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JPH0814016B2 - High frequency non-oriented electrical steel sheet - Google Patents
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JPH0814016B2 - High frequency non-oriented electrical steel sheet - Google Patents

High frequency non-oriented electrical steel sheet

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Publication number
JPH0814016B2
JPH0814016B2 JP2015755A JP1575590A JPH0814016B2 JP H0814016 B2 JPH0814016 B2 JP H0814016B2 JP 2015755 A JP2015755 A JP 2015755A JP 1575590 A JP1575590 A JP 1575590A JP H0814016 B2 JPH0814016 B2 JP H0814016B2
Authority
JP
Japan
Prior art keywords
grain size
crystal grain
less
steel sheet
electrical steel
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Lifetime
Application number
JP2015755A
Other languages
Japanese (ja)
Other versions
JPH03223445A (en
Inventor
高英 島津
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Nippon Steel Corp
Original Assignee
Nippon Steel Corp
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Filing date
Publication date
Application filed by Nippon Steel Corp filed Critical Nippon Steel Corp
Priority to JP2015755A priority Critical patent/JPH0814016B2/en
Publication of JPH03223445A publication Critical patent/JPH03223445A/en
Publication of JPH0814016B2 publication Critical patent/JPH0814016B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、モータ及び小型トランス用として一般に用
いられる電気製品の素材、特に周波数が高い領域、400H
z以上での使用に有効な無方向性電磁鋼板に関するもの
である。
DETAILED DESCRIPTION OF THE INVENTION [Industrial field of application] The present invention relates to a material for electric products generally used for motors and small transformers, especially in a high frequency region, 400H.
The present invention relates to a non-oriented electrical steel sheet which is effective for use at z or higher.

利用分野としては例えば、掃除機用モータ、インテリ
ジェント・ビル用の蛍光灯などの小型トランス、各種モ
ータ、飛行機・機内用のモータや照明機器、更に、ロボ
ット制御用モータなどがある。
The fields of application include, for example, motors for vacuum cleaners, small transformers such as fluorescent lights for intelligent buildings, various motors, motors and lighting equipment for airplanes and cabins, and robot control motors.

〔従来の技術〕[Conventional technology]

この利用分野は、最近急速に注目され始めた分野で、
電気機器のエネルギー効率向上、精密モータの厳密な位
置制御などに有効なものであるが、周波数としては400H
z以上が必要となってきた。このため、従来の電磁鋼板
に使用される所謂、商用周波数50〜60Hzと違い、400Hz
以上の例えば700Hzに着目して研究しなければならない
が、未だこの領域に最適な鋼板は製造・販売されていな
い。例えば、無方向性電磁鋼板の最高級品としては、Si
3%,Al1%程度で板厚が0.35mm、結晶粒径が150μm程度
のものが市販されている。これは50Hzで優れた磁気特性
を有するが、高周波では満足すべき特性が得られていな
い。
This field of application is a field that has recently begun to receive attention rapidly,
It is effective for improving the energy efficiency of electrical equipment and strict position control of precision motors, but with a frequency of 400H
z or more is needed. Therefore, unlike the so-called commercial frequency of 50 to 60 Hz used for conventional electrical steel sheets, 400 Hz
We have to focus on the above 700 Hz, for example, but we have not yet manufactured and sold the optimum steel plate in this area. For example, the highest grade non-oriented electrical steel sheet is Si
A 3%, 1% Al plate having a thickness of 0.35 mm and a crystal grain size of about 150 μm is commercially available. Although it has excellent magnetic properties at 50 Hz, it does not have satisfactory properties at high frequencies.

従来の考え方として、周波数が高くなれば、トータル
鉄損の内でうず電流損が増加することが一般に知られて
いた。このうず電流損Weは、古典的うず電流損の式とし
ての公知の以下(1)式で計算されるとされてきた。
As a conventional idea, it is generally known that the eddy current loss in the total iron loss increases as the frequency increases. It has been said that this eddy current loss W e is calculated by the following known equation (1) as a classical eddy current loss equation.

