JPH061742B2 - Alloy magnet manufacturing method - Google Patents
Alloy magnet manufacturing methodInfo
- Publication number
- JPH061742B2 JPH061742B2 JP60025268A JP2526885A JPH061742B2 JP H061742 B2 JPH061742 B2 JP H061742B2 JP 60025268 A JP60025268 A JP 60025268A JP 2526885 A JP2526885 A JP 2526885A JP H061742 B2 JPH061742 B2 JP H061742B2
- Authority
- JP
- Japan
- Prior art keywords
- billet
- magnet
- peripheral surface
- inner peripheral
- anisotropic
- 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
- 229910045601 alloy Inorganic materials 0.000 title claims description 23
- 239000000956 alloy Substances 0.000 title claims description 23
- 238000004519 manufacturing process Methods 0.000 title claims description 11
- 230000002093 peripheral effect Effects 0.000 claims description 37
- 238000007906 compression Methods 0.000 claims description 35
- 230000006835 compression Effects 0.000 claims description 33
- 230000005415 magnetization Effects 0.000 claims description 30
- 238000000034 method Methods 0.000 claims description 13
- 229910001339 C alloy Inorganic materials 0.000 claims description 3
- RQMIWLMVTCKXAQ-UHFFFAOYSA-N [AlH3].[C] Chemical compound [AlH3].[C] RQMIWLMVTCKXAQ-UHFFFAOYSA-N 0.000 claims 1
- 230000005291 magnetic effect Effects 0.000 description 19
- 238000001125 extrusion Methods 0.000 description 6
- 238000007796 conventional method Methods 0.000 description 4
- 230000001747 exhibiting effect Effects 0.000 description 4
- 230000004907 flux Effects 0.000 description 3
- 239000000314 lubricant Substances 0.000 description 3
- 230000005405 multipole Effects 0.000 description 3
- 229910052799 carbon Inorganic materials 0.000 description 2
- 238000005266 casting Methods 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
- 230000015572 biosynthetic process Effects 0.000 description 1
- 230000000052 comparative effect Effects 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
- 238000005520 cutting process Methods 0.000 description 1
- 230000007423 decrease Effects 0.000 description 1
- 230000000694 effects Effects 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
- -1 manganese-aluminum-carbon Chemical compound 0.000 description 1
- 238000005259 measurement Methods 0.000 description 1
- 239000000203 mixture Substances 0.000 description 1
- 229910002059 quaternary alloy Inorganic materials 0.000 description 1
- 230000000452 restraining effect Effects 0.000 description 1
- 229910002058 ternary alloy Inorganic materials 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F41/00—Apparatus or processes specially adapted for manufacturing or assembling magnets, inductances or transformers; Apparatus or processes specially adapted for manufacturing materials characterised by their magnetic properties
- H01F41/02—Apparatus or processes specially adapted for manufacturing or assembling magnets, inductances or transformers; Apparatus or processes specially adapted for manufacturing materials characterised by their magnetic properties for manufacturing cores, coils, or magnets
- H01F41/0253—Apparatus or processes specially adapted for manufacturing or assembling magnets, inductances or transformers; Apparatus or processes specially adapted for manufacturing materials characterised by their magnetic properties for manufacturing cores, coils, or magnets for manufacturing permanent magnets
Landscapes
- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Manufacturing & Machinery (AREA)
- Hard Magnetic Materials (AREA)
- 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係り、とくに多結晶マン
ガン-アルミニウム-炭素(Mn-Al-C)系合金を用いた高
性能な多極着磁用Mn-Al-C系合金磁石の製造法に関す
る。Description: TECHNICAL FIELD The present invention relates to a method for manufacturing a permanent magnet, and particularly to a high-performance multi-purpose alloy using a polycrystalline manganese-aluminum-carbon (Mn-Al-C) alloy. The present invention relates to a method for manufacturing an Mn-Al-C alloy magnet for polar magnetization.
(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元系及び少量の添加元素を含む4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。The (prior art) Mn-Al-C alloy magnet is composed mainly face-centered tetragonal (tau phase, L1 0 type ordered lattice) is a ferromagnetic phase of tissue, those containing C as the essential constituent elements There are known ternary alloy magnets containing no additional element other than impurities and quaternary alloy magnets containing a small amount of additive element, and these are collectively referred to.
