JPH06220592A - Amorphous alloy with low iron loss and high magnetic flux density - Google Patents
Amorphous alloy with low iron loss and high magnetic flux densityInfo
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- JPH06220592A JPH06220592A JP1283793A JP1283793A JPH06220592A JP H06220592 A JPH06220592 A JP H06220592A JP 1283793 A JP1283793 A JP 1283793A JP 1283793 A JP1283793 A JP 1283793A JP H06220592 A JPH06220592 A JP H06220592A
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- flux density
- magnetic flux
- amorphous alloy
- iron loss
- amorphous
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Abstract
(57)【要約】
【目的】 飽和磁束密度Bsが高く、Bs向上にともなう鉄
損の劣化のない電力トランス鉄心用非晶質合金を提供す
る。
【構成】 FeCoSiBM(MはSn,Cu,Sの少なくとも1
種)で表示される組成の片面急冷法で作製される非晶質
磁性合金。ただしFe:60〜83、Co:3〜20、かつ、80≦
Fe+Co≦86で、1≦Si≦10、11≦B≦16、MはSnのと
き、 0.1≦Sn≦1、Cuのとき、 0.1≦Cu≦2.0 、Sのと
き0.01≦S≦0.07である。この合金は磁界中アニール後
の特性が、Bs≧1.7T,1Oeにおける磁束密度が 1.55T以
上、50Hz,1.6Tにおける鉄損が0.30W/kg以下のすぐれた
高Bs、低損失特性を有することを特徴とする。
【効果】 高Bs、低損失性は電力トランス、航空機用ト
ランスの鉄心として、小型化、高効率化に寄与する。
(57) [Summary] [Object] To provide an amorphous alloy for a power transformer iron core, which has a high saturation magnetic flux density Bs and is free from deterioration of iron loss accompanying the improvement of Bs. [Structure] FeCoSiBM (M is at least 1 of Sn, Cu, S)
Amorphous magnetic alloy produced by the single-sided quenching method with the composition indicated by (Seed). However, Fe: 60 to 83, Co: 3 to 20, and 80 ≦
Fe + Co ≦ 86, 1 ≦ Si ≦ 10, 11 ≦ B ≦ 16, M is Sn ≦ 0.1 ≦ Sn ≦ 1, Cu is 0.1 ≦ Cu ≦ 2.0, and S is 0.01 ≦ S ≦ 0.07. The properties of this alloy after annealing in a magnetic field are Bs ≧ 1.7T, magnetic flux density at 1Oe is 1.55T or more, and iron loss at 50Hz, 1.6T is 0.30W / kg or less. Is characterized by. [Effect] High Bs and low loss contribute to miniaturization and high efficiency as an iron core for power transformers and aircraft transformers.
Description
【0001】[0001]
【産業上の利用分野】本発明は、電力トランス、航空機
用トランス、磁気スイッチ、平滑チョークの鉄心など高
飽和磁束密度で低損失性を要求される用途に適した非晶
質磁性合金に関するものである。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an amorphous magnetic alloy suitable for applications such as power transformers, aircraft transformers, magnetic switches, and iron cores of smooth chokes that require high saturation magnetic flux density and low loss. is there.
【0002】[0002]
【従来の技術】液体急冷法で作製されるFe基非晶質合
金は、鉄損がきわめて小さいという特徴により電力トラ
ンスや高周波トランスの鉄心材料として有望視されてき
た。しかし、本格的な実用化にはまだ至っていない。そ
の要因の一つとして飽和磁束密度がけい素鋼板に比べて
かなり低いため、所定の磁束を得るために鉄心断面積を
大きくしなければならないことが挙げられる。鉄心寸法
の増大はトランス重量および体積の増加となり、これが
トランスのコストアップの2次的要因となる。従って鉄
心材料のコストを若干犠牲にして、飽和磁束密度を高め
ることによりトランスコストを最小にするという設計思
想が生まれる。2. Description of the Related Art Fe-based amorphous alloys produced by liquid quenching have been regarded as promising as iron core materials for power transformers and high-frequency transformers because of their extremely small iron loss. However, it has not yet been fully commercialized. One of the factors is that the saturation magnetic flux density is considerably lower than that of silicon steel sheets, and therefore the iron core cross-sectional area must be increased to obtain a predetermined magnetic flux. Increasing the size of the iron core increases the weight and volume of the transformer, which is a secondary factor in increasing the cost of the transformer. Therefore, a design concept is created in which the transformer cost is minimized by increasing the saturation magnetic flux density while slightly sacrificing the cost of the iron core material.
