JPH0663064B2 - Method for producing manganese-aluminum-carbon alloy magnet - Google Patents
Method for producing manganese-aluminum-carbon alloy magnetInfo
- Publication number
- JPH0663064B2 JPH0663064B2 JP5639185A JP5639185A JPH0663064B2 JP H0663064 B2 JPH0663064 B2 JP H0663064B2 JP 5639185 A JP5639185 A JP 5639185A JP 5639185 A JP5639185 A JP 5639185A JP H0663064 B2 JPH0663064 B2 JP H0663064B2
- Authority
- JP
- Japan
- Prior art keywords
- billet
- magnet
- aluminum
- carbon alloy
- alloy magnet
- 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
Links
- 229910001339 C alloy Inorganic materials 0.000 title claims description 20
- 238000004519 manufacturing process Methods 0.000 title claims description 11
- -1 manganese-aluminum-carbon Chemical compound 0.000 title claims description 7
- 238000007906 compression Methods 0.000 claims description 42
- 230000006835 compression Effects 0.000 claims description 36
- 230000005415 magnetization Effects 0.000 claims description 29
- 230000002093 peripheral effect Effects 0.000 claims description 29
- 238000000034 method Methods 0.000 claims description 16
- RQMIWLMVTCKXAQ-UHFFFAOYSA-N [AlH3].[C] Chemical compound [AlH3].[C] RQMIWLMVTCKXAQ-UHFFFAOYSA-N 0.000 claims 2
- 230000005291 magnetic effect Effects 0.000 description 18
- 229910045601 alloy Inorganic materials 0.000 description 7
- 239000000956 alloy Substances 0.000 description 7
- 230000001747 exhibiting effect Effects 0.000 description 3
- 230000004907 flux Effects 0.000 description 3
- 230000005405 multipole Effects 0.000 description 3
- 230000015572 biosynthetic process Effects 0.000 description 2
- 238000001125 extrusion Methods 0.000 description 2
- 239000000314 lubricant Substances 0.000 description 2
- 239000000203 mixture Substances 0.000 description 2
- 229910002059 quaternary alloy Inorganic materials 0.000 description 2
- 238000000304 warm extrusion Methods 0.000 description 2
- 230000003245 working effect Effects 0.000 description 2
- 239000000654 additive Substances 0.000 description 1
- 230000000996 additive effect Effects 0.000 description 1
- 229910052799 carbon Inorganic materials 0.000 description 1
- 238000005266 casting Methods 0.000 description 1
- 239000000470 constituent Substances 0.000 description 1
- RKTYLMNFRDHKIL-UHFFFAOYSA-N copper;5,10,15,20-tetraphenylporphyrin-22,24-diide Chemical compound [Cu+2].C1=CC(C(=C2C=CC([N-]2)=C(C=2C=CC=CC=2)C=2C=CC(N=2)=C(C=2C=CC=CC=2)C2=CC=C3[N-]2)C=2C=CC=CC=2)=NC1=C3C1=CC=CC=C1 RKTYLMNFRDHKIL-UHFFFAOYSA-N 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 229910001325 element alloy Inorganic materials 0.000 description 1
- 230000005294 ferromagnetic effect Effects 0.000 description 1
- 238000010438 heat treatment Methods 0.000 description 1
- 239000012535 impurity Substances 0.000 description 1
- 230000005389 magnetism Effects 0.000 description 1
- 238000005259 measurement Methods 0.000 description 1
- 238000003672 processing method Methods 0.000 description 1
- 238000007493 shaping process Methods 0.000 description 1
- 229910002058 ternary alloy Inorganic materials 0.000 description 1
Landscapes
- Manufacturing Cores, Coils, And Magnets (AREA)
Description
【発明の詳細な説明】 産業上の利用分野 本発明は、永久磁石の製造法に関するものである。さら
に詳細には、多結晶マンガン−アルミニウム−炭素系
(Mn−Al−C系)合金磁石の製造法に関し、特に高性能
能な多極着磁用Mn−Al−C系合金磁石の製造法に関する
ものである。TECHNICAL FIELD The present invention relates to a method for manufacturing a permanent magnet. More specifically, it relates to a method for producing a polycrystalline manganese-aluminum-carbon system (Mn-Al-C system) alloy magnet, and more particularly to a method for producing a high-performance Mn-Al-C system alloy magnet for magnetizing multipoles. It is a thing.
