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JP4855221B2 - Non-oriented electrical steel sheet for split core - Google Patents
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JP4855221B2 - Non-oriented electrical steel sheet for split core - Google Patents

Non-oriented electrical steel sheet for split core Download PDF

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JP4855221B2
JP4855221B2 JP2006312064A JP2006312064A JP4855221B2 JP 4855221 B2 JP4855221 B2 JP 4855221B2 JP 2006312064 A JP2006312064 A JP 2006312064A JP 2006312064 A JP2006312064 A JP 2006312064A JP 4855221 B2 JP4855221 B2 JP 4855221B2
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岳顕 脇坂
聡 新井
高英 島津
憲人 阿部
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Nippon Steel Corp
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Description

本発明は、モーターやトランスのコア(鉄芯)材料として用いる無方向性電磁鋼板に関する。   The present invention relates to a non-oriented electrical steel sheet used as a core (iron core) material for a motor or a transformer.

近年、環境保全や、省エネルギーの観点から、電気自動車への関心が高まり、駆動用モーターには、高速回転と小型化とともに、周波数400〜数kHzで駆動できることが求められている。   In recent years, interest in electric vehicles has increased from the viewpoints of environmental protection and energy saving, and drive motors are required to be capable of being driven at a frequency of 400 to several kHz along with high-speed rotation and miniaturization.

このため、モーターのコア材料である無方向性電磁鋼板においては、渦電流損失を低減するため、板厚を薄くするとともに、固有抵抗を高め、さらに、鋼板強度(ローター剛性を上げる)を改善するため、Si量及びAl量を増加する必要がある。さらに、無方向性電磁鋼板には、モーターの初動トルクを改善するため、高い磁束密度も要求される。   For this reason, in the non-oriented electrical steel sheet that is the core material of the motor, in order to reduce eddy current loss, the sheet thickness is reduced, the specific resistance is increased, and further the steel sheet strength (increasing the rotor rigidity) is improved. Therefore, it is necessary to increase the amount of Si and the amount of Al. Furthermore, non-oriented electrical steel sheets are also required to have a high magnetic flux density in order to improve the initial torque of the motor.

モーターコアは、無方向性電磁鋼板を打ち抜いて製造されるが、最近は、打抜き歩留りを改善する観点や、巻き線を効率化して銅損を低減する観点から、モーターコアを、ティース部分で個々に分割した分割コアで構成する傾向にある。そして、分割コアのティース部分には、長さ方向及び幅方向に磁界が印加されるので、磁束密度が高いことが要求される。   Motor cores are manufactured by stamping non-oriented electrical steel sheets. Recently, motor cores are individually manufactured in the teeth part from the viewpoint of improving punching yield and reducing winding loss by improving winding efficiency. Tend to consist of split cores. And since a magnetic field is applied to the teeth part of a division | segmentation core in a length direction and a width direction, it is requested | required that magnetic flux density is high.

通常、無方向性電磁鋼板から、一つのモーターコアを打ち抜く場合、無方向性電磁鋼板の磁気特性には、鋼板の圧延方向(コイル長手方向、以下「L方向」ということがある。)、L方向と直角の方向(コイル幅方向、以下「C方向」ということがある。)、L方向と45度の方向(以下「X方向」ということがる)において、差(異方性)が小さいことが望まれる(特許文献1〜6、参照)。   Usually, when one motor core is punched from a non-oriented electrical steel sheet, the magnetic properties of the non-oriented electrical steel sheet include the rolling direction of the steel sheet (coil longitudinal direction, hereinafter referred to as “L direction”), L. The difference (anisotropy) is small in the direction perpendicular to the direction (coil width direction, hereinafter referred to as “C direction”) and in the L direction and 45 degrees (hereinafter referred to as “X direction”). It is desired (see Patent Documents 1 to 6).

しかし、分割コアを打ち抜く場合、磁気特性の優れた方向に沿って、ティース部分を打ち抜けばよいから、無方向性電磁鋼板を分割コア専用として用いる場合、L方向、C方向、及び、X方向における磁気特性の異方性は、必ずしも、小さくなくてもよい。つまり、磁気特性の異方性が大きいほうが、即ち、X方向の磁気特性を犠牲にしても、L方向とC方向の磁気特性を改善したほうが、分割コアの設計において、分割コアのティース部分で所要の磁気特性を確保することができる点で、好ましい。   However, when punching the split core, it is only necessary to punch through the teeth portion along the direction of excellent magnetic properties. Therefore, when using a non-oriented electrical steel sheet exclusively for the split core, the L direction, the C direction, and the X direction The anisotropy of the magnetic characteristics in is not necessarily small. In other words, the larger the magnetic property anisotropy, that is, the improvement of the magnetic properties in the L direction and the C direction at the sacrifice of the magnetic properties in the X direction, the teeth of the divided core in the design of the divided cores. This is preferable in that required magnetic characteristics can be secured.

なお,特許文献1には、二回目の冷間圧延(以下、「冷延」ということがある。)をスキンパス圧延することが開示されているが、これは、スキンパス圧延の後に、製鉄所サイドで仕上焼鈍を行なう、いわゆる、フルプロセスを採用しており、コスト的な問題、また、打抜き歪みによる鉄損特性の劣化などの問題を抱えるものである。   Patent Document 1 discloses that the second cold rolling (hereinafter sometimes referred to as “cold rolling”) is performed by skin pass rolling, which is performed after the skin pass rolling. A so-called full process is used, in which finish annealing is performed at a low cost, and there are problems such as cost and deterioration of iron loss characteristics due to punching distortion.

特開2001−49402号公報Japanese Patent Laid-Open No. 2001-49402 特開2001−164343号公報Japanese Patent Laid-Open No. 2001-164343 特開2006−45613号公報JP 2006-45613 A 特開2006−45641号公報JP 2006-45641 A 特開2006−144036号公報JP 2006-144036 A 特開2006−199999号公報JP 2006-199999 A

本発明者は、無方向性電磁鋼板において、磁気特性を高めるため、鋼板の板厚を薄くし、かつ、Si量及び/又はAl量を増加すると、磁束密度の異方性が小さくなるという現象に気がついた。即ち、特定の方向、例えば、L方向やC方向の磁束密度が低下し、所望の磁束密度が得られず、結局、このような磁気特性を有する無方向性電磁鋼板は、分割コア用に適さないという問題に遭遇した。   The present inventor has a phenomenon that, in a non-oriented electrical steel sheet, in order to enhance magnetic properties, when the thickness of the steel sheet is reduced and the Si content and / or Al content is increased, the magnetic flux density anisotropy is reduced. I noticed. That is, the magnetic flux density in a specific direction, for example, the L direction or the C direction is reduced, and a desired magnetic flux density cannot be obtained. As a result, a non-oriented electrical steel sheet having such magnetic characteristics is suitable for a split core. Encountered the problem of not.

