JPH0816258B2 - Clad type non-oriented electrical steel sheet - Google Patents
Clad type non-oriented electrical steel sheetInfo
- Publication number
- JPH0816258B2 JPH0816258B2 JP2298922A JP29892290A JPH0816258B2 JP H0816258 B2 JPH0816258 B2 JP H0816258B2 JP 2298922 A JP2298922 A JP 2298922A JP 29892290 A JP29892290 A JP 29892290A JP H0816258 B2 JPH0816258 B2 JP H0816258B2
- Authority
- JP
- Japan
- Prior art keywords
- steel sheet
- layer
- content
- oriented electrical
- skin layer
- 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 - Fee Related
Links
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F1/00—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties
- H01F1/01—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials
- H01F1/03—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity
- H01F1/12—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of soft-magnetic materials
- H01F1/14—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of soft-magnetic materials metals or alloys
- H01F1/147—Alloys characterised by their composition
- H01F1/14766—Fe-Si based alloys
- H01F1/14775—Fe-Si based alloys in the form of sheets
- H01F1/14783—Fe-Si based alloys in the form of sheets with insulating coating
Landscapes
- Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Chemical & Material Sciences (AREA)
- Dispersion Chemistry (AREA)
- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Pressure Welding/Diffusion-Bonding (AREA)
- Soft Magnetic Materials (AREA)
Description
〔産業上の利用分野〕 この発明は磁気特性、特に鉄損−磁束密度バランスに
優れた無方向性電磁鋼板に関するものである。 〔従来の技術〕 昨今、電気機器の小型、高効率化、省エネルギー化が
進む中で、鉄芯として用いられる無方向性電磁鋼板につ
いても、低鉄損−高磁束密度化の要求が益々増大しつつ
ある。しかしながら、このような低鉄損−高磁束密度化
を実現する上で化学成分上の重大な制約があり、従来よ
り種々の改善がなされてはいるものの、未だ十分な成果
を見ないのが実情である。 すなわち、よく知られるように鉄損、磁束密度をはじ
めとする磁気特性は化学成分、特にSi量に大きく依存す
る。具体的には、Si量の増加に伴い鉄損、磁気密度がと
もに低下し、したがって、低鉄損化実現のため高Si鋼を
用いれば不可避的に磁速密度の低下をきたし、一方、高
磁束密度化のためSiの低下を図れば、同時に鉄損の上昇
を招くことになる。 従来、このような化学成分上の制約は不可避のもので
あると考えられ、このため研究の対象を専ら磁気特性の
二次的な支配因子である粒径や集合組織の改善に限定し
ていた。 〔発明が解決しようとする課題〕 しかしながら、従来のように低鉄損−高磁束密度化を
阻む最大の要因である化学成分上の制約を容認し、二次
的因子の改善に終始した場合には、低鉄損−高磁束密度
化に自ずと限界があることは事実であり、これまでに開
示されたいかなる技術をもってしても、特性上十分な低
鉄損−高磁束密度化が達成されているとは言い難い。 本発明はこのような問題点に鑑み、上述したような化
学成分上の制約条件を打破し、従来にない低鉄損−高磁
束密化が達成された鋼板の提供を目的とし、全く新規な
着想に基づきなされたものである。 〔課題を解決するための手段〕 従来、無方向性電磁鋼板に関しては磁化過程を円滑に
行なわしめるために、換言すれば、磁壁の運動を阻害し
ないために、組織をはじめとする全ての因子はそれを均
一化するという方向で検討がなされてきた。このような
従来の考え方に対し、本発明者らは発想を逆転させ、不
均一化の観点から改めて無方向性電磁鋼板の磁気特性を
検討し直した。その結果、低鉄損−高磁束密度材として
従来の無方向性電磁鋼板とは全く異なるクラッド型の無
方向性電磁鋼板を得るに至った。 すなわち、従来の無方向性電磁鋼板のように全圧にわ
たって単層、同一成分であれば、Si量の増加に伴う鉄
損、磁束密度の同時低下は避けられないが、板厚方向で
表皮層(スキン層)−中央層(コア層)−表皮層(スキ
ン層)の3層からなるクラッド型の電磁鋼板とした場合
には、スキン層とコア層のSi量を変えることで、低鉄損
化は高Si側の層によらしめ、同時に起こる磁束密度の低
下は、元来磁束密度の高い低Si側の層で補うことが可能
なこと、換言すれば、高Si鋼、低Si鋼、両者の利点が活
かされ、且つ欠点が相互に補完される、いわゆる複合効
果が発生することを新たに知見した。また、さらに検討
を重ねた結果、各層の成分、クラッド比を適正化するこ
とにより、スキン層−コア層間の組織形成過程での相互
作用を通じて、上記複合効果から期待される以上の磁気
特性の向上が達成可能であるとの結論を得、本発明を完
成するに至った。 また、無方向性電磁鋼板に要求される特性の一つに打
抜き性がある。一般に打抜き性と言った場合、打抜き金
型の摩耗で評価されるが、磁気特性に影響する要因とし
て、金型により打抜き剪断された鋼板の剪断面の形状が
ある。すなわち、この形状や残留歪によって打抜き後の
磁気特性が劣化する。金型のクリアランスを小さく取る
と、剪断面形状が改善されるが、金型の摩耗が早く起き
るため経済的でなくまた、クリアランスが小さすぎると
鋼板に残留歪を与え、磁気特性を劣化させる。これに対
し、本発明のように鋼板を3層にクラッド化することに
より、剪断面形状が著しく改善され、実際にモーターコ