従来の技術 Mn−Al−C系合金磁石は、主として強磁性相である面心
正方晶(τ相、L10型規則格子)の組織で構成され、C
を必須構成元素として含むものであり、不純物以外に添
加元素を含まない3元系及び小量の添加元素を含む4元
系以上の多元系合金磁石が知られており、これらを総称
するものである。ART Mn-Al-C alloy magnet is composed of mainly face-centered tetragonal (tau phase, L1 0 type ordered lattice) is a ferromagnetic phase of tissue, C
Is included as an essential constituent element, and ternary alloy magnets of quaternary system or more containing no additional element other than impurities and quaternary system or more containing a small amount of additive element are known. is there.
また、このMn−Al−C系合金磁石の製造法としては、鋳
造・熱処理によるもの以外に、温間押出加工等の温間塑
性加工工程を含むものが知られている。特に後者は、高
い磁気特性、機械的強度、耐候性、機械加工性等の優れ
た性質を有する異方性磁石の製造法として取られてい
る。Further, as a method of manufacturing the Mn-Al-C alloy magnet, a method including a warm plastic working step such as warm extrusion processing is known in addition to the method of casting and heat treatment. In particular, the latter is taken as a method for producing an anisotropic magnet having excellent properties such as high magnetic properties, mechanical strength, weather resistance, and machinability.
多極着磁用Mn−Al−C系合金磁石の製造法としては、等
方性磁石、圧縮加工によるもの、あらかじめ温間押出加
工等の公知の方法で得た一軸異方性の多結晶Mn−Al−C
系合金磁石に異方性方向への温間自由圧縮加工によるも
の(例えば特開昭56−119762号公報)、及びあらかじめ
異方性化した多結晶Mn−Al−C系合金磁石からなる中空
体状のビレットの軸方向に圧縮ひずみを与える各種の塑
性加工によるもの(例えば特開昭58−182206〜8号公
報)が知られている。The method for producing the Mn-Al-C alloy magnet for multipolar magnetization is an isotropic magnet, a compression processing method, or a uniaxially anisotropic polycrystalline Mn obtained by a known method such as warm extrusion processing in advance. -Al-C
A hollow body made of a system alloy magnet by warm free compression in an anisotropic direction (for example, Japanese Patent Laid-Open No. 56-119762) and a pre-anisotropic polycrystalline Mn-Al-C system alloy magnet. There are known various types of plastic working (for example, JP-A-58-182206-8) which give a compressive strain in the axial direction of the billet.
発明が解決しようとする問題点 多極着磁用磁石の形状は一般に円筒体であり、主な着磁
としては、第2図に示したような着磁がある。第2図は
円筒磁石の内周面に多極着磁した場合の磁石内部での磁
路の形成を模式的に示したものである。このような着磁
をここでは内周着磁と称する。Problems to be Solved by the Invention The shape of a multi-pole magnetizing magnet is generally a cylindrical body, and the main magnetizing is magnetizing as shown in FIG. FIG. 2 schematically shows the formation of a magnetic path inside the magnet when the inner peripheral surface of the cylindrical magnet is magnetized in multiple poles. Such magnetization is referred to as inner circumference magnetization here.
前述したあらかじめ異方性化した多結晶Mn−Al−C系合
金磁石からなる中空体状のビレットの軸方向に圧縮ひず
みを与える各種の塑性加工によって得られ磁石では、前
記内周着磁を施した場合、局部的には磁路に沿った方向
に異方性化しているが、全体をみた場合には望ましい方
向に異方性化いていない。また、前述した公知の方法
で、円筒磁石の内周部は径方向に異方性化し、外周部で
は周方向(弦方向)に異方性化したものが得られている
が、磁路が径方向から周方向(弦方向)に変化する途中
ではその方向に沿った異方性構造ではなく、さらに高温
度での塑性加工を2回以上行う必要がある。In the magnet obtained by various plastic workings that give compressive strain in the axial direction of the hollow body billet made of the previously anisotropy-crystallized polycrystalline Mn-Al-C alloy magnet, the inner circumferential magnetization is applied. In this case, locally anisotropy was made in the direction along the magnetic path, but when viewed as a whole, it was not anisotropy in the desired direction. Further, according to the above-mentioned known method, the inner circumferential portion of the cylindrical magnet is anisotropic in the radial direction and the outer circumferential portion is anisotropic in the circumferential direction (the chord direction). During the process of changing from the radial direction to the circumferential direction (chordal direction), it is not an anisotropic structure along that direction, and it is necessary to perform plastic working at a higher temperature twice or more.
