JP2008169451A - Component made of electrical sheet having excellent magnetic property, bar wire rod for component made of electrical sheet, and method for producing the same - Google Patents

Component made of electrical sheet having excellent magnetic property, bar wire rod for component made of electrical sheet, and method for producing the same Download PDF

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JP2008169451A
JP2008169451A JP2007005690A JP2007005690A JP2008169451A JP 2008169451 A JP2008169451 A JP 2008169451A JP 2007005690 A JP2007005690 A JP 2007005690A JP 2007005690 A JP2007005690 A JP 2007005690A JP 2008169451 A JP2008169451 A JP 2008169451A
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soft iron
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JP4772703B2 (en
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Manabu Kubota
学 久保田
Toshizo Tarui
敏三 樽井
Takeshi Kubota
猛 久保田
Masao Yabumoto
政男 籔本
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Nippon Steel Corp
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Abstract

<P>PROBLEM TO BE SOLVED: To provide a component made of an electrical sheet such as a solenoid, to provide a steel member for a component made of an electrical sheet having excellent magnetic properties and used as the stock for the electrical sheet component, particularly, to provide a bar wire rod for a component made of an electrical sheet, and to provide a method for producing the same. <P>SOLUTION: The electrical sheet component having excellent magnetic properties has a composition comprising, by mass, >0.20 to 0.50% Mn, further comprising either or both of 0.05 to 1.00% Ni and 0.05 to 1.00% Co, and in which the content of C is limited to ≤0.02%, Si to ≤0.10%, P to ≤0.010% (inclusive of 0%), S to ≤0.010% (inclusive of 0%), Total Al to ≤0.010% (inclusive of 0%), Sol.Al to ≤0.005% (inclusive of 0%), Ti to ≤0.005%, N to ≤0.0050% and O to 0.0200%, and the balance Fe with inevitable impurities, and has the ferrite grain size number of ≤5. <P>COPYRIGHT: (C)2008,JPO&INPIT

Description

本発明はソレノイド等の電磁軟鉄製部品、電磁軟鉄部品の素材である電磁軟鉄製部品用鋼材及びその製造方法に関するものである。   The present invention relates to an electromagnetic soft iron part such as a solenoid, a steel material for an electromagnetic soft iron part which is a material of the electromagnetic soft iron part, and a method for manufacturing the same.

電磁軟鉄製部品用鋼材、特に、電磁軟鉄製部品用棒線材は、軟磁性材料として、例えば、自動車、産業機器類の電装部品、オートマチックトランスミッション、電磁クラッチ等に使用される、ソレノイド等の直流電気機器、即ち電磁軟鉄製部品の材料として主に利用されている。近年、自動車に使用される電子制御部品は増加しており、電磁軟鉄製部品の高性能化、小型化が求められている。そのため、電磁軟鉄製部品用棒線材の磁気特性に対しても更なる高性能化が求められている。この軟磁性材料に要求される磁気特性とは、外部磁界に対して発生する磁束密度が大きいこと(高磁束密度)、消費電力低減のためヒステリシス損が小さいこと(低保磁力)である。即ち、磁界の強さに伴う磁束密度の変化曲線(いわゆるヒステリシス曲線)において、保磁力(Hc)が小さく、飽和磁束密度(Bm)が大きい材料が要求されている。   Steel materials for electromagnetic soft iron parts, especially rod wires for electromagnetic soft iron parts, are used as soft magnetic materials, for example, electric parts for automobiles, industrial equipment, automatic transmissions, electromagnetic clutches, etc. It is mainly used as a material for equipment, that is, electromagnetic soft iron parts. In recent years, electronic control parts used in automobiles are increasing, and high performance and downsizing of electromagnetic soft iron parts are required. Therefore, higher performance is also required for the magnetic properties of the bar wire for electromagnetic soft iron parts. The magnetic properties required for this soft magnetic material are a high magnetic flux density generated with respect to an external magnetic field (high magnetic flux density) and a small hysteresis loss (low coercive force) to reduce power consumption. That is, a material having a small coercive force (Hc) and a large saturation magnetic flux density (Bm) is required in a change curve (so-called hysteresis curve) of the magnetic flux density accompanying the strength of the magnetic field.

このような要求に応える電磁部品用の材料として、純鉄系の軟磁性材料が提案されている。一般に純鉄系軟磁性材料の磁気特性を向上のためには、次のような方策が取られている。即ち、(1)高磁束密度を得るために鉄中のC量、及び合金元素量を極力低減して高純度化すること、(2)低保磁力を得るためにフェライト結晶粒を大きくし、(3)格子欠陥密度や晶析出物量を低減して磁区移動を容易化すること、である。   Pure iron-based soft magnetic materials have been proposed as materials for electromagnetic parts that meet such requirements. In general, the following measures are taken to improve the magnetic properties of pure iron-based soft magnetic materials. (1) To obtain a high magnetic flux density, the amount of C in iron and the amount of alloying elements are reduced as much as possible, and (2) the ferrite crystal grains are enlarged to obtain a low coercive force. (3) To reduce the lattice defect density and the amount of crystal precipitates to facilitate magnetic domain movement.

例えば、C量を大幅に低減してフェライト単相組織とし、Al、Nを低減して結晶粒の不均一さを抑制した軟磁性鋼が提案されている(例えば、特許文献1、非特許文献1)。特許文献1及び非特許文献1に提案されている電磁部品、軟磁性材料は、Mnの添加によってSを無害化し、冷間加工後の焼鈍によってフェライト結晶粒を成長させ、保磁力を小さくしたものである。非特許文献1には、フェライト結晶粒度を4番以下と粗大にすると、保磁力が急激に減少し、また良好な磁束密度特性が得られることが示されている。   For example, soft magnetic steel has been proposed in which the amount of C is significantly reduced to form a ferrite single phase structure, and Al and N are reduced to suppress crystal grain non-uniformity (for example, Patent Document 1, Non-Patent Document). 1). The electromagnetic parts and soft magnetic materials proposed in Patent Document 1 and Non-Patent Document 1 are made by detoxifying S by adding Mn and growing ferrite crystal grains by annealing after cold working to reduce the coercive force. It is. Non-Patent Document 1 shows that when the ferrite crystal grain size is as coarse as 4 or less, the coercive force is drastically reduced and good magnetic flux density characteristics can be obtained.

しかしながら、従来レベル以上に磁気特性を向上するためにはC、Al、N量を従来レベルよりも大幅に、極限まで低減する必要がある。そのため、大量生産を前提とする現行の製鋼工場の精錬能力では、上記成分の極限までの低減は極めて難しく、また製造できたとしても製造コストが非常に高くなるという問題があった。   However, in order to improve the magnetic characteristics beyond the conventional level, it is necessary to significantly reduce the amounts of C, Al, and N to the limit as compared with the conventional level. For this reason, with the refining ability of the current steelmaking factory premised on mass production, there has been a problem that it is extremely difficult to reduce the above components to the limit, and even if it can be produced, the production cost becomes very high.

また、磁気特性を向上させるため、脱水素処理及びNiの添加により、厚鋼板が提案されている(例えば、特許文献2)。なお、特許文献2には、AlNによる結晶粒微細化作用が磁気特性に有害であることも開示されている。しかし、特許文献2に提案されている厚鋼板は、Alを脱酸剤として使用するものであり、棒線材の製造方法については記載されていない。   In order to improve magnetic properties, a thick steel plate has been proposed by dehydrogenation treatment and addition of Ni (for example, Patent Document 2). Patent Document 2 also discloses that the effect of crystal grain refining by AlN is harmful to magnetic properties. However, the thick steel plate proposed in Patent Document 2 uses Al as a deoxidizing agent, and does not describe a method for manufacturing a bar wire.