アやEIコアを製造したときの磁気特性が向上することが
判った。 以上のような知見に基づく本発明の無方向性電磁鋼板
は、厚さ方向でスキン層−コア層−スキン層からなる3
層構造のクラッド型無方向性電磁鋼板であって、スキン
層およびコア層の化学成分が重量%で、C:0.0050%以
下、Si:0.7〜3.4%、Mn:0.1〜1.0%、P:0.15%以下、S:
0.015%以下、Al:0.1〜1.0%、N:0.0050%以下であり、
且つ、スキン層のSi量およびAl量とコア層のSi量および
Al量とが、 〔Si〕+〔Al〕≦3.5%[Field of Industrial Application] The present invention relates to a non-oriented electrical steel sheet having excellent magnetic properties, particularly iron loss-magnetic flux density balance. [Prior Art] In recent years, as electrical equipment has become smaller, more efficient, and more energy efficient, the demand for low iron loss and high magnetic flux density is increasing even for non-oriented electrical steel sheets used as iron cores. It's starting. However, in order to realize such a low iron loss-high magnetic flux density, there are serious restrictions on the chemical composition, and although various improvements have been made from the past, the actual results are still not achieved. Is. That is, as is well known, magnetic properties such as iron loss and magnetic flux density greatly depend on chemical components, especially the amount of Si. Specifically, both the iron loss and the magnetic density decrease with the increase of the Si content. Therefore, if high Si steel is used to achieve the low iron loss, the magnetic velocity density will inevitably decrease. If Si is reduced to increase the magnetic flux density, the iron loss will increase at the same time. Conventionally, such restrictions on chemical components were considered to be unavoidable, and therefore the research target was limited to the improvement of grain size and texture, which are the secondary controlling factors of magnetic properties. . [Problems to be Solved by the Invention] However, in the case of accepting the restriction on the chemical composition which is the largest factor preventing the low iron loss-high magnetic flux density as in the conventional case, and when it is necessary to improve the secondary factor, It is true that there is a limit to the low iron loss-high magnetic flux density, and any of the techniques disclosed thus far has achieved sufficient low iron loss-high magnetic flux density. It is hard to say that In view of the above problems, the present invention aims to provide a steel sheet that overcomes the above-described restrictions on the chemical composition and that achieves an unprecedented low iron loss-high magnetic flux density. It was made based on the idea. [Means for Solving the Problems] Conventionally, for non-oriented electrical steel sheets, in order to smoothly carry out the magnetization process, in other words, in order not to inhibit the motion of the domain wall, all factors including the structure are Studies have been conducted in the direction of making it uniform. With respect to such a conventional idea, the present inventors reversed the idea and reconsidered the magnetic characteristics of the non-oriented electrical steel sheet from the viewpoint of nonuniformity. As a result, a clad type non-oriented electrical steel sheet which is completely different from the conventional non-oriented electrical steel sheet has been obtained as