JPH0135065B2 - - Google Patents

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Publication number
JPH0135065B2
JPH0135065B2 JP58221974A JP22197483A JPH0135065B2 JP H0135065 B2 JPH0135065 B2 JP H0135065B2 JP 58221974 A JP58221974 A JP 58221974A JP 22197483 A JP22197483 A JP 22197483A JP H0135065 B2 JPH0135065 B2 JP H0135065B2
Authority
JP
Japan
Prior art keywords
iron loss
loss
amorphous alloy
flux density
low
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
Application number
JP58221974A
Other languages
Japanese (ja)
Other versions
JPS59107062A (en
Inventor
Koichiro Inomata
Michio Hasegawa
Masakatsu Haga
Senji Shimanuki
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.)
Toshiba Corp
Original Assignee
Tokyo Shibaura Electric Co Ltd
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Tokyo Shibaura Electric Co Ltd filed Critical Tokyo Shibaura Electric Co Ltd
Priority to JP58221974A priority Critical patent/JPS59107062A/en
Publication of JPS59107062A publication Critical patent/JPS59107062A/en
Publication of JPH0135065B2 publication Critical patent/JPH0135065B2/ja
Granted legal-status Critical Current

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  • Soft Magnetic Materials (AREA)

Description

【発明の詳細な説明】[Detailed description of the invention]

