JPH11307351A - High frequency transformer and yoke - Google Patents
High frequency transformer and yokeInfo
- Publication number
- JPH11307351A JPH11307351A JP10978998A JP10978998A JPH11307351A JP H11307351 A JPH11307351 A JP H11307351A JP 10978998 A JP10978998 A JP 10978998A JP 10978998 A JP10978998 A JP 10978998A JP H11307351 A JPH11307351 A JP H11307351A
- Authority
- JP
- Japan
- Prior art keywords
- surface layer
- high frequency
- concentration
- magnetic flux
- frequency
- 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.)
- Pending
Links
Landscapes
- Soft Magnetic Materials (AREA)
Abstract
Description
【0001】[0001]
【発明の属する技術分野】輸送、産業用機器、誘導加
熱、電力、家電、情報などのインバータ、コンバータ電
源に用いられるトランスおよびヨークに関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a transformer and a yoke used for an inverter and a converter power supply for transportation, industrial equipment, induction heating, electric power, home appliances, information, and the like.
【0002】[0002]
【従来の技術】昨今のIGBTインバータ技術によりそ
のスイッチング周波数は10〜30kHz程度となり、
インバータ電源内部に用いられる高周波昇圧、降圧、絶
縁トランスや誘導加熱、オゾン発生、非接触給電を目的
とした高周波電源用トランスやヨークの需要が増えつつ
ある。このため、こういったトランスやヨークの低損失
化がインバータ電源あるいは高周波電源系統の効率化の
ポイントとなっている。このため、フェライトをはじめ
アモルファスや極薄方向性けい素鋼板、6.5%けい素
鋼板等の高周波低損失の軟磁性材料が実用化されている
が、その鉄損、コスト、耐久・耐震性のいずれも兼ね備
えているとはいえない。2. Description of the Related Art With the recent IGBT inverter technology, the switching frequency is about 10 to 30 kHz.
There is an increasing demand for high-frequency power transformers and yokes used for high-frequency step-up and step-down, insulating transformers, induction heating, ozone generation, and non-contact power supply used inside inverter power supplies. For this reason, reducing the loss of such a transformer or yoke is a point of increasing the efficiency of the inverter power supply or the high-frequency power supply system. For this reason, high-frequency low-loss soft magnetic materials such as ferrite, amorphous and ultra-thin oriented silicon steel sheets, and 6.5% silicon steel sheets have been put to practical use, but their iron loss, cost, durability, and earthquake resistance are high. It cannot be said that they have both.
【0003】[0003]
【発明が解決しようとする課題】すなわち、1kHz以
上100kHz程度までの高周波トランス、ヨークは1
kHz程度の場合は容量や用途、形状に応じてけい素鋼
板やアモルファス、6.5%けい素鋼板などが用いら
れ、10kHzを超えるあたりからフェライトも使用さ
れているが、1kHz以上の周波数では渦電流損失が鉄
心、銅線共に問題となってくるため、特に鉄心材料はそ
の材料選択が難しい。フェライトは金属系磁性材料と異
なり電気抵抗が高いため渦電流が抑えられるが低磁束密
度や大容量コアの高コスト化、機械的脆さ(衝撃に弱
い)といった問題点を有する。アモルファスも低鉄損材
料であるが、高加工コストと形状に制限がある(板厚2
5μmで極めて硬いため巻きコア以外に加工が困難)た
め中、大容量トランスやさまざまな形状のヨークに加工
することは難しい。That is, a high-frequency transformer and yoke of 1 kHz to 100 kHz is one
In the case of about kHz, silicon steel sheet, amorphous, 6.5% silicon steel sheet, etc. are used depending on the capacity, application and shape, and ferrite is used from around 10 kHz. Since current loss becomes a problem for both the iron core and the copper wire, it is difficult to select an iron core material in particular. Ferrite, unlike metal-based magnetic materials, has high electrical resistance and can suppress eddy currents, but has problems such as low magnetic flux density, high cost of large-capacity cores, and mechanical brittleness (weak against impact). Amorphous is also a low iron loss material, but high processing cost and shape are limited (thickness 2
(Because it is extremely hard at 5 μm, it is difficult to process other than a wound core.) It is difficult to process into a medium-capacity transformer and yokes of various shapes.