特開2003−226946号公報JP 2003-226946 A 特開平4−268022号公報JP-A-4-268822 千葉政道、鹿礒正人、「純鉄系軟磁性材料」、神戸製鋼技報、第52巻、第3号、2002年12月1日、株式会社神戸製鋼所発行、p.66−69Masamichi Chiba, Masato Shikabe, “Pure Iron-Based Soft Magnetic Materials”, Kobe Steel Technical Report, Vol. 52, No. 3, December 1, 2002, issued by Kobe Steel, p. 66-69

本発明は以上のような課題点に鑑み、ソレノイド等の電磁軟鉄製部品、その電磁軟鉄部品の素材として使用される、磁気特性に優れた電磁軟鉄製部品用鋼材、特に電磁軟鉄製部品用棒線材及びその製造方法の提供を目的とするものである。   In view of the above-described problems, the present invention is an electromagnetic soft iron component such as a solenoid, a steel material for an electromagnetic soft iron component excellent in magnetic properties, particularly a rod for an electromagnetic soft iron component, used as a material for the electromagnetic soft iron component. The object is to provide a wire rod and a manufacturing method thereof.

本発明は、Ni、Coの一方又は双方の添加により磁気特性を向上させ、更に、熱間圧延により棒線材に生じた集合組織に起因する磁気特性の劣化を抑制した電磁軟鉄製部品、その電磁軟鉄部品の素材として使用される、磁気特性に優れた電磁軟鉄製部品用鋼材及びその製造方法であり、その要旨は、以下の通りである。   The present invention relates to an electromagnetic soft iron part that improves magnetic properties by adding one or both of Ni and Co, and further suppresses deterioration of magnetic properties caused by a texture formed in a rod and wire by hot rolling, and its electromagnetic A steel material for electromagnetic soft iron parts having excellent magnetic properties, which is used as a raw material for soft iron parts, and a method for producing the same, the summary of which is as follows.

(1) 質量%で、
Mn:0.20超〜0.50%
を含有し、さらに、
Ni:0.05〜1.00%、
Co:0.05〜1.00%
の一方又は双方を含有し、
C:0.02%以下、
Si:0.10%以下、
P:0.010%以下(0%を含む)、
S:0.010%以下(0%を含む)、
Total Al:0.010%以下(0%を含む)、
Sol.Al:0.005%以下(0%を含む)、
Ti:0.005%以下(0%を含む)、
N:0.0050%以下、
O:0.0200%
に制限し、残部がFe及び不可避的不純物からなり、フェライト粒度番号が5番以下であることを特徴とする磁気特性に優れた電磁軟鉄製部品。
(1) In mass%,
Mn: more than 0.20 to 0.50%
In addition,
Ni: 0.05-1.00%,
Co: 0.05-1.00%
One or both of
C: 0.02% or less,
Si: 0.10% or less,
P: 0.010% or less (including 0%),
S: 0.010% or less (including 0%),
Total Al: 0.010% or less (including 0%),
Sol. Al: 0.005% or less (including 0%),
Ti: 0.005% or less (including 0%),
N: 0.0050% or less,
O: 0.0200%
An electromagnetic soft iron part with excellent magnetic properties, characterized in that the balance is Fe and inevitable impurities, and the ferrite grain size number is 5 or less.

(2) 軸方向断面のフェライト粒度番号Gと軸方向に垂直な方向の断面のフェライト粒度番号Gの比G/Gが、0.80〜1.20であることを特徴とする上記(1)に記載の磁気特性に優れた電磁軟鉄製部品。 (2) the ratio of the axial cross ferrite grain size number of G L and the axial direction perpendicular to the direction of the cross ferrite grain size number G C G L / G C, characterized in that a 0.80 to 1.20 An electromagnetic soft iron part having excellent magnetic properties as described in (1) above.

(3) 上記(1)に記載の電磁軟鉄製部品の素材であって、質量%で、
Mn:0.20超〜0.50%
を含有し、さらに、
Ni:0.05〜1.00%、
Co:0.05〜1.00%
の一方又は双方を含有し、
C:0.02%以下、
Si:0.10%以下、
P:0.010%以下(0%を含む)、
S:0.010%以下(0%を含む)、
Total Al:0.010%以下(0%を含む)、
Sol.Al:0.005%以下(0%を含む)、
Ti:0.005%以下(0%を含む)、
N:0.0050%以下、
O:0.0200%
に制限し、残部がFe及び不可避的不純物からなることを特徴とする磁気特性に優れた電磁軟鉄製部品用棒線材。
(3) The material of the electromagnetic soft iron part described in (1) above, in mass%,
Mn: more than 0.20 to 0.50%
In addition,
Ni: 0.05-1.00%,
Co: 0.05-1.00%
One or both of
C: 0.02% or less,
Si: 0.10% or less,
P: 0.010% or less (including 0%),
S: 0.010% or less (including 0%),
Total Al: 0.010% or less (including 0%),
Sol. Al: 0.005% or less (including 0%),
Ti: 0.005% or less (including 0%),
N: 0.0050% or less,
O: 0.0200%
The wire rod for electromagnetic soft iron parts excellent in magnetic properties, characterized in that the balance is made of Fe and inevitable impurities.

(4) 上記(2)に記載の電磁軟鉄製部品の素材であって、圧延方向断面のフェライト粒度番号Gと圧延方向に垂直な方向の断面のフェライト粒度番号Gの比G/Gが、0.80〜1.20であることを特徴とする上記(3)に記載の磁気特性に優れた電磁軟鉄製部品用用棒線材。 (4) above a material of an electromagnetic soft iron component according to (2), the ratio G R / G of the ferrite grain size number G T of the ferrite grain size number G R to the rolling direction in the vertical direction of the cross section of the rolling direction cross-section The wire rod for electromagnetic soft iron parts having excellent magnetic properties as described in (3) above, wherein T is 0.80 to 1.20.

(5) 上記(3)に記載の電磁軟鉄製部品用棒線材の製造方法であって、質量%で、
Mn:0.20超〜0.50%
を含有し、さらに、
Ni:0.05〜1.00%、
Co:0.05〜1.00%
の一方又は双方を含有し、
C:0.02%以下、
Si:0.10%以下、
P:0.010%以下(0%を含む)、
S:0.010%以下(0%を含む)、
Total Al:0.010%以下(0%を含む)、
Sol.Al:0.005%以下(0%を含む)、
Ti:0.005%以下(0%を含む)、
N:0.0050%以下、
O:0.0200%
に制限し、残部がFe及び不可避的不純物からなる圧延素材を熱間圧延することを特徴とする磁気特性に優れた電磁軟鉄製部品用棒線材の製造方法。
(5) A method for producing a bar wire for electromagnetic soft iron parts as described in (3) above, in mass%,
Mn: more than 0.20 to 0.50%
In addition,
Ni: 0.05-1.00%,
Co: 0.05-1.00%
One or both of
C: 0.02% or less,
Si: 0.10% or less,
P: 0.010% or less (including 0%),
S: 0.010% or less (including 0%),
Total Al: 0.010% or less (including 0%),
Sol. Al: 0.005% or less (including 0%),
Ti: 0.005% or less (including 0%),
N: 0.0050% or less,
O: 0.0200%
A method for producing a bar wire material for electromagnetic soft iron parts excellent in magnetic properties, characterized in that a rolled material consisting of Fe and inevitable impurities is hot-rolled.