本発明は電磁気装置としての磁心等に用いられ
る低損失非晶質合金に係わるもので、特にスイツ
チングレギユレータなど高周波用磁心に適した低
損失非晶質合金に関するものである。 スイツチングレギユレータなど高周波で使用さ
れる磁心としては、従来、パーマロイ、フエライ
トなどの結晶質材料が用いられている。しかしパ
ーマロイは比抵抗が小さいため高周波での鉄損が
大きいという欠点を有していた。またフエライト
は高周波での損失は小さいが、磁束密度がせいぜ
い5000Gと小さいため動作磁束密度の高い使用に
おいては飽和に近くなり、鉄損が増大する。スイ
ツチングレギユレータに使用される電源トランス
など高周波で使用されるトランスは小形化が望ま
れており、従つて動作磁束密度の上昇が必要とさ
れているが、この場合のフエライトの鉄損増大が
実用上大きな問題となつていた。 最近注目されている結晶構造を持たない非晶質
磁性合金は高透磁率、低保磁力など優れた軟質磁
気特性を示すことが知られている。これらの非晶
質磁性合金はFe、Co、Niを基本に非晶質化元素
(メタロイド)としてP、C、B、Si、Al、Geな
どを含むものであるが、これらが普遍的に高周波
での鉄損が小さいというものではない。例えば
Fe系非晶質合金は50〜60Hzの低い周波数ではけ
い素鋼の〜1/4という非常に小さな鉄損を示すが
10〜50kHzという高周波では著しく大きな鉄損を
示し、とてもスイツチングレギユレータ等の高周
波での使用に適したものとは言えなかつた。 本発明は上記の点に鑑み磁束密度の高い状態で
使用される高周波用磁心に関し、かつ鉄損の小さ
い低損失非晶質合金を用いた高周波用磁心を提供
することを目的とするものである。 本発明は (Fe1-aNia)100-x-ySixBy(原子比) ただし (0.2a0.7 1x20 5y9.5) からなる低損失非晶質合金を用いた高周波用磁心
であり、特にBを5y7、Niを0.3a
0.45とする事によりさらに高周波における鉄損を
低下させる事ができるというものである。 なお本発明における低損失非晶質合金の組成成
分の限定理由は次の如くである。 Niは高周波での鉄損を低下させる効果を有す
るが0.2原子%未満ではその効果があまりなく、
0.7原子%を超えるとキユリー点が著しく小さく
なるとともに磁束密度が5000G以下となり実用性
がなくなるので上記範囲とした。さらに好ましく
はNiを0.3a0.45とする事により、一層磁束
密度が高く、かつ小さな鉄損のものが得られる。 また、Bを5〜9.5原子%としたのは、この範
囲外では非晶質合金の作製が困難になり、さらに
鉄損を少なくするという効果が顕著でなくなるか
らである。特にBは5y7とすると鉄損が著
しく小さくなり、実用上この範囲とする事が好ま
しい。 Siは非晶質化を助成し、鉄損を低下させる効果
を有する元素であるが、1原子%未満では特にそ
れらの効果がなく、20原子%を越えるとかえつて
非晶質合金の作製が困難になるのでこの範囲とし
た。 以下、実施例に基ずいて本発明を詳細に説明す
る。 実施例 1 (Fe0.6Ni0.4)80Si14B6非晶質合金を圧延急冷法
を用いて作製した。即ち、2つの高速回転するロ
ール間に石英管ノズルより溶融合金をアルゴンガ
ス圧によつて噴出させ、急冷して幅2mm、厚さ
30μm、長さ10mの薄帯試料を作製した。この試
料から長さ140cmを切取り、直径20φのアルミナ
製ボビンに巻きつけ、400℃で30分熱処理後1次
コイル、2次コイルとも70回巻きワツトメータを
用いて鉄損を測定した。また飽和磁化を試料振動
形磁力計を用いて測定した。磁束密度Bm=3kG
における鉄損を、高周波10kHz、20kHzに対して
飽和磁化と併せて第1表に示す。第1表には比較
のため従来、スイツチング電源用に使用されてい
るMn−Znフエライトの結果も示した。表よりわ
かるように、本発明の非晶質合金は磁束密度がフ
エライトよりも大きく、かつフエライトよりも小
さな鉄損を示す。 実施例 2 第1表に示す非晶質合金を実施例1と同じ方法
を用いて作製し、鉄損を評価した。本発明の非晶
質合金は小さな鉄損を示すことがわかる。
The present invention relates to a low-loss amorphous alloy used in magnetic cores of electromagnetic devices, and particularly relates to a low-loss amorphous alloy suitable for high-frequency magnetic cores such as switching regulators. Conventionally, crystalline materials such as permalloy and ferrite have been used as magnetic cores used in high frequency applications such as switching regulators. However, permalloy has a drawback of high iron loss at high frequencies due to its low resistivity. Furthermore, although ferrite has a small loss at high frequencies, its magnetic flux density is as small as 5000G at most, so when used with a high operating magnetic flux density, it approaches saturation and increases iron loss. Transformers used at high frequencies, such as power transformers used in switching regulators, are desired to be made smaller and therefore require an increase in operating magnetic flux density, but in this case the iron loss of ferrite increases. has become a big problem in practice. Amorphous magnetic alloys without a crystalline structure, which have recently attracted attention, are known to exhibit excellent soft magnetic properties such as high magnetic permeability and low coercive force. These amorphous magnetic alloys are based on Fe, Co, and Ni, and include P, C, B, Si, Al, Ge, etc. as amorphous elements (metalloids), but these are universally compatible with high frequencies. This does not mean that iron loss is small. for example
Fe-based amorphous alloys exhibit very small iron loss of ~1/4 of silicon steel at low frequencies of 50 to 60 Hz.
At high frequencies of 10 to 50 kHz, it exhibited a significantly large iron loss, making it unsuitable for high frequency applications such as switching regulators. In view of the above points, the present invention relates to a high-frequency magnetic core used in a state of high magnetic flux density, and an object of the present invention is to provide a high-frequency magnetic core using a low-loss amorphous alloy with low iron loss. . The present invention is a high-frequency magnetic core using a low-loss amorphous alloy consisting of (Fe 1-a Ni a ) 100-xy Si x B y (atomic ratio) where (0.2a0.7 1x20 5y9.5), Especially B is 5y7, Ni is 0.3a
By setting it to 0.45, it is possible to further reduce iron loss at high frequencies. The reasons for limiting the compositional components of the low-loss amorphous alloy in the present invention are as follows. Ni has the effect of reducing iron loss at high frequencies, but if it is less than 0.2 atomic percent, the effect is not so great.
If it exceeds 0.7 atomic %, the Curie point will become extremely small and the magnetic flux density will become less than 5000G, making it impractical, so it was set in the above range. More preferably, by setting Ni to 0.3a0.45, it is possible to obtain an even higher magnetic flux density and a smaller core loss. Further, the reason why B is set to 5 to 9.5 atomic % is that outside this range, it becomes difficult to produce an amorphous alloy, and furthermore, the effect of reducing iron loss becomes less noticeable. In particular, if B is set to 5y7, the iron loss will be significantly reduced, and it is preferable for practical purposes to set it within this range. Si is an element that has the effect of promoting amorphization and reducing iron loss, but if it is less than 1 atomic %, it has no particular effect, and if it exceeds 20 atomic %, it may actually hinder the creation of an amorphous alloy. This range was chosen because it would be difficult. Hereinafter, the present invention will be explained in detail based on Examples. Example 1 (Fe 0.6 Ni 0.4 ) 80 Si 14 B 6 amorphous alloy was produced using a rolling quenching method. That is, the molten alloy is jetted between two high-speed rotating rolls from a quartz tube nozzle under argon gas pressure, and is rapidly cooled to a thickness of 2 mm in width and thickness.
A ribbon sample of 30 μm and 10 m in length was prepared. A length of 140cm was cut from this sample, wound around an alumina bobbin with a diameter of 20φ, and after heat treatment at 400°C for 30 minutes, both the primary and secondary coils were wound 70 times and iron loss was measured using a Wattmeter. The saturation magnetization was also measured using a sample vibrating magnetometer. Magnetic flux density Bm=3kG
Table 1 shows the iron loss at high frequencies of 10kHz and 20kHz, together with the saturation magnetization. For comparison, Table 1 also shows the results for Mn--Zn ferrite, which has been conventionally used for switching power supplies. As can be seen from the table, the amorphous alloy of the present invention has a larger magnetic flux density than ferrite and exhibits smaller core loss than ferrite. Example 2 Amorphous alloys shown in Table 1 were produced using the same method as in Example 1, and core loss was evaluated. It can be seen that the amorphous alloy of the present invention exhibits small iron loss.