【0003】Fe基非晶質合金の飽和磁束密度(Bs)
を高めるために、Feの一部をCoで置換する技術思想
は、HattaらがFe−B−C系で、Fujimor
iらがFe−Si−B系で提案している。しかし、前者
は熱安定性が低いこと、後者はCoの置換にもかかわら
ず、Bsは1.65T程度で実用的価値が認められなか
った。Saturation magnetic flux density (Bs) of Fe-based amorphous alloy
In order to increase the temperature, the technical idea of substituting a part of Fe with Co is that Hatta et al.
i et al. have proposed the Fe-Si-B system. However, the former had a low thermal stability, and the latter had a practical value of Bs of about 1.65 T despite the substitution of Co.
【0004】その後、Fujimoriらと同じFe−
Co−Si−B系で各元素の組成範囲を限定することに
より、高いBsの非晶質合金が得られることが特開昭5
6−139653号公報によって提案された。具体的組
成は原子%で表すとき、Fe:64.0〜80.0%、
Co:7.0〜20.0%、B:13.0〜15.0
%、Si:0超〜1.5%である。この組成条件を満足
する非晶質合金は、80A/m の磁界における磁束密度
が、1.69〜1.73Tであり、直流の保磁力が小さ
く、400Hzの交番磁界の下で1.6Tにおける鉄損お
よび励磁VAの小さいことが実施例に示されている。ま
た、この非晶質合金の代表例の結晶化温度は約430℃
であることが示されており、航空機用のトランス鉄心に
適した特性をもつことが強調されている。After that, the same Fe-- as in Fujimori et al.
By limiting the composition range of each element in the Co-Si-B system, it is possible to obtain an amorphous alloy having a high Bs.
It was proposed by the publication 6-139653. When the specific composition is expressed in atomic%, Fe: 64.0 to 80.0%,
Co: 7.0 to 20.0%, B: 13.0 to 15.0
%, Si: more than 0 to 1.5%. An amorphous alloy satisfying this composition condition has a magnetic flux density of 1.69 to 1.73 T in a magnetic field of 80 A / m, a small DC coercive force, and a magnetic field density of 1.6 T under an alternating magnetic field of 400 Hz. It is shown in the examples that the iron loss and the excitation VA are small. The crystallization temperature of the typical example of this amorphous alloy is about 430 ° C.
It is emphasized that it has characteristics suitable for transformer cores for aircraft.
【0005】上記特開昭56−139653号公報に開
示される非晶質合金は、現在市販されているFe−Si
−B系非晶質合金に比べるとBsは最高15%程度高い
が、半面、鉄損が増大するため電力用トランスの鉄心に
適用する可能性は見出せなかった。また、熱安定性も上
記Fe−Si−B系非晶質合金に比べて劣っていた。The amorphous alloy disclosed in Japanese Unexamined Patent Publication (Kokai) No. 56-139553 is an Fe-Si alloy currently on the market.
Although Bs is up to about 15% higher than that of the -B type amorphous alloy, iron loss is increased, but it has not been possible to apply it to the iron core of a power transformer. Also, the thermal stability was inferior to that of the Fe-Si-B based amorphous alloy.
【0006】[0006]
【発明が解決しようとする課題】本発明は、飽和磁束密
度の向上にともなう鉄損の劣化のない電力トランス鉄心
用非晶質合金を提供することを目的とする。SUMMARY OF THE INVENTION It is an object of the present invention to provide an amorphous alloy for a power transformer iron core, which is free from deterioration of iron loss due to improvement of saturation magnetic flux density.
【0007】[0007]
【課題を解決するための手段】本発明の要旨とするとこ
ろは、(1)組成がFea Cob Sic Bd Mx である
ことを特徴とする、片面冷却法で作製された、低損失・
高磁束密度非晶質合金。ただし、MはSn,Cu,Sの
少なくとも1種であり、a,b,c,d,xは原子%
で、60≦a≦83、3≦b≦15、かつ80≦a+b
≦86で、1≦c≦10、11≦d≦16、xはSnの
場合0.1≦x≦1.0、Cuの場合0.1≦x≦2.