(6) 圧延素材を1000℃〜1250℃に加熱し、仕上げ温度を800℃以上として熱間圧延することを特徴とする上記(5)に記載の磁気特性に優れた電磁軟鉄製部品用棒線材の製造方法。   (6) The bar wire for electromagnetic soft iron parts having excellent magnetic properties as described in (5) above, wherein the rolled material is heated to 1000 ° C. to 1250 ° C. and hot rolled at a finishing temperature of 800 ° C. or higher. Manufacturing method.

(7) 上記(4)に記載の電磁軟鉄製部品用棒線材の製造方法であって、熱間圧延後、880〜1250℃の温度範囲に加熱し、60〜3600s保持し、冷却する熱処理を施すことを特徴とする上記(5)又は(6)に記載の磁気特性に優れた電磁軟鉄製部品用棒線材の製造方法。   (7) A method for manufacturing a bar wire for electromagnetic soft iron parts as described in (4) above, wherein after the hot rolling, heat treatment is performed by heating to a temperature range of 880 to 1250 ° C., holding for 60 to 3600 s, and cooling. The manufacturing method of the bar wire for electromagnetic soft iron parts excellent in the magnetic characteristics as described in said (5) or (6) characterized by performing.

(8) 加熱、保持後の冷却速度が0.1〜5℃/sであることを特徴とする上記(7)に記載の磁気特性に優れた電磁軟鉄製部品用棒線材の製造方法。   (8) The method for producing a bar wire for electromagnetic soft iron parts having excellent magnetic properties according to (7) above, wherein the cooling rate after heating and holding is 0.1 to 5 ° C./s.

本発明の磁気特性に優れた電磁軟鉄製部品用棒線材及びその製造方法によれば、ソレノイド等、電磁軟鉄製部品の直流磁気特性が改善され、これにより、自動車、産業機器類の電装部品、オートマチックトランスミッション、電磁クラッチなどの高性能化、小型化が可能になるなど、産業上の貢献が極めて顕著である。   According to the rod and wire material for electromagnetic soft iron parts excellent in magnetic characteristics of the present invention and the manufacturing method thereof, the direct current magnetic characteristics of electromagnetic soft iron parts such as solenoids are improved. Industrial contributions such as automatic transmissions and electromagnetic clutches with high performance and miniaturization are very significant.

本発明者らは、電磁軟鉄製部品及び電磁軟鉄製部品用棒線材の磁気特性に及ぼす各種因子について鋭意検討し、以下の知見を見出した。即ち、
(1)保磁力を小さくするためには磁区移動を容易化する必要があり、そのためには磁区移動の障害となる結晶粒界、介在物、晶析出物を低減する必要があり、特に、析出物、介在物等を極力低減することが有効である。
(2)結晶粒をピン止めする粒子(各種合金炭窒化物、硫化物、酸化物等)を形成する元素(Al、Ti、N、S、O)の中で、特にフェライト結晶粒を微細化する効果が大きいAlNを形成するAl量(特に、Sol.Al量)を規制しなくてはならない。
(3)Mn量を極端に低減すると圧延加熱中にMnSの一部がマトリックスに固溶し、その後の冷却過程や熱処理時に再析出することによってMnSが微細化するため、ある範囲での添加が必要である。
(4)Ni、Coは、鉄の飽和磁束密度を上昇させ、鉄中で炭窒化物、硫化物を生成しないため、保磁力にも悪影響を及ぼさないので、磁気特性向上に極めて有効な手段である。
(5)特に、棒鋼、線材形状に熱間圧延を行った場合、圧延による結晶方位の異方性(集合組織)が最終製品まで受け継がれ、磁気特性に悪影響を与える。即ち、棒鋼、線材を熱間圧延によって製造する際には、圧延方向(R方向)断面で観察されるフェライト結晶粒径よりも、圧延方向に対して垂直方向(T方向)断面で観察される結晶粒径の方が小さくなる傾向がある。これにより、棒線材を冷間鍛造、切削し、最終焼鈍を施して製造される最終製品である電磁軟鉄製部品に、集合組織に起因する磁気特性の異方性を生じる。これを防止するためには、電磁軟鉄製部品の軸方向(L方向)と軸方向に垂直な方向(C方向)のフェライト粒度の比を1に近づけることが好ましい。そのためには、熱間圧延後の棒線材に、組織がオーステナイト単相になる温度範囲に加熱する熱処理を行い、結晶方位の異方性を軽減することが有効である。
The present inventors diligently studied various factors affecting the magnetic characteristics of electromagnetic soft iron parts and bar wires for electromagnetic soft iron parts, and found the following findings. That is,
(1) In order to reduce the coercive force, it is necessary to facilitate the movement of magnetic domains. For this purpose, it is necessary to reduce the grain boundaries, inclusions, and crystal precipitates that hinder magnetic domain movement. It is effective to reduce objects and inclusions as much as possible.
(2) Among the elements (Al, Ti, N, S, O) that form particles (various alloy carbonitrides, sulfides, oxides, etc.) that pin the crystal grains, especially ferrite grains are refined It is necessary to regulate the amount of Al (particularly the amount of Sol.Al) that forms AlN, which has a large effect.
(3) When the amount of Mn is extremely reduced, part of MnS is dissolved in the matrix during rolling and heating, and MnS is refined by reprecipitation during the subsequent cooling process or heat treatment. is necessary.
(4) Ni and Co increase the saturation magnetic flux density of iron and do not generate carbonitrides and sulfides in iron, so they do not adversely affect the coercive force, so they are extremely effective means for improving magnetic properties. is there.
(5) In particular, when hot rolling is performed on the shape of a steel bar or wire rod, the anisotropy (texture) of the crystal orientation due to rolling is inherited to the final product, which adversely affects the magnetic properties. That is, when manufacturing steel bars and wire rods by hot rolling, the ferrite crystal grain size observed in the rolling direction (R direction) section is observed in the section perpendicular to the rolling direction (T direction). The crystal grain size tends to be smaller. As a result, anisotropy of magnetic properties due to the texture is generated in the electromagnetic soft iron part, which is the final product manufactured by cold forging, cutting, and final annealing of the bar wire. In order to prevent this, it is preferable that the ratio of the ferrite grain size in the axial direction (L direction) and the direction perpendicular to the axial direction (C direction) of the electromagnetic soft iron part is close to 1. For this purpose, it is effective to reduce the crystal orientation anisotropy by subjecting the rod-and-wire material after hot rolling to a temperature range in which the structure becomes an austenite single phase.

以下、本発明について詳細に説明する。まず、本発明の電磁軟鉄製部品及び電磁軟鉄製部品用棒線材の成分について説明する。   Hereinafter, the present invention will be described in detail. First, the components of the electromagnetic soft iron part and the bar wire for the electromagnetic soft iron part of the present invention will be described.

Mn:Mnは鉄の飽和磁束密度を低下させるため、0.50%以下とすることが必要である。一方、Mnは鋼中のSと結合してMnSを形成することにより、結晶粒の成長をピン止めし、結晶粒を微細化する効果を有する。このため、Mn添加量を0.20%以下に低減すると、圧延加熱中にMnSの一部がマトリックスに固溶し、その後の冷却過程や熱処理時にMnSが微細に再析出し、結晶粒がより微細になり、保持力が大きくなる。したがって、電磁軟鉄製部品及びその素材の飽和磁束密度の低下を抑制し、MnSの微細析出による結晶粒の微細化を防止するためには、0.20超〜0.50%の範囲にする必要がある。なお、Mnの添加により、素材の硬さが上昇して冷間加工性も低下するので、Mnを0.30%以下に低減することが好ましい。   Mn: Mn needs to be 0.50% or less in order to reduce the saturation magnetic flux density of iron. On the other hand, Mn combines with S in steel to form MnS, thereby pinning the growth of crystal grains and having the effect of refining the crystal grains. For this reason, when the amount of Mn added is reduced to 0.20% or less, a part of MnS is dissolved in the matrix during rolling and heating, and MnS is finely re-precipitated during the subsequent cooling process or heat treatment, so that the crystal grains are more It becomes fine and the holding power increases. Therefore, in order to suppress the decrease of the saturation magnetic flux density of the electromagnetic soft iron part and its material and prevent the refinement of crystal grains due to the fine precipitation of MnS, it is necessary to be in the range of more than 0.20 to 0.50%. There is. In addition, since the hardness of a raw material raises and cold workability also falls by addition of Mn, it is preferable to reduce Mn to 0.30% or less.