a low iron loss-high magnetic flux density material. That is, like a conventional non-oriented electrical steel sheet, a single layer over the entire pressure, if the same component, iron loss due to the increase of Si content, simultaneous decrease of magnetic flux density is inevitable, but the skin layer in the thickness direction. When a clad type electromagnetic steel sheet consisting of three layers (skin layer) -center layer (core layer) -skin layer (skin layer) is used, low iron loss can be obtained by changing the Si content of the skin layer and the core layer. The higher the Si side layer is, the lowering of the magnetic flux density that occurs at the same time can be supplemented by the low Si side layer having a high magnetic flux density, in other words, the high Si steel, the low Si steel, It was newly found that a so-called combined effect occurs in which the advantages of both are utilized and the drawbacks are complemented with each other. Further, as a result of further studies, by optimizing the components of each layer and the clad ratio, the magnetic properties are improved more than expected from the above composite effect through the interaction in the texture formation process between the skin layer and the core layer. It was concluded that the above can be achieved, and the present invention has been completed. Further, one of the properties required of the non-oriented electrical steel sheet is punchability. Generally speaking, the term "punching property" is evaluated by the wear of the punching die, and the factor affecting the magnetic properties is the shape of the sheared surface of the steel sheet punched and sheared by the die. That is, the magnetic characteristics after punching deteriorate due to this shape and residual strain. If the clearance of the mold is made small, the sheared cross-sectional shape is improved, but this is not economical because the mold wears quickly, and too small clearance gives residual strain to the steel sheet and deteriorates the magnetic properties. On the other hand, it was found that by clad the steel sheet into three layers as in the present invention, the shear cross-section shape was remarkably improved, and the magnetic characteristics when the motor core or EI core was actually manufactured were improved. The non-oriented electrical steel sheet of the present invention based on the above findings comprises a skin layer-core layer-skin layer in the thickness direction.
A clad type non-oriented electrical steel sheet having a layered structure, wherein the chemical composition of the skin layer and the core layer is% by weight, C: 0.0050% or less, Si: 0.7 to 3.4%, Mn: 0.1 to 1.0%, P: 0.15 % Or less, S:
0.015% or less, Al: 0.1 to 1.0%, N: 0.0050% or less,
Also, the Si content and Al content of the skin layer and the Si content of the core layer and
Al amount is [Si] + [Al] ≦ 3.5%
【Si】+[Si] +
【Al】≧1.7% (〔Si〕+〔Al〕)−([Al] ≧ 1.7% ([Si] + [Al])-(
【Si】+[Si] +
【Al】)≧0.5% 但し、 〔Si〕:スキン層のSi含有量(重量%) 〔Al〕:スキン層のAl含有量(重量%)[Al]) ≧ 0.5% where [Si]: Si content of the skin layer (wt%) [Al]: Al content of the skin layer (wt%)
【Si】:コア層のSi含有量(重量%)[Si]: Si content of the core layer (% by weight)