0、Sの場合0.01≦x≦0.07で、かつ、a+b
+c+d+x=100である。また、(2)前項1にお
いて、Si,Bの一部を合計最大4原子%の範囲でCで
置換したことを特徴とする低鉄損・高磁束密度非晶質合
金であり、(3)室温で測定した、磁界中アニール後の
薄帯の特性として、飽和磁束密度が1.7テスラ(T)
以上、1エルステッド(Oe)(1Oe=80A/m)の磁界を印
加したときの磁束密度が1.55テスラ以上であり、か
つ50Hz,1.6テスラにおける鉄損が0.30W/kg以
下であることを特徴とする前各項記載の低鉄損・高磁束
密度非晶質合金。さらに、(4)板厚が40〜100μ
mであることを特徴とする前各項記載の低鉄損・高磁束
密度非晶質合金である。尚、前記した非晶質合金はアニ
ール後の機械的性質が改善されるものである。The gist of the present invention resides in that (1) the composition is Fe a Co b Si c B d M x, which is produced by a single-sided cooling method and has a low temperature. loss·
High magnetic flux density amorphous alloy. However, M is at least one of Sn, Cu and S, and a, b, c, d and x are atomic%
, 60 ≦ a ≦ 83, 3 ≦ b ≦ 15, and 80 ≦ a + b
≦ 86, 1 ≦ c ≦ 10, 11 ≦ d ≦ 16, x is 0.1 ≦ x ≦ 1.0 for Sn, and 0.1 ≦ x ≦ 2 for Cu.
In the case of 0 and S, 0.01 ≦ x ≦ 0.07 and a + b
+ C + d + x = 100. (2) A low iron loss / high magnetic flux density amorphous alloy as set forth in (1) above, wherein a part of Si and B is replaced with C in a total maximum of 4 atom%. Saturation magnetic flux density is 1.7 Tesla (T) as a characteristic of the ribbon after annealing in a magnetic field measured at room temperature.
The magnetic flux density is 1.55 tesla or more when a magnetic field of 1 oersted (Oe) (1 Oe = 80 A / m) is applied, and the iron loss at 50 Hz and 1.6 tesla is 0.30 W / kg or less. A low iron loss and high magnetic flux density amorphous alloy as described in the above items. Further, (4) the plate thickness is 40 to 100 μ.
m is the low iron loss / high magnetic flux density amorphous alloy as described in the preceding items. Incidentally, the above-mentioned amorphous alloy has improved mechanical properties after annealing.
【0008】すなわち、本発明は、Feの一部をCoで
置換した非晶質合金において、微量のSn,Cu、ある
いはSを添加することにより、高い動作磁束密度におけ
る鉄損が低く、熱安定性の高い非晶質合金薄帯を実現し
たものである。また、Sn,Cu,Sの添加は非晶質形
成能をも向上させることを見出し、厚い板厚とアニール
後の改善された機械的性質を同時に付与したものであ
る。That is, according to the present invention, by adding a trace amount of Sn, Cu, or S to an amorphous alloy in which a part of Fe is replaced by Co, the iron loss at high operating magnetic flux density is low and the thermal stability is high. This is an amorphous alloy ribbon with high properties. It was also found that the addition of Sn, Cu, and S also improves the ability to form an amorphous substance, and simultaneously imparts a thick plate thickness and improved mechanical properties after annealing.
【0009】図1の(a),(b),(c)はそれぞ
れ、単ロール急冷法で作製された幅25mm、板厚30μ
mのFe−Co−Si−B−X(X=Sn,Cu,S)
非晶質合金薄帯における添加元素Xの鉄損におよぼす添
加量の影響を示している。図1のように、本発明のS
n,Cu,Sを添加したFe−Co−Si−B合金は、
従来の無添加の場合に比べて、鉄損の改善が著しい。S
n,Cu,Sは薄帯表面層の結晶化を抑制する効果が認
められ、これが、アニール後の磁気特性の改善に寄与し
ているものと考えられる。FIGS. 1A, 1B and 1C are respectively 25 mm wide and 30 μ thick prepared by the single roll quenching method.
m Fe-Co-Si-B-X (X = Sn, Cu, S)
The effect of the addition amount on the iron loss of the additional element X in the amorphous alloy ribbon is shown. As shown in FIG. 1, S of the present invention
The Fe-Co-Si-B alloy added with n, Cu and S is
The iron loss is remarkably improved as compared with the conventional case of no addition. S
It is considered that n, Cu, and S have the effect of suppressing crystallization of the ribbon surface layer, and this is considered to contribute to the improvement of magnetic properties after annealing.