Ni及びCo:Ni及びCoは飽和磁束密度を上昇させる元素であり、また鋼中で炭窒化物、硫化物を生成しないため、保磁力にも悪影響を及ぼさない。したがって、電磁軟鉄製部品及びその素材の磁気特性向上に極めて有効な元素である。一方、過度の添加は効果が飽和するのみならず磁気特性を却って低下させる場合もあることから、0.05〜1.00%の範囲にする必要がある。好適範囲は0.05〜0.30%である。本発明において、Ni及びCoは極めて重要な元素であり、それぞれ、0.05〜1.00%の範囲で、一方又は双方を添加することが必要である。   Ni and Co: Ni and Co are elements that increase the saturation magnetic flux density, and do not produce carbonitrides and sulfides in the steel, and thus do not adversely affect the coercive force. Therefore, it is an element that is extremely effective in improving the magnetic properties of electromagnetic soft iron parts and their materials. On the other hand, since excessive addition may not only saturate the effect but also decrease the magnetic properties, it must be in the range of 0.05 to 1.00%. A preferable range is 0.05 to 0.30%. In the present invention, Ni and Co are extremely important elements, and it is necessary to add one or both in the range of 0.05 to 1.00%.

C:Cは鋼中でセメンタイトを形成し、これにより飽和磁束密度が低下し、保磁力も増加する。そのため、C量を0.02%以下に低減することが必要である。また、Cの含有により素材の硬さが上昇し、冷間加工性が低下するため、極力低減することが好ましいが、Cを低減させるためには精錬上のコストがかかる。好適な上限は0.01%以下である。   C: C forms cementite in the steel, thereby decreasing the saturation magnetic flux density and increasing the coercive force. Therefore, it is necessary to reduce the C content to 0.02% or less. Moreover, since the hardness of a raw material raises by containing C and cold workability falls, it is preferable to reduce as much as possible, However, In order to reduce C, the cost on refining starts. A suitable upper limit is 0.01% or less.

Si:Siは飽和磁束密度を低下させ、また素材硬さの上昇を通じて冷間加工性も低下するため、0.10%以下に低減することが必要である。また直流での使用を前提とした電磁軟鉄製部品の場合、渦電流損の低減を考慮する必要はないので、好適範囲は0.05%以下である。   Si: Si lowers the saturation magnetic flux density, and the cold workability decreases as the material hardness increases, so it is necessary to reduce it to 0.10% or less. In addition, in the case of electromagnetic soft iron parts that are assumed to be used in direct current, it is not necessary to consider the reduction of eddy current loss, so the preferred range is 0.05% or less.

P:Pは冷間加工性を低下させる元素であり、0.010%以下(0%を含む)に低減することが必要である。なお、好適範囲は0.008%以下である。   P: P is an element that decreases the cold workability, and needs to be reduced to 0.010% or less (including 0%). The preferred range is 0.008% or less.

S:Sは不可避的に含有され、鋼中のMnと結合してMnSを形成し、結晶粒の成長をピン止めして、結晶粒を微細化する効果を有する元素であり、0.010%以下(0%をとする必要がある。そのため、Sが存在すると、Mnの添加量を0.010%以下に低減する必要がある。保磁力を小さくするためには、Mn量を0.008%以下とすることが好ましい。   S: S is inevitably contained, and is an element having an effect of refining crystal grains by combining Mn in steel to form MnS, pinning the growth of crystal grains, and 0.010% (It is necessary to make it 0%. Therefore, when S is present, it is necessary to reduce the amount of Mn added to 0.010% or less. In order to reduce the coercive force, the amount of Mn is set to 0.008. % Or less is preferable.

Total Al:Alは、磁区移動の障壁となるAl等の介在物を形成するため、Alを過剰に含有すると保磁力が大きくなり、更に冷間加工時に介在物が破壊の起点となり、冷間加工性が低下する。したがって、Total Al量を0.010%以下(0%を含む)に低減する必要がある。また、鋼中に固溶したAlは、鋼中のNと結合してAlNを形成し、結晶粒の成長をピン止めする。AlNは結晶粒を微細化する大きな効果を有するため、保磁力が大きくなり、磁気特性が低下する。そのため、Total Al量を0.005%以下とすることが好ましい。なお、Total Alは、鋼中に含まれるAlの総量であり、鋼中の固溶量と、酸化物等の介在物として存在する量の合計である。 Total Al: Al forms inclusions such as Al 2 O 3 that acts as a barrier for magnetic domain movement. Therefore, if Al is contained excessively, the coercive force increases, and the inclusions become the starting point of fracture during cold working. Cold workability decreases. Therefore, it is necessary to reduce the total Al amount to 0.010% or less (including 0%). Further, Al dissolved in the steel combines with N in the steel to form AlN and pin the growth of crystal grains. Since AlN has a great effect of refining crystal grains, the coercive force is increased and the magnetic properties are deteriorated. Therefore, it is preferable that the total Al amount is 0.005% or less. Total Al is the total amount of Al contained in the steel, and is the total of the amount of solid solution in the steel and the amount existing as inclusions such as oxides.

Sol.Al:鋼中に固溶したAlは、上述のようにAlNを生じて結晶粒を微細化し、磁気特性を大きく低下させる。特に、AlN低減の観点からはAlNを形成する可能性のあるSol.Al量を規制することが効果的であるので、Sol.Al量は0.005%以下(0%を含む)に低減する必要がある。好適範囲は0.003%以下である。なお、Sol.Alは、鋼中に酸化物等の介在物として存在するAlを除く固溶量であり、電解抽出残渣分析により測定することができる。   Sol. Al: Al dissolved in the steel generates AlN as described above, refines the crystal grains, and greatly reduces the magnetic properties. In particular, from the viewpoint of AlN reduction, Sol. Since it is effective to regulate the amount of Al, Sol. The amount of Al needs to be reduced to 0.005% or less (including 0%). The preferred range is 0.003% or less. In addition, Sol. Al is a solid solution amount excluding Al present as inclusions such as oxides in steel, and can be measured by electrolytic extraction residue analysis.

Ti:TiはTiNを形成する元素であり、過剰に添加すると粗大なTiNを生じて、冷間加工時に破壊の起点となり、冷間加工性が低下する。そのため、Ti量は0.005%以下(0%を含む)に低減する必要がある。また、Tiが、AlNと同様に微細なTiNを生じると、結晶粒が微細化し、磁気特性を低下させる。したがって、Ti量は0.003%以下とすることが好ましい。   Ti: Ti is an element that forms TiN. When excessively added, coarse TiN is generated, which becomes a starting point of fracture during cold working, and cold workability is lowered. Therefore, the amount of Ti needs to be reduced to 0.005% or less (including 0%). Further, when Ti produces fine TiN like AlN, the crystal grains become fine and the magnetic properties are deteriorated. Therefore, the Ti content is preferably 0.003% or less.

