静磁歪を利用
する構成体の素子として有用な、大きな静磁歪を有する
磁歪作動体の製造法に関するものである。
Detailed Description of the Invention (Industrial Application Field) The present invention is an element for a magnetostrictive sensor used in a load cell, a force meter for measuring pressure, tension, etc., and an element for a magnetostrictive vibrator for generating ultrasonic waves. Alternatively, the present invention relates to a method for manufacturing a magnetostrictive actuator having large magnetostriction, which is useful as an element of a structure that utilizes magnetostriction, such as a magnetostrictive bimetal.

(従来の技術) 近年、金属磁歪材料を用いた力計測の分野では、種々の
工程や装置の自動化、小型化、省力化等の急速な進展に
ともなって、センサーの信頼性の向上、高精度化、小型
化か要望されるようになった。
(Prior art) In recent years, in the field of force measurement using metal magnetostrictive materials, with the rapid progress in automation, miniaturization, and labor saving of various processes and devices, improvements in sensor reliability and high precision have been made. There was a demand for miniaturization and miniaturization.

これらの多様なニーズに対応できる磁歪材料としては第
1に大なる静磁歪を有している大なる信号出力が得られ
ること、第2に冷間加工性か良好で所要の形状に成形し
得ること、第3に低磁場におけるひずみ量の発現か大な
ることが必要である。
As a magnetostrictive material that can meet these diverse needs, firstly, it has large magnetostriction and can provide a large signal output, and secondly, it has good cold workability and can be formed into the desired shape. Thirdly, it is necessary that the amount of strain be expressed in a low magnetic field.

(発明が解決しようとする課題) 従来、力計測に利用されている磁歪材料としては、Ni
,Fe−Ni合金,Fe−Si合金あるいはFe−Af
f合金等の金属や合金が目的に応じて使用されている。
(Problem to be solved by the invention) Conventionally, the magnetostrictive material used for force measurement is Ni.
, Fe-Ni alloy, Fe-Si alloy or Fe-Af
Metals and alloys such as f alloys are used depending on the purpose.

これらの磁歪材料の飽和磁歪値はNiの1l/1ξ−3
5X 10−” ( 1 =長さ)程度あるいはそれよ
りも小さな値であり、合金の場合には冷間加工性に乏し
いものもある。
The saturation magnetostriction value of these magnetostrictive materials is 1l/1ξ−3 of Ni.
The value is about 5×10-” (1=length) or smaller, and some alloys have poor cold workability.

本発明においてはバラジウムーコバルト系合金の特定組
成において、従来の磁歪材料の静磁歪値をはるかに超え
る大なる静磁歪特性が簡易な熱処理または加工によって
発現し得ることを見出したものであって、その目的とす
るところは、冷間加工が容易であって、静磁歪が−40
〜−1.70 XIO−”の値で、磁歪作動体としての
用途に充分適合する新規な材料を提供することにある。
In the present invention, it has been discovered that with a specific composition of a palladium-cobalt alloy, a large magnetostriction characteristic that far exceeds the magnetostriction value of conventional magnetostrictive materials can be developed by simple heat treatment or processing. The purpose is to be easy to cold work and have a magnetostatic strain of -40.
The object of the present invention is to provide a new material which has a value of ˜-1.70 XIO-'' and is fully suitable for use as a magnetostrictive actuator.

(課題を解決するための手段) 本発明は、重量比にてパラジウム40〜92%およびコ
バルト60〜8%から成り、少量の不純物を含む合金を
、900゜C以上1400゜C以下の温度で熱間加工し
、次いで冷間加工により線材あるいは薄板材などの所望
形状とした後、空気中、不活性ガス中あるいは真空中に
おいて900゜C以上融点以下の温度でl分間以上加熱
し、ついで任意の速度で徐冷し、静磁歪が−40〜−1
70 XIO−’である磁歪作動体を得ることを特徴と
する磁歪作動体の製造法にある。
(Means for Solving the Problems) The present invention consists of an alloy consisting of 40 to 92% palladium and 60 to 8% cobalt by weight and containing a small amount of impurities at a temperature of 900°C to 1400°C. After hot working and then cold working into a desired shape such as a wire rod or thin plate material, it is heated in air, in an inert gas, or in a vacuum at a temperature of 900°C or more and the melting point or less for 1 minute or more, and then optionally The magnetostatic strain is -40 to -1.
70 XIO-'.