We=0.1645B2f2d2/ρD ここに、B:最大磁束密度(T) f:周波数(Hz,サイクル/sec) d:板厚(mm) ρ:固有抵抗(μΩ−cm) D:密度(g/cm3) つまり、うず電流損を下げるためには、設計の磁束密
度Bを下げ、板厚dを薄くし、固有抵抗ρを上げるため
にSi量などを増やすなどの方法があることが分かってい
る。
Here W e = 0.1645B 2 f 2 d 2 / ρD, B: maximum magnetic flux density (T) f: Frequency (Hz, cycles / sec) d: thickness (mm) ρ: specific resistance (μΩ-cm) D : Density (g / cm 3 ) In other words, in order to reduce the eddy current loss, there are methods such as decreasing the design magnetic flux density B, reducing the plate thickness d, and increasing the Si content etc. to increase the specific resistance ρ. I know there is.

従って、この考え方で行けば、例えば700Hz、0.5Tで
の鉄損W5/700を12W/kg以下にしようとすれば、Si6.5%
とし板厚を0.15mmとするような手段がある。しかしなが
ら、この手段は、製造側での冷延破断や客先での打抜き
時の割れが問題で、工業的には無理があった。更には、
700Hz、500A/mの磁化力での磁束密度B5/700が0.05T程
度しか得られない品質上の重大な問題があった。一般の
電気機器としては、磁化特性として磁束密度は1.0T程度
は必要で、鉄損も同時に良好なものが要求される。
Therefore, if this approach is taken, for example, if the iron loss W 5/700 at 700 Hz and 0.5T is to be 12 W / kg or less, Si6.5%
There is a means to make the plate thickness 0.15 mm. However, this method has a problem of cold rolling rupture on the manufacturing side and cracking at the customer's punching, and was industrially impossible. Furthermore,
There was a serious quality problem that the magnetic flux density B 5/700 at a magnetizing force of 700 Hz and 500 A / m was only about 0.05T . For general electric equipment, a magnetic flux density of about 1.0 T is required as a magnetization characteristic, and iron loss is also required to be good at the same time.

〔発明が解決しようとする課題〕[Problems to be Solved by the Invention]

本発明は上記の点に鑑み、400Hz以上での高周波領域
での鉄損と磁束密度が同時に優れている電磁鋼板を、工
業的な方法により提供することを目的とする。
In view of the above points, an object of the present invention is to provide an electrical steel sheet having excellent iron loss and magnetic flux density in a high frequency region of 400 Hz or higher at the same time by an industrial method.

〔課題を解決するための手段〕[Means for solving the problem]

本発明は、SiとAlの合計量が2.0〜4.0%、C0.005%以
下、Mn1%以下、S0.01%以下、N0.01%以下で、残部が
鉄と不可避的不純物よりなる無方向性電磁鋼板であっ
て、板厚0.10〜0.25mmで、該鋼板の平均結晶粒径が5〜
60μmである鉄損W5/700が12W/kg以下、磁束密度B
5/700が1.0T以上の優れた磁気特性を有する周波数400Hz
以上で使用される高周波用無方向性電磁鋼板を要旨とす
るものである。
The present invention, the total amount of Si and Al is 2.0 ~ 4.0%, C0.005% or less, Mn1% or less, S0.01% or less, N0.01% or less, the balance is iron and unavoidable impurities Magnetic steel sheet having a plate thickness of 0.10 to 0.25 mm and an average crystal grain size of 5 to 5
Iron loss W 5/700 of 60 μm is 12 W / kg or less, magnetic flux density B
Frequency 400Hz with excellent magnetic characteristics of 5/700 of 1.0T or more
The gist is the high-frequency non-oriented electrical steel sheet used above.