【0004】また6.5%けい素鋼板は最適な鉄心材料
の一つと考えられるが、加工性や飽和磁束密度の点で従
来の無方向性けい素鋼板と比べて多少劣る。そこで本発
明者らは、こういった問題を解決すべく鋭意努力した結
果、板厚方向にSi濃度を付けること、具体的には表層
部のけい素量を中心部のけい素量より高くすることによ
って高周波鉄損が特に改善されることが発見された。A 6.5% silicon steel sheet is considered to be one of the most suitable core materials, but is somewhat inferior to the conventional non-oriented silicon steel sheet in workability and saturation magnetic flux density. The inventors of the present invention have made intensive efforts to solve such a problem, and as a result, provide Si concentration in the plate thickness direction, specifically, make the silicon content in the surface layer higher than the silicon content in the central portion. It has been found that high frequency iron loss is thereby particularly improved.
【0005】本発明はこの知見に基づいてなされたもの
で、高周波鉄損にすぐれ、しかも加工性や飽和磁束密度
に優れている高周波トランスおよびヨークを提供するも
のである。The present invention has been made based on this finding, and provides a high-frequency transformer and a yoke which are excellent in high-frequency iron loss and excellent in workability and saturation magnetic flux density.
【0006】[0006]
【課題を解決するための手段】すなわち本発明は、 (1) 周波数が1kHz以上で駆動し、鉄心材料が板
厚方向表層のSi濃度が中心層のSi濃度より0.3%
以上高いけい素鋼板からなる低損失高周波トランスおよ
びヨーク。 (2) 鋼板表層部のSi量が6〜7%で、低騒音であ
ることを特徴とする(1)の低損失高周波トランスおよ
びヨーク。That is, the present invention provides: (1) When the driving is performed at a frequency of 1 kHz or more, the core material is made such that the Si concentration in the surface layer in the thickness direction is 0.3% of the Si concentration in the center layer
Low loss high frequency transformer and yoke made of high silicon steel plate. (2) The low-loss high-frequency transformer and yoke according to (1), wherein the amount of Si in the surface layer of the steel sheet is 6 to 7% and the noise is low.
【0007】[0007]
【発明の実施の形態】本発明は、鋼板の板厚方向にSi
濃度勾配をつけている。このように板厚方向にSi濃度
勾配をつけるにはいくつかの方法がある。例えば、鉄あ
るいはけい素鋼板の表面にSiペーストを塗布したあと
熱拡散を行う方法やPVDによりSiイオンを蒸着し、
同様に熱拡散させる方法あるいはSiCl4 などの高
温ガスを鋼板に吹き付けてSiを蒸着したあと熱拡散さ
せる熱CVD法(浸けい法)などである。特に最後の熱
CVD法は最も実用的な方法でありこの方法で作製した
鋼板の板厚断面のSi濃度分布を図1に、代表磁気特性
を表1に示す。BEST MODE FOR CARRYING OUT THE INVENTION The present invention relates to a steel sheet in a thickness direction.
It has a concentration gradient. There are several methods for providing a Si concentration gradient in the thickness direction as described above. For example, a method of performing heat diffusion after applying a Si paste on the surface of an iron or silicon steel sheet or depositing Si ions by PVD,
Similarly, there is a method of thermal diffusion, or a thermal CVD method (immersion method) of spraying a high-temperature gas such as SiCl 4 onto a steel sheet to deposit Si and then thermally diffusing the Si. In particular, the last thermal CVD method is the most practical method. FIG. 1 shows the Si concentration distribution in the cross section of the steel sheet produced by this method, and Table 1 shows the representative magnetic characteristics.