(作 用) 次に本発明合金の製法について説明する。(for production) Next, a method for producing the alloy of the present invention will be explained.

まず上記の組成範囲のパラジウムとコバルI・とを、空
気中または不活性ガス中または真空中において通常の溶
解炉によって溶解したのち、充分に撹拌して組成的に均
一な溶融合金を造る。次にこれを鋳型に注入して鋳塊を
つくり、さらにこれを900 ’C以上1400゜C以
下の温度て鍛造、圧延あるいはスウエージ等の熱間加工
を施した後、常温あるいは常温以上で冷間加工して、用
途に適合する形状の素材を形戒する。この或形体は90
0゜C以上融点以下の温度、例えば1000゜Cにおい
てl分間以上、通常1時間程度加熱保持したのち徐冷し
て製品とするのである。次に本発明の実施例について述
べる。
First, palladium and Kobal I having the above composition range are melted in a conventional melting furnace in air, an inert gas, or a vacuum, and then sufficiently stirred to produce a compositionally uniform molten alloy. Next, this is poured into a mold to make an ingot, which is then subjected to hot working such as forging, rolling, or swaging at a temperature of 900°C to 1400°C, and then cold worked at room temperature or above room temperature. Process and shape the material to suit the purpose. This certain shape is 90
The product is heated and maintained at a temperature of 0°C or higher and lower than the melting point, for example 1000°C, for 1 minute or more, usually for about 1 hour, and then slowly cooled to form a product. Next, examples of the present invention will be described.

実施例 パラジウムおよびコバルトをタンマン炉(電気抵抗炉)
を用い、内径約10mmのアルミナるつぼ中でアルゴン
ガスを通じながら溶解し、溶湯をよく撹拌したのち、内
径約3mmの石英管中に吸い上げて冷却した。次にそれ
を常温においてスウエージング加工を施して直径2mm
の丸捧にし、この丸捧から長さ約10cmの試料を切り
取った。ついでそれをl000゜Cで1時間加熱後、1
00゜C/時間の速度で冷却して測定試料とした。試料
の長手方向の縦磁歪の測定は、2本の回転子を有する光
学梃子方式による装置を用いて行った。一方、溶融合金
を鉄型に注入して造った鋳塊を、熱間鍛造、冷間圧延に
よって約0.2mmの薄板とした。この薄板から内径3
3mm、外径45mmの環状試料を打ち抜き、それに丸
棒試料の場合と同じ熱処理を施して、動磁歪特性測定試
料とした。動磁歪特性の測定は、通常のマックスウエル
ブリッジ方式による装置を用いて行った。
Example Palladium and cobalt were prepared in a Tammann furnace (electric resistance furnace)
The molten metal was melted in an alumina crucible with an inner diameter of about 10 mm while passing argon gas through it, and the molten metal was thoroughly stirred, then sucked into a quartz tube with an inner diameter of about 3 mm and cooled. Next, it was swaged at room temperature to a diameter of 2 mm.
A sample with a length of about 10 cm was cut from this round offering. Then, after heating it at 1000°C for 1 hour,
The sample was cooled at a rate of 00°C/hour and used as a measurement sample. The longitudinal magnetostriction of the sample in the longitudinal direction was measured using an optical lever type device having two rotors. On the other hand, an ingot made by pouring the molten alloy into an iron mold was hot forged and cold rolled into a thin plate of approximately 0.2 mm. From this thin plate, the inner diameter is 3
An annular sample with a diameter of 3 mm and an outer diameter of 45 mm was punched out and subjected to the same heat treatment as the round bar sample to obtain a sample for measuring dynamic magnetostriction characteristics. The dynamic magnetostriction characteristics were measured using an ordinary Maxwell bridge system.