第1表に示す鋼A〜Gを用い、第2表に示すクラッド
材スラブを作製した。また、比較材として、各クラッド
材のスキン層、コア層の成分とクラッド比から、クラッ
ド材相当の成分をもつ通常の単層材(相当成分単層材)
の成分を算出し、第1表に示す鋼H〜Zのスラブを得
た。 これらのスラブを第2表の条件で仕上板厚2mmまで熱
間圧延し、次いで熱延板焼鈍(一部はこれを省略)、酸
洗の後、板厚0.5mmまで冷間圧延した後、仕上焼鈍を施
して、所定のクラッド材電磁鋼板および相当成分単層材
電磁鋼板を得た。 第3表は、リング試料(内径33φ−外径45φ)にて両
者の磁気特性を測定した結果であるが、本発明材(No1
〜15)の磁気特性は相当成分単層材に比べて磁束密度B
50で0.02T以上高磁束密度化(ΔB50≧0.02T)、鉄損W
15/50で0.25w/kg以上低鉄損化(ΔW15/50≦−0.25w/k
g)しており、本発明によるクラッド材電磁鋼板が極め
て優れた磁束密度−鉄損バランスを持っていることが判
る。 これに対し、比較材(No.16〜19)は、ΔB50:−0.013
〜0.008T、ΔW15/50:−0.12〜−0.05w/kgであり、そ
の磁気特性はいずれも相当成分単層材と磁束密度B50で
同等かやや低く、鉄損W15/50でやや低い程度であり、
本発明範囲外のクラッド材電磁鋼板では優れた磁束密度
−鉄損バランスが得られないことが判る。 〔発明の効果〕 以上述べたように、本発明の無方向性電磁鋼板は、こ
れまで実現不可能であった低鉄損および高磁束密度の両
者を同時に具備しており、しかもこれを従来プロセスに
よって得ることができるため、工業的な価値は非常に大
きく、特に、近年の電気機器における小型化、高効率
化、省エネルギー化等の要請に応えることができる極め
て有効な発明である。Using the steels A to G shown in Table 1, the clad material slabs shown in Table 2 were produced. Also, as a comparative material, an ordinary single-layer material having a component equivalent to the clad material from the components of the skin layer and core layer of each clad material and the clad ratio (equivalent component single-layer material)
The components were calculated to obtain the slabs of Steels H to Z shown in Table 1. These slabs were hot-rolled under the conditions shown in Table 2 to a finished sheet thickness of 2 mm, then hot-rolled sheet annealed (some parts are omitted), pickled, and then cold-rolled to a sheet thickness of 0.5 mm. Finishing annealing was performed to obtain a predetermined clad material electromagnetic steel sheet and equivalent component single-layer electromagnetic steel sheet. Table 3 shows the results of measuring the magnetic properties of both of the ring samples (inner diameter 33φ-outer diameter 45φ).
The magnetic properties of 15 to 15) are equivalent to the magnetic flux density B compared to the single layer material of the equivalent component.
0.02 T or more high magnetic flux density at 50 (ΔB 50 ≧ 0.02T), the iron loss W
0.25 w / kg or more 15/50 reduce iron loss (ΔW 15/50 ≦ -0.25w / k
g), it can be seen that the clad electromagnetic steel sheet according to the present invention has an extremely excellent magnetic flux density-iron loss balance. On the other hand, the comparative material (No. 16 to 19) has ΔB 50 : -0.013
~ 0.008T, ΔW 15/50 : -0.12 to -0.05w / kg, all of which have magnetic properties equivalent to or slightly lower than the equivalent component single layer material with magnetic flux density B 50 , and iron loss W 15/50 somewhat. Low degree,
It can be seen that an excellent magnetic flux density-iron loss balance cannot be obtained with the clad electromagnetic steel sheet outside the scope of the present invention. [Advantages of the Invention] As described above, the non-oriented electrical steel sheet of the present invention has both low iron loss and high magnetic flux density, which have not been realized so far, at the same time. Since it can be obtained by the method, it has a great industrial value, and in particular, it is an extremely effective invention that can meet the recent demands for downsizing, high efficiency, energy saving, etc. in electric devices.