問題点を解決するための手段 以上述べてきた問題点を解決するために本発明は、あら
かじめ異方性化した多結晶Mn−Al−C系合金磁石からな
る中空体状の軸対称形状のビレットに、530〜830℃の温
度で、ビレットの軸方向に圧縮加工し、この圧縮加工に
よってビレットの内周面の断面形状を(2n+2)角形
(n=1,2,3…)状に成形するものである。Means for Solving the Problems In order to solve the problems described above, the present invention provides a hollow body-shaped axisymmetric billet made of a pre-anisotropic polycrystalline Mn-Al-C alloy magnet. Then, the billet is compressed in the axial direction at a temperature of 530 to 830 ° C, and the cross-section of the inner peripheral surface of the billet is formed into a (2n + 2) square (n = 1,2,3 ...) It is a thing.
作用 この方法によって、つまりこの圧縮加工によってビレッ
トの内周面の断面形状を(2n+2)角形(n=1,2,3
…)状に成形することにより、第2図に示した内周着磁
を施した場合の磁路に沿って異方性化させることがで
き、高い磁気特性を示す異方性磁石を得ることができ
る。Action By this method, that is, by this compression processing, the cross-sectional shape of the inner peripheral surface of the billet is changed to (2n + 2) square (n = 1,2,3
...) to obtain an anisotropic magnet exhibiting high magnetic characteristics, which can be anisotropy along the magnetic path when the inner circumferential magnetization shown in FIG. 2 is applied. You can
実施例 以下本発明の一実施例を図面に基づいて説明する。本発
明はあらかじめ異方性化した多結晶Mn−Al−C系合金磁
石からなる中空体状の軸対称形状のビレットに、530〜8
30℃の温度で、前記ビレットの軸方向に圧縮加工を施す
ことによって、前記ビレットの内周面の断面形状を(2n
+2)角形(n=1,2,3…)状に成形するものである。Embodiment An embodiment of the present invention will be described below with reference to the drawings. The present invention provides a hollow body-shaped axisymmetric billet made of a pre-anisotropic polycrystalline Mn-Al-C alloy magnet.
By performing compression processing in the axial direction of the billet at a temperature of 30 ° C, the cross-sectional shape of the inner peripheral surface of the billet is (2n
+2) It is formed into a rectangular shape (n = 1,2,3 ...).
すなわち、公知のMn−Al−C系磁石用合金、例えば68〜
73質量%のMnと(1/10Mn−6.6)〜(1/3Mn−22.2)
質量%のCと残部のAlからなる合金を530〜830℃の温度
域で押出加工等の塑性加工を施すことによって異方性化
した多結晶Mn−Al−C系合金磁石を得る。前記磁石の代
表的なものとしては、前記塑性加工を押出加工とした場
合に得られる、押出方向に磁化容易方向を有する一軸異
方性磁石と、押出加工後さらに押出方向に自由圧縮加工
して得られる面異方性磁石などがある。前記異方性化し
た多結晶Mn−Al−C系合金磁石からなる中空体状の軸対
称の形状のビレットに、ビレットの内周面の断面形状が
(2n+2)角形(n=1,2,3…)状になるようにビレッ
トの軸方向に圧縮加工を施すことによって、第2図に示
した内周着磁において高い磁気特性を示す磁石を得るこ
とができる。That is, a known alloy for Mn-Al-C magnets, for example, 68-
73 mass% Mn and (1 / 10Mn-6.6) to (1 / 3Mn-22.2)
An anisotropic polycrystal Mn-Al-C alloy magnet is obtained by subjecting an alloy composed of C by mass% and the balance Al to plastic working such as extrusion in the temperature range of 530 to 830C. Typical examples of the magnet include a uniaxial anisotropic magnet having an easy magnetization direction in the extruding direction, which is obtained when the plastic working is extruding, and a free compression process in the extruding direction after the extruding process. There are obtained plane anisotropic magnets and the like. The hollow body of the billet having the axially symmetric shape made of the anisotropic Mn-Al-C alloy magnet has a cross section of the inner peripheral surface of the billet of (2n + 2) square (n = 1, 2, (3 ...) By performing compression processing in the axial direction of the billet so as to obtain a magnet exhibiting high magnetic characteristics in the inner circumferential magnetization shown in FIG.