第1表に本発明例の印加磁場Hex=1.2 koeに
於ける縦磁歪の値と3種の従来合金の飽和磁歪の値とを
示した。
Table 1 shows the longitudinal magnetostriction values of the present invention example at an applied magnetic field Hex=1.2 koe and the saturation magnetostriction values of the three conventional alloys.

第1表 第1図には測定結果のうち、パラジウムおよびコバルト
の重量割合か57%=43%,77%=23%,80%
:20%. 82% : 18%および90%:lO%
の各組成になる合金ならびに比較例としてニッケルにつ
いての縦磁歪値と印加磁場Hex  との関係が示して
ある。これらの結果から縦磁歪については本発明の磁歪
作動体はすへての組成においてニッケルのそれよりも大
きく、特にパラジウム82%、コバルトI8%の磁歪作
動体の値は11000eの磁場において、ニッケルの約
5倍の−167 XIO−’という大きな値を示すこと
がわかる。
Table 1 Figure 1 shows the weight percentage of palladium and cobalt among the measurement results: 57% = 43%, 77% = 23%, 80%.
:20%. 82%: 18% and 90%: lO%
The relationship between the longitudinal magnetostriction value and the applied magnetic field Hex is shown for alloys having each composition and for nickel as a comparative example. These results show that the longitudinal magnetostriction of the magnetostrictive actuator of the present invention is larger than that of nickel in all compositions, and in particular, the value of the magnetostrictive actuator with 82% palladium and 8% cobalt I is higher than that of nickel in a magnetic field of 11000 e. It can be seen that it exhibits a large value of -167 XIO-', which is about five times as large.

第2図には本発明の組成範囲における各種磁歪作動体に
、100 0e , 200 0eおよびl2000e
の印加磁場を作用させたときの縦磁歪値か示してある。
Figure 2 shows various magnetostrictive actuators in the composition range of the present invention, 100 0e, 200 0e, and 12000e.
The longitudinal magnetostriction value when an applied magnetic field is applied is shown.

すなわち、いずれの印加磁場においてもコバルト!5〜
20%において最大となっている。
That is, cobalt in any applied magnetic field! 5~
It is maximum at 20%.

第3図には本発明の磁歪作動体の縦磁歪と印加磁場との
比の最大値(λ/ H ex) maxと濃度との関係
が示してある。ここで、(λ/Hex) maXはコバ
ルト含有tto〜20%の合金では−1.1〜−1.5
xlO−@oe−’で、ニッケルのそれと比較して同程
度かあるいはそれ以上の値となっている。特にコバルト
含有量が1896の合金では−1.53X 10−’O
e−’で、ニッケルの約1.5倍の大きさである。なお
、磁歪振動子においては、性能指数である電気機械結合
係数kの値も重要なので、これをパラジウム82%、コ
バルト18%の合金について測定した結果が第4図に示
してある。図にみるように本発明の磁歪作動体のkはニ
ッケルと比較すると、直流偏倚磁場が約350e以下で
は小さいか、それを超えるとニッケルのkより大きくな
っている。
FIG. 3 shows the relationship between the maximum value (λ/H ex) max of the ratio of the longitudinal magnetostriction of the magnetostrictive body of the present invention to the applied magnetic field and the concentration. Here, (λ/Hex) maX is -1.1 to -1.5 for alloys containing tto ~20% cobalt.
xlO-@oe-', which is comparable to or greater than that of nickel. Especially for alloys with cobalt content of 1896 -1.53X 10-'O
e-', which is approximately 1.5 times larger than nickel. Note that in a magnetostrictive vibrator, the value of the electromechanical coupling coefficient k, which is a figure of merit, is also important, and the results of measuring this for an alloy of 82% palladium and 18% cobalt are shown in FIG. As shown in the figure, k of the magnetostrictive actuator of the present invention is small when the DC deflection magnetic field is about 350e or less when compared with nickel, or becomes larger than k of nickel when the DC bias magnetic field exceeds about 350e.