【0010】このようなSn,Cu,Sの添加が上記の
効果を示す理由は現時点で明らかではない。本発明者ら
が行ったグロー放電発光分光法(GDS)による表面分
析結果は、Sn,Cu,Sを添加したFe−Co−Si
−B非晶質薄帯の表面とくに自由面(ロールに接触する
面と反対の面)には、それら添加元素の著しい濃度偏析
がみられ、それとともにFe,Si,B,Coなど主成
分も分布状態が変化している。このことから、Sn,C
u,Sが不安定な非晶質薄帯表面層を保護して結晶化か
ら守り、安定化しているものと推定している。通常、結
晶化の開始点となる表面層の結晶化が抑えられる結果と
して、応力の発生が小さく、鉄損改善をもたらすものと
考えられる。またCuの場合はバルク(薄帯内部)の結
晶化温度を下げる作用をする。表面と内部の結晶化の開
始に時間差がなくなると、結晶化は一様に進行し歪みの
発生を低減し、結果として磁気特性の劣化を抑えるもの
と考えられる。本発明は、自らの発見による上記Sn,
Cu,Sの表面結晶化抑制作用をもとに、これを高Bs
のFe−Co−Si−B非晶質合金の安定化に応用し、
完成されたものである。The reason why the addition of Sn, Cu, and S exhibits the above effect is not clear at this time. The results of surface analysis by glow discharge emission spectroscopy (GDS) conducted by the present inventors show that Fe, Co, and Si containing Sn, Cu, and S are added.
-B Amorphous concentration segregation of these additive elements is observed on the surface of the amorphous ribbon, especially on the free surface (the surface opposite to the surface in contact with the roll), and the main components such as Fe, Si, B and Co are also present. The distribution is changing. From this, Sn, C
It is presumed that u and S protect the unstable amorphous ribbon surface layer by protecting it from crystallization and stabilizing it. Usually, as a result of suppressing the crystallization of the surface layer which is the starting point of crystallization, it is considered that the stress generation is small and the iron loss is improved. Further, in the case of Cu, it acts to lower the crystallization temperature of the bulk (inside the ribbon). It is considered that when there is no time difference between the start of crystallization on the surface and the inside, the crystallization progresses uniformly and the occurrence of strain is reduced, and as a result, the deterioration of magnetic properties is suppressed. The present invention relates to the Sn,
Based on the surface crystallization suppressing effect of Cu and S, it has a high Bs
Applied to the stabilization of the Fe-Co-Si-B amorphous alloy of
It has been completed.
【0011】次に、本発明において組成を限定する理由
を述べる。Fe,Coの含有量a,bは非晶質薄帯のB
sがアニール後に1.70T以上となるように設定され
た。その条件は、60≦a≦83、3≦b≦20、か
つ、80≦a+b≦86である。a,bいずれかが下限
値を下回るとBsは1.7T未満となるのでそれぞれの
下限を限定した。また上限は非晶質形成能と経済性を勘
案して設定した。すなわち、FeとCoの和が86%を
超えると非晶質化が困難になるのでa+bの上限は86
とし、Bsを1.7T以上とするためにCoの添加を少
なくとも3(原子%)とし、上限は経済性の観点から2
0にとどめた。またCoが上記の範囲であってもFeが
不足するとBs≧1.7Tを達成できない。以上の理由
でa+bの下限を80、またFeの下限を60とした。Next, the reason for limiting the composition in the present invention will be described. Fe and Co contents a and b are amorphous ribbons B
s was set to be 1.70 T or higher after annealing. The conditions are 60 ≦ a ≦ 83, 3 ≦ b ≦ 20, and 80 ≦ a + b ≦ 86. If either a or b falls below the lower limit value, Bs will be less than 1.7 T, so the respective lower limits were set. Further, the upper limit was set in consideration of the amorphous forming ability and the economical efficiency. That is, if the sum of Fe and Co exceeds 86%, amorphization becomes difficult, so the upper limit of a + b is 86.
And the addition of Co is at least 3 (atomic%) in order to make Bs 1.7 T or more, and the upper limit is 2 from the viewpoint of economic efficiency.
I kept it at 0. Even if Co is in the above range, Bs ≧ 1.7T cannot be achieved if Fe is insufficient. For the above reasons, the lower limit of a + b is set to 80, and the lower limit of Fe is set to 60.
【0012】Sn,Cu,Sについては、主に表面結晶
化の抑制作用の観点から添加量を規定した。それぞれの
下限値は、表面結晶化の抑制作用を発現するために必要
な最小値であり、それは、SnおよびCuに対してとも
に0.1(原子%)で、Sに対して0.01である。そ
れぞれの上限値は、主に薄帯の機械的性質を考慮して限
定した。添加量が上限値を超えると薄帯が脆くなること
があり、これを避けるために、Snでは1.0(原子
%)、Cuでは2.0、Sに対しては0.07以下に限
定した。The addition amounts of Sn, Cu and S are specified mainly from the viewpoint of suppressing the surface crystallization. The respective lower limit values are the minimum values required to exert the suppressing effect on the surface crystallization, and are 0.1 (atomic%) for both Sn and Cu and 0.01 for S. is there. The upper limit of each was limited mainly considering the mechanical properties of the ribbon. If the addition amount exceeds the upper limit value, the ribbon may become brittle, and in order to avoid this, it is limited to 1.0 (atomic%) for Sn, 2.0 for Cu, and 0.07 or less for S. did.