SiとAlは鋼板の固有抵抗を増加させるために有効で、
安価であるからよく用いられる成分である。周知の如く
Si量とAl量の固有抵抗に及ぼす効果はほぼ等価なので、
Si+Al量が少ないと、固有抵抗が十分でないため鉄損が
劣化する。一方、周知のようにSiとAlは原子量がほぼ等
しく単位重量当たりのFe原子数を減らす作用が等価であ
って、Si+Alが多すぎると強磁性のFeが少なくなるた
め、磁束密度が劣化する。
Si and Al are effective for increasing the specific resistance of the steel sheet,
It is a commonly used ingredient because it is inexpensive. As is well known
Since the effects of Si content and Al content on the specific resistance are almost equivalent,
When the amount of Si + Al is small, the iron resistance is deteriorated because the specific resistance is not sufficient. On the other hand, as is well known, Si and Al have almost the same atomic weight and have an equivalent effect of reducing the number of Fe atoms per unit weight. If Si + Al is too large, the amount of ferromagnetic Fe decreases, and the magnetic flux density deteriorates.

また、板厚はうず電流損を減少させるために効果が大
きく、0.25mm超では鉄損が不十分で、また0.10mm未満で
は、圧延能力や破断等の問題で工業的に製造が難しい。
Further, the plate thickness has a great effect to reduce the eddy current loss. If it exceeds 0.25 mm, the iron loss is insufficient, and if it is less than 0.10 mm, it is industrially difficult to manufacture due to problems such as rolling ability and breakage.

結晶粒径の効果については、従来の古典的うず電流損
の計算式からは予測されない、本発明の特徴であるが、
700Hz程度の磁気特性には非常に重要な意味を持つ。す
なわち、高周波での磁気特性の鉄損と磁束密度を同時に
満足させる、例えば、鉄損W5/700を12W/kg以下、磁束
密度B5/700を1.0T以上にしようとすれば、結晶粒径の
効果を利用しなければならない。
The effect of the crystal grain size is a characteristic of the present invention, which is not predicted from the conventional classical eddy current loss calculation formula,
It has a very important meaning for the magnetic characteristics around 700 Hz. That is, if the iron loss and the magnetic flux density of the magnetic characteristics at a high frequency are simultaneously satisfied, for example, if the iron loss W 5/700 is 12 W / kg or less and the magnetic flux density B 5/700 is 1.0 T or more, the crystal grains are We must take advantage of the diameter effect.

本発明の構成要件の限定理由について、以下に詳しく
説明する。
The reasons for limiting the constituent features of the present invention will be described in detail below.

第1図,第2図は、0.20mm厚の無方向性電磁鋼板にお
ける製品での結晶粒径の効果を調べたものである。第1
図に鉄損、第2図に磁束密度に及ぼす影響を示す。結晶
粒径のサイズは、最終焼鈍の温度でコントロールした。
図に示す如く、Si+Al量が1.5%ではB5/700は良好だ
が、W5/700が12W/kgを切る結晶粒径の領域が、狭く限
定される。また、Si+Al量が本発明範囲の3%のもの
は、W5/700とB5/700がともに結晶粒径が5〜60μmの
広い範囲で満足される。更に、Si+Al量が4.5%ではW
5/700が良好ではあるが、B5/700が1.0T以上のものが少
ししか得られない。なお、結晶粒径が20μm以下で磁性
が劣化するのは、内部応力のためであろう。結晶粒径が
5μm未満では未再結晶粒が残るので磁性が著しく落ち
る。また、40μm以上でも磁性劣化が認められるが、こ
れは容易磁化の{100}が減少するためであろう。
1 and 2 show the effect of the crystal grain size on the product in a 0.20 mm thick non-oriented electrical steel sheet. First
Fig. 2 shows the iron loss, and Fig. 2 shows the effect on the magnetic flux density. The size of the crystal grain size was controlled by the temperature of the final annealing.
As shown in the figure, B 5/700 is good when the amount of Si + Al is 1.5%, but the region of the crystal grain size where W 5/700 is less than 12 W / kg is narrowly limited. Further, if the amount of Si + Al is 3% within the range of the present invention, both W 5/700 and B 5/700 are satisfied in a wide range of crystal grain sizes of 5 to 60 μm. Furthermore, when Si + Al content is 4.5%, W
5/700 is good, but B5 / 700 with a value of 1.0T or more can be obtained only slightly. The reason why the magnetism deteriorates when the crystal grain size is 20 μm or less is probably due to internal stress. If the crystal grain size is less than 5 μm, unrecrystallized grains remain, so that the magnetism remarkably deteriorates. Also, magnetic deterioration is recognized at 40 μm or more, which is probably because {100} of easy magnetization is reduced.