以上詳細に説明したように、本発明の磁歪作動体は磁歪
振動体用素子としても利用し得るものである。また、本
発明の磁歪作動体は非常に大きな飽和磁歪値を示すばか
りでなく、面心立方晶の単一固溶体からなっているから
、冷間あるいは熱間加工がまことに容易で、任意の形状
の戒形体を得ることが可能である。このことは磁歪振動
体や、磁歪バイメタル等の薄板を製造する際にも大きな
利点である。
As explained above in detail, the magnetostrictive actuator of the present invention can also be used as an element for a magnetostrictive vibrator. In addition, the magnetostrictive actuator of the present invention not only exhibits a very large saturation magnetostriction value, but also consists of a single solid solution of face-centered cubic crystals, so cold or hot working is extremely easy, and it can be formed into any shape. It is possible to obtain a precept form. This is also a great advantage when manufacturing thin plates such as magnetostrictive vibrators and magnetostrictive bimetals.

最後に、本発明においてパラジウム40〜92%と限定
した理由はパラジウム40%以下および92%以上では
静磁歪の飽和値の絶対値か所期の目的とする40X10
−”以上の値よりも小さくなるからである。
Finally, the reason why palladium is limited to 40 to 92% in the present invention is that when palladium is below 40% and above 92%, the absolute value of the saturation value of magnetostriction is
This is because the value is smaller than the value greater than or equal to "-".

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

第1図はバラジウムーコバルト系磁歪作動体の縦磁歪と
印加磁場との関係を示した特性曲線図、第2図はバラジ
ウムーコバルト系磁歪作動体の100 , 200およ
び12000eの印加磁場における縦磁歪と合金濃度と
の関係を示した特性曲線図、第3図はパラジウムーコバ
ルト系磁歪作動体の(λ/Hex) maxと合金濃度
との関係を示した特性曲線図、 第4図はパラジウム82%、コバルト18%の磁歪作動
体の電気機械結合係数と直流偏倚磁場との関係を示した
特性曲線図である。 第1図 0 200 400 600   500   /θω EPNrA jJj }−1eX (Oe)/7oo 1400 第2図 コ/ζルFi4*(”.) 図面の浄書(内容に変更なし) 1!! >iviRi”fr 40 塙(Oe)第3図 コバ゜ル}−さ肴蛋(%) 手 続 補 正 書(方式) 平戒 2年 7月 2日
Fig. 1 is a characteristic curve diagram showing the relationship between longitudinal magnetostriction and applied magnetic field of a magnetostrictive actuator based on palladium-cobalt, and Fig. 2 is a characteristic curve diagram showing the relationship between longitudinal magnetostriction and applied magnetic field of a magnetostrictive actuator based on palladium-cobalt. Figure 3 is a characteristic curve diagram showing the relationship between longitudinal magnetostriction and alloy concentration. Figure 3 is a characteristic curve diagram showing the relationship between (λ/Hex) max and alloy concentration of a palladium-cobalt magnetostrictive actuator. It is a characteristic curve diagram showing the relationship between the electromechanical coupling coefficient and the DC bias magnetic field of a magnetostrictive actuator made of 82% palladium and 18% cobalt. Fig. 1 0 200 400 600 500 /θω EPNrA jJj }-1eX (Oe) /7oo 1400 Fig. 2 Ko/ζru Fi4*(”.) Engraving of drawing (no change in content) 1!! >iviRi”fr 40 Hanawa (Oe) Figure 3 Kobaru}-Sapphire (%) Procedural amendment (method) July 2, 2017

Claims (1)