前記ビレットが対称軸の方向に磁化容易方向を有する多
結晶Mn−Al−C系合金磁石(一軸異方性磁石)からなる
場合には、前記圧縮加工における対称軸の方向に圧縮ひ
ずみは対数ひずみの絶対値で0.05以上必要である。これ
は圧縮加工前のビレットは圧縮ひずみを与える方向に異
方性化したものであり、内周着磁において高い磁気特性
を示すような構造の変化に最低0.05の圧縮ひずみが必要
であるためである。When the billet is composed of a polycrystalline Mn-Al-C alloy magnet (uniaxial anisotropic magnet) having an easy magnetization direction in the direction of the symmetry axis, the compressive strain is logarithmic strain in the direction of the symmetry axis in the compression processing. An absolute value of 0.05 or more is required. This is because the billet before compression processing is anisotropy in the direction of giving compressive strain, and at least 0.05 compressive strain is required for the structural change that shows high magnetic characteristics in inner circumference magnetization. is there.
前記ビレットが対称軸に垂直な平面に平行に磁化容易方
向を有し、しかも前記平面内では磁気的に等方性であ
り、かつ前記軸方向と前記平面に平行な直線を含む平面
内では異方性である多結晶Mn−Al−C系合金磁石(両異
方性磁石)からなる場合には、圧縮加工前のビレットは
すでに、径方向と弦方向を含む平面内のすべての方向に
高い磁気特性を示しているが、本発明の圧縮加工を施す
ことによって、、内周着磁において高い磁気特性を示す
磁石を得ることができる。The billet has an easy magnetization direction parallel to a plane perpendicular to the axis of symmetry, is magnetically isotropic in the plane, and is different in a plane including a straight line parallel to the axial direction and the plane. When it is composed of a polycrystalline Mn-Al-C alloy magnet (bianisotropic magnet) that is anisotropic, the billet before compression is already high in all directions in the plane including the radial direction and the chord direction. Although the magnetic properties are shown, by performing the compression processing of the present invention, it is possible to obtain a magnet having high magnetic properties in the inner circumference magnetization.
前述した圧縮加工は、必ずしも連続的な圧縮加工である
必要はなく、複数回に分割して与えても良い。また、前
記ビレットとして、一軸異方性磁石及び面異方性磁石の
場合について示したが、放射状に磁化容易方向を有する
磁石、周方向に磁化容易方向を有する磁石などでもよ
く、必要なことはMn−Al−C系磁石用合金に所定の温度
域でなんらかの塑性加工が施されていることである。The compression processing described above does not necessarily have to be continuous compression processing, and may be given by dividing into a plurality of times. Further, although the uniaxial anisotropic magnet and the plane anisotropic magnet have been shown as the billet, a magnet having an easy magnetization direction in a radial direction, a magnet having an easy magnetization direction in the circumferential direction, and the like may be used. That is, some plastic working is applied to the Mn-Al-C magnet alloy in a predetermined temperature range.
前述した本発明の圧縮加工の一例をビレットの形状を円
筒体状とし、圧縮加工後のビレットの内周面の断面形状
を正方形(n=1の場合)として第1図を用いて説明す
る。第1図aは圧縮加工前の状態をビレットの軸方向か
らみた断面図である。1は円筒体状のビレット、2は外
型で、この外型2はビレットの外周面を圧縮加工によっ
て変形するのを防ぐための金型である。第1図bは圧縮
加工後の状態を示した断面図である。第1図bに示した
ように、円筒体状のビレットは圧縮加工の進行に伴なっ
て内径が小さくなり、内周面の一部がポンチ3の表面と
接触するようになる。さらに圧縮加工を施すことによっ
て第1図bに示したようにビレット1の内周面がほぼポ
ンチ3の表面に接触するまで圧縮加工を行うことができ
る。An example of the compression processing of the present invention described above will be described with reference to FIG. 1 in which the billet has a cylindrical shape and the cross-sectional shape of the inner peripheral surface of the billet after compression processing is square (when n = 1). FIG. 1a is a sectional view of the state before compression processing as seen from the axial direction of the billet. 1 is a cylindrical billet, 2 is an outer die, and this outer die 2 is a die for preventing the outer peripheral surface of the billet from being deformed by compression processing. FIG. 1b is a sectional view showing a state after compression processing. As shown in FIG. 1B, the inner diameter of the cylindrical billet becomes smaller as the compression process progresses, and a part of the inner peripheral surface comes into contact with the surface of the punch 3. By further performing the compression process, the compression process can be performed until the inner peripheral surface of the billet 1 almost contacts the surface of the punch 3 as shown in FIG.