N:Nは鋼中のAl、Nと結合し、結晶粒を微細化する効果を有するAlN、TiNを形成する。これにより、保磁力が大きくなるため、N量を0.0050%以下に低減する必要がある。好適範囲は0.0030%以下である。   N: N combines with Al and N in steel to form AlN and TiN having an effect of refining crystal grains. Thereby, since the coercive force is increased, the N amount needs to be reduced to 0.0050% or less. The preferred range is 0.0030% or less.

O:Oは、鋼中でAl、Si、Ti等と酸化物を形成する元素である。これらの酸化物は、磁区移動の障壁となる介在物であり、保磁力が大きくするだけでなく、冷間加工時に介在物が破壊の起点となり、冷間加工性が低下するので0.0200%以下に低減する必要がある。好適範囲は0.0150%以下である。   O: O is an element that forms an oxide with Al, Si, Ti and the like in steel. These oxides are inclusions that serve as barriers for magnetic domain movement, and not only increase the coercive force, but also the inclusions become the starting point of breakage during cold working, resulting in a decrease in cold workability. It is necessary to reduce to the following. The preferred range is 0.0150% or less.

次に、本発明の電磁軟鉄製部品の組織について説明する。   Next, the structure of the electromagnetic soft iron part of the present invention will be described.

フェライト粒度番号:本発明においては、結晶粒径が微細化すると、磁気特性が低下するため、フェライト粒度番号を5以下とすることが必要である。フェライト粒度番号は、JIS G 0551に準拠して比較法又は切断法によって測定することができる。なお、フェライト粒度を測定する試料は測定面を任意の方向として採取すれば良い。例えば、軸方向(L方向)又は軸方向に垂直な方向(C方向)の何れかで良い。   Ferrite grain size number: In the present invention, when the crystal grain size is refined, the magnetic properties are lowered, so the ferrite grain size number needs to be 5 or less. The ferrite particle size number can be measured by a comparison method or a cutting method in accordance with JIS G 0551. In addition, what is necessary is just to extract | collect the sample which measures a ferrite particle size by making a measurement surface into arbitrary directions. For example, it may be either the axial direction (L direction) or the direction perpendicular to the axial direction (C direction).

なお、電磁軟鉄製部品が棒状である場合、その軸方向は、棒線材の長手方向、即ち圧延方向(R方向)に相当し、電磁軟鉄製部品の軸方向に直交する方向は、棒線材の圧延方向に垂直な方向(T方向)に相当する。   When the electromagnetic soft iron part is rod-shaped, its axial direction corresponds to the longitudinal direction of the bar wire, that is, the rolling direction (R direction), and the direction perpendicular to the axial direction of the electromagnetic soft iron part is This corresponds to the direction perpendicular to the rolling direction (T direction).

また、電磁軟鉄製部品が平板状である場合は、棒線材を圧延方向と平行に冷間鍛造したものであることが多いため、厚み方向を軸方向、水平方向を軸方向に垂直な方向と定義する。したがって、円盤、リング等の平板状の電磁軟鉄製部品は、厚み方向が素材である棒線材のR方向である場合と、T方向である場合が有り得る。厚み方向が素材のR方向に相当する場合は、水平方向がT方向に相当し、厚み方向が素材のT方向に相当する場合は、水平方向が素材のR方向に相当する。   In addition, when the electromagnetic soft iron part has a flat plate shape, a bar wire is often cold forged parallel to the rolling direction, so the thickness direction is the axial direction and the horizontal direction is the direction perpendicular to the axial direction. Define. Therefore, a flat electromagnetic soft iron part such as a disk or a ring may have a thickness direction that is the R direction of a bar wire that is a material or a T direction. When the thickness direction corresponds to the R direction of the material, the horizontal direction corresponds to the T direction, and when the thickness direction corresponds to the T direction of the material, the horizontal direction corresponds to the R direction of the material.

更に、電磁軟鉄製部品が底と縦壁からなるカップ状である場合も、平板状と同様、棒線材を圧延方向と平行に冷間鍛造したものであることが多いため、カップの深さ方向を軸方向、底と平行な方向を軸方向に垂直な方向と定義する。したがって、カップ状の電磁軟鉄製部品では、カップの深さ方向が素材である棒線材のR方向である場合と、T方向である場合が有る。このうち、カップの深さ方向及び底の厚み方向が素材のR方向に相当する場合は、底と平行な方向がT方向に相当し、カップの深さ方向及び底の厚み方向が素材のT方向に相当する場合は、底と平行な方向が素材のR方向に相当する。   Furthermore, even when the electromagnetic soft iron part has a cup shape composed of a bottom and a vertical wall, the bar wire is often cold forged in parallel with the rolling direction, as in the flat plate shape. Is defined as the axial direction, and the direction parallel to the bottom is defined as the direction perpendicular to the axial direction. Therefore, in a cup-shaped electromagnetic soft iron part, there are cases where the depth direction of the cup is the R direction of the bar wire material, and the T direction. Among these, when the depth direction of the cup and the thickness direction of the bottom correspond to the R direction of the material, the direction parallel to the bottom corresponds to the T direction, and the depth direction of the cup and the thickness direction of the bottom correspond to the T direction of the material. When it corresponds to the direction, the direction parallel to the bottom corresponds to the R direction of the material.

本発明では、電磁軟鉄製部品の軸方向のフェライト結晶粒度Gと軸方向に垂直な方向のフェライト結晶粒度Gの比G/Gを0.80〜1.20とすることが好ましい。これにより、線材圧延によって形成された集合組織に起因する磁気特性の異方性が軽減され、磁気特性が更に向上する。 In the present invention, the ratio G L / G C of the ferrite crystal grain size G L in the axial direction and the ferrite crystal grain size G C in the direction perpendicular to the axial direction of the electromagnetic soft iron part is preferably 0.80 to 1.20. . Thereby, the anisotropy of the magnetic property resulting from the texture formed by wire rod rolling is reduced, and the magnetic property is further improved.

次に、本発明の電磁軟鉄製部品の製造方法について説明する。   Next, a method for manufacturing the electromagnetic soft iron part of the present invention will be described.

上述の成分からなる鋼を転炉、又は電気炉で溶製し、二次精錬、連続鋳造を行う。連続鋳造を行って得られた鋳片をそのまま圧延素材としても良いが、分塊圧延を行い、圧延素材としても良い。圧延素材を1000℃〜1250℃に加熱し、熱間圧延を行い、棒鋼、又は線材とする。   The steel composed of the above components is melted in a converter or electric furnace, and secondary refining and continuous casting are performed. The slab obtained by performing continuous casting may be used as a rolling material as it is, but it may be subjected to split rolling and used as a rolling material. The rolled material is heated to 1000 ° C. to 1250 ° C. and hot-rolled to obtain a bar or wire.

熱間圧延の仕上げ温度は800℃以上とすることが好ましい。これにより、圧延材の再結晶が促進され、結晶方位の異方性を軽減でき、最終製品のフェライト結晶粒度の異方性が軽減される。圧延後の冷却は空冷、又は徐冷で良い。   The finishing temperature of hot rolling is preferably 800 ° C. or higher. Thereby, recrystallization of the rolled material is promoted, the anisotropy of the crystal orientation can be reduced, and the anisotropy of the ferrite crystal grain size of the final product is reduced. Cooling after rolling may be air cooling or slow cooling.