そこで、本発明は、モーターやトランスの分割コア用として最適な磁気特性を有する無方向性電磁鋼板を提供することを目的とする。   Then, an object of this invention is to provide the non-oriented electrical steel sheet which has the optimal magnetic characteristic for the division | segmentation cores of a motor or a transformer.

本発明者は、質量%で、Si:2〜4%、及び、Al:0.3〜2%を含有する板厚0.1〜0.3mmの無方向性電磁鋼板において、Snを0.003〜0.2%添加して、ゴス方位の結晶粒を増加し、L方向及びC方向の磁気特性(磁束密度)を改善することを基本思想とし、分割コア用として最適な磁気特性を確保する手法について、鋭意研究した。その結果、次の知見を得るに至った。   The inventor of the present invention is a non-oriented electrical steel sheet having a thickness of 0.1 to 0.3 mm containing Si: 2 to 4% and Al: 0.3 to 2% by mass%. Add 003 to 0.2% to increase the Goss-oriented crystal grains and improve the magnetic properties (magnetic flux density) in the L and C directions, ensuring optimum magnetic properties for the split core We studied earnestly about the technique to do. As a result, the following knowledge was obtained.

(x)L、C、及び、X方向の磁気特性の差(異方性)は、板厚(製品板厚)、冷間圧延での圧下率、該圧下率の配分、スキンパス圧延前後の結晶粒径に密接に関連するが、最終的に、これらを制御すれば、異方性の大きい所要の磁束密度B50(磁化力5000A/mで得られる磁束密度[T])を確保することができる。 (X) Differences in magnetic properties (anisotropy) in the L, C, and X directions are sheet thickness (product sheet thickness), reduction ratio in cold rolling, distribution of the reduction ratio, and crystals before and after skin pass rolling. Although it is closely related to the particle diameter, if these are finally controlled, it is possible to secure a required magnetic flux density B 50 having a large anisotropy (magnetic flux density [T] obtained with a magnetizing force of 5000 A / m). it can.

(y)L方向とC方向も磁気特性を繋ぐ、X方向の磁束密度B50を低減すると、L方向及びC方向の磁束密度B50が改善される傾向にあるから、X方向の磁気特性は、分割コア用無方向性電磁鋼板の磁気特性を評価する上で重要な指標であり、L方向の磁気特性との関係で、所定の差の範囲に維持する必要がある。 (Y) L direction and the C direction connecting the magnetic properties and to reduce the magnetic flux density B 50 in the X direction, because there is a tendency that the magnetic flux density B 50 in the L direction and C direction are improved, the magnetic properties of the X-direction This is an important index for evaluating the magnetic properties of the non-oriented electrical steel sheet for the split core, and it is necessary to maintain it within a predetermined difference range in relation to the magnetic properties in the L direction.

本発明は、上記知見に基づいてなされたもので、その要旨は以下のとおりである。   This invention was made | formed based on the said knowledge, and the summary is as follows.

(1) 質量%で、C:0.005%以下、Si:2〜4%、Mn:1%以下、Al:0.3〜2%、Sn:0.003〜0.2%を含有し、残部がFe及び不可避的不純物からなる熱延板に焼鈍を施した後、冷間圧延を施し、次いで、再結晶焼鈍を施し、その後、スキンパス圧延、歪取焼鈍を施して製造した板厚:0.1〜0.3mmのセミプロセス無方向性電磁鋼板であって、
(i)歪取焼鈍後の平均結晶粒径が80〜300μmの再結晶組織を有し、かつ、
(ii)圧延方向(L方向)の磁束密度B50(L)と、圧延方向(L方向)と45°の方向(X方向)の磁束密度B50(X)が、下記式(1)を満たす磁気特性を有する
ことを特徴とする分割コア用無方向性電磁鋼板。
50(L)−B50(X)≧0.07T ・・・(1)
(1) By mass%, C: 0.005% or less, Si: 2-4%, Mn: 1% or less, Al: 0.3-2%, Sn: 0.003-0.2% The thickness of the steel sheet manufactured by annealing the hot-rolled sheet consisting of Fe and unavoidable impurities, followed by cold rolling, followed by recrystallization annealing, followed by skin pass rolling and strain relief annealing: A 0.1 to 0.3 mm semi-processed non-oriented electrical steel sheet,
(I) having a recrystallized structure having an average crystal grain size after strain relief annealing of 80 to 300 μm, and
(Ii) The magnetic flux density B 50 (L) in the rolling direction (L direction) and the magnetic flux density B 50 (X) in the rolling direction (L direction) and 45 ° (X direction) A non-oriented electrical steel sheet for a split core, characterized by having magnetic properties to satisfy.
B 50 (L) −B 50 (X) ≧ 0.07T (1)

(2) 前記磁気特性において、鉄損W10/800が38W/kg以下であることを特徴とする前記(1)に記載の分割コア用無方向性電磁鋼板。 (2) The non-oriented electrical steel sheet for split core according to (1), wherein the iron loss W 10/800 is 38 W / kg or less in the magnetic characteristics.

(3) 前記熱延板の焼鈍温度が900℃超であることを特徴とする前記(1)又は(2)に記載の分割コア用無方向性電磁鋼板。   (3) The non-oriented electrical steel sheet for split core according to (1) or (2), wherein the annealing temperature of the hot-rolled sheet is higher than 900 ° C.

(4) 前記スキンパス圧延前の平均結晶粒径が10〜60μmであることを特徴とする前記(1)〜(3)のいずれか記載の分割コア用無方向性電磁鋼板。   (4) The non-oriented electrical steel sheet for split core according to any one of (1) to (3), wherein an average crystal grain size before the skin pass rolling is 10 to 60 μm.