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あり、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知られている。In addition, as a method for manufacturing this Mn-Al-C alloy magnet, in addition to those by casting and heat treatment, there are those that include warm plastic working steps such as warm extrusion, and especially the latter have high magnetic properties, It is known as a method for producing an anisotropic magnet having excellent properties such as 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
(たとえば特開昭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(たとえば特開昭58-182206ないし182
208号公報)が知られている。As a method for producing Mn-Al-C alloy magnet for multi-pole magnetization, an isotropic magnet, one by compression processing, uniaxially anisotropic polycrystalline Mn obtained by a known method such as warm extrusion processing in advance. -Al-C alloy magnets by warm free compression in the anisotropic direction (for example, JP-A-56-119762), and pre-anisotropic polycrystalline Mn-Al-C alloy magnets By various plastic workings that give a compressive strain in the axial direction of a hollow billet made of (for example, JP-A-58-182206 to 182).
No. 208) is known.
(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4図に示したような着磁がある。第4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磁路は点線のようにな
る。このような着磁をここでは内周面着磁と称する。(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. 4 schematically shows formation of a magnetic path inside the magnet when the inner peripheral surface of the cylindrical magnet is magnetized in multiple poles, and the magnetic path is shown by a dotted line. Such magnetization is referred to as inner circumferential surface 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た磁石では、
前記の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
い方向に異方性化していない。また、前述した従来公知
の方法によって、円筒磁石の内周部が径方向に異方性化
し、外周部では周方向(弦方向、以下同じ)に異方性化
したものが得られるが、磁路が径方向から周方向に変化
する途中では、その方向に沿った異方性構造ではなく、
したがってさらに高温度での塑性加工を2回以上行なう
必要がある。In the axial direction of the hollow body-shaped billet made of the above-mentioned anisotropy polycrystalline Mn-Al-C alloy magnet, in the magnet obtained by various plastic workings that give compressive strain,
When the inner circumference is magnetized, it is locally anisotropic in the direction along the magnetic path, but when viewed as a whole, it is not anisotropic in the desired direction. Further, according to the above-mentioned conventionally known method, the inner peripheral portion of the cylindrical magnet is anisotropic in the radial direction and the outer peripheral portion thereof is anisotropic in the circumferential direction (the chord direction, the same hereinafter). In the course of changing the path from the radial direction to the circumferential direction, it is not an anisotropic structure along that direction,
Therefore, 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) 以上述べたような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
る中空体状のビレットを、そ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中空内周面を凹凸上に形
成することにより解決する。(Means for Solving Problems) In order to solve the problems described above, the present invention provides a hollow body-shaped billet made of a pre-anisotropic polycrystalline Mn-Al-C alloy magnet. The problem is solved by performing compression processing in the axial direction and forming the hollow inner peripheral surface of the billet on the unevenness by this compression processing.
(作 用) 本発明は上記の方法、すなわち、圧縮加工によってビレ
ットの中空内周面を凹凸状に形成することにより、第4
図に示した内周着磁を施した場合の点線で示す磁路に沿
って、異方性化させることができ、そのため高い磁気特
性を示す異方性磁石を得ることができる。(Operation) The present invention provides the fourth method by the above method, that is, by forming the hollow inner peripheral surface of the billet into an uneven shape by compression processing.
It is possible to anisotropy along the magnetic path shown by the dotted line when the inner circumference is magnetized as shown in the figure, so that it is possible to obtain an anisotropic magnet exhibiting high magnetic characteristics.
(実施例) 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ビレットをその軸方向に530な
いし830℃の温度で圧縮加工することによって、ビレッ
トの中空内周面を凹凸上に成形させるものである。(Examples) The present invention is a billet of a hollow body formed by pre-anisotropic polycrystal Mn-Al-C alloy magnet by compression processing in the axial direction at a temperature of 530 to 830 ℃. The inner peripheral surface of the hollow is formed on the uneven surface.