従って、W5/700とB5/700がともに満足されるSi+Al
量は、2.0〜4.0%であり、結晶粒径は5〜60μmであ
る。
Therefore, Si + Al satisfying both W 5/700 and B 5/700
The amount is 2.0 to 4.0%, and the crystal grain size is 5 to 60 μm.

なお、従来、無方向性電磁鋼板の高級品グレードの結
晶粒径は100〜200μmであった。これは、50〜60Hzの商
用周波数での鉄損が、この結晶粒径で最良となるためで
ある。
Conventionally, the crystal grain size of a high grade non-oriented electrical steel sheet was 100 to 200 μm. This is because the iron loss at the commercial frequency of 50 to 60 Hz is the best at this grain size.

測定法に関してであるが、結晶粒径の測定は腐食面に
現れた結晶粒の数を切断法でカウントし求めた。磁気測
定は、JIS C 2550の可聴周波鉄損試験により、試験片サ
イズは30mm幅×300mm長さとし、半分は圧延方向、半分
は圧延方向と直角の方向を長さ方向とした。
Regarding the measurement method, the crystal grain size was measured by counting the number of crystal grains appearing on the corroded surface by the cutting method. The magnetic measurement was performed by JIS C 2550 audio iron loss test, and the size of the test piece was 30 mm width × 300 mm length, half was the rolling direction, and half was the direction perpendicular to the rolling direction.

次いで、板厚の効果について第3図、第4図に示す。
第3図の素材はSi+Al量2.0%のもので、板厚を0.1〜0.
5mmに変更し結晶粒径を3種に調整して調べた。第3図
に示す如く、結晶粒径が本発明範囲の50〜55μmのもの
は、板厚が0.1〜0.25mmの範囲で、鉄損W5/700が12W/kg
を安定して切ることが出来る。しかしながら、90μm以
上の結晶粒のものは、12W/kgを安定して切ることが出来
ない。
Next, the effect of the plate thickness is shown in FIGS. 3 and 4.
The material shown in Fig. 3 has a Si + Al content of 2.0% and a plate thickness of 0.1-0.
The size was changed to 5 mm and the crystal grain size was adjusted to 3 types. As shown in FIG. 3, when the crystal grain size is 50 to 55 μm in the range of the present invention, the iron loss W 5/700 is 12 W / kg in the plate thickness range of 0.1 to 0.25 mm.
Can be cut stably. However, a crystal grain of 90 μm or more cannot stably cut 12 W / kg.

第4図は、Si+Al量が4.0%のもので、磁束密度につ
いても同様に、B5/700が1.0T以上が板厚0.1〜0.25mmの
範囲で安定して得られるものは、結晶粒径が本発明の50
〜55μm材のみである。
Fig. 4 shows that the amount of Si + Al is 4.0%, and similarly for the magnetic flux density, B 5/700 of 1.0T or more can be stably obtained in the plate thickness range of 0.1 to 0.25 mm. 50 of the present invention
Only ~ 55μm material.

第5図は、鉄損W5が最良値となる結晶粒径についての
グラフで、Si+Alを3.0%、板厚0.15mmとして調べた。
図で見る如く、周波数が上がるにつれて最良となる結晶
粒径は小さくなる。本発明の対象である400Hz以上では6
0μm以下の粒径が適当である。また、第6図には、同
様にして1.0Tの透磁率μ10が最良値となる結晶粒径につ
いてプロットした。高周波になるにつれて、結晶粒径を
小さくする必要があることが分かる。
FIG. 5 is a graph showing the crystal grain size at which the iron loss W 5 has the best value, which was examined with Si + Al of 3.0% and a plate thickness of 0.15 mm.
As can be seen from the figure, the best crystal grain size becomes smaller as the frequency increases. 6 above 400 Hz, which is the subject of the present invention
A particle size of 0 μm or less is suitable. Further, in FIG. 6, similarly, the crystal grain size at which the magnetic permeability μ 10 of 1.0 T is the best value is plotted. It can be seen that it is necessary to reduce the crystal grain size as the frequency becomes higher.