(5) 前記スキンパス圧延における圧下率が2〜15%であることを特徴とする前記(1)〜(4)のいずれかに記載の分割コア用無方向性電磁鋼板。   (5) The non-oriented electrical steel sheet for split core according to any one of (1) to (4), wherein a rolling reduction in the skin pass rolling is 2 to 15%.

(6) 前記歪取焼鈍を、770〜850℃で施すことを特徴とする前記(1)〜(5)のいずれかに記載の分割コア用無方向性電磁鋼板。   (6) The non-oriented electrical steel sheet for split core according to any one of (1) to (5), wherein the strain relief annealing is performed at 770 to 850 ° C.

本発明によれば、モーターやトランスの分割コア用として最適な磁気特性を有する無方向性電磁鋼板を提供することができる。また、本発明によれば、分割コアの形状、及び/又は、分割コアのティース部分に求める磁気特性に応じて、分割コアを設計し、打ち抜くことができるので、無方向性電磁鋼板の利用度が増す。   ADVANTAGE OF THE INVENTION According to this invention, the non-oriented electrical steel sheet which has the optimal magnetic characteristic as an object for the split cores of a motor or a transformer can be provided. Further, according to the present invention, since the split core can be designed and punched according to the shape of the split core and / or the magnetic characteristics required for the tooth portion of the split core, the utilization of the non-oriented electrical steel sheet Increase.

本発明は、質量%で、C:0.005%以下、Si:2〜4%、Mn:1%以下、Al:0.3〜2%、Sn:0.003〜0.2%を含有し、残部がFe及び不可避的不純物からなる熱延板に焼鈍を施した後、冷間圧延を施し、次いで、再結晶焼鈍を施し、その後、スキンパス圧延、歪取焼鈍を施した板厚0.1〜0.3mmのセミプロセス無方向性電磁鋼板であって、
(i)歪取焼鈍後の平均結晶粒径が80〜300μmの再結晶組織を有し、かつ、
(ii)圧延方向(L方向)の磁束密度B50(L)と、圧延方向(L方向)と45°の方向(X方向)の磁束密度B50(X)が、下記式(1)を満たす磁気特性を有する
ことを特徴とする。
50(L)−B50(X)≧0.07T ・・・(1)
The present invention contains, in mass%, C: 0.005% or less, Si: 2-4%, Mn: 1% or less, Al: 0.3-2%, Sn: 0.003-0.2% Then, after the hot rolled sheet consisting of Fe and inevitable impurities is annealed, the sheet is cold rolled, then recrystallized annealed, and then subjected to skin pass rolling and strain relief annealing. 1 to 0.3 mm semi-process non-oriented electrical steel sheet,
(I) having a recrystallized structure having an average crystal grain size after strain relief annealing of 80 to 300 μm, and
(Ii) The magnetic flux density B 50 (L) in the rolling direction (L direction) and the magnetic flux density B 50 (X) in the rolling direction (L direction) and 45 ° (X direction) It is characterized by having magnetic properties that satisfy.
B 50 (L) −B 50 (X) ≧ 0.07T (1)

50(L)は、L方向に5000A/mで磁化して測定したL方向の磁束密度(単位:T)であり、B50(X)は、鋼板面上で、X方向に5000A/mで磁化して測定したX方向の磁束密度である。なお、B50(C)は、鋼板面上で、C方向に5000A/mで磁化して測定したC方向の磁束密度である。 B 50 (L) is the magnetic flux density (unit: T) in the L direction measured by magnetizing at 5000 A / m in the L direction, and B 50 (X) is 5000 A / m in the X direction on the steel plate surface. Is the magnetic flux density in the X direction measured by magnetization. B 50 (C) is a magnetic flux density in the C direction measured by being magnetized at 5000 A / m in the C direction on the steel plate surface.

まず、熱延板の成分組成を限定する理由について説明する。なお、以下、%は、質量%を意味する。   First, the reason for limiting the component composition of the hot-rolled sheet will be described. Hereinafter, “%” means mass%.

Cは、鋼板を強化する元素であるが、磁気特性の点で有害な元素であり、極力低減するのが好ましいので、Cは、0.005%以下に限定した。好ましくは、0.003%以下である。   C is an element that reinforces the steel sheet. However, C is an element harmful in terms of magnetic properties and is preferably reduced as much as possible. Therefore, C is limited to 0.005% or less. Preferably, it is 0.003% or less.

Siは、鋼板の電気抵抗を高め、鉄損を低減する元素であるので、2%以上を含有する。4%を超えて含有すると、鋼板が脆化し、また、所要の磁束密度B50が得られないので、Siの上限を4%とした。 Since Si is an element that increases the electrical resistance of the steel sheet and reduces iron loss, it contains 2% or more. When the content exceeds 4%, the steel sheet is embrittled, and since the required magnetic flux density B 50 is not obtained, and 4% the upper limit of Si.

Mnは、熱間圧延時に、MnSとしてSを固定し、熱間圧延時の鋼板耳割れを防止する元素である。固溶Mnは、鋼板の電気抵抗を高め、鉄損を低減するが、Mnが多すぎると結晶粒成長性が阻害されるので、Mnの上限を1%とした。   Mn is an element that fixes S as MnS at the time of hot rolling and prevents steel plate ear cracks during hot rolling. The solute Mn increases the electrical resistance of the steel sheet and reduces the iron loss. However, if Mn is too much, crystal grain growth is inhibited, so the upper limit of Mn is set to 1%.

Alは、Siと同様に、鋼板の電気抵抗を高め、鉄損を低減する元素であるので、0.3%を超えて含有する。しかし、2%を超えて含有すると、飽和磁束密度が劣化するので、上限を2%とした。   Al, like Si, is an element that increases the electrical resistance of the steel sheet and reduces the iron loss, so it contains more than 0.3%. However, if the content exceeds 2%, the saturation magnetic flux density deteriorates, so the upper limit was made 2%.