熱間圧延によって得られた棒線材を、鍛造などの冷間加工、切削加工の一方又は双方によって部品形状に加工する。部品形状への加工後、加工歪みを取り除き、フェライト結晶粒を再結晶、成長させて磁気特性を向上させるため、最終焼鈍を施す。最終焼鈍の加熱温度が低すぎるか、加熱時間が短すぎると、結晶粒が十分に成長しないことがある。一方、最終焼鈍の加熱温度が高すぎるか、加熱時間が長すぎると、組織の一部がオーステナイト化し、変態によって結晶粒径が微細化し、磁気特性が劣化することがある。そのため、最終焼鈍の加熱温度を800〜880℃、加熱時間を1〜10時間とすることが好ましい。最終焼鈍後の冷却は、空冷又は徐冷とするのが好適である。   A rod and wire obtained by hot rolling is processed into a part shape by one or both of cold processing such as forging and cutting. After processing to the part shape, final annealing is performed to remove the processing strain and recrystallize and grow the ferrite crystal grains to improve the magnetic properties. If the final annealing heating temperature is too low or the heating time is too short, the crystal grains may not grow sufficiently. On the other hand, if the heating temperature of the final annealing is too high or the heating time is too long, part of the structure becomes austenite, the crystal grain size becomes fine due to transformation, and the magnetic properties may deteriorate. Therefore, it is preferable that the heating temperature of the final annealing is 800 to 880 ° C. and the heating time is 1 to 10 hours. The cooling after the final annealing is preferably air cooling or slow cooling.

熱間圧延で製造した棒線材は、そのまま冷間加工しても良く、熱間圧延後に冷間加工性を向上させるための中間焼鈍を施しても良い。中間焼鈍は、集合組織の異方性の解消にも有効であり、電磁軟鉄製部品の軸方向の断面と軸方向に垂直な断面の結晶粒度の比を1に近づけるために有効である。中間焼鈍の加熱温度が低すぎるか、加熱時間が短すぎると軟化が不十分になることがある。また、中間焼鈍の加熱温度が高すぎるか、加熱時間が長すぎると、セメンタイトがマトリックス中に再溶解し、冷却中に微細析出して軟化が不十分になることがある。したがって、中間焼鈍の効果を十分に得るため、好適な加熱温度及び加熱時間があり、本発明の鋼材の場合、加熱温度を650〜720℃、加熱時間を2〜24時間とすることが好ましい。中間焼鈍後の冷却は、空冷又は徐冷とするのが好適である。なお、中間焼鈍は冷間加工率が高い場合は有効であるが、必ずしも施す必要はない。   The rod and wire manufactured by hot rolling may be cold worked as it is, or may be subjected to intermediate annealing for improving cold workability after hot rolling. Intermediate annealing is effective in eliminating texture anisotropy, and is effective in bringing the ratio of the grain size of the cross section perpendicular to the axial direction to the axial cross section of the electromagnetic soft iron part close to 1. If the heating temperature of the intermediate annealing is too low or the heating time is too short, softening may be insufficient. Moreover, when the heating temperature of intermediate annealing is too high or the heating time is too long, cementite may be re-dissolved in the matrix and finely precipitated during cooling, resulting in insufficient softening. Therefore, in order to sufficiently obtain the effect of the intermediate annealing, there are suitable heating temperature and heating time. In the case of the steel material of the present invention, it is preferable that the heating temperature is 650 to 720 ° C. and the heating time is 2 to 24 hours. The cooling after the intermediate annealing is preferably air cooling or slow cooling. In addition, although intermediate annealing is effective when the cold work rate is high, it does not necessarily need to be performed.

なお、特に優れた磁気特性が必要である部品に適用するものは、熱間圧延後、中間焼鈍、冷間加工を行う前に、高温に加熱してオーステナイト単相に変態させる熱処理を行うことが好ましい。これにより、熱間圧延によって生じた集合組織の異方性を解消することができる。   In addition, what is applied to parts that require particularly excellent magnetic properties may be subjected to a heat treatment that is heated to a high temperature and transformed into an austenite single phase after hot rolling, before intermediate annealing and cold working. preferable. Thereby, the anisotropy of the texture produced by hot rolling can be eliminated.

この、熱間圧延後に熱処理を行った、本発明の電磁軟鉄製部品用線材の組織について説明する。   The structure of the wire for an electromagnetic soft iron part of the present invention, which is heat-treated after the hot rolling, will be described.

圧延方向断面のフェライト粒度番号Gと圧延方向に垂直な方向の断面のフェライト粒度番号Gの比G/G:棒鋼、線材の形状に熱間圧延を行った場合に生じる結晶方位の異方性が最終製品まで受け継がれると、磁気特性に悪影響を与える。そのため、中間焼鈍、冷間加工前の熱間圧延後の電磁軟鉄製部品用棒線材の、圧延方向断面のフェライト粒度番号Gと圧延方向に垂直な方向断面のフェライト粒度番号Gの比G/Gは極力1に近いことが好ましい。具体的には、G/Gは、0.80〜1.20であることが好ましい。 Ratio G L / G C of ferrite grain size number G L in the cross section in the rolling direction and ferrite grain size number G C in the cross section in the direction perpendicular to the rolling direction: of crystal orientation generated when hot rolling is performed on the shape of the bar steel and wire rod If the anisotropy is inherited to the final product, the magnetic properties are adversely affected. Therefore, the intermediate annealing, cold working before or after hot rolling of an electromagnetic soft iron component rod wire, the ratio of the ferrite grain size number G T perpendicular cross section in the rolling direction and the ferrite grain size number G R in the rolling direction cross-section G R 1 / G T is preferably as close to 1 as possible. Specifically, G R / G T is preferably 0.80 to 1.20.

この電磁軟鉄製部品用線材を用いて製造された電磁軟鉄製部品は、軸方向とそれに垂直な方向のフェライト粒度の比G/Gが0.80〜1.20となる。これにより、棒線材の形状への熱間圧延によって形成された集合組織に起因する磁気特性の異方性が軽減され、電磁軟鉄製部品の磁気特性が更に向上する。 In the electromagnetic soft iron part manufactured using this electromagnetic soft iron part wire, the ratio G L / G C of the ferrite grain size in the axial direction and the direction perpendicular thereto is 0.80 to 1.20. Thereby, the anisotropy of the magnetic characteristic resulting from the texture formed by hot rolling to the shape of a bar wire is reduced, and the magnetic characteristic of the electromagnetic soft iron part is further improved.

次に、本発明の電磁軟鉄製部品用棒線材の製造方法のうち、熱間圧延後の熱処理について説明する。   Next, heat treatment after hot rolling will be described in the method for producing a bar wire for electromagnetic soft iron parts of the present invention.

熱間圧延後熱処理:熱間圧延後の棒鋼、線材の集合組織の異方性を軽減するには、熱処理によって組織の一部、又は全部を一旦オーステナイト化することが好ましい。加熱温度が低すぎるか、保持時間が短すぎるとオーステナイト化が不十分になって異方性の軽減効果が不十分になることがある。一方、加熱温度が高すぎるか、保持時間が長すぎるとコスト、設備制約、歩留まり等が低下する。したがって、加熱温度は880〜1250℃の範囲にすることが好ましく、より好適範囲は900〜1100℃である。また、保持時間は、60〜3600sが好ましく、保持時間の好適範囲は900〜1800sである。   Heat treatment after hot rolling: In order to reduce the anisotropy of the texture of steel bars and wire rods after hot rolling, it is preferable that a part or all of the structure is once austenitized by heat treatment. If the heating temperature is too low or the holding time is too short, austenitization may be insufficient and the effect of reducing anisotropy may be insufficient. On the other hand, if the heating temperature is too high or the holding time is too long, the cost, facility restrictions, yield, etc. are reduced. Therefore, it is preferable to make heating temperature into the range of 880-1250 degreeC, and a more suitable range is 900-1100 degreeC. Further, the holding time is preferably 60 to 3600 s, and the preferable range of the holding time is 900 to 1800 s.