次に、結晶粒径の効果のメカニズムについて述べる。
従来の周波数50Hzでは、150μm程度の鉄損が最小であ
る。しかし、高周波ではうず電流が占める割合が大きく
なり、鋼板内部では表皮効果によって誘起される磁束は
小さくなる。本発明者は400Hz以上での周波数では結晶
粒径が比較的小さい方が、透磁率が大きいことを見出し
たが、透磁率が大きいと表皮効果が強く効き、うず電流
損が減少する。このため、400Hz以上、とくに700Hzでは
結晶粒径が5〜60μmで鉄損が良好となったものであ
る。
Next, the mechanism of the effect of the crystal grain size will be described.
At the conventional frequency of 50 Hz, the iron loss of about 150 μm is the minimum. However, at high frequencies, the eddy current occupies a large proportion, and inside the steel sheet, the magnetic flux induced by the skin effect becomes small. The present inventors have found that at frequencies above 400 Hz, the smaller the crystal grain size, the higher the magnetic permeability. However, when the magnetic permeability is high, the skin effect is strong and the eddy current loss is reduced. Therefore, at 400 Hz or higher, especially at 700 Hz, the iron loss was good when the crystal grain size was 5 to 60 μm.

製造方法は、まず溶鋼で成分調整する。SiとAlの合計
重量%は2.0〜4.0%とする。Cは0.005%以下であれ
ば、磁気時効の問題はなく、また後で脱炭する必要もな
いが、0.005%を越えると、それ以下になるように後で
脱炭焼鈍を行うことを要する。Mnは無方向性電磁鋼板に
おける通常の範囲で、即ち1%以下とする。SとNは磁
気特性を劣化させる元素であり、通常の無方向性電磁鋼
板と同様に、それぞれ0.01%以下に制限する。この溶鋼
を鋳造し通常の熱間圧延を行う。次いで、熱延板焼鈍を
製品の集合組織を改善する目的で実施しても良いが、必
須ではない。更に、中間焼鈍をはさむ1〜2回の冷延を
行い板厚0.10〜0.25mmとした後、最終1次再結晶焼鈍を
実施する。この再結晶焼鈍は結晶粒径を5〜60μmとす
るべく厳密に制御されなければならない。この時の温度
は、粒成長抑制元素のありなしによって異なるが、650
〜900℃が適当である。
In the manufacturing method, first, the composition of molten steel is adjusted. The total weight% of Si and Al is 2.0 to 4.0%. If C is 0.005% or less, there is no problem of magnetic aging and there is no need to decarburize later, but if it exceeds 0.005%, it is necessary to perform decarburization annealing later so as to be less than that. Mn is in the normal range for non-oriented electrical steel sheets, that is, 1% or less. S and N are elements that deteriorate the magnetic properties, and are limited to 0.01% or less, respectively, as in a normal non-oriented electrical steel sheet. This molten steel is cast and ordinary hot rolling is performed. Next, hot-rolled sheet annealing may be performed for the purpose of improving the texture of the product, but it is not essential. Further, cold rolling is performed once or twice with an intermediate anneal to obtain a plate thickness of 0.10 to 0.25 mm, and then a final primary recrystallization anneal is performed. This recrystallization annealing must be strictly controlled so that the crystal grain size is 5 to 60 μm. The temperature at this time depends on the presence or absence of the grain growth suppressing element, but is 650
A temperature of ~ 900 ° C is suitable.

なお、鋳造は例えば、双ロールによる急冷凝固で行
い、熱延を省略することも可能である。
The casting may be performed by rapid solidification with twin rolls, and the hot rolling may be omitted.

〔実施例〕〔Example〕

以下に、本発明の実施例について具体的に説明する。 Examples of the present invention will be specifically described below.