すなわち、従来のMn-Al-C系磁石用合金、例えば68ない
し73質量%のMnと(1/10Mn-6.6)ないし(1/3Mn-22.2)
質量%のCと残部がAlからなる合金に、530ないし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系合金磁石を得ることがで
き、代表的なものとしては、塑性加工を押出加工により
行なった場合に得られる、押出方向に磁化容易方向を有
する一軸異方性磁石と、その押出加工後、さらに押出方
向に自由圧縮加工を行なって得られる面異方性磁石など
がある。このように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に、その中空内周面が
凹凸状になるようにビレットの軸方向に圧縮加工を施せ
ば、第2図に示した内周着磁において高い磁気特性を示
す磁石が得られる。That is, a conventional alloy for Mn-Al-C magnets, for example, 68 to 73 mass% Mn and (1 / 10Mn-6.6) to (1 / 3Mn-22.2)
530 to 830 ℃ for alloys consisting of C in mass% and the balance Al
By performing plastic working such as extrusion in the temperature range of
Anisotropic polycrystalline Mn-Al-C alloy magnets can be obtained, and a typical example is a uniaxial magnet having an easy magnetization direction in the extrusion direction, which is obtained when plastic working is performed by extrusion. There are anisotropic magnets and plane anisotropic magnets obtained by performing free compression processing in the extrusion direction after the extrusion processing. In this way, a hollow body-shaped billet made of an anisotropic Mn-Al-C alloy magnet, if subjected to compression processing in the axial direction of the billet so that the hollow inner peripheral surface becomes uneven, A magnet having high magnetic characteristics can be obtained in the inner circumference magnetization shown in FIG.
上記において、ビレットが中空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、いわゆる一軸異
方性磁石からなる場合には、圧縮加工における対称軸の
方向の圧縮ひずみは、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が圧縮ひずみを
与える方向に異方性化されたものであるため、内周着磁
において高い磁気特性を示すように構造の変化に、最低
0.05の圧縮ひずみが必要であるからである。In the above, when the billet is composed of a polycrystalline Mn-Al-C alloy magnet having an easy magnetization direction in the axial direction of the hollow body, a so-called uniaxial anisotropic magnet, the compressive strain in the direction of the axis of symmetry in compression processing is The absolute value of logarithmic strain must be 0.05 or more. This is because the billet before compression processing is anisotropy in the direction that gives compressive strain, so the structure changes to the minimum in order to show high magnetic characteristics in inner circumference magnetization.
This is because a compressive strain of 0.05 is necessary.
また、前記のビレットが中空体の軸方向に垂直な平面に
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、いわゆる面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。Further, the billet has a direction of easy magnetization parallel to a plane perpendicular to the axial direction of the hollow body, is magnetically isotropic in the plane, and is a straight line parallel to the axial direction and the plane. In the case of a polycrystalline Mn-Al-C alloy magnet that is anisotropic in the plane containing the so-called plane anisotropic magnet, the billet before compression processing is already in the plane containing the radial direction and the chord direction. Although it exhibits high magnetic properties in all directions, it is possible to obtain a magnet exhibiting high magnetic properties in inner circumference magnetization by performing the compression processing of the present invention.
なお、上述の圧縮加工は、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、上記はビレットとして、一軸異方性磁石および面異
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 above-mentioned compression processing does not necessarily have to be continuous compression processing, and may be given by dividing it into a plurality of times. The billet described above is a uniaxial anisotropic magnet or a plane anisotropic magnet, but a magnet having an easy magnetization direction in the radial direction, a magnet having an easy magnetization direction in the circumferential direction, or the like may be used. Means that the Mn-Al-C magnet alloy has been subjected to some plastic working in a predetermined temperature range.
以下本発明の圧縮加工の一例をビレットの形状を円筒体
として第1図を用いて説明する。An example of the compression processing of the present invention will be described below with reference to FIG. 1 in which the billet has a cylindrical body.