Snは、Si:2〜4%、及び、Al:0.3〜2%を含有する無方向性電磁鋼板の再結晶組織において、Goss方位粒を増加し、特に、L方向の磁気特性(磁束密度)を改善するために、0.003%以上含有する必要がある。一方、0.2%を超えて含有しても、上記改善効果は飽和するし、熱間脆性の問題で表面疵が増加するので、上限を0.2%とした。   Sn increases the number of Goss orientation grains in the recrystallized structure of non-oriented electrical steel sheets containing Si: 2 to 4% and Al: 0.3 to 2%. In order to improve (density), it is necessary to contain 0.003% or more. On the other hand, even if the content exceeds 0.2%, the above improvement effect is saturated, and surface defects increase due to hot brittleness, so the upper limit was made 0.2%.

本発明は、上記元素の他、不可避的不純物として、S、P、N、O、Cu、Ni、Cr、Ca、REM、Nb、Ti等を、本発明の機械特性及び磁気特性を損なわない範囲で含有してもよい。ただし、従来どおり、不純物としてのS、N、及び、Oは、少ないほうが好ましい。それら各成分は、それぞれ、0.003%以下、0.0025%以下、及び、0.003%以下が好ましい。   In the present invention, in addition to the above elements, S, P, N, O, Cu, Ni, Cr, Ca, REM, Nb, Ti, etc. are included as inevitable impurities, and the mechanical and magnetic properties of the present invention are not impaired. You may contain. However, as in the past, it is preferable that S, N, and O as impurities are small. Each of these components is preferably 0.003% or less, 0.0025% or less, and 0.003% or less.

また,所望の異方性を阻害しないことを確認している範囲は、Cu<0.2%、Ni<0.1%、Cr<0.1%、Ca<0.01%、REM<0.01%、Nb<0.003%、Ti<0.003%であるので、これら元素は、それぞれ上記範囲内に抑制するのが好ましい。なお、Sbは、異方性を小さくするので、添加してはならない。Sbは、不可避的に含有する場合は、0.001%未満が好ましい。   In addition, the range in which the desired anisotropy is not inhibited is Cu <0.2%, Ni <0.1%, Cr <0.1%, Ca <0.01%, REM <0. 0.01%, Nb <0.003%, and Ti <0.003%, so that these elements are preferably suppressed within the above ranges. Note that Sb should not be added because it reduces anisotropy. When Sb is inevitably contained, it is preferably less than 0.001%.

上記成分組成の熱延板に焼鈍を施した後、冷間圧延を施し、次いで、再結晶焼鈍を施し、その後、スキンパス圧延を施す。その後,顧客又は加工センターで、分割コアに打ち抜かれた後、歪取焼鈍が施され、平均結晶粒径が80〜300μmの再結晶組織が形成される。   After annealing the hot-rolled sheet having the above component composition, cold rolling is performed, then recrystallization annealing is performed, and then skin pass rolling is performed. Thereafter, after being punched into the split core at the customer or processing center, strain relief annealing is performed, and a recrystallized structure having an average crystal grain size of 80 to 300 μm is formed.

本発明においては、前述した知見(x)に基づいて、歪取焼鈍後の平均結晶粒径を80〜300μmに規定する。平均結晶粒径が大きいと、鉄損特性は改善されるが,磁束密度が劣化し、また、磁束密度の異方性(B50(L)−B50(X))は、若干ではあるが、小さくなる傾向にある。 In the present invention, based on the knowledge (x) described above, the average crystal grain size after strain relief annealing is regulated to 80 to 300 μm. When the average crystal grain size is large, the iron loss characteristics are improved, but the magnetic flux density is deteriorated, and the magnetic flux density anisotropy (B 50 (L) −B 50 (X)) is slight. , Tend to be smaller.

歪取焼鈍後の平均結晶粒径が80μm未満であると、鉄損特性が不満であり、また、300μmを超えると、磁束密度B50(L)の劣化が大きいので、歪取焼鈍後の平均結晶粒径は、80〜300μmに制限する。なお,平均結晶粒径は,鋼板断面を光学顕微鏡で観察した組織において、L方向の線分と交差する結晶粒界の個数を数え、平均化して求めた。 If the average grain size after strain relief annealing is less than 80 μm, the iron loss characteristics are unsatisfactory, and if it exceeds 300 μm, the magnetic flux density B 50 (L) is greatly deteriorated. The crystal grain size is limited to 80 to 300 μm. The average crystal grain size was obtained by counting and averaging the number of crystal grain boundaries intersecting the line segment in the L direction in the structure obtained by observing the cross section of the steel sheet with an optical microscope.

本発明は、歪取焼鈍後の平均結晶粒径が80〜300μmの再結晶組織を有する板厚0.1〜0.3mmのセミプロセス無法工背電磁鋼板が、下記式(1)を満たす磁気特性を有することを特徴とする。
50(L)−B50(X)≧0.07T ・・・(1)
In the present invention, a semi-processed illegal back electrical steel sheet having a thickness of 0.1 to 0.3 mm having a recrystallized structure having an average crystal grain size of 80 to 300 μm after strain relief annealing satisfies the following formula (1): It has the characteristics.
B 50 (L) −B 50 (X) ≧ 0.07T (1)

なお、B50(L)、及び、B50(X)については、前述したとおりである。 B 50 (L) and B 50 (X) are as described above.

「B50(L)−B50(X)」は、L方向とX方向のB50の差そのものである。そして、この差を所定の範囲にすることは、下記の理由で、無方向性電磁鋼板の分割コア用としての適確性を判断する上で、極めて重要であり、分割コア用無法工背電磁鋼板の磁気特性を評価する指標として、「B50(L)−B50(X)」を導入した。 “B 50 (L) −B 50 (X)” is the difference itself between B 50 in the L direction and the X direction. And, it is extremely important to determine this difference within a predetermined range in determining the appropriateness of the non-oriented electrical steel sheet for the split core for the following reasons. “B 50 (L) −B 50 (X)” was introduced as an index for evaluating the magnetic properties of the film.