【特許請求の範囲】[Claims] 1、重量比にてパラジウム40〜92%およびコバルト
60〜8%から成り、少量の不純物を含む合金を、90
0℃以上1400゜C以下の温度で熱間加工し、次いで
冷間加工により線材あるいは薄板材などの所望形状とし
た後、空気中、不活性ガス中あるいは真空中において9
00℃以上融点以下の温度で1分間以上加熱し、ついで
任意の速度で徐冷し、¥静磁歪が−40〜−170¥×
10^−^6る磁歪作動体を得ることを特徴とする磁歪
作動体の製造法。
1. An alloy consisting of 40-92% palladium and 60-8% cobalt by weight and containing a small amount of impurities is
After hot working at a temperature of 0°C or higher and 1400°C or lower, and then cold working to form a desired shape such as a wire or thin plate, it is heated in air, in an inert gas, or in a vacuum for 90 minutes.
Heating for 1 minute or more at a temperature of 00℃ or higher and lower than the melting point, then slowly cooling at an arbitrary speed until the magnetostriction is -40 to -170
A method for producing a magnetostrictive actuating body, characterized in that a magnetostrictive actuating body is obtained.
JP3221190A 1990-02-13 1990-02-13 Magnetostrictive actuator manufacturing method Expired - Lifetime JPH0645850B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP3221190A JPH0645850B2 (en) 1990-02-13 1990-02-13 Magnetostrictive actuator manufacturing method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3221190A JPH0645850B2 (en) 1990-02-13 1990-02-13 Magnetostrictive actuator manufacturing method

Related Parent Applications (1)

Application Number Title Priority Date Filing Date
JP57035048A Division JPS58153743A (en) 1982-03-08 1982-03-08 Palladium-cobalt alloy useful as magnetostrictive working body and manufacture thereof

Publications (2)

Publication Number Publication Date
JPH0317248A true JPH0317248A (en) 1991-01-25
JPH0645850B2 JPH0645850B2 (en) 1994-06-15

Family

ID=12352585

Family Applications (1)

Application Number Title Priority Date Filing Date
JP3221190A Expired - Lifetime JPH0645850B2 (en) 1990-02-13 1990-02-13 Magnetostrictive actuator manufacturing method

Country Status (1)

Country Link
JP (1) JPH0645850B2 (en)

Cited By (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH055984U (en) * 1991-07-05 1993-01-29 淡路技建株式会社 Anti-vibration adjust type floor support leg
JPH0566141U (en) * 1992-02-17 1993-08-31 富泰 本多 Floor board support device
KR100417332B1 (en) * 2001-02-20 2004-02-05 김대관 a spine protector
WO2004053175A3 (en) * 2002-09-27 2004-10-14 Univ Utah Res Found Control of engineering processes using magnetostrictive alloy compositions
JP2006110179A (en) * 2004-10-15 2006-04-27 Fuairudo Kk Lumbar pressure belt
EP1724368A3 (en) * 2004-10-12 2010-02-17 Heraeus, Inc. Low oxygen content alloy compositions
WO2015083821A1 (en) * 2013-12-06 2015-06-11 国立大学法人弘前大学 Method for producing magnetostrictive material and method for increasing amount of magnetostriction

Cited By (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH055984U (en) * 1991-07-05 1993-01-29 淡路技建株式会社 Anti-vibration adjust type floor support leg
JPH0566141U (en) * 1992-02-17 1993-08-31 富泰 本多 Floor board support device
KR100417332B1 (en) * 2001-02-20 2004-02-05 김대관 a spine protector
WO2004053175A3 (en) * 2002-09-27 2004-10-14 Univ Utah Res Found Control of engineering processes using magnetostrictive alloy compositions
US7179338B2 (en) 2002-09-27 2007-02-20 University Of Utah Research Foundation Control of engineering processes using magnetostrictive alloy compositions
EP1724368A3 (en) * 2004-10-12 2010-02-17 Heraeus, Inc. Low oxygen content alloy compositions
JP2006110179A (en) * 2004-10-15 2006-04-27 Fuairudo Kk Lumbar pressure belt
WO2015083821A1 (en) * 2013-12-06 2015-06-11 国立大学法人弘前大学 Method for producing magnetostrictive material and method for increasing amount of magnetostriction

Also Published As

Publication number Publication date
JPH0645850B2 (en) 1994-06-15

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