第1図(a)は圧縮加工前の状態をビレットの軸方向から
見た断面図である。1は円筒体状のビレット、2は外型
で、圧縮加工時にビレット1の外周面を拘束するための
金型である。3はポンチで図に示すように断面は所定の
凹凸状である。同じく(b)図は加工後の状態を示し、円
筒体状のビレット1は圧縮加工の進行につれて内径が縮
まり、内周面の一部がポンチ3の凸部と接触、さらに圧
縮加工が進行することによって図のようにビレット1の
内周面はほぼポンチ3の外面形状になる。なお、圧縮は
(b)図に示した状態まで行なう必要はなく、ビレット1
の内周面の一部がポンチ3と接触した後は、適宜な時点
で圧縮加工を終了してもよい。言い換えれば、ビレット
1の内周面に凹凸が形成されればよい。また、前述した
例では圧縮加工前すでにビレット1の外周面と、外型2
の内面がほぼ接触状態であったが、接触していなくても
よい。つまり、ビレット1の外径が外型2の空洞部の径
よりかなり小さくてもよい。この場合は圧縮加工の進行
につれて、ビレット1の外径は大きくなり内径は小さく
なり、やがてビレット1の外周面が外型2の内面に接触
する。それ以降は前述した変化と同じである。一方、ビ
レット1の内径は、最小のときでポンチ3の凸部に接す
る大きさである。圧縮加工前にすでにビレット1と外型
2が接触した状態であれば、ビレット1の内周面の一部
が、つまりポンチ3の凸部と接触している部分が拘束さ
れた状態で圧縮加工が施される。FIG. 1 (a) is a sectional view of the state before compression processing as seen from the axial direction of the billet. Reference numeral 1 is a cylindrical billet, and 2 is an outer die, which is a die for restraining the outer peripheral surface of the billet 1 during compression processing. Reference numeral 3 is a punch, and as shown in the figure, its cross section has a predetermined uneven shape. Similarly, Fig. (B) shows a state after processing. The inner diameter of the cylindrical billet 1 shrinks as the compression processing progresses, a part of the inner peripheral surface contacts the convex portion of the punch 3, and the compression processing further progresses. As a result, the inner peripheral surface of the billet 1 becomes substantially the outer surface shape of the punch 3 as shown in the figure. The compression is
(b) It is not necessary to carry out the process shown in the figure
After a part of the inner peripheral surface of the punch 3 comes into contact with the punch 3, the compression processing may be finished at an appropriate time. In other words, irregularities may be formed on the inner peripheral surface of the billet 1. Further, in the above-mentioned example, the outer peripheral surface of the billet 1 and the outer die 2 have already been compressed.
Although the inner surface of was almost in contact, it does not have to be in contact. That is, the outer diameter of the billet 1 may be considerably smaller than the diameter of the cavity of the outer mold 2. In this case, as the compression processing progresses, the outer diameter of the billet 1 increases and the inner diameter decreases, and the outer peripheral surface of the billet 1 eventually contacts the inner surface of the outer mold 2. After that, it is the same as the change described above. On the other hand, the inner diameter of the billet 1 is the size that contacts the convex portion of the punch 3 at the minimum. If the billet 1 and the outer mold 2 are already in contact with each other before the compression processing, the compression processing is performed with a part of the inner peripheral surface of the billet 1, that is, a portion in contact with the convex portion of the punch 3 being restrained. Is applied.
このように、圧縮加工ではポンチ3の表面に凹凸が設け
てあることによって、ビレット1には内周面に凹凸が形
成される。ビレットの圧縮加工過程において、最初に内
周面が拘束された部分、すなわち加工後のビレットの内
周面の凹部は周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、つまり加工後のビレットの内
周面の凹部は径方向に磁化容易方向を有する部分とな
る。その中間の部分の磁化容易方向は周方向から径方向
へ次第に変化していく部分である。言い換えると、第1
図においてポンチ3の凸部によって形成されるビレット
1の内周面の凹部の曲面に沿った方向に磁化容易方向
が、ビレット1の内周面から連続的に変化する。As described above, in the compression process, since the surface of the punch 3 is provided with unevenness, the billet 1 is provided with unevenness on the inner peripheral surface thereof. In the billet compression process, the part where the inner peripheral surface was constrained first, that is, the recessed part of the inner peripheral surface of the billet after processing became the part having the easy magnetization direction in the circumferential direction, and finally the inner peripheral surface was restricted. The part or the part where the inner peripheral surface is not constrained to the end, that is, the concave part of the inner peripheral surface of the billet after processing is a part having the easy magnetization direction in the radial direction. The easy magnetization direction of the intermediate portion is a portion that gradually changes from the circumferential direction to the radial direction. In other words, the first
In the drawing, the easy magnetization direction continuously changes from the inner peripheral surface of the billet 1 in a direction along the curved surface of the concave portion of the inner peripheral surface of the billet 1 formed by the convex portion of the punch 3.