SiとAlの重量%を第1表に示す如く調整し、C0.002
%,Mn0.30%,S0.006%,N0.005%とした溶鋼を連続鋳造
してスラブとなし、熱延により2.5mm厚の熱延板にし
た。これを冷延し、次いで連続焼鈍し絶縁皮膜を塗布・
焼付して、第1表に示す板厚の電磁鋼板を製造した。こ
の時、均熱時間を30秒とし、温度を650〜950℃に変更し
て第1表の結晶粒径を得た。製品は700Hzの高周波で磁
気測定に供した。
Adjust the weight% of Si and Al as shown in Table 1, and add C0.002
%, Mn 0.30%, S0.006%, N0.005% molten steel was continuously cast into a slab and hot rolled into a 2.5 mm thick hot rolled sheet. This is cold rolled and then continuously annealed to apply an insulating film.
Baking was carried out to manufacture an electromagnetic steel plate having a plate thickness shown in Table 1. At this time, the soaking time was set to 30 seconds and the temperature was changed to 650 to 950 ° C. to obtain the crystal grain size in Table 1. The product was subjected to magnetic measurement at a high frequency of 700 Hz.

実験No.1〜4は板厚と結晶粒径をほぼ同じにして、成
分の影響を見たもので、実験No.1と4のそれぞれ成分の
下限と上限を外れた鋼板は、鉄損と磁束密度が本発明の
範囲外になる。この現象は特に、板厚が上限の0.25mm
で、結晶粒径も本発明の下限に近い厳しい場合に出る。
In Experiment Nos. 1 to 4, the plate thickness and the crystal grain size were made almost the same, and the effect of the components was observed. Steel plates that deviated from the lower and upper limits of the components of Experiment Nos. 1 and 4 respectively showed iron loss. The magnetic flux density falls outside the range of the present invention. This phenomenon is especially 0.25 mm, which is the upper limit of the plate thickness.
Then, the crystal grain size comes out in a severe case close to the lower limit of the present invention.

実験No.5〜7は板厚の効果を調べたもので、Si+Alを
2.1%とし、結晶粒径を57〜59μm程度としたものであ
るが、実験No.5の板厚0.26mmで鉄損が本発明範囲から外
れた。実験No.6,7の本発明範囲の板厚のものは鉄損、磁
束密度ともに満足される特性値である。
Experiment Nos. 5 to 7 are for examining the effect of the plate thickness.
Although it was 2.1% and the crystal grain size was about 57 to 59 μm, the iron loss was out of the range of the present invention at the plate thickness of 0.26 mm in Experiment No. 5. Experiment Nos. 6 and 7 having plate thicknesses within the range of the present invention have characteristic values satisfying both iron loss and magnetic flux density.

実験No.8〜10も板厚の効果を見たものであるが、板厚
0.26mmで磁束密度が本発明範囲から外れる。これはSi+
Al量が4.0%と上限の場合の傾向である。
Experiment Nos. 8 to 10 also show the effect of the plate thickness.
At 0.26 mm, the magnetic flux density is out of the range of the present invention. This is Si +
This is a tendency when the Al amount is 4.0%, which is the upper limit.

実験No.11〜16では結晶粒径の影響を調べた。実験No.
11の最終焼鈍温度650℃では、再結晶を完了しておら
ず、未再結晶部分が存在していたが、磁気特性が非常に
悪い。また、結晶粒径が7〜58μmの本発明範囲内の実
験No.12〜14は、良好な特性値を示した。60μmを越え
た実験No.15,16は鉄損が本発明範囲から外れている。
In Experiment Nos. 11 to 16, the influence of the crystal grain size was investigated. Experiment No.
At the final annealing temperature of 650 ° C of No. 11, recrystallization was not completed and there were unrecrystallized parts, but the magnetic properties were very poor. In addition, Experiment Nos. 12 to 14 having a crystal grain size of 7 to 58 μm within the range of the present invention showed good characteristic values. In Experiment Nos. 15 and 16 in which the thickness exceeds 60 μm, the iron loss is out of the range of the present invention.