図1(a)及び(b)に、分割コアの打ち抜き態様を示す。図1(a)は、分割コアのティース部分をC方向(L方向と90°)に設定し、打抜き歩留りを最優先して打ち抜く態様(以下「打抜き態様A」ということがある。)を示し、図1(b)は、分割コアのティース部分をL方向に設定し、打抜き歩留りとともに、鉄心特性(ティース部の磁束密度)を重視して打ち抜く態様(以下「打抜き態様B」ということがある。)を示す。   1 (a) and 1 (b) show how the split core is punched. FIG. 1A shows an aspect in which the tooth portion of the split core is set in the C direction (90 degrees with respect to the L direction) and punching is performed with the highest priority on the punching yield (hereinafter sometimes referred to as “punching aspect A”). In FIG. 1B, the tooth portion of the split core is set in the L direction, and punching is performed with emphasis on the core characteristics (magnetic flux density of the tooth portion) as well as the punching yield (hereinafter referred to as “punching mode B”). .)

直近、電動モーターの分野では、従来の一体コアに加え、打抜き歩留まりの向上や、巻き線の効率化による銅損向上の観点から、分割コアを用いるケースが増加している。分割コアは、圧延後コイル状に巻き取った電磁鋼板コイルの圧延方向(L方向)に対し、打抜き態様A又は打抜き態様Bで打ち抜かれる場合が多い。   Recently, in the field of electric motors, in addition to the conventional integrated core, the number of cases using a split core is increasing from the viewpoint of improving the punching yield and improving copper loss by increasing the efficiency of winding. In many cases, the split core is punched in the punching mode A or the punching mode B with respect to the rolling direction (L direction) of the magnetic steel sheet coil wound in a coil shape after rolling.

一般に、工業的に製造される無方向性電磁鋼板は、C方向及びX方向の磁気特性(磁化特性、鉄損特性)が、L方向の磁気特性(磁化特性、鉄損特性)に比べ劣位であり、C方向又はX方向の磁気特性が、分割コア鉄心全体の磁気特性を左右することになる。   In general, non-oriented electrical steel sheets manufactured industrially have inferior magnetic properties (magnetization characteristics, iron loss characteristics) in the C direction and X direction compared to magnetic characteristics (magnetization characteristics, iron loss characteristics) in the L direction. Yes, the magnetic characteristics in the C direction or the X direction influence the magnetic characteristics of the entire split core iron core.

そして、分割コア鉄芯の磁束流には、打抜き態様A及び打抜き態様Bで打ち抜かれた分割コアのいずれの場合も、磁束がL方向からC方向に回転する途中に、遷移的なX方向の磁束流が存在するが、分割コアでは,このX方向の遷移的な磁束流領域は少なく、分割コア鉄心の磁気特性に及ぼす影響度は小さいと推測される。   The flux flow of the split core iron core includes a transitional X direction in the middle of the magnetic flux rotating from the L direction to the C direction in both cases of the split core punched in the punching mode A and the punching mode B. Although there is a magnetic flux flow, in the split core, the transitional magnetic flux region in the X direction is small, and it is estimated that the degree of influence on the magnetic properties of the split core iron core is small.

つまり、本発明者は、L方向の磁気特性とX方向の磁気特性の差:B50(L)−B50(X)が所定値(0.07T)以上に大きくなるように材料設計すれば、分割コア鉄心全体の磁気特性を改善することができると発想した。 That is, the present inventor should design the material so that the difference between the magnetic characteristics in the L direction and the magnetic characteristics in the X direction: B 50 (L) −B 50 (X) is greater than a predetermined value (0.07T). The idea was that the magnetic properties of the entire split core could be improved.

なお、L方向とC方向における適正な磁気特性のバランスは、分割コア一片の寸法、形状により決定される。   The appropriate balance of magnetic characteristics in the L direction and the C direction is determined by the size and shape of the split core piece.

50(L)−B50(X)を所定の範囲に規定することは、無方向性電磁鋼板の磁気特性の異方性を所定の範囲に限定することであるから、分割コアを設計する際、分割コア鉄心全体の磁気特性の向上を考慮して、分割コアの形状、及び、打ち抜き態様を設計することができる。 Since defining B 50 (L) −B 50 (X) within a predetermined range is to limit the anisotropy of the magnetic properties of the non-oriented electrical steel sheet to a predetermined range, a split core is designed. At this time, the shape of the split core and the punching mode can be designed in consideration of the improvement of the magnetic characteristics of the entire split core iron core.

したがって、「B50(C)−B50(X)」は、無方向性電磁鋼板の分割コア用としての適確性を判断する上で、極めて重要な指標である。 Therefore, “B 50 (C) −B 50 (X)” is an extremely important index for judging the accuracy of the non-oriented electrical steel sheet for the split core.

本発明において、「B50(L)−B50(X)」が、0.07T未満であれば、異方性が小さくなり、必要なL方向とC方向の磁気特性が得られないので、「B50(L)−B50(X)」は0.007T以上とする。 In the present invention, if “B 50 (L) −B 50 (X)” is less than 0.07T, the anisotropy is small, and the required magnetic properties in the L and C directions cannot be obtained. “B 50 (L) −B 50 (X)” is 0.007T or more.

また、板厚(製品板厚)については,所望の高周波特性、即ち、W10/800≦38W/kgを得るために、0.3mm以下が必要である。しかし、0.1mm未満では、薄すぎて、再結晶焼鈍時における破断などが増え、工業的でない。 Further, the plate thickness (product plate thickness) needs to be 0.3 mm or less in order to obtain a desired high-frequency characteristic, that is, W 10/80038 W / kg. However, if it is less than 0.1 mm, it is too thin, and breakage and the like during recrystallization annealing increase, which is not industrial.

本発明は、熱延板に焼鈍を施した後、冷間圧延を施し、次いで、再結晶焼鈍を施し、その後、スキンパス圧延、歪取焼鈍を施すことを要件とするものであるので、次に、好ましい製造要件について、説明する。なお、この製造工程により製造される無方向性電磁鋼板は、スキンパス圧延の後、製鉄所から出荷されるので、セミプロセス無方向性電磁鋼板と称される。 Since the present invention requires that the hot-rolled sheet is annealed, then cold- rolled, then recrystallized annealed, and then subjected to skin pass rolling and strain relief annealing. The preferable manufacturing requirements will be described. In addition, since the non-oriented electrical steel sheet manufactured by this manufacturing process is shipped from a steel mill after skin pass rolling, it is called a semi-processed non-oriented electrical steel sheet.