【0008】[0008]
【表1】 [Table 1]
【0009】いずれの方法においても板厚方向に均一な
Si濃度を有する高けい素鋼板、例えば軟磁気特性を有
する6.5%けい素鋼板を製造するためには熱拡散が必
要であり、このためライン長を大きくするかライン速度
を抑えるあるいはこの両方を併用する等の製造コスト上
のデメリットがあるが、板厚方向にSi濃度勾配を有す
る本願鋼板は拡散を途中でやめるためこのデメリットが
解消される。このため、均一な6.5%けい素鋼板より
もコストメリットを有する。In any method, thermal diffusion is necessary to produce a high silicon steel sheet having a uniform Si concentration in the thickness direction, for example, a 6.5% silicon steel sheet having soft magnetic properties. Therefore, there is a disadvantage in manufacturing cost such as increasing the line length and / or suppressing the line speed, or using both of them. Is done. For this reason, there is a cost advantage over a uniform 6.5% silicon steel sheet.
【0010】本発明では、板厚方向表層のSi濃度が中
心層のSi濃度より0.3%以上高い。一般に鉄中のS
i量を増やしていくと軟磁気特性は向上し、6〜7%、
特に6.5%で最高となるが、表層と中心のSi濃度差
を0.3%以上にすると、表層部の透磁率が中心部の透
磁率に差が現われる。Si均一材の場合、渦電流が磁束
の方向と垂直な面全体に流れるため板厚によって渦電流
損失は大きく異なり、薄くなればなるほどこの損失は減
少する。ところが表層と中心の透磁率にある程度大きな
違いがあると、磁束は表層に閉じ込められ易くなり、渦
電流は表裏表面断面2ケ所に分散して流れるため、あた
かも低Si鋼板を高Si鋼板2枚で挟んだかの効果が得
られるためと考えることができる。この場合、このSi
濃度差は0.3%未満では効果が少ない。ただし、4%
を超えるとヒステリシス損失が増大するため好ましくな
い。In the present invention, the Si concentration in the surface layer in the thickness direction is 0.3% or more higher than the Si concentration in the center layer. Generally S in iron
As the amount of i increases, the soft magnetic properties improve,
Particularly, the highest value is obtained at 6.5%. However, when the difference in Si concentration between the surface layer and the center is 0.3% or more, the difference in the magnetic permeability between the surface layer portion and the central portion appears. In the case of a uniform Si material, an eddy current flows through the entire surface perpendicular to the direction of the magnetic flux, so that the eddy current loss greatly differs depending on the thickness of the sheet. However, if there is a large difference in the magnetic permeability between the surface layer and the center, the magnetic flux is likely to be confined in the surface layer, and the eddy current flows in two different cross-sections on the front and back surfaces. It can be considered that the effect of pinching is obtained. In this case, this Si
If the concentration difference is less than 0.3%, the effect is small. However, 4%
Exceeding the range is not preferable because the hysteresis loss increases.
【0011】また、平均Si量が高くする方が高周波鉄
損を抑えられ、表層Si量は6.5%とするともっとも
高周波鉄損を抑えられるため望ましい。さらに、磁気歪
みについてみると表層Si量を6.5%にすることによ
り高周波磁束は表層部を流れるため磁束密度がある程度
の大きさまでであれば実質的には磁気歪みはほぼゼロと
なり、低騒音になる。これは一般的に駆動周波数が1k
Hz〜30kHz程度では設計磁束密度は0.05T〜
0.3T程度であり、表裏の6.5%Si層が合計して
20〜30%程度であれば十分に磁束が表裏部から漏れ出
さないと推定される。It is desirable to increase the average Si amount to suppress high-frequency iron loss, and it is desirable to set the surface Si amount to 6.5% since the high-frequency iron loss can be suppressed most. Further, regarding the magnetostriction, by setting the amount of surface Si to 6.5%, the high-frequency magnetic flux flows through the surface layer, so that when the magnetic flux density is up to a certain level, the magnetostriction becomes substantially zero and low noise. become. This generally means that the driving frequency is 1k
The design magnetic flux density is 0.05T ~
It is about 0.3T, and the 6.5% Si layers on the front and back
It is presumed that the magnetic flux does not sufficiently leak from the front and back portions if it is about 20 to 30%.
【0012】また、打ち抜き性の面からSi濃度勾配を
有する鋼板は中心部は延性を有するためクラックが入り
にくく表層部は硬いため打ち抜き時に発生するバリ(ダ
レ)を小さく抑えることができる。Further, from the viewpoint of punching properties, a steel sheet having a Si concentration gradient has ductility at the center and is hardly cracked, so that the surface layer is hard, so that burrs generated at the time of punching can be reduced.