また、第1図bに示した状態まで圧縮加工を行う必要が
なく、ビレット1の内周面の一部がポンチ3の表面と接
触した後は、任意の時点で圧縮加工を終了してもよい。Further, it is not necessary to perform the compression processing to the state shown in FIG. 1B, and even if the compression processing is finished at any time after a part of the inner peripheral surface of the billet 1 comes into contact with the surface of the punch 3. Good.
本発明のビレットの圧縮加工前の内径の最小は、ポンチ
3の表面と接する大きさである。その場合は、圧縮加工
前にすでにビレット1の内周面の一部がポンチ3の表面
によって拘束された状態で圧縮加工が施される。The minimum inner diameter of the billet of the present invention before compression processing is the size in contact with the surface of the punch 3. In that case, the compression processing is performed in a state where a part of the inner peripheral surface of the billet 1 is already constrained by the surface of the punch 3 before the compression processing.
また、前記の例では、圧縮加工前にすでにビレット1の
外周面は外型2の内面と接触しており、拘束された状態
であるが、ビレット1の外径が外型2の内径よりかなり
小さく、かなりのクリアランスがあっても良い。この場
合、圧縮加工の進行に伴なってビレット1の外径および
内径が共に大きくなり、ビレット1の外周面が外型2の
内面と接触し、ほぼ第1図aに示した状態になる。以下
の変化は前述した変化と同様である。Further, in the above example, the outer peripheral surface of the billet 1 is already in contact with the inner surface of the outer mold 2 before being compressed, and thus the billet 1 is in a restrained state, but the outer diameter of the billet 1 is considerably larger than the inner diameter of the outer mold 2. It may be small and have some clearance. In this case, both the outer diameter and the inner diameter of the billet 1 increase with the progress of the compression process, and the outer peripheral surface of the billet 1 contacts the inner surface of the outer mold 2, and the state becomes substantially as shown in FIG. The following changes are similar to the changes described above.
前述した例では、ビレットの内周面の断面形状の変化は
円形からほぼ正方形(各角が多少の面取りをしたような
Rが存在してもよい)であり、このような変化によって
内周着磁に適した異方性構造を有するようになる。圧縮
加工過程において、最も早く内周面が拘束された部分は
弦方向に磁化容易方向を有する部分となり、最後に内周
面が拘束された部分又は最後まで内周面が拘束されなか
った部分は径方向に磁化容易方向を有するようになる。
それらの間の部分は磁化容易方向が径方向から弦方向へ
順次変化する部分である。このように内周着磁において
何極着磁するかによって、圧縮加工後のビレットの形状
を決定すればよい。つまり、前述した例では圧縮加工後
のビレットの内周面の断面形状がほぼ正方形であったた
め、4極着磁に適した異方性構造を有する。圧縮加工後
のビレットの内周面の断面形状を(2n+2)角形(n=
1,2,3…)状としているのは、前述したように、内周着
磁は偶数極であり、偶数の多角形状の断面形状である必
要がある。n=1のとき4極用、n=2の時6極用とい
うようになる。nが小さいほど、前述した位置による異
方性構造が明確であるが、大きくなるにつれて次第に不
明確になる。In the above-mentioned example, the change in the cross-sectional shape of the inner peripheral surface of the billet is from circular to almost square (there may be R with a chamfer at each corner). It has an anisotropic structure suitable for magnetism. In the compression process, the part where the inner peripheral surface is constrained earliest becomes the part having the easy magnetization direction in the chord direction, and the part where the inner peripheral surface is restricted at the end or the part where the inner peripheral surface is not restricted until the end is It has an easy magnetization direction in the radial direction.
The portion between them is a portion in which the easy magnetization direction sequentially changes from the radial direction to the chord direction. In this way, the shape of the billet after compression processing may be determined depending on how many poles are magnetized in the inner circumference magnetization. That is, in the above-mentioned example, since the sectional shape of the inner peripheral surface of the billet after compression processing is substantially square, it has an anisotropic structure suitable for quadrupole magnetization. The cross-sectional shape of the inner peripheral surface of the billet after compression processing is (2n + 2) square (n =
As described above, it is necessary that the inner circumferential magnetization has an even number of poles and an even polygonal cross-sectional shape. When n = 1, 4 poles are used, and when n = 2, 6 poles are used. The smaller n is, the clearer the anisotropic structure due to the above-mentioned position becomes, but the larger n becomes, the more unclear it becomes.