熱延板の焼鈍は、磁束密度の異方性を大きくする利点がある。焼鈍条件としては、通常の800℃以上の温度でよいが,900℃以上がより好ましい。なお、焼鈍は、連続焼鈍でも箱焼鈍でもよい。焼鈍後の冷間圧延は、通常の、タンデム圧延又はレバース圧延を採用する。   Annealing of a hot-rolled sheet has the advantage of increasing the magnetic flux density anisotropy. The annealing condition may be a normal temperature of 800 ° C. or higher, but more preferably 900 ° C. or higher. The annealing may be continuous annealing or box annealing. Cold rolling after annealing employs normal tandem rolling or lever rolling.

続く、再結晶焼鈍では,結晶粒径を制御することが望ましい。結晶粒径は、小さすぎても大きすぎても、異方性が小さくなるので、適切な範囲の結晶粒径にする必要がある。所望の異方性を得るためには、10〜60μmが好ましい。この範囲の結晶粒径に制御するための焼鈍温度は,700〜850℃程度である。   In the subsequent recrystallization annealing, it is desirable to control the crystal grain size. If the crystal grain size is too small or too large, the anisotropy is small, so it is necessary to make the crystal grain size within an appropriate range. In order to obtain desired anisotropy, 10 to 60 μm is preferable. The annealing temperature for controlling the crystal grain size within this range is about 700 to 850 ° C.

通常の1回冷延法による高級無方向性電磁鋼板の製造においては、1000℃前後の高温で、再結晶焼鈍が実施されていることから、特に薄い鋼板の形状を、フラットにすることが難しかった。しかし、本発明プロセスでの再結晶焼鈍温度は低いので,工業的には、非常に有利である。   In the manufacture of high-grade non-oriented electrical steel sheets by the usual single cold rolling method, since recrystallization annealing is performed at a high temperature of about 1000 ° C., it is difficult to flatten the shape of a particularly thin steel sheet. It was. However, since the recrystallization annealing temperature in the process of the present invention is low, it is very advantageous industrially.

なお,結晶組織中に未再結晶を残すと、歪取焼鈍後の結晶粒径が不安定となって好ましくないので、結晶組織中に未再結晶を残すことは避けなければならない。絶縁皮膜の焼付けは、この段階(再結晶焼鈍後)で実施するのが、工業的である。   If unrecrystallized is left in the crystal structure, the crystal grain size after strain relief annealing becomes unstable and is not preferable. Therefore, it is necessary to avoid leaving unrecrystallized in the crystal structure. It is industrial that the insulating film is baked at this stage (after recrystallization annealing).

本発明においては、冷間圧延後の再結晶組織にスキンパス圧延を施して、L方向の磁束密度B50(L)と、X方向の磁束密度B50(X)の差、即ち、磁気特性の異方性を大きくすることが特徴である。 In the present invention, the recrystallized structure after cold rolling is subjected to skin pass rolling, and the difference between the magnetic flux density B 50 (L) in the L direction and the magnetic flux density B 50 (X) in the X direction, that is, the magnetic property It is characterized by increasing the anisotropy.

磁気特性の異方性を大きくした無方向性電磁鋼板において、分割コアを、ティース部分が、L方向に設定して打ち抜けば、磁束密度の高いティース部分を有する分割コアを得ることができる。   In a non-oriented electrical steel sheet with increased magnetic property anisotropy, a split core having a teeth portion with a high magnetic flux density can be obtained by setting the split core in the L direction.

スキンパス圧延の圧下率を調整することにより、L方向とX方向の磁束密度B50の差(異方性)を調整することができるので、分割コアの要求される磁束密度に応じて、鋼板の磁気特性を設計して、無方向性電磁鋼板を製造することができる。 By adjusting the reduction ratio of the skin pass rolling, the difference (anisotropy) between the magnetic flux density B 50 in the L direction and the X direction can be adjusted, so that depending on the required magnetic flux density of the split core, A non-oriented electrical steel sheet can be manufactured by designing magnetic characteristics.

スキンパス圧延における圧下率は、2〜15%が好ましい。圧下率が2%未満であると、磁気特性の異方性を所望のレベルまで大きくすることが困難であり、また、15%を超えても、磁気特性の異方性が小さくなる。最も大きい異方性が得られる圧下率は、4〜7%である。   The rolling reduction in skin pass rolling is preferably 2 to 15%. If the rolling reduction is less than 2%, it is difficult to increase the magnetic property anisotropy to a desired level, and if it exceeds 15%, the magnetic property anisotropy becomes small. The rolling reduction that provides the greatest anisotropy is 4-7%.

スキンパス圧延によるメタラジーは、一般に、歪み誘起粒成長という一種の異常粒成長機構であり、スキンパス後の数時間の長時間焼鈍(歪取焼鈍のこと)により、爆発的に、粒成長が起きるということである。このときの方位選択的粒成長機構は、基本的には、内部歪が少ない方位粒が爆発的に成長するというものである。しかし、介在物、成分系、結晶粒径、スキンパス圧延の圧下率などにより、この方位選択は微妙に変わることが知られているが、これらの複雑な現象を統一する理論は、まだ形成されていない。   Metallurgy by skin pass rolling is generally a kind of abnormal grain growth mechanism called strain-induced grain growth, and grain growth occurs explosively by prolonged annealing (strain relief annealing) for several hours after skin pass. It is. The orientation-selective grain growth mechanism at this time is basically that orientation grains with little internal strain grow explosively. However, the orientation selection is known to change slightly depending on the inclusion, component system, grain size, reduction rate of skin pass rolling, etc., but the theory that unifies these complex phenomena has not yet been formed. Absent.

歪取焼鈍は、通常の700〜850℃で、2時間、均熱する程度のものであるが、結晶組織を狙いの粗大粒とするために、焼鈍温度は高温側が好ましい。好ましい焼鈍温度は、770〜850℃である。焼鈍温度が850℃を超えると、絶縁皮膜の密着性が劣化することがある。   The strain relief annealing is performed at a normal temperature of 700 to 850 [deg.] C. for 2 hours, but the annealing temperature is preferably on the high temperature side in order to obtain coarse grains aimed at the crystal structure. A preferable annealing temperature is 770 to 850 ° C. When the annealing temperature exceeds 850 ° C., the adhesion of the insulating film may be deteriorated.