そのため内周着磁においては何極着磁するかによって、
凹凸部の数を決定すればよい。第1図では加工後のビレ
ット1の内周面の凸部が6つあるため、6極着磁に適し
た異方性構造を有する磁石となり、加工後の凸部に当る
部分が、内周着磁における極の部分になる。Therefore, depending on how many poles are magnetized in the inner circumference magnetization,
The number of uneven portions may be determined. In Fig. 1, since there are 6 convex portions on the inner peripheral surface of the billet 1 after processing, the magnet has an anisotropic structure suitable for 6-pole magnetization, and the portion corresponding to the convex portion after processing is the inner peripheral surface. It becomes the pole part in magnetization.
ビレットがそ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、前述したように圧縮
ひずみは対数ひずみの絶対値で0.05以上必要である。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せておきたい場合は、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ってもよい。Polycrystalline Mn whose billet has an easy magnetization direction in its axial direction
In the case of the -Al-C alloy magnet, the compressive strain must be 0.05 or more in absolute value of logarithmic strain as described above. However, in actual application, if you want to preserve the easy magnetization direction 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. Areas may be created.
以上述べたように本発明は、ビレットをその軸方向に圧
縮加工する際に、外面に凹凸のある金型等を用いてビレ
ツトの内周面を凹凸上に形成圧縮することによって、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 above, according to the present invention, when the billet is compressed in the axial direction, the inner peripheral surface of the billet is formed and compressed by using a mold having an outer surface having irregularities to form an inner peripheral surface. It is intended to obtain a magnet having an anisotropic structure that exhibits high magnetic properties when magnetized.
なお、圧縮加工の可能な温度範囲については、530ない
し830℃の温度領域において加工が行なえたが、780℃を
超える温度領域では、磁気特性がかなり低下し、より好
ましい温度範囲としては560ないし760℃であった。Regarding the temperature range in which compression processing is possible, processing could be performed in the temperature range of 530 to 830 ° C, but in the temperature range of higher than 780 ° C, the magnetic properties are considerably deteriorated, and a more preferable temperature range is 560 to 760. It was ℃.
次に本発明を数値例により更に具体的に説明する。Next, the present invention will be described more specifically with reference to numerical examples.
具体例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および0.7%のNiを溶解鋳造し、直径
70mm、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
理を行ない、次に潤滑剤を介して720℃の温度で直径45m
mまでの押出加工を行なった。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なって得た押出
棒を長さ20mmに切断し、切削して、外径30mm、内径24m
m、長さ20mmの円筒ビレットを作製した。このビレット
を第2図および第3図に示した金型を用いて高さ12mmま
で圧縮加工を行なった。なお、第2図は第1図と同様の
金型の断面図である。図においてDK外径2の内径=30m
m、XA=8mm、ポンチ3の凸部の曲率半径RS=2.5mm、ポ
ンチ3の径DP=16mmでポンチ3の凸部は8個である。ま
た第3図は第2図の中心、断面図を示し、3および4が
ポンチで、それらは凹凸部が嵌合する表面を有し、図の
上下方向に移動することができる。Specific Example 1 69.5% by mass of compounded composition (hereinafter simply referred to as%) of Mn, 29.3
% Al, 0.5% C and 0.7% Ni by melt casting, diameter
A cylindrical billet having a length of 70 mm and a length of 50 mm was produced. After holding this billet at 1100 ° C for 2 hours, it was left to cool to room temperature and then heat-treated at a temperature of 720 ° C through a lubricant to a diameter of 45 m.
Extrusion processing up to m was performed. 680 through the lubricant
Extruded rods up to 31 mm in diameter at a temperature of ℃ were cut into 20 mm long extruded rods and cut to an outer diameter of 30 mm and an inner diameter of 24 m.