本発明でいう(2n+2)角形(n=1,2,3…)状という
のは、幾何学的な正確な(2n+2)角形である必要はな
く、多少の面取り等があっても問題はない。The (2n + 2) polygon (n = 1,2,3 ...) in the present invention does not need to be a geometrically accurate (2n + 2) polygon, and there is no problem even if some chamfering etc. .
ビレットが円筒体の軸方向に磁化容易方向を有する多結
晶Mn−Al−C系合金磁石からなる場合は、前述した様に
圧縮ひずみが対数ひずみの絶対値で0.05以上必要であ
る。しかし、実際の応用上磁石の一部分を一軸異方性の
ままで磁化容易方向を保存されておきたい場合は、ビレ
ットの一部分の内周面を拘束することによって、局部的
に圧縮ひずみを与えない領域を作る方法でもよい。When the billet is made of a polycrystalline Mn-Al-C alloy magnet having an easy magnetization direction in the axial direction of the cylindrical body, the compressive strain must be 0.05 or more in absolute value of logarithmic strain as described above. However, in an actual application, if you want to preserve the direction of easy magnetization while keeping a part of the magnet as uniaxial anisotropy, constrain the inner peripheral surface of the part of the billet so that no compressive strain is locally applied. A method of creating a region may be used.
前記の一例で述べたように、本発明はビレットの軸方向
に圧縮加工する際に、金型(ポンチ)等を用いてビレッ
トの内周面の断面形状を(2n+2)角形(n=1,2,3
…)状になるように成形圧縮加工することによって、内
周着磁を施した場合に高い磁気特性を示す異方性構造を
有する磁石を得るものである。As described in the above example, in the present invention, when the billet is compressed in the axial direction, the cross-sectional shape of the billet inner peripheral surface is (2n + 2) square (n = 1, 2,3
..) to obtain a magnet having an anisotropic structure that exhibits high magnetic characteristics when subjected to inner circumference magnetization.
前述したような圧縮加工の可能な温度範囲については、
530〜830℃の温度領域において加工が行えたが、780℃
を越える温度では、磁気特性がかなり低下した。より望
ましい温度範囲としては560〜760℃であった。Regarding the temperature range in which compression processing as described above is possible,
Processing was possible in the temperature range of 530-830 ℃, but 780 ℃
At temperatures above, the magnetic properties deteriorated considerably. A more desirable temperature range was 560 to 760 ° C.
次に本発明の更に具体的な実施例について説明する。Next, more specific examples of the present invention will be described.
実施例1 配合組成で69.5質量%(以下単に%で示す)のMn、29.3
%のAl、0.5%のC及び0.7%のNiを溶解鋳造し、直径70
mm、長さ50mmの円柱ビレットを作製した。このビレット
を1100℃で2時間保持した後、室温まで放冷する熱処理
を行った。次に潤滑剤を介して720℃の温度で直径50mm
までの押出加工を行った。さらに潤滑剤を介して680℃
の温度で直径31mmまでの押出加工を行った。この押出棒
を長さ20mmに切断し、切削加工して、外径30mm、内径24
mm、長さ20mmの円筒ビレットを作製した。このビレット
を用いて、第1図に示した金型を用いて圧縮加工を行っ
た。第1図において、外型2の内径は30mmで、ポンチ3
の正方形の一辺の長さは14mmである。このような金型を
用いて、高さ10mmまで圧縮加工を行った。Example 1 69.5% by mass (hereinafter simply referred to as%) of Mn, 29.3 in the composition of the composition
% Al, 0.5% C and 0.7% Ni melt-cast, diameter 70
A cylindrical billet having a length of 50 mm and a length of 50 mm was produced. After holding this billet at 1100 ° C. for 2 hours, it was heat-treated by allowing it to cool to room temperature. Then through the lubricant at a temperature of 720 ℃ diameter 50 mm
Was extruded. 680 ℃ through lubricant
Extrusion processing was performed at a temperature of up to 31 mm in diameter. This extruded rod is cut to a length of 20 mm and cut to form an outer diameter of 30 mm and an inner diameter of 24
A cylindrical billet having a length of 20 mm and a length of 20 mm was produced. Using this billet, compression processing was performed using the mold shown in FIG. In FIG. 1, the inner diameter of the outer mold 2 is 30 mm, and the punch 3
The length of one side of the square is 14 mm. Using such a mold, compression processing was performed to a height of 10 mm.