高周波鉄損W10/800は、38W/kg以下であることが好ましい。コンパクトなサイズのモーターコアにするための高速回転仕様に対応するためである。 The high-frequency iron loss W 10/800 is preferably 38 W / kg or less. This is to meet the high-speed rotation specification for a compact motor core.

次に、本発明の実施例について説明するが、実施例の条件は、本発明の実施可能性及び効果を確認するために採用した一条件例であり、本発明は、この一条件例に限定されるものではない。本発明は、本発明の要旨を逸脱せず、本発明の目的を達成する限りにおいて、種々の条件を採用し得るものである。   Next, examples of the present invention will be described. The conditions of the examples are one example of conditions adopted for confirming the feasibility and effects of the present invention, and the present invention is limited to this one example of conditions. Is not to be done. The present invention can adopt various conditions as long as the object of the present invention is achieved without departing from the gist of the present invention.

(実施例1)
鋼を真空溶解炉で溶解しつつ、成分組成を調整し、表1に示す成分組成を有するインゴットを鋳造した。これを、1050℃に加熱して熱間圧延し、2.3mm厚の熱延板とした。次いで,N2雰囲気中、920℃で90秒均熱して焼鈍を行った。酸洗後、冷間圧延を施して、板厚0.315mm(圧下率86.3%)の冷延板とした。
Example 1
The component composition was adjusted while melting steel in a vacuum melting furnace, and an ingot having the component composition shown in Table 1 was cast. This was heated to 1050 ° C. and hot-rolled to obtain a hot-rolled sheet having a thickness of 2.3 mm. Next, annealing was performed by soaking at 920 ° C. for 90 seconds in an N 2 atmosphere. After pickling, cold rolling was performed to obtain a cold-rolled sheet having a sheet thickness of 0.315 mm (reduction rate of 86.3%).

再結晶焼鈍を、H2雰囲気中で、750℃、30秒均熱の条件で実施した。平均結晶粒径は、15〜20μmの範囲に入っていた。次いで、スキンパス圧延を施し、板厚を0.300mm(5%圧下)とした。55mm角に打抜いてから、H2雰囲気中、750℃、2時間の焼鈍を行い、SSTで、角度別に磁気特性を測定した。 Recrystallization annealing was performed in a H 2 atmosphere at 750 ° C. for 30 seconds. The average grain size was in the range of 15-20 μm. Next, skin pass rolling was performed to obtain a plate thickness of 0.300 mm (5% reduction). After punching out to 55 mm square, annealing was performed at 750 ° C. for 2 hours in an H 2 atmosphere, and the magnetic characteristics were measured for each angle by SST.

平均結晶粒径は130〜150μmであった。得られた結果を表1に示す。W10/800は、磁束密度1.0T、周波数800Hzでの鉄損であり、L方向とC方向の測定値を平均化したものである。A値を、以下の式で定義した。
A値(単位はT)=B50(L)−B50(X)
The average grain size was 130-150 μm. The obtained results are shown in Table 1. W 10/800 is an iron loss at a magnetic flux density of 1.0 T and a frequency of 800 Hz, and is an average of measured values in the L direction and the C direction. The A value was defined by the following formula.
A value (unit: T) = B 50 (L) −B 50 (X)

なお、実施例2以下も、これらの記号に準じるものとする。   In addition, Example 2 and the following also conform to these symbols.

Figure 0004855221
Figure 0004855221

Sn量が本発明の範囲で、優れたB50(L)と、所望の異方性を得ることができた。 The Sn amount was within the range of the present invention, and excellent B 50 (L) and desired anisotropy could be obtained.

(実施例2)
表1に示す実験No.4の板厚0.315mmの冷延板を用い、再結晶焼鈍条件の均熱時間を15秒に固定し、焼鈍温度を変更して結晶粒径を変化させた。焼鈍雰囲気は、10%H2+90%N2とした。次いで、スキンパス圧延を施し、板厚を0.28mm(11.1%圧下)とした。55mm角に打抜いてから、N2雰囲気中で、780℃、2時間の焼鈍を行い、SSTで、角度別に磁気特性を測定し、また、結晶粒径も測定した。得られた結果を表2に示す。
(Example 2)
Experiment No. 1 shown in Table 1. No. 4 cold-rolled sheet having a thickness of 0.315 mm was used, the soaking time under recrystallization annealing conditions was fixed at 15 seconds, and the annealing temperature was changed to change the crystal grain size. The annealing atmosphere was 10% H 2 + 90% N 2 . Next, skin pass rolling was performed to make the plate thickness 0.28 mm (11.1% reduction). After punching into a 55 mm square, annealing was performed at 780 ° C. for 2 hours in an N 2 atmosphere, and magnetic properties were measured for each angle by SST, and the crystal grain size was also measured. The obtained results are shown in Table 2.

Figure 0004855221
Figure 0004855221

再結晶焼鈍後の平均結晶粒径が、本発明の範囲に入っているものは、分割コア用として優れた異方性を有する磁気特性を示している。また,再結晶焼鈍後の平均結晶粒径は、歪取焼鈍後の平均結晶粒径と関係が強く、再結晶焼鈍で粗大粒であれば、歪取焼鈍後も粗大粒であることが分かる。   Those whose average crystal grain size after recrystallization annealing is within the range of the present invention show magnetic characteristics having excellent anisotropy for a split core. Further, the average crystal grain size after recrystallization annealing is strongly related to the average crystal grain size after strain relief annealing, and it can be seen that if recrystallization annealing is a coarse grain, the grain size is also coarse after strain relief annealing.

(実施例3)
質量%で、C:0.001%、Si:3.0%、Mn:0.7%、Al:0.3%、Sn:0.01%、その他、不可避的成分として、Cu:0.1%、Ni:0.05%、Ni:0.01%、Ti:0.002%、Mo:0.002%、P:0.01%を含むスラブを、1100℃に加熱し、仕上圧延温度870℃で、板厚2.8mmの熱延板を得た。
(Example 3)
In terms of mass%, C: 0.001%, Si: 3.0%, Mn: 0.7%, Al: 0.3%, Sn: 0.01%, and other inevitable components, Cu: 0.00%. A slab containing 1%, Ni: 0.05%, Ni: 0.01%, Ti: 0.002%, Mo: 0.002%, P: 0.01% is heated to 1100 ° C and finish-rolled A hot-rolled sheet having a thickness of 2.8 mm was obtained at a temperature of 870 ° C.