A cylindrical billet having a length of m and a length of 20 mm was produced. This billet was compressed to a height of 12 mm using the mold shown in FIGS. 2 and 3. Note that FIG. 2 is a sectional view of a mold similar to FIG. In the figure, D K outer diameter 2 inner diameter = 30 m
m, X A = 8 mm, the radius of curvature of the convex portion of the punch 3 R S = 2.5 mm, the diameter of the punch 3 D P = 16 mm, and the punch 3 has 8 convex portions. Further, FIG. 3 shows the center and cross-sectional view of FIG. 2, and 3 and 4 are punches, which have a surface to which the uneven portion fits, and can move in the vertical direction of the figure.
上記高さ12mmに圧縮加工後のビレットを内径20mmまで、
切削加工し、8曲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、長さ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て高さ12mmの面異方性
磁石を作り、前記具体例と同様に切削加工し、着磁し、
表面束密度を測定した。The billet after compression processing to the above height of 12 mm up to an inner diameter of 20 mm,
It was machined and magnetized with 8 tracks. Magnetization is 2000μF
It was pulse-magnetized at 1500 V using the oil condenser of No. 1. The surface magnetic flux density of the inner peripheral surface was measured with a Hall element. For comparison, a cylindrical billet with a diameter of 18 mm and a length of 20 mm is freely compressed in the direction of the cylinder axis at a temperature of 680 ° C. to make a surface anisotropic magnet with a height of 12 mm, and cut in the same manner as the above specific example. , Magnetized,
The surface bundle density was measured.
上記両測定値を比較すると、本発明の方法で得た磁石の
表面磁束密度の値は、比較例の面異方性磁石のそれの約
1.6倍であった。Comparing the above measured values, the value of the surface magnetic flux density of the magnet obtained by the method of the present invention is about that of the surface anisotropic magnet of the comparative example.
It was 1.6 times.
具体例2 具体例1で得た直径31mmの押出棒をさらに潤滑剤を介し
て680℃の温度で押出加工を行ない直径22mmの押出棒を
つくり、これを長さ40mmに切断したビレットを680℃の
温度で円柱の軸方向に高さが20mmになるまで自由圧縮加
工を行なった。加工後のビレットは面異方性磁石であ
る。このビレットを切削加工して、外径30mm、内径24m
m、高さ24mmの円筒ビレットを作製した。このビレット
を用いて、具体例1と同様の圧縮加工を行ない、加工後
のビレットを内径20mmまで切削加工した。さらに、具体
例1と同様の内周着磁を行ない、表面磁束密度を測定し
たところ、その値は、具体例1で得た本発明の方法によ
って得た磁石のそれと大差はなかった。Example 2 The extruded rod having a diameter of 31 mm obtained in Example 1 was further extruded through a lubricant at a temperature of 680 ° C. to form an extruded rod having a diameter of 22 mm. The extruded rod was cut into a length of 40 mm to form a billet at 680 ° C. Free compression processing was performed at a temperature of up to 20 mm in the axial direction of the cylinder. The billet after processing is a plane anisotropic magnet. By cutting this billet, the outer diameter is 30 mm and the inner diameter is 24 m.
A cylindrical billet having a height of m and a height of 24 mm was produced. Using this billet, the same compression processing as in Example 1 was performed, and the billet after processing was cut to an inner diameter of 20 mm. Further, when the surface magnetic flux density was measured by performing inner circumferential magnetization similar to that in Example 1, the value was not much different from that of the magnet obtained by the method of the present invention obtained in Example 1.
具体例1および2で得た本発明の方法による磁石は、磁
気トルク測定の結果、前述したように磁化容易方向は内
周面の凹部を表面に沿って径方向から周方向に連続的に
次第に変化していることが確認された。As a result of the magnetic torque measurement, the magnets obtained by the methods of the present invention obtained in Examples 1 and 2 showed that the direction of easy magnetization was such that the concave portion of the inner peripheral surface was continuously and gradually increased from the radial direction to the circumferential direction along the surface. It was confirmed that it was changing.
(発明の効果) 以上詳細に説明して明らかなように、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
体状のビレットをその軸方向に圧縮加工することによっ
てビレットの内周面を凹凸状に形成することにより、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 is clear from the above description, the present invention compresses a hollow billet made of a pre-anisotropic polycrystalline Mn-Al-C alloy magnet in its axial direction. By forming the inner peripheral surface of the billet in a concavo-convex shape by doing so, a magnet exhibiting high magnetic characteristics when the inner peripheral is magnetized is obtained.