圧縮加工後のビレットをその内周面の四隅を除く部分で
内径15mmまで切削加工し、4極の内周着磁を施した。着
磁は2000μFのオイルコンデンサを用い1500Vでパルス
着磁した。内周面の表面磁束密度をホール素子で測定し
た。比較のために、直径18mm、高さ20mmの円柱ビレット
を680℃の温度で円柱軸方向に自由圧縮加工した。な
お、圧縮加工後のビレットの高さは10mmであった。加工
後のビレットは面異方性磁石であり、前記と同様に切削
加工し、着磁し、表面磁束密度を測定した。The billet after compression processing was machined to an inner diameter of 15 mm except the four corners of the inner peripheral surface, and magnetized with four poles on the inner peripheral surface. For the magnetization, a 2000 μF oil condenser was used and pulsed at 1500 V. The surface magnetic flux density of the inner peripheral surface was measured with a Hall element. For comparison, a cylindrical billet having a diameter of 18 mm and a height of 20 mm was freely compressed in the axial direction of the cylinder at a temperature of 680 ° C. The height of the billet after compression processing was 10 mm. The billet after processing was a plane anisotropic magnet, cut and magnetized in the same manner as described above, and the surface magnetic flux density was measured.
以上の両者の値を比較すると、本発明の方法で得た磁石
の表面磁束密度の値は、面異方性磁石のそれの約1.6倍
であった。Comparing the above two values, the value of the surface magnetic flux density of the magnet obtained by the method of the present invention was about 1.6 times that of the surface anisotropic magnet.
上記実施例で得られた本発明の方法によって得た磁石
は、磁気トルク測定の結果、前述したように磁化容易方
向は圧縮加工後のビレットの内周面の辺の部分では径方
向に沿い、中間では弦方向に沿い、それらの間では径方
向から弦方向(周方向)に連続的に変化していることが
判明した。The magnet obtained by the method of the present invention obtained in the above example, as a result of the magnetic torque measurement, as described above, the easy magnetization direction is along the radial direction at the side portion of the inner peripheral surface of the billet after compression processing, It was found that it was along the chord direction in the middle, and between them was continuously changing from the radial direction to the chord direction (circumferential direction).
発明の効果 本発明は、実施例によって述べたように、あらかじめ異
方性化した多結晶Mn−Al−C系合金磁石からなる中空体
状の軸対称形状のビレットに、530〜830℃の温度で、ビ
レットの軸方向に圧縮加工を施してビレットの内周面の
断面形状を(2n+2)角形(n=1,2,3…)状に成形す
ることによって、内周着磁を施した場合に高い磁気特性
を示す磁石を得るものである。EFFECTS OF THE INVENTION As described in the embodiments, the present invention provides a hollow body-shaped axisymmetric billet made of a pre-anisotropic polycrystalline Mn-Al-C alloy magnet at a temperature of 530 to 830 ° C. When the inner circumference is magnetized by performing compression processing in the axial direction of the billet and shaping the cross-sectional shape of the inner circumference of the billet into a (2n + 2) square (n = 1,2,3 ...) It is intended to obtain a magnet exhibiting extremely high magnetic characteristics.
公知の方法によって得られる磁石と比較すると、本発明
の方法によって得られた磁石は内周着磁を施した場合公
知の方法による磁石より優れた磁気特性を示し、さらに
公知の方法で磁石の内周部が径方向に磁化容易方向を有
し、それよりも外周部で周方向(弦方向)に磁化容易方
向を有する構造を得るには少なくとも2回以上の塑性加
工を必要としたが、本発明の方法では少なくとも1回で
それよりも望ましい異方性構造を有する磁石を得ること
ができる。Compared with the magnet obtained by the known method, the magnet obtained by the method of the present invention shows superior magnetic characteristics to the magnet obtained by the known method when subjected to inner circumferential magnetization, and further At least two or more plastic workings were required to obtain a structure in which the peripheral portion has the easy magnetization direction in the radial direction, and the outer peripheral portion has the easy magnetization direction in the circumferential direction (chord direction). The method of the invention can at least once yield a magnet with a more desirable anisotropic structure.