また、加熱、保持後の冷却速度は、5℃/sよりも速すぎる場合はベイナイト、マルテンサイト組織が生成して、加工性を損なうことがある。また、冷却速度が、0.1℃/sよりも遅すぎる場合は、生産性が低下する。したがって、冷却速度は、0.1〜5℃/sとすることが好ましい。   In addition, when the cooling rate after heating and holding is too higher than 5 ° C./s, a bainite and martensite structure may be generated, and workability may be impaired. Further, when the cooling rate is too slower than 0.1 ° C./s, the productivity is lowered. Therefore, the cooling rate is preferably 0.1 to 5 ° C./s.

本発明の電磁軟鉄製部品用棒線材の製造方法では、熱間圧延後に、伸線などの二次加工を行っても良い。なお、冷間での二次加工、例えば、伸線加工を行う場合は、冷間加工性を向上させるために、熱間圧延後、又は熱処理後の素材に焼鈍、又は球状化焼鈍処理を施しても良い。   In the method for manufacturing a bar wire for electromagnetic soft iron parts of the present invention, secondary processing such as wire drawing may be performed after hot rolling. In addition, when performing secondary processing in cold, for example, wire drawing, in order to improve cold workability, the material after hot rolling or heat treatment is subjected to annealing or spheroidizing annealing treatment. May be.

以下に、実施例により本発明を詳細に説明する。   Hereinafter, the present invention will be described in detail by way of examples.

表1に示す組成を有する転炉溶製鋼を連続鋳造により製造し、分塊圧延工程を経て162mm角の圧延素材とした。次に熱間圧延によって直径が25mmの線材形状とした。一部の圧延材については、圧延後に表2に示す条件で、熱処理を施した。   Converter molten steel having the composition shown in Table 1 was manufactured by continuous casting, and a rolling raw material of 162 mm square was obtained through a block rolling process. Next, a wire rod having a diameter of 25 mm was formed by hot rolling. Some rolled materials were heat-treated under the conditions shown in Table 2 after rolling.

次に線材に、680℃で5時間保持した後、空冷する中間焼鈍を施し、試料を採取して、JIS Z 2244に準拠してビッカース硬さを測定した。中間焼鈍後の線材を切断し、部品成形の冷間鍛造工程を模擬した50%の据え込み加工を室温で行った後、磁気特性評価用の試験片であるリング状試験片(外形10mm、内径6mm、高さ3mm)に切削加工した。したがって、リング状試験片では、厚み方向が軸方向に相当し、水平方向が軸方向に垂直な方向に相当する。   Next, the wire was held at 680 ° C. for 5 hours, then subjected to air-cooling intermediate annealing, a sample was taken, and Vickers hardness was measured according to JIS Z 2244. After cutting the wire after the intermediate annealing, 50% upsetting was performed at room temperature to simulate the cold forging process of component molding, and then a ring-shaped test piece (outer diameter 10 mm, inner diameter) as a test piece for magnetic property evaluation 6 mm, height 3 mm). Therefore, in the ring-shaped test piece, the thickness direction corresponds to the axial direction, and the horizontal direction corresponds to the direction perpendicular to the axial direction.

リング状試験片を850℃に加熱し、2時間保持した後、炉冷する最終焼鈍を行った。その後、軸方向の断面のフェライト粒度番号(G)及び軸方向に垂直な方向の断面のフェライト粒度番号(G)を測定した。なお、熱間圧延後に熱処理を行った線材については、線材の圧延方向の断面と圧延方向に垂直な断面のフェライト結晶粒度の比G/Gが、最終焼鈍後のリング状試験片のG/Gと同等であることを確認した。 The ring-shaped test piece was heated to 850 ° C., held for 2 hours, and then subjected to final annealing for furnace cooling. Thereafter, the ferrite grain size number (G L ) of the cross section in the axial direction and the ferrite grain size number (G C ) of the cross section in the direction perpendicular to the axial direction were measured. Note that the wire material subjected to heat treatment after hot rolling, G ratio G R / G T of the ferrite grain size of a cross section perpendicular to the cross section to the rolling direction of the rolling direction of the wire is, the final annealing after the ring specimens It was confirmed to be equivalent to the L / G C.

リング状試験片の直流磁気特性の測定は、JIS C 2504(IEC 60404−4)に準じてヒステリシス曲線(B−H曲線)を求めることによって行った。保磁力(Hc)は磁界の強さ400A/m印加、反転時の条件で測定し、外部磁界に対する磁束密度は、外部磁界が100〜4000A/mのときに発生した磁束密度(B)を測定した。   The DC magnetic characteristics of the ring-shaped test piece were measured by obtaining a hysteresis curve (BH curve) according to JIS C 2504 (IEC 60404-4). The coercive force (Hc) is measured under a magnetic field strength of 400 A / m applied and reversed. The magnetic flux density for an external magnetic field is the magnetic flux density (B) generated when the external magnetic field is 100 to 4000 A / m. did.

結果を表2に示す。磁束密度の測定値は、1000A/mのときの磁束密度(B1000)を代表値として示した。なお、磁気特性の優劣の基準は、Hcに関しては60A/m以上のもの、B1000に関しては1.65以下のものについては磁気特性に劣ると判断した。   The results are shown in Table 2. The measured value of the magnetic flux density represented the magnetic flux density (B1000) at 1000 A / m as a representative value. The criteria for superiority or inferiority of the magnetic properties were determined to be inferior in magnetic properties for Hc of 60 A / m or more and B1000 of 1.65 or less.

Figure 2008169451
Figure 2008169451

Figure 2008169451
Figure 2008169451

本発明例の製造No.2及び4は圧延後の熱処理の効果を示している。それぞれ同一成分の製造No.1、No.3と比較すると、フェライト粒度番号が小さく、G/Gが1により近くなっている。即ち、フェライト粒径が大きくなっており、また、異方性が改善され、そのため、Hcが小さくなり、磁気特性が向上していることが分かる。また、製造No.3はNo.1及び2と同一成分であり、熱間圧延後の熱処理条件が好ましい範囲から外れている本発明例であり、製造No.3の磁気特性は、製造No.1と同等である。 Production No. of the present invention example. 2 and 4 show the effect of heat treatment after rolling. Production Nos. Of the same component respectively. 1, no. 3 and by comparison, small ferrite grain size number, G L / G C becomes closer to 1. That is, it can be seen that the ferrite grain size is increased and the anisotropy is improved, so that Hc is reduced and the magnetic properties are improved. In addition, production No. 3 is No.3. It is the same component as 1 and 2, and is an example of the present invention in which the heat treatment conditions after hot rolling are out of the preferred range. The magnetic characteristics of No. 3 are as follows. Is equivalent to 1.

比較例である製造No.12〜17はいずれもNi、Coを含有していないため、B1000が発明例に比べて小さく、目標値に達していない。製造No.15〜17はMn量、Al量も本発明の範囲外であるため、フェライト粒度番号が大きくなっており、Hc、B1000ともに劣化している。   Production No. which is a comparative example. Since 12 to 17 do not contain Ni or Co, B1000 is smaller than the inventive examples and does not reach the target value. Production No. Since the amounts of Mn and Al are also outside the scope of the present invention in Nos. 15 to 17, the ferrite particle size number is large, and both Hc and B1000 are deteriorated.

これらから明らかなように、本発明で規定する条件を全て満たすものは比較例に比べて直流磁気特性に優れている。   As is clear from these, those satisfying all the conditions defined in the present invention are superior in DC magnetic characteristics as compared with the comparative example.

