JPS60263413A - Arc welder - Google Patents

Arc welder

Info

Publication number
JPS60263413A
JPS60263413A JP59119049A JP11904984A JPS60263413A JP S60263413 A JPS60263413 A JP S60263413A JP 59119049 A JP59119049 A JP 59119049A JP 11904984 A JP11904984 A JP 11904984A JP S60263413 A JPS60263413 A JP S60263413A
Authority
JP
Japan
Prior art keywords
frequency
welding
iron core
magnetic material
amorphous metal
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.)
Granted
Application number
JP59119049A
Other languages
Japanese (ja)
Other versions
JPH0552651B2 (en
Inventor
Hideyuki Koyama
秀行 小山
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial 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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP59119049A priority Critical patent/JPS60263413A/en
Publication of JPS60263413A publication Critical patent/JPS60263413A/en
Publication of JPH0552651B2 publication Critical patent/JPH0552651B2/ja
Granted legal-status Critical Current

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  • Arc Welding Control (AREA)

Abstract

PURPOSE:To reduce weight of an iron core by using an amorphous metal magnetic mateial for the iron core of an insulating transformer for welding, determining the value of frequency (f) satisfying the specific relation, and the weight of the iron core to be less than a half of a rated input. CONSTITUTION:A frequency conversion circuit 6 is provided at linear side of the insulating transformer 2 for welding, which is supplied with a power source of a cycle (f)Hz higher than a commercial cycle (f0)Hz. The amorphous metal magnetic material can be used for the iron core in this kind of the arc welder. In case of setting an iron loss (w/kg) value at frequency (f0) and (f) to be Pio and Pi when a flux density of the amorphous metal magnetic material is fixed, the value of frequency (f) is determined to be (Pi/Pio)/(f/f0)<=1. Besides, the relation between a weight Akg of the iron core of the insulating transformer 2 for welding and a rated input capacity BkVA becomes A<=B/2.

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は、小形軽量化を目的とした経済的な設計製作の
できるアーク溶接機に関するものである。
DETAILED DESCRIPTION OF THE INVENTION (Field of Industrial Application) The present invention relates to an arc welding machine that can be economically designed and manufactured with the aim of reducing size and weight.

(従来例の構成とその問題点) 従来のアーク溶接機は、第1図に示すように商用周波数
電源入力端子11溶接用絶縁変圧器2、整流器3、リア
クトル4、出力端子5等を備え、商用周波数の電源がそ
の壕ま、溶接用絶縁変圧器2に印加されるものがほとん
どであり、したがって、この場合の溶接用絶縁変圧器2
は、商用周波r 9 ) 数で設計されたものが使用されている。
(Configuration of conventional example and its problems) As shown in FIG. 1, a conventional arc welding machine is equipped with a commercial frequency power input terminal 11, a welding isolation transformer 2, a rectifier 3, a reactor 4, an output terminal 5, etc. In most cases, a commercial frequency power source is applied to the welding isolation transformer 2, and therefore, in this case, the welding isolation transformer 2
The one designed at the commercial frequency r 9 ) is used.

ところで、最近、第2図に示すように溶接用絶縁変圧器
2の一次側に、周波数変換回路6を接続し、商用周波数
より、高い周波数の電源を溶接用絶縁変圧器の一次側に
供給するようにしたアーク溶接機が製作されるようにな
って来た。
By the way, recently, as shown in Fig. 2, a frequency conversion circuit 6 has been connected to the primary side of the welding insulation transformer 2, and a power source with a frequency higher than the commercial frequency is supplied to the primary side of the welding insulation transformer 2. Arc welding machines with this type of technology have begun to be manufactured.

第2図に示すような、周波数変換回路6によシ、溶接用
絶縁変圧器2の一次側に高周波数の電源を供給すると、
変圧器2の起電力Eは下記の理論式%式%(1) ) により、巻数N、磁束密度Bmを一定と仮定すれば、周
波数fに比例して鉄芯断面積Sを小さくすることができ
る。したがって、周波数変換回路により、高周波数の電
源を、溶接用絶縁変圧器の一次側に供給することにより
、溶接用絶縁変圧器2の小形” 軽量化を図ることがで
きる利点があるため、最近は、この方式がアーク溶接機
にも採用されるようになって来た。
When a high frequency power source is supplied to the primary side of the welding isolation transformer 2 through the frequency conversion circuit 6 as shown in FIG.
The electromotive force E of the transformer 2 is determined by the following theoretical formula (% formula % (1)). Assuming that the number of turns N and the magnetic flux density Bm are constant, the cross-sectional area S of the iron core can be reduced in proportion to the frequency f. can. Therefore, by supplying high-frequency power to the primary side of the welding isolation transformer 2 using a frequency conversion circuit, there is an advantage that the welding isolation transformer 2 can be made smaller and lighter. This method has also come to be used in arc welding machines.