第1図はクラッド材の構成とクラッド比を表した模式図
である。第2図はクラッド材の磁束密度に及ぼすスキン
層およびコア層のSi+Al量の影響とその限定範囲を示し
たグラフである。第3図はクラッド材の鉄損に及ぼすス
キン層およびコア層のSi+Al量の影響とその限定範囲を
示したグラフである。第4図はスキン層、コア層のSi+
Alに関する本発明の限定範囲を示したグラフである。第
5図(a)、(b)および第6図(a)、(b)は、ク
ラッド材の磁気特性に及ぼすクラッド比の影響とその限
定範囲を示したグラフである。FIG. 1 is a schematic diagram showing the structure of the clad material and the clad ratio. FIG. 2 is a graph showing the influence of the amount of Si + Al in the skin layer and the core layer on the magnetic flux density of the clad material and its limiting range. FIG. 3 is a graph showing the influence of the amount of Si + Al in the skin layer and the core layer on the iron loss of the clad material and its limiting range. Fig. 4 shows the skin layer and core layer of Si +
3 is a graph showing a limited range of the present invention regarding Al. FIGS. 5 (a) and 5 (b) and FIGS. 6 (a) and 6 (b) are graphs showing the influence of the clad ratio on the magnetic properties of the clad material and its limited range.
Claims (1)
らなる3層構造のクラッド型無方向性電磁鋼板であっ
て、スキン層およびコア層の化学成分が重量%で、C:0.
0050%以下、Si:0.7〜3.4%、Mn:0.1〜1.0%、P:0.15%
以下、S:0.015%以下、Al:0.1〜1.0%、N:0.0050%以下
であり、且つ、スキン層のSi量およびAl量とコア層のSi
量およびAl量とが、 〔Si〕+〔Al〕≦3.5% 【Si】+【Al】≧1.7% (〔Si〕+〔Al〕)−(【Si】+【Al】)≧0.5% 但し、 〔Si〕:スキン層のSi含有量(重量%) 〔Al〕:スキン層のAl含有量(重量%) 【Si】:コア層のSi含有量(重量%) 【Al】:コア層のAl含有量(重量%) を満足し、残部Feおよび不可避的不純物からなり、且
つ、クラッド比R(%)が、 5%≦R≦30% 但し、 R(%)=(〔スキン層片側分の板厚〕/〔全板厚〕)×100 を満足することを特徴とするクラッド型無方向性電磁鋼
板。1. A clad type non-oriented electrical steel sheet having a three-layer structure consisting of a skin layer, a core layer and a skin layer in the thickness direction, wherein the chemical composition of the skin layer and the core layer is% by weight, and C: 0. .
0050% or less, Si: 0.7 to 3.4%, Mn: 0.1 to 1.0%, P: 0.15%
Below, S: 0.015% or less, Al: 0.1 to 1.0%, N: 0.0050% or less, and the Si content and Al content of the skin layer and the Si content of the core layer
Amount and Al amount are [Si] + [Al] ≦ 3.5% [Si] + [Al] ≧ 1.7% ([Si] + [Al]) − ([Si] + [Al]) ≧ 0.5% , [Si]: Si content of the skin layer (wt%) [Al]: Al content of the skin layer (wt%) [Si]: Si content of the core layer (wt%) [Al]: Core layer Al content (wt%) is satisfied, the balance is Fe and unavoidable impurities, and the clad ratio R (%) is 5% ≤ R ≤ 30%, where R (%) = ([skin layer Sheet thickness] / [total sheet thickness]) × 100. A clad type non-oriented electrical steel sheet.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2298922A JPH0816258B2 (en) | 1990-11-06 | 1990-11-06 | Clad type non-oriented electrical steel sheet |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2298922A JPH0816258B2 (en) | 1990-11-06 | 1990-11-06 | Clad type non-oriented electrical steel sheet |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH04173940A JPH04173940A (en) | 1992-06-22 |
| JPH0816258B2 true JPH0816258B2 (en) | 1996-02-21 |
Family
ID=17865922
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP2298922A Expired - Fee Related JPH0816258B2 (en) | 1990-11-06 | 1990-11-06 | Clad type non-oriented electrical steel sheet |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0816258B2 (en) |
Families Citing this family (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP5272688B2 (en) * | 2008-12-02 | 2013-08-28 | Jfeスチール株式会社 | Clad type electrical steel sheet |
| JP6464750B2 (en) * | 2015-01-06 | 2019-02-06 | 新日鐵住金株式会社 | Soft magnetic Fe-based metal plate having a plurality of crystal orientation layers and manufacturing method thereof |