【0013】また、Si,Bは非晶質を形成するために
不可欠な元素でありそれぞれ、1≦Si≦10および1
1≦B≦16を満たすことが必要である。ただし、合計
4原子%を超えない範囲でSiおよびBの一部をCで置
換することができる。Si,Bのいずれかがこの下限を
下回ると非晶質相が形成されにくくなり、また、上限を
超えると目的とする磁気特性、とくに飽和磁束密度が達
成できなくなるので好ましくない。Si and B are indispensable elements for forming an amorphous material, and 1≤Si≤10 and 1 respectively.
It is necessary to satisfy 1 ≦ B ≦ 16. However, a part of Si and B can be replaced with C within a range not exceeding 4 atom% in total. If either Si or B is less than this lower limit, an amorphous phase is less likely to be formed, and if it exceeds the upper limit, the desired magnetic characteristics, particularly the saturation magnetic flux density, cannot be achieved, which is not preferable.
【0014】次に本発明の実施態様について述べる。ま
ず、Fe,Co,Si,Bの主成分と添加元素Sn,C
u,Sの少なくとも1種を上述した所定の組成範囲とな
るように配合した原料あるいは母合金を溶解する。ただ
し、上記の元素以外に次の元素が、本発明の目的とする
高飽和磁束密度、低損失性を損なわない範囲で含まれて
もよい。具体的には、V,Mn,Mo,Nb,Ta,
W,Cr,Hf,Niの2(原子%)以下である。これ
らの元素は、透磁率、耐食性、熱的安定性の向上に有効
であることが知られている。Next, embodiments of the present invention will be described. First, the main components of Fe, Co, Si and B and the additional elements Sn and C
A raw material or a mother alloy in which at least one of u and S is mixed so as to have the above-described predetermined composition range is melted. However, in addition to the above-mentioned elements, the following elements may be contained in a range that does not impair the high saturation magnetic flux density and the low loss property which are the objects of the present invention. Specifically, V, Mn, Mo, Nb, Ta,
It is 2 (atomic%) or less of W, Cr, Hf, and Ni. It is known that these elements are effective in improving magnetic permeability, corrosion resistance, and thermal stability.
【0015】溶解された合金の溶湯は、通常の単ロール
急冷法など片面冷却法を用いて非晶質薄帯に形成する。
このとき使用するノズルは単一スリットノズル、あるい
は多重スリットノズルを用いることができる。ここで単
一スリットノズルは、冷却基板の移動方向に測った幅が
0.2〜1.0mmの細長いスリット状開口部をもつノズ
ルで、板厚が40μm以下の薄い薄帯の製造に適してい
る。また、多重スリットノズル法は特公昭63−406
29号公報に開示される方法で、複数のスリット状開口
部を基板の移動方向に所定の間隔(通常1mm〜4mm)に
配列したノズルを用いるもので、45μm以上の厚肉材
料の製造に適している。なお、鋳造雰囲気は大気中、不
活性ガス中、真空中のいずれでもよい。The melt of the melted alloy is formed into an amorphous ribbon by using a single-sided cooling method such as a normal single roll quenching method.
The nozzle used at this time may be a single slit nozzle or a multiple slit nozzle. Here, the single slit nozzle is a nozzle having an elongated slit-shaped opening having a width of 0.2 to 1.0 mm measured in the moving direction of the cooling substrate, and is suitable for manufacturing a thin ribbon having a plate thickness of 40 μm or less. There is. The multiple slit nozzle method is disclosed in Japanese Examined Patent Publication No. 63-406.
The method disclosed in Japanese Patent No. 29, which uses a nozzle in which a plurality of slit-shaped openings are arranged at a predetermined interval (usually 1 mm to 4 mm) in the moving direction of the substrate, and is suitable for manufacturing thick materials of 45 μm or more. ing. The casting atmosphere may be air, inert gas, or vacuum.
【0016】以上のように作製された非晶質合金薄帯の
磁界中アニール後の特性は、Bsが少なくとも1.7T
であり、1エルステッド(Oe)の磁界を印加したときの磁
束密度が1.55テスラ以上であり、かつ50Hz,1.
6テスラにおける鉄損が0.30W/kg以下である。上記
アニールの条件は、最高温度が260℃〜360℃の範
囲となるように設定し、この温度に1分以上120分未
満保持する。The characteristics of the amorphous alloy ribbon produced as described above after annealing in a magnetic field have Bs of at least 1.7 T.