2雰囲気中で、1000℃、120秒、焼鈍した後、酸洗し、冷間圧延を施した。再結晶焼鈍を、770℃で10秒、H2雰囲気中で実施した。 After annealing in a N 2 atmosphere at 1000 ° C. for 120 seconds, pickling and cold rolling were performed. Recrystallization annealing was performed at 770 ° C. for 10 seconds in an H 2 atmosphere.

結晶粒径は、13〜15μmの範囲内であった。次いで、表3に示す圧下率のスキンパス圧延を行って、板厚を0.12mmとした。エプスタイン試料を切り出してから、820℃で2時間、H2雰囲気中で歪取焼鈍を行い、角度別に磁気特性及び結晶粒径を計測した。得られた結果を表3に示す。 The crystal grain size was in the range of 13-15 μm. Next, skin pass rolling with a reduction rate shown in Table 3 was performed to obtain a plate thickness of 0.12 mm. After the Epstein sample was cut out, strain relief annealing was performed in an H 2 atmosphere at 820 ° C. for 2 hours, and the magnetic characteristics and crystal grain size were measured for each angle. The obtained results are shown in Table 3.

Figure 0004855221
Figure 0004855221

スキンパス圧延の圧下率が本発明の範囲のものは,分割コアに適した異方性が発現し、また、適正な結晶粒径を歪取焼鈍で得ることができ、高周波鉄損も満足するものが得られた。   When the rolling reduction ratio of the skin pass rolling is within the range of the present invention, anisotropy suitable for the split core is developed, an appropriate crystal grain size can be obtained by strain relief annealing, and high frequency iron loss is also satisfied. was gotten.

前述したように、本発明によれば、モーターやトランスの分割コア用として最適な磁気特性を有し、かつ、利用度の高い無方向性電磁鋼板を提供することができる。したがって、本発明は、無方向性電磁鋼板を素材として用いる電気機器製造産業において利用可能性が大きいものである。   As described above, according to the present invention, it is possible to provide a non-oriented electrical steel sheet that has optimum magnetic characteristics for a split core of a motor or a transformer and has high utilization. Therefore, the present invention has great applicability in the electrical equipment manufacturing industry using non-oriented electrical steel sheets as raw materials.

分割コアの打ち抜き態様を示す図である。(a)は、分割コアのティース部分をC方向(L方向に90℃の方向)に設定して打ち抜く態様を示し、(b)は、分割コアのティース部分をL方向に設定して打ち抜く態様を示す。It is a figure which shows the punching aspect of a split core. (A) shows a mode in which the tooth portion of the split core is set in the C direction (90 ° C. in the L direction) and punched, and (b) shows a mode in which the tooth portion of the split core is set in the L direction and punched. Indicates.

符号の説明Explanation of symbols

1 分割コア
2 ティース部分
1 split core 2 teeth

Claims (6)

質量%で、C:0.005%以下、Si:2〜4%、Mn:1%以下、Al:0.3〜2%、Sn:0.003〜0.2%を含有し、残部がFe及び不可避的不純物からなる熱延板に焼鈍を施した後、冷間圧延を施し、次いで、再結晶焼鈍を施し、その後、スキンパス圧延、歪取焼鈍を施して製造した板厚:0.1〜0.3mmのセミプロセス無方向性電磁鋼板であって、
(i)歪取焼鈍後の平均結晶粒径が80〜300μmの再結晶組織を有し、かつ、
(ii)圧延方向(L方向)の磁束密度B50(L)と、圧延方向(L方向)と45°の方向(X方向)の磁束密度B50(X)が、下記式(1)を満たす磁気特性を有する
ことを特徴とする分割コア用無方向性電磁鋼板。
50(L)−B50(X)≧0.07T ・・・(1)
In mass%, C: 0.005% or less, Si: 2-4%, Mn: 1% or less, Al: 0.3-2%, Sn: 0.003-0.2%, the balance being Thickness of 0.1 mm produced by annealing a hot rolled sheet made of Fe and unavoidable impurities, followed by cold rolling, followed by recrystallization annealing, followed by skin pass rolling and strain relief annealing: 0.1 -0.3mm semi-processed non-oriented electrical steel sheet,
(I) having a recrystallized structure having an average crystal grain size after strain relief annealing of 80 to 300 μm, and
(Ii) The magnetic flux density B 50 (L) in the rolling direction (L direction) and the magnetic flux density B 50 (X) in the rolling direction (L direction) and 45 ° (X direction) A non-oriented electrical steel sheet for a split core, characterized by having magnetic properties to satisfy.
B 50 (L) −B 50 (X) ≧ 0.07T (1)
前記磁気特性において、鉄損W10/800が38W/kg以下であることを特徴とする請求項1に記載の分割コア用無方向性電磁鋼板。 2. The non-oriented electrical steel sheet for split core according to claim 1, wherein an iron loss W 10/800 is 38 W / kg or less in the magnetic characteristics. 前記熱延板の焼鈍温度が900℃超であることを特徴とする請求項1又は2に記載の分割コア用無方向性電磁鋼板。   The non-oriented electrical steel sheet for a split core according to claim 1 or 2, wherein an annealing temperature of the hot-rolled sheet is higher than 900 ° C. 前記スキンパス圧延前の平均結晶粒径が10〜60μmであることを特徴とする請求項1〜3のいずれか1項に記載の分割コア用無方向性電磁鋼板。   The non-oriented electrical steel sheet for split core according to any one of claims 1 to 3, wherein an average crystal grain size before the skin pass rolling is 10 to 60 µm. 前記スキンパス圧延における圧下率が2〜15%であることを特徴とする請求項1〜4のいずれか1項に記載の分割コア用無方向性電磁鋼板。   The non-oriented electrical steel sheet for split core according to any one of claims 1 to 4, wherein a rolling reduction in the skin pass rolling is 2 to 15%. 前記歪取焼鈍を、770〜850℃で施すことを特徴とする請求項1〜5のいずれか1項に記載の分割コア用無方向性電磁鋼板。   The non-oriented electrical steel sheet for split core according to any one of claims 1 to 5, wherein the strain relief annealing is performed at 770 to 850 ° C.
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