| JP6464753B2 (en) * | 2015-01-09 | 2019-02-06 | 新日鐵住金株式会社 | Soft magnetic Fe-based metal plate having a plurality of crystal orientation layers and manufacturing method thereof |
-
1990
- 1990-11-06 JP JP2298922A patent/JPH0816258B2/en not_active Expired - Fee Related
Also Published As
| Publication number | Publication date |
|---|---|
| JPH04173940A (en) | 1992-06-22 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| KR20190093615A (en) | Non-oriented electrical steel sheet and manufacturing method thereof | |
| KR20200020013A (en) | Non-oriented electromagnetic steel sheet and manufacturing method of same | |
| JP5671872B2 (en) | Non-oriented electrical steel sheet and manufacturing method thereof | |
| JP4319889B2 (en) | Non-oriented electrical steel sheet with excellent all-round magnetic properties and method for producing the same | |
| JP2008127612A (en) | Non-oriented electrical steel sheet for split core | |
| KR20200093037A (en) | Double-layered electrical steel sheet | |
| JP2910508B2 (en) | Non-oriented electrical steel sheet for high frequency with excellent iron loss characteristics | |
| JP3243099B2 (en) | Manufacturing method of laminated electromagnetic steel sheet | |
| JPH0888114A (en) | Non-oriented electrical steel sheet manufacturing method | |
| JPH0816258B2 (en) | Clad type non-oriented electrical steel sheet | |
| JP4360349B2 (en) | Soft magnetic steel bar | |
| JP2022509670A (en) | Non-oriented electrical steel sheet and its manufacturing method | |
| JP4622162B2 (en) | Non-oriented electrical steel sheet | |
| JPH0860311A (en) | Thin non-oriented electrical steel sheet with low iron loss and method of manufacturing the same | |
| JP2019183231A (en) | Nonoriented electromagnetic steel sheet, stater core, rotor core, and manufacturing method therefor | |
| EP2639326A1 (en) | Wire rod and steel wire having superior magnetic characteristics, and method for manufacturing same | |
| JP2917776B2 (en) | Non-oriented electrical steel sheet for high frequency | |
| JP7375985B1 (en) | Non-oriented electrical steel sheet | |
| JP7388597B1 (en) | Non-oriented electrical steel sheet | |
| JP2003034821A (en) | Method for producing grain-oriented electrical steel sheet having no magnetic undercoat and high magnetic flux density | |
| JP2004363512A (en) | Electromagnetic steel wire with excellent workability and high-frequency magnetic properties | |
| JPH0726154B2 (en) | Manufacturing method of low iron loss non-oriented electrical steel sheet | |
| JP2639290B2 (en) | Manufacturing method of non-oriented electrical steel sheet for rotating machines | |
| JPH0860247A (en) | Manufacturing method of non-oriented electrical steel sheet with excellent magnetic properties | |
| JPH08104923A (en) | Non-oriented electrical steel sheet manufacturing method |
Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| FPAY | Renewal fee payment (event date is renewal date of database) |
Free format text: PAYMENT UNTIL: 20080221 Year of fee payment: 12 |
|
| FPAY | Renewal fee payment (event date is renewal date of database) |
Free format text: PAYMENT UNTIL: 20090221 Year of fee payment: 13 |
|
| FPAY | Renewal fee payment (event date is renewal date of database) |
Free format text: PAYMENT UNTIL: 20100221 Year of fee payment: 14 |
|
| LAPS | Cancellation because of no payment of annual fees |