The magnetic flux density is 1.55 tesla or more when a magnetic field of 1 Oersted (Oe) is applied, and 50 Hz, 1.
Iron loss at 6 Tesla is less than 0.30 W / kg. The annealing conditions are set such that the maximum temperature is in the range of 260 ° C. to 360 ° C., and this temperature is maintained for 1 minute or more and less than 120 minutes.
【0017】[0017]
【実施例】以下、実施例に基づいて説明する。 (実施例1)表1に示した各組成の母合金を作製した
後、この母合金を高周波溶解した。溶解した母合金はス
リット状の開口部をもつノズルを通して、周速毎秒24
mで回転するCu製ロールの外周面で急冷され薄帯に形
成された。ここで、用いたノズルは単一スリット(幅
0.6mm、長さ25mm)である。得られた薄帯の板厚、
X線回折法で解析した非晶質性は表1の通りであった。EXAMPLES Hereinafter, examples will be described. (Example 1) After producing a master alloy having each composition shown in Table 1, this master alloy was subjected to high frequency melting. The melted mother alloy is passed through a nozzle having a slit-shaped opening, and the peripheral speed is 24 seconds per second.
It was rapidly cooled on the outer peripheral surface of the Cu roll rotating at m to form a ribbon. The nozzle used here is a single slit (width 0.6 mm, length 25 mm). Thickness of the obtained ribbon,
The amorphous properties analyzed by X-ray diffraction are shown in Table 1.
【0018】この非晶質薄帯の異なる3か所から採取し
た試料を単板試験器で鉄損、透磁率を測定した。試料の
寸法は長さ120mm、幅25mmである。各試料は磁気測
定の前に10Oeに磁界を試料長手方向に印加しながら、
最高温度が260℃〜360℃の範囲の温度で、10分
〜60分間、窒素雰囲気中でアニールした。なお、飽和
磁束密度Bsはアニール後、VSM(振動試料型磁力
計)で測定した。諸特性の測定結果を比較例とともに表
1にまとめて示した。数字はいずれも3試料の平均値で
ある。Samples taken from three different points of the amorphous ribbon were measured for iron loss and magnetic permeability with a single plate tester. The dimensions of the sample are 120 mm long and 25 mm wide. Before each magnetic measurement, a magnetic field of 10 Oe was applied to each sample in the longitudinal direction of the sample,
Annealing was performed in a nitrogen atmosphere at a maximum temperature of 260 ° C. to 360 ° C. for 10 minutes to 60 minutes. The saturated magnetic flux density Bs was measured with a VSM (vibrating sample magnetometer) after annealing. The measurement results of various characteristics are summarized in Table 1 together with Comparative Examples. All numbers are average values of 3 samples.
【0019】[0019]
【表1】 [Table 1]
【0020】[0020]
【表2】 [Table 2]
【0021】表1から明らかなように、本発明のSn,
Cu、あるいはSを添加したFe−Co−Si−B非晶
質合金は、Bsが1.7T以上、B1が1.55T以上
と高い値で、かつW16/50 が0.3W/kg以下であり、従
来のFe−Co−Si−B非晶質合金に比べて、高磁束
密度における鉄損が低いことが分かる。さらに、本発明
の非晶質合金薄帯は、同時にアニール後の機械的性質も
改善されている。一方、本発明の範囲外の組成の合金
は、非晶質性、高磁束密度における軟磁気特性のいずれ
かで、本発明の目標に到達せず、機械的性質も本発明よ
り劣っている。As is clear from Table 1, Sn,
The Fe-Co-Si-B amorphous alloy added with Cu or S has a high Bs of 1.7 T or more and B1 of 1.55 T or more, and W 16/50 of 0.3 W / kg or less. It can be seen that the iron loss at high magnetic flux density is lower than that of the conventional Fe-Co-Si-B amorphous alloy. Further, the amorphous alloy ribbon of the present invention has improved mechanical properties after annealing at the same time. On the other hand, the alloy having a composition outside the scope of the present invention does not reach the target of the present invention and has mechanical properties inferior to those of the present invention in either of amorphousness and soft magnetic characteristics at high magnetic flux density.