第1図は本発明の一実施例の圧縮加工で用いる金型の断
面図でビレットの圧縮加工前後の断面形状の変化を示す
図、第2図は円筒状磁石の内周面に多極着磁を施した場
合の磁石内部での磁路の形成を模式的に示す図である。 1……ビレット、2……外型、3……ポンチFIG. 1 is a cross-sectional view of a die used for compression processing according to an embodiment of the present invention, showing a change in cross-sectional shape of a billet before and after compression processing, and FIG. 2 is a multi-pole attached to an inner peripheral surface of a cylindrical magnet. It is a figure which shows typically formation of the magnetic path inside a magnet when magnetizing. 1 ... Billet, 2 ... External type, 3 ... Punch
Claims (4)
アルミニウム−炭素系合金磁石からなる、円柱状の中空
部を有した軸対称の中空体状のビレットを、530〜830℃
の温度で、前記ビレットの軸方向に圧縮加工して、前記
ビレットの中空部を(2n+2)角柱(n=1、2、3
…)状に成形する第1工程と、前記第1工程において成
形した前記ビレットの(2n+2)角柱状の中空部の側面
の一平面の中間に極着磁する第2工程とを有したマンガ
ン−アルミニウム−炭素系合金磁石の製造法。1. Pre-anisotropic polycrystalline manganese-
An axisymmetric hollow body-shaped billet having a cylindrical hollow portion made of an aluminum-carbon alloy magnet was heated at 530 to 830 ° C.
At the temperature of, the billet is compressed in the axial direction to form a hollow part of the billet into a (2n + 2) prism (n = 1, 2, 3).
Manganese-having a first step of magnetizing the billet formed in the first step and a second step of magnetizing the billet in the middle of one plane of the side surface of the hollow part of the (2n + 2) prism A method for manufacturing an aluminum-carbon alloy magnet.
を有する多結晶マンガン−アルミニウム−炭素系合金磁
石からなり、圧縮加工における圧縮ひずみが対数ひずみ
の絶対値で0.05以上であることを特徴とする特許請求の
範囲第1項記載のマンガン−アルミニウム−炭素系合金
磁石の製造法。2. A billet is made of a polycrystalline manganese-aluminum-carbon alloy magnet having a direction of easy magnetization in the direction of the axis of symmetry, and the compression strain in compression processing is 0.05 or more in absolute value of logarithmic strain. The method for producing a manganese-aluminum-carbon alloy magnet according to claim 1.
磁化容易方向を有し、しかも前記平面内では磁気的に等
方性であり、かつ前記軸方向と前記平面に平行な直線を
含む平面内では異方性である多結晶マンガン−アルミニ
ウム−炭素系合金磁石からなることを特徴とする特許請
求の範囲第1項記載のマンガン−アルミニウム−炭素系
合金磁石の製造法。3. A billet has a straight line which has a direction of easy magnetization parallel to a plane perpendicular to the axis of symmetry, is magnetically isotropic in the plane, and is parallel to the axial direction and the plane. The method for producing a manganese-aluminum-carbon alloy magnet according to claim 1, which is composed of a polycrystalline manganese-aluminum-carbon alloy magnet which is anisotropic in a plane including the magnet.
拘束した状態で行うものであることを特徴とする特許請
求の範囲第1項記載のマンガン−アルミニウム−炭素系
合金磁石の製造法。4. The method for producing a manganese-aluminum-carbon alloy magnet according to claim 1, wherein the compression working is carried out with a part of the inner peripheral surface of the billet being constrained. .
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP5639185A JPH0663064B2 (en) | 1985-03-19 | 1985-03-19 | Method for producing manganese-aluminum-carbon alloy magnet |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP5639185A JPH0663064B2 (en) | 1985-03-19 | 1985-03-19 | Method for producing manganese-aluminum-carbon alloy magnet |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS61213356A JPS61213356A (en) | 1986-09-22 |
| JPH0663064B2 true JPH0663064B2 (en) | 1994-08-17 |
Family
ID=13025921
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP5639185A Expired - Lifetime JPH0663064B2 (en) | 1985-03-19 | 1985-03-19 | Method for producing manganese-aluminum-carbon alloy magnet |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0663064B2 (en) |
-
1985
- 1985-03-19 JP JP5639185A patent/JPH0663064B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS61213356A (en) | 1986-09-22 |
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