しかし々から、こうした溶接用変圧器に使用される鉄芯
の磁性材料としては、従来は硅素鋼板による磁性材料を
使用したものがほとんどである。
However, most of the magnetic materials for the iron cores used in such welding transformers have conventionally been made from silicon steel plates.

そのため硅素鋼板による磁性材料では、鉄損に問題があ
り、溶接用絶縁変圧器の小形軽量化に限界があった。
Therefore, magnetic materials made of silicon steel plates have problems with iron loss, and there are limits to how small and lightweight welding insulating transformers can be made.

すなわち、一般には硅素鋼板の鉄損は次式で計算される
That is, generally, the iron loss of a silicon steel plate is calculated by the following formula.

P、 = Ph+ P8(w/kg) ・・・・・・(
2)f 1゛6 ・・・・・・(3) Ph=σ5・■・Bm(W/kg) p、 =σe(t’ 100 ”f・Bm)2(WAg
)・・・(4)(Pl;鉄損、 ph:ヒステリシス損
、P8;うず電流積、σ5・σ。は材料による定数、f
;周波数。
P, = Ph+ P8 (w/kg) ・・・・・・(
2) f 1゛6 ・・・・・・(3) Ph=σ5・■・Bm(W/kg) p, =σe(t' 100 ”f・Bm)2(WAg
)...(4) (Pl: iron loss, ph: hysteresis loss, P8: eddy current product, σ5・σ. is a constant depending on the material, f
;frequency.

t;鉄芯の厚み、 kf;波形率’ Bm ;最大磁束
密度) 上記(4)式より、うず電流積Peは周波数の2乗に比
例するため、周波数が高くなればなるほど、うず電流積
Peが増える。また、ヒステリシス損へも、周波数に比
例するため、周波数が高くなれば、ヒステリシス損P、
が増加し、したがって、(2)式より鉄損Piは、周波
数が高くなればなるほど増大する。このため、従来の硅
素鋼板による磁性材料では、周波数を高くしても、鉄芯
断面積を(1)式にもとづいて、小さくすることが出来
ない。したがって第2図に示す回路構成において、周波
数変換装置により、高い電源周波数を溶接用絶縁変圧器
に供給する方法のメリットが生かされない。また、磁束
密度を低くするために、巻数を多くすれば、巻線の使用
量が増えて、コストアップになり、巻線工数も上昇し、
安価な溶接用絶縁変圧器が供給できないという欠点があ
った。
t: Thickness of the iron core, kf: Waveform ratio 'Bm: Maximum magnetic flux density) From the above equation (4), the eddy current product Pe is proportional to the square of the frequency, so the higher the frequency, the smaller the eddy current product Pe. increases. In addition, since the hysteresis loss is proportional to the frequency, the higher the frequency, the hysteresis loss P,
Therefore, from equation (2), the iron loss Pi increases as the frequency becomes higher. For this reason, with conventional magnetic materials made of silicon steel plates, even if the frequency is increased, the cross-sectional area of the iron core cannot be reduced based on equation (1). Therefore, in the circuit configuration shown in FIG. 2, the advantage of the method of supplying a high power frequency to the welding isolation transformer using the frequency converter cannot be utilized. In addition, if the number of turns is increased in order to lower the magnetic flux density, the amount of winding wire used will increase, which will increase costs and increase the number of winding man-hours.
There was a drawback that inexpensive insulating transformers for welding could not be supplied.

(発明の目的) 本発明は、上記のような従来の欠点を解決し、必要以下
に鉄芯断面積を大きくせずに、小形軽量で効率のよい経
済的々溶接用絶縁変圧器を有するアーク溶接機を提供し
ようとするものである。
(Object of the Invention) The present invention solves the above-mentioned conventional drawbacks, and provides an arc welding insulation transformer that is small, lightweight, efficient, and economical without increasing the cross-sectional area of the iron core more than necessary. The company aims to provide welding machines.