【表】 実施例 3 (Fe0.55Ni0.45)78Si22-yBy非晶質合金を実施例1
と同じ方法を用いて作製し、鉄損を測定した。
Bm=3kG、周波数20kHzにおける鉄損のB量依
存性を第1図に示した。図よりわかるようにBが
5〜9.5原子%において特に小さな鉄損を示す。 以上、本発明の非晶質合金は磁束密度がフエラ
イトよりも大きく特に高周波での鉄損もフエライ
トよりも優れており、従つて高周波トランスなど
の小形化が可能であり工業上有益なものである。
[Table] Example 3 (Fe 0.55 Ni 0.45 ) 78 Si 22-y B y Amorphous alloy Example 1
It was manufactured using the same method as above, and the iron loss was measured.
Figure 1 shows the dependence of iron loss on the amount of B at Bm = 3kG and frequency of 20kHz. As can be seen from the figure, the core loss is particularly small when B is 5 to 9.5 at%. As described above, the amorphous alloy of the present invention has a higher magnetic flux density than ferrite, and is also superior to ferrite in core loss especially at high frequencies. Therefore, it is possible to miniaturize high frequency transformers, etc., and is industrially useful. .

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

第1図は本発明に係る非晶質合金の鉄損を示す
曲線図である。
FIG. 1 is a curve diagram showing the iron loss of the amorphous alloy according to the present invention.

Claims (1)

【特許請求の範囲】 1 (Fe1-aNia)100-x-ySixBy(原子比) ただし [0.2≦a≦0.7 1≦x≦20 5≦y≦9.5] から成る事を特徴とする低損失非晶質合金を用い
た高周波用磁心。 2 特許請求の範囲第1項において、Bを5≦y
≦7とした事を特徴とする高周波用磁心。 3 特許請求の範囲第1項又は第2項において、
Niを0.3≦a≦0.45とした事を特徴とする高周波
用磁心。
[Claims] 1 (Fe 1-a Ni a ) 100-xy Si x B y (atomic ratio), characterized by consisting of [0.2≦a≦0.7 1≦x≦20 5≦y≦9.5] A high-frequency magnetic core using a low-loss amorphous alloy. 2 In claim 1, B is 5≦y
A magnetic core for high frequency, characterized in that ≦7. 3 In claim 1 or 2,
A magnetic core for high frequency use, characterized in that Ni is 0.3≦a≦0.45.
JP58221974A 1983-11-28 1983-11-28 Low iron loss amorphous alloy Granted JPS59107062A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP58221974A JPS59107062A (en) 1983-11-28 1983-11-28 Low iron loss amorphous alloy

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP58221974A JPS59107062A (en) 1983-11-28 1983-11-28 Low iron loss amorphous alloy

Related Parent Applications (1)

Application Number Title Priority Date Filing Date
JP55084588A Division JPS5933183B2 (en) 1980-06-24 1980-06-24 Low loss amorphous alloy

Publications (2)

Publication Number Publication Date
JPS59107062A JPS59107062A (en) 1984-06-21
JPH0135065B2 true JPH0135065B2 (en) 1989-07-24

Family

ID=16775081

Family Applications (1)

Application Number Title Priority Date Filing Date
JP58221974A Granted JPS59107062A (en) 1983-11-28 1983-11-28 Low iron loss amorphous alloy

Country Status (1)

Country Link
JP (1) JPS59107062A (en)

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS581183B2 (en) * 1976-09-16 1983-01-10 東北大学金属材料研究所長 High magnetic permeability amorphous alloy with high magnetic flux density and large squareness ratio
JPS55161048A (en) * 1979-06-01 1980-12-15 Nippon Steel Corp Amorphous alloy for transformer

Also Published As

Publication number Publication date
JPS59107062A (en) 1984-06-21

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