【0022】(実施例2)表3に示した各組成の合金1
kgを非晶質薄帯に形成した。製造は、40μm以上の板
厚を得るために多重スリット法(スリット長さ25mm、
幅0.4mm、スリット間隔1mmのダブルスリットノズ
ル、あるいはトリプルスリットノズルを用いた)を採用
した以外は実施例1と同様の条件である。この非晶質薄
帯を実施例1と同様にアニールしたのち、単板試験器で
鉄損、透磁率を測定した。測定結果を表3に示す。(Example 2) Alloy 1 of each composition shown in Table 3
kg was formed into an amorphous ribbon. Manufacture is performed by the multiple slit method (slit length 25 mm, to obtain a plate thickness of 40 μm or more,
The conditions are the same as in Example 1 except that a double slit nozzle having a width of 0.4 mm and a slit interval of 1 mm or a triple slit nozzle is used. After annealing this amorphous ribbon in the same manner as in Example 1, the core loss and magnetic permeability were measured with a single plate tester. The measurement results are shown in Table 3.
【0023】表3から、厚い板厚においても本発明のS
n,Cu、あるいはSを含有するFe−Co−Si−B
非晶質合金は、これらを添加しない従来のFe−Co−
Si−B非晶質合金に比べてすぐれた特徴をもつことが
分かる。すなわち、Sn,Cu、あるいはS無添加ある
いはこれらが本発明の下限値以下のとき、FeとCoの
含有量の和が83原子%以上の強磁性金属含有量が多い
合金は40μm以上の板厚で非晶質化が不完全で軟磁気
特性の劣化が著しいが、本発明の合金は板厚40μm以
上においてもすぐれた軟磁気特性が保持される。From Table 3, S of the present invention can be obtained even at a thick plate thickness.
Fe-Co-Si-B containing n, Cu, or S
Amorphous alloy is a conventional Fe-Co-
It can be seen that it has excellent characteristics as compared with the Si-B amorphous alloy. That is, when Sn, Cu, or S is not added or when these are below the lower limit of the present invention, the alloy having a large ferromagnetic metal content of 83 atomic% or more of the total content of Fe and Co has a plate thickness of 40 μm or more. However, the amorphization is incomplete and the soft magnetic properties are significantly deteriorated, but the alloy of the present invention retains excellent soft magnetic properties even at a plate thickness of 40 μm or more.
【0024】[0024]
【表3】 [Table 3]
【0025】[0025]
【発明の効果】以上説明したように本発明の非晶質合金
薄帯は、高磁束密度非晶質合金として知られる従来のF
e−Si−B非晶質合金ならびにFe−Co−Si−B
非晶質合金に比べて、飽和磁束密度および透磁率が高
く、高磁束密度における鉄損が低いため、電力トラン
ス、チョークコイル、航空機用トランスなど高飽和磁束
密度で低損失性を要求される鉄心材料に適している。ま
た、厚い板厚を容易に得ることができるので磁気シール
ド材、磁気センサにおいても有利に使用できる。As described above, the amorphous alloy ribbon of the present invention has a conventional F content known as a high magnetic flux density amorphous alloy.
e-Si-B amorphous alloy and Fe-Co-Si-B
Compared to amorphous alloys, the saturation magnetic flux density and magnetic permeability are high, and the iron loss at high magnetic flux density is low, so iron cores that require high saturation magnetic flux density and low loss, such as power transformers, choke coils, and aircraft transformers. Suitable for materials. In addition, since a thick plate can be easily obtained, it can be advantageously used in a magnetic shield material and a magnetic sensor.
【図1】(a),(b),(c)は、基本成分(Fe−
Co−Si−B)にそれぞれSn,Cu,Sを添加した
場合の鉄損に及ぼす影響を示す図である。1 (a), (b), and (c) are basic components (Fe-
It is a figure which shows the influence which acts on iron loss when adding Sn, Cu, and S to Co-Si-B), respectively.
Claims (4)
ることを特徴とする、片面冷却法で作製された、低損失
・高磁束密度非晶質合金。ただし、MはSn,Cu,S
の少なくとも1種であり、 a,b,c,d,xは原子%で、 60≦a≦83、 3≦b≦20、かつ 80≦a+b≦86で、 1≦c≦10、 11≦d≦16、 xはSnの場合、0.1≦x≦1.0、 Cuの場合、0.1≦x≦2.0、 Sの場合、0.01≦x≦0.07で、かつ、 a+b+c+d+x=100である。[Claim 1], wherein the composition is Fe a Co b Si c B d M x, made with single-sided cooling method, low loss and high magnetic flux density amorphous alloy. However, M is Sn, Cu, S
A, b, c, d, and x are atomic%, 60 ≦ a ≦ 83, 3 ≦ b ≦ 20, and 80 ≦ a + b ≦ 86, 1 ≦ c ≦ 10, 11 ≦ d ≦ 16, x is Sn ≦ 0.1 ≦ x ≦ 1.0, Cu is 0.1 ≦ x ≦ 2.0, S is 0.01 ≦ x ≦ 0.07, and a + b + c + d + x = 100.