Claims (8)

質量%で、
Mn:0.20超〜0.50%
を含有し、さらに、
Ni:0.05〜1.00%、
Co:0.05〜1.00%
の一方又は双方を含有し、
C:0.02%以下、
Si:0.10%以下、
P:0.010%以下(0%を含む)、
S:0.010%以下(0%を含む)、
Total Al:0.010%以下(0%を含む)、
Sol.Al:0.005%以下(0%を含む)、
Ti:0.005%以下(0%を含む)、
N:0.0050%以下、
O:0.0200%
に制限し、残部がFe及び不可避的不純物からなり、フェライト粒度番号が5番以下であることを特徴とする磁気特性に優れた電磁軟鉄製部品。
% By mass
Mn: more than 0.20 to 0.50%
In addition,
Ni: 0.05-1.00%,
Co: 0.05-1.00%
One or both of
C: 0.02% or less,
Si: 0.10% or less,
P: 0.010% or less (including 0%),
S: 0.010% or less (including 0%),
Total Al: 0.010% or less (including 0%),
Sol. Al: 0.005% or less (including 0%),
Ti: 0.005% or less (including 0%),
N: 0.0050% or less,
O: 0.0200%
An electromagnetic soft iron part with excellent magnetic properties, characterized in that the balance is Fe and inevitable impurities, and the ferrite grain size number is 5 or less.
軸方向断面のフェライト粒度番号Gと軸方向に垂直な方向の断面のフェライト粒度番号Gの比G/Gが、0.80〜1.20であることを特徴とする請求項1に記載の磁気特性に優れた電磁軟鉄製部品。 Claim ratio of axial sectional ferrite grain size number G L and the axial direction perpendicular to the direction of the cross ferrite grain size number G C of G L / G C, characterized in that a 0.80 to 1.20 1 Electromagnetic soft iron parts with excellent magnetic properties as described in 1. 請求項1に記載の電磁軟鉄製部品の素材であって、質量%で、
Mn:0.20超〜0.50%
を含有し、さらに、
Ni:0.05〜1.00%、
Co:0.05〜1.00%
の一方又は双方を含有し、
C:0.02%以下、
Si:0.10%以下、
P:0.010%以下(0%を含む)、
S:0.010%以下(0%を含む)、
Total Al:0.010%以下(0%を含む)、
Sol.Al:0.005%以下(0%を含む)、
Ti:0.005%以下(0%を含む)、
N:0.0050%以下、
O:0.0200%
に制限し、残部がFe及び不可避的不純物からなることを特徴とする磁気特性に優れた電磁軟鉄製部品用棒線材。
The material of the electromagnetic soft iron part according to claim 1, wherein the raw material is mass%.
Mn: more than 0.20 to 0.50%
In addition,
Ni: 0.05-1.00%,
Co: 0.05-1.00%
One or both of
C: 0.02% or less,
Si: 0.10% or less,
P: 0.010% or less (including 0%),
S: 0.010% or less (including 0%),
Total Al: 0.010% or less (including 0%),
Sol. Al: 0.005% or less (including 0%),
Ti: 0.005% or less (including 0%),
N: 0.0050% or less,
O: 0.0200%
The wire rod for electromagnetic soft iron parts excellent in magnetic properties, characterized in that the balance is made of Fe and inevitable impurities.
請求項2に記載の電磁軟鉄製部品の素材であって、圧延方向断面のフェライト粒度番号Gと圧延方向に垂直な方向の断面のフェライト粒度番号Gの比G/Gが、0.80〜1.20であることを特徴とする請求項3に記載の磁気特性に優れた電磁軟鉄製部品用用棒線材。 A material of the electromagnetic soft iron component according to claim 2, the ratio G R / G T of the ferrite grain size number G T of the ferrite grain size number G R to the rolling direction in the vertical direction of the cross section of the rolling direction cross-section, 0 The bar wire material for electromagnetic soft iron parts having excellent magnetic properties according to claim 3, wherein the rod wire material has a magnetic property of .80 to 1.20. 請求項3に記載の電磁軟鉄製部品用棒線材の製造方法であって、質量%で、
Mn:0.20超〜0.50%
を含有し、さらに、
Ni:0.05〜1.00%、
Co:0.05〜1.00%
の一方又は双方を含有し、
C:0.02%以下、
Si:0.10%以下、
P:0.010%以下(0%を含む)、
S:0.010%以下(0%を含む)、
Total Al:0.010%以下(0%を含む)、
Sol.Al:0.005%以下(0%を含む)、
Ti:0.005%以下(0%を含む)、
N:0.0050%以下、
O:0.0200%
に制限し、残部がFe及び不可避的不純物からなる圧延素材を熱間圧延することを特徴とする磁気特性に優れた電磁軟鉄製部品用棒線材の製造方法。
It is a manufacturing method of the bar wire material for electromagnetic soft iron parts of Claim 3, Comprising: In mass%,
Mn: more than 0.20 to 0.50%
In addition,
Ni: 0.05-1.00%,
Co: 0.05-1.00%
One or both of
C: 0.02% or less,
Si: 0.10% or less,
P: 0.010% or less (including 0%),
S: 0.010% or less (including 0%),
Total Al: 0.010% or less (including 0%),
Sol. Al: 0.005% or less (including 0%),
Ti: 0.005% or less (including 0%),
N: 0.0050% or less,
O: 0.0200%
A method for producing a bar wire material for electromagnetic soft iron parts excellent in magnetic properties, characterized in that a rolled material consisting of Fe and inevitable impurities is hot-rolled.
圧延素材を1000℃〜1250℃に加熱し、仕上げ温度を800℃以上として熱間圧延することを特徴とする請求項5に記載の磁気特性に優れた電磁軟鉄製部品用棒線材の製造方法。   The method for producing a bar wire for an electromagnetic soft iron part having excellent magnetic properties according to claim 5, wherein the rolled material is heated to 1000 ° C. to 1250 ° C. and hot rolled at a finishing temperature of 800 ° C. or higher. 請求項4に記載の電磁軟鉄製部品用棒線材の製造方法であって、熱間圧延後、880〜1250℃の温度範囲に加熱し、60〜3600s保持し、冷却する熱処理を施すことを特徴とする請求項5又は6に記載の磁気特性に優れた電磁軟鉄製部品用棒線材の製造方法。   It is a manufacturing method of the bar wire material for electromagnetic soft iron parts of Claim 4, Comprising: After hot rolling, it heats to the temperature range of 880-1250 degreeC, and is heat-processed to hold | maintain and cool for 60-3600 s. The manufacturing method of the bar wire for electromagnetic soft iron parts excellent in the magnetic characteristics of Claim 5 or 6. 加熱、保持後の冷却速度が0.1〜5℃/sであることを特徴とする請求項7に記載の磁気特性に優れた電磁軟鉄製部品用棒線材の製造方法。   The method for producing a bar wire for an electromagnetic soft iron part having excellent magnetic properties according to claim 7, wherein the cooling rate after heating and holding is 0.1 to 5 ° C./s.
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JP2003226945A (en) * 2002-02-06 2003-08-15 Kobe Steel Ltd Soft magnetic steel having excellent cold forgeability and magnetic permeability, soft magnetic steel parts having excellent magnetic permeability and production method therefor

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JP2001158914A (en) * 1999-11-30 2001-06-12 Sumitomo Metal Ind Ltd Method for producing double oriented silicon steel sheet
JP2003226945A (en) * 2002-02-06 2003-08-15 Kobe Steel Ltd Soft magnetic steel having excellent cold forgeability and magnetic permeability, soft magnetic steel parts having excellent magnetic permeability and production method therefor

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JP2013211489A (en) * 2012-03-30 2013-10-10 Keihin Corp Magnetic anisotropic plastic working article and method of manufacturing the same, and electromagnetic device using the same
CN105238985A (en) * 2015-07-02 2016-01-13 苏州科技学院 Sulfur-doped iron-nickel oxygen alloy and preparing method thereof
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