これらの実験事実から、W5/700とB5/700がそれぞれ
12W/kg以下、1.0T以上の磁気特性を確保することのでき
るSiとAlの合計量の範囲は2.0〜4.0%で、板厚の範囲は
0.10〜0.25mmで、なお且つ、結晶粒径も本発明範囲でな
ければならないことが分かる。
From these experimental facts, W 5/700 and B 5/700 are respectively
The total amount of Si and Al that can secure magnetic properties of 12 W / kg or less and 1.0 T or more is 2.0 to 4.0%, and the thickness range is
It can be seen that the grain size must be 0.10 to 0.25 mm and the crystal grain size must be within the range of the present invention.

〔発明の効果〕 以上の如く本発明によれば、400Hz以上の高周波で優
れた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。
[Effects of the Invention] As described above, according to the present invention, it is possible to provide a non-oriented electrical steel sheet having excellent magnetic properties at a high frequency of 400 Hz or higher.

【図面の簡単な説明】[Brief description of drawings]

第1図は結晶粒径と成分が鉄損に及ぼす影響を示したも
のである。 第2図は結晶粒径と成分が磁束密度に及ぼす影響を示し
たものである。 第3図は板厚と結晶粒径が鉄損に及ぼす影響を示したも
のである。 第4図は板厚と結晶粒径が磁束密度に及ぼす影響を示し
たものである。 第5図は周波数毎の鉄損の最良値を与える結晶粒径を示
したものである。 第6図は周波数毎の透磁率の最良値を与える結晶粒径を
示したものである。
Figure 1 shows the effect of grain size and composition on iron loss. FIG. 2 shows the influence of the crystal grain size and composition on the magnetic flux density. FIG. 3 shows the influence of the plate thickness and the crystal grain size on the iron loss. FIG. 4 shows the influence of the plate thickness and the crystal grain size on the magnetic flux density. FIG. 5 shows the crystal grain size that gives the best iron loss value for each frequency. FIG. 6 shows the crystal grain size that gives the best value of magnetic permeability for each frequency.

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】SiとAlの合計量が2.0〜4.0%、C0.005%以
下、Mn1%以下、S0.01%以下、N0.01%以下で、残部が
鉄と不可避的不純物よりなる無方向性電磁鋼板であっ
て、板厚0.10〜0.25mmで、該鋼板の平均結晶粒径が5〜
60μmである鉄損W5/700が12W/kg以下、磁束密度B
5/700が1.0T以上の優れた磁気特性を有する周波数400Hz
以上で使用される高周波用無方向性電磁鋼板。
1. The total amount of Si and Al is 2.0 to 4.0%, C0.005% or less, Mn1% or less, S0.01% or less, N0.01% or less, and the balance is iron and inevitable impurities. A grain-oriented electrical steel sheet having a plate thickness of 0.10 to 0.25 mm and an average crystal grain size of 5 to 5 mm.
Iron loss W 5/700 of 60 μm is 12 W / kg or less, magnetic flux density B
Frequency 400Hz with excellent magnetic characteristics of 5/700 of 1.0T or more
The high frequency non-oriented electrical steel sheet used above.
JP2015755A 1990-01-25 1990-01-25 High frequency non-oriented electrical steel sheet Expired - Lifetime JPH0814016B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2015755A JPH0814016B2 (en) 1990-01-25 1990-01-25 High frequency non-oriented electrical steel sheet

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2015755A JPH0814016B2 (en) 1990-01-25 1990-01-25 High frequency non-oriented electrical steel sheet

Publications (2)

Publication Number Publication Date
JPH03223445A JPH03223445A (en) 1991-10-02
JPH0814016B2 true JPH0814016B2 (en) 1996-02-14

Family

ID=11897594

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2015755A Expired - Lifetime JPH0814016B2 (en) 1990-01-25 1990-01-25 High frequency non-oriented electrical steel sheet

Country Status (1)

Country Link
JP (1) JPH0814016B2 (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP2474636B9 (en) * 2009-09-03 2019-05-08 Nippon Steel & Sumitomo Metal Corporation Non-oriented electrical steel sheet
JP2011084778A (en) * 2009-10-15 2011-04-28 Nippon Steel Corp Nonoriented electrical steel sheet for high frequency excitation

Also Published As

Publication number Publication date
JPH03223445A (en) 1991-10-02

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