従来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る磁石は内周着磁を施した場合、
従来の方法による磁石より優れた磁気特性を示し、さら
に磁石の内周面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に磁化容易方向を有する磁石を得る
には、従来方法では少なくとも2回以上の塑性加工を必
要としたが、本発明では1回ですみ、かつ、従来よりも
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 conventional method, the magnet obtained by the method of the present invention, when subjected to inner circumference magnetization,
In order to obtain a magnet exhibiting superior magnetic characteristics to the magnet by the conventional method, the inner peripheral surface of the magnet further has the easy magnetization direction in the radial direction, and the outer peripheral portion having the easy magnetization direction in the circumferential direction, Although the conventional method requires plastic working at least twice or more, the present invention requires only once, and a magnet having a more desirable anisotropic structure than the conventional method can be obtained.
第1図は本発明の一実施例の圧縮加工に用いる金型の断
面図、第2図ないし第3図は本発明に用いる金型例の断
面図、第4図は円筒状磁石の内周面に多極着磁した場合
の磁路を摸式的に示す図である。 1…ビレット、2…外型、3,4…ポンチ。FIG. 1 is a sectional view of a mold used for compression processing of an embodiment of the present invention, FIGS. 2 to 3 are sectional views of an example of a mold used in the present invention, and FIG. 4 is an inner circumference of a cylindrical magnet. It is a figure which shows schematically the magnetic path at the time of carrying out multi-pole magnetization to the surface. 1 ... Billet, 2 ... Outer mold, 3, 4 ... Punch.
Claims (5)
アルミニウム-炭素系合金磁石からなる中空体状のビレ
ットを、その軸方向に530ないし830℃の温度で圧縮加工
することによって上記ビレットの内周面を凹凸状に形成
することを特徴とする合金磁石の製造法。1. Pre-anisotropic polycrystalline manganese-
A hollow body-shaped billet made of an aluminum-carbon alloy magnet is compressed at a temperature of 530 to 830 ° C. in the axial direction to form an inner peripheral surface of the billet in an uneven shape. Manufacturing method.
向を有し、かつ、圧縮加工によ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)項記載の合金磁石の製造法。2. The billet according to claim 1, wherein the billet has an easy magnetization direction in the axial direction of the hollow body, and the compression strain due to compression processing is 0.05 or more in absolute value of logarithmic strain. The method for producing an alloy magnet according to the item 1).
に平行に磁化容易方向を有し、しかも上記平面内では磁
気的に等方性であり、かつ上記軸方向及び平面に平行な
直線を含む平面内では異方性であることを特徴とする特
許請求の範囲第(1)項記載の合金磁石の製造法。3. The billet has an easy magnetization direction parallel to a plane perpendicular to the axial direction of the hollow body, is magnetically isotropic in the plane, and is parallel to the axial direction and the plane. The method for producing an alloy magnet according to claim (1), which is anisotropic in a plane including a straight line.
束した状態で行なうことを特徴とする特許請求の範囲第
(1)項記載の合金磁石の製造法。4. The method according to claim 1, wherein the compression processing is performed with a part of the inner peripheral surface of the billet being constrained.
The method for producing an alloy magnet according to the item (1).
態で行なうことを特徴とする特許請求の範囲第(1)項記
載の合金磁石の製造法。5. The method for producing an alloy magnet according to claim 1, wherein the compression processing is performed with the outer peripheral surface of the billet being constrained.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP60025268A JPH061742B2 (en) | 1985-02-14 | 1985-02-14 | Alloy magnet manufacturing method |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP60025268A JPH061742B2 (en) | 1985-02-14 | 1985-02-14 | Alloy magnet manufacturing method |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS61187215A JPS61187215A (en) | 1986-08-20 |
| JPH061742B2 true JPH061742B2 (en) | 1994-01-05 |
Family
ID=12161279
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP60025268A Expired - Lifetime JPH061742B2 (en) | 1985-02-14 | 1985-02-14 | Alloy magnet manufacturing method |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH061742B2 (en) |
-
1985
- 1985-02-14 JP JP60025268A patent/JPH061742B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS61187215A (en) | 1986-08-20 |
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