【0013】トランス鉄心の形状は短冊コア、短冊積層
ブロックコアや積層EIコアやEEコア、UUコアなど
プレス+積層鉄心やトロイダルコアやカットコアのよう
な巻きコアでも構わないが、磁気回路上は積層鉄心の方
が鉄損特性は多少優れる。ただし、小ロットの場合には
コイル巻きや組み立てにおいてカットコアの方が組み立
てコストにメリットのある場合もある。The shape of the transformer core may be a pressed core such as a strip core, a strip laminated block core, a laminated EI core, an EE core, or a UU core, or a wound core such as a toroidal core or a cut core. The laminated iron core has somewhat better iron loss characteristics. However, in the case of a small lot, there is a case where a cut core is more advantageous in assembling cost in coil winding and assembling.
【0014】[0014]
【実施例】(実施例1)表2に示す鉄心材料を用いて1
0kHz、設計磁束密度0.06T、10kVA、1
次,2次がそれぞれ16ターンの単相のトランスを試作
し、トランスの無負荷損失をワットメータにて評価する
とともに騒音測定を行った。このように、本願の鉄心材
料を使用することにより低損失で低騒音のトランスを提
供することができる。EXAMPLES (Example 1) Using the iron core material shown in Table 2, 1
0 kHz, design magnetic flux density 0.06 T, 10 kVA, 1
A prototype of a single-phase transformer having 16 turns each for the second and second turns was prototyped, the no-load loss of the transformer was evaluated by a wattmeter, and noise was measured. As described above, by using the iron core material of the present application, a low-loss, low-noise transformer can be provided.
【0015】[0015]
【表2】 但し、上記けい素%は平均値を示しΔSiは中心部と表
層部のSi量の差を示す。[Table 2] However, the above-mentioned silicon% indicates an average value, and ΔSi indicates a difference between the amounts of Si in the central portion and the surface portion.
【0016】[0016]
【発明の効果】高周波鉄損にすぐれ、しかも加工性や飽
和磁束密度に優れている高周波トランスおよびヨークを
提供することができる。According to the present invention, it is possible to provide a high-frequency transformer and a yoke which are excellent in high-frequency iron loss and excellent in workability and saturation magnetic flux density.
【図1】板厚断面のSi濃度分布の例(板厚0.1mm )を
示す図。FIG. 1 is a diagram showing an example of a Si concentration distribution (sheet thickness 0.1 mm) in a sheet thickness cross section.
───────────────────────────────────────────────────── フロントページの続き (72)発明者 笠井 勝司 東京都千代田区丸の内一丁目1番2号 日 本鋼管株式会社内 ──────────────────────────────────────────────────の Continued on the front page (72) Inventor Katsushi Kasai 1-2-1 Marunouchi, Chiyoda-ku, Tokyo Nihon Kokan Co., Ltd.
Claims (2)
料が板厚方向表層のSi濃度が中心層のSi濃度より
0.3%以上高いけい素鋼板からなる低損失高周波トラ
ンスおよびヨーク。1. A low-loss high-frequency transformer and yoke driven at a frequency of 1 kHz or more and made of a silicon steel sheet whose core material has a Si concentration in a surface layer in a thickness direction 0.3% or more higher than a Si concentration in a center layer.
音であることを特徴とする請求項1の低損失高周波トラ
ンスおよびヨーク。2. The low-loss high-frequency transformer and yoke according to claim 1, wherein the amount of Si in the surface layer of the steel sheet is 6 to 7% and the noise is low.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP10978998A JPH11307351A (en) | 1998-04-20 | 1998-04-20 | High frequency transformer and yoke |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP10978998A JPH11307351A (en) | 1998-04-20 | 1998-04-20 | High frequency transformer and yoke |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH11307351A true JPH11307351A (en) | 1999-11-05 |
Family
ID=14519270
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP10978998A Pending JPH11307351A (en) | 1998-04-20 | 1998-04-20 | High frequency transformer and yoke |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH11307351A (en) |
-
1998
- 1998-04-20 JP JP10978998A patent/JPH11307351A/en active Pending
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