囲でCで置換したことを特徴とする請求項1記載の低損
失・高磁束密度非晶質合金。2. The low-loss, high-flux-density amorphous alloy according to claim 1, wherein a part of Si and B is replaced by C in a total amount of at most 4 atom%.
帯の特性として、飽和磁束密度が1.7テスラ(T)以
上、1エルステッド(Oe)の磁界を印加したときの磁束
密度が1.55テスラ以上であり、かつ、50Hz,1.
6テスラにおける鉄損が0.30W/kg以下であることを
特徴とする請求項1記載の低鉄損・高磁束密度非晶質合
金。3. As a characteristic of the ribbon after annealing in a magnetic field measured at room temperature, the magnetic flux density when a magnetic field having a saturation magnetic flux density of 1.7 Tesla (T) or more and 1 Oersted (Oe) is applied is 1. 0.55 Tesla or more and 50 Hz, 1.
The low iron loss and high magnetic flux density amorphous alloy according to claim 1, wherein the iron loss at 6 Tesla is 0.30 W / kg or less.
徴とする請求項1記載の低鉄損・高磁束密度非晶質合
金。4. The low iron loss / high magnetic flux density amorphous alloy according to claim 1, wherein the plate thickness is 40 to 100 μm.
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|---|---|---|---|
| JP01283793A JP3434844B2 (en) | 1993-01-28 | 1993-01-28 | Low iron loss, high magnetic flux density amorphous alloy |
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| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP01283793A JP3434844B2 (en) | 1993-01-28 | 1993-01-28 | Low iron loss, high magnetic flux density amorphous alloy |
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| Publication Number | Publication Date |
|---|---|
| JPH06220592A true JPH06220592A (en) | 1994-08-09 |
| JP3434844B2 JP3434844B2 (en) | 2003-08-11 |
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ID=11816499
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|---|---|---|---|
| JP01283793A Expired - Lifetime JP3434844B2 (en) | 1993-01-28 | 1993-01-28 | Low iron loss, high magnetic flux density amorphous alloy |
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| Country | Link |
|---|---|
| JP (1) | JP3434844B2 (en) |
Cited By (8)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0718388A (en) * | 1993-06-18 | 1995-01-20 | Hitachi Metals Ltd | Nanocrystal alloy thin strip improved in asymmetry of b-h loop, magnetic core and production of nanocrystal alloy thin strip |
| US5690704A (en) * | 1994-07-05 | 1997-11-25 | Nippon Shokubai Co., Ltd. | Additive for carbonaceous solid-water slurry, method for production thereof, and carbonaceous solid-water slurry compositions |
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1993
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| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0718388A (en) * | 1993-06-18 | 1995-01-20 | Hitachi Metals Ltd | Nanocrystal alloy thin strip improved in asymmetry of b-h loop, magnetic core and production of nanocrystal alloy thin strip |
| US5690704A (en) * | 1994-07-05 | 1997-11-25 | Nippon Shokubai Co., Ltd. | Additive for carbonaceous solid-water slurry, method for production thereof, and carbonaceous solid-water slurry compositions |
| US6416879B1 (en) | 2000-11-27 | 2002-07-09 | Nippon Steel Corporation | Fe-based amorphous alloy thin strip and core produced using the same |
| JP2007107094A (en) * | 2005-09-16 | 2007-04-26 | Hitachi Metals Ltd | Soft magnetic alloy, method for producing the same and magnetic component |
| JP2007107095A (en) * | 2005-09-16 | 2007-04-26 | Hitachi Metals Ltd | Magnetic alloy, amorphous alloy thin band, and magnetic component |
| JP2013067863A (en) * | 2005-09-16 | 2013-04-18 | Hitachi Metals Ltd | Soft magnetic alloy powder and magnetic part using the same |
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| JP2008231462A (en) * | 2007-03-16 | 2008-10-02 | Hitachi Metals Ltd | Magnetic alloy, amorphous alloy strip and magnetic component |
| EP2128291A4 (en) * | 2007-03-16 | 2010-09-08 | Hitachi Metals Ltd | MAGNETIC ALLOY, AMORPHOUS ALLOY RIBBON AND MAGNETIC PIECE |
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| WO2009096382A1 (en) * | 2008-01-28 | 2009-08-06 | Hitachi Metals, Ltd. | Amorphous soft magnetic alloy, amorphous soft magnetic alloy ribbon, amorphous soft magnetic alloy powder, and magnetic core and magnetic component using the same |
| US11970761B2 (en) | 2017-12-21 | 2024-04-30 | Qingdao Yunlu Advanced Materials Technology Co., Ltd. | Iron-based amorphous alloy and preparation method therefor |
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