(発明の構成) 本発明の第1の態様は、溶接用絶縁変圧器の一次側に、
周波数変換回路を有し、商用周波数f。
(Structure of the Invention) A first aspect of the present invention is that on the primary side of an insulating transformer for welding,
It has a frequency conversion circuit, and the commercial frequency f.

(5) (Hz)より高い周波数/(Hz )の電源を、前記溶
接用絶縁変圧器に供給するように構成したアーク溶接機
において、前記溶接用絶縁変圧器の鉄芯に非晶質金属磁
性材料を用い、前記非晶質金属磁性材料の磁束密度を一
定としたときの、前記周波数f。
(5) In an arc welding machine configured to supply a power source with a frequency higher than (Hz) to the welding insulating transformer, an amorphous metal magnetic material is provided in the iron core of the welding insulating transformer. The frequency f when the magnetic flux density of the amorphous metal magnetic material is constant.

fの値を定め、かつ、前記溶接用絶縁変圧器の鉄芯の重
量A(kg)と、定格入力容量B (KVA)との関係
が、A≦1となるようにしたことを特徴とする。
The value of f is determined, and the relationship between the weight A (kg) of the iron core of the welding insulating transformer and the rated input capacity B (KVA) is such that A≦1. .

2 となるよう溶接用絶縁変圧器の鉄芯重量A (kg)と
定格入力容量Bを設定したことを特徴とする。
The present invention is characterized in that the iron core weight A (kg) and rated input capacity B of the welding insulating transformer are set so as to be 2.

(6) (実施例の説明) 周波数の高い領域においても鉄損の少い磁性材料として
、非晶質金属(アモルファス)による磁性材料があげら
れる。従来の硅素鋼板と、非晶質金属磁性材料の鉄損の
特性比較を第3図および第4図により示す。第3図およ
び第4図かられかるように、非晶質金属磁性材料の鉄損
は、硅素鋼板のそれに比べて小さい。したがって、磁性
材料を非晶質金属とすれば、周波数を高くしても、鉄損
が少いため、必要以上に鉄芯断面積を大きくする必要が
なく、溶接用絶縁変圧器が小形軽量に製作できることに
よシ、第2図に示す構成の周波数変換回路を有するアー
ク溶接機が、小形軽量化して提供できる。すなわち、第
3図および第4図より、非晶質金属磁性材料は、硅素鋼
板の約1/4以下の鉄損であり、他の条件が同一であれ
ば、鉄芯重量も約1/4以下にすることが可能である。
(6) (Description of Examples) As a magnetic material with low core loss even in a high frequency range, a magnetic material made of amorphous metal can be mentioned. A comparison of the core loss characteristics of a conventional silicon steel plate and an amorphous metal magnetic material is shown in FIGS. 3 and 4. As can be seen from FIGS. 3 and 4, the core loss of the amorphous metal magnetic material is smaller than that of the silicon steel plate. Therefore, if the magnetic material is an amorphous metal, the iron loss will be small even if the frequency is increased, so there is no need to increase the cross-sectional area of the iron core more than necessary, and the insulating transformer for welding can be made smaller and lighter. As a result, an arc welding machine having a frequency conversion circuit having the configuration shown in FIG. 2 can be provided in a smaller size and lighter weight. That is, from FIG. 3 and FIG. 4, the iron loss of amorphous metal magnetic material is about 1/4 or less of silicon steel plate, and if other conditions are the same, the iron core weight is also about 1/4 It is possible to do the following.

8 第5図は、従来の硅素鋼板を磁性材料に用いた溶接
用絶縁変圧器の、入力KVAと鉄芯重量との関係を示し
た一例である。第5図に示すように、硅素鋼板による鉄
芯の重量の1g値をA1人力KKVA値Bとすると、A
はBの約2倍(A≧2B)である。したがって第3図お
よび第4図より、非晶質金属磁性材料による鉄芯の重量
をA′とするとΔ′ユニ 10091111.(5) 4 であるから(5)式にA≧2Bを代入すると、A′さ工
すなわちA′≧旦 ・・・(6)2B−42 となり、鉄芯重量A′は入力KVA値Bの約1/2とな
る。
8 FIG. 5 is an example showing the relationship between the input KVA and the iron core weight of a conventional welding insulation transformer using a silicon steel plate as the magnetic material. As shown in Figure 5, if the 1g value of the weight of the iron core made of silicon steel plate is A1 manual KKVA value B, then A
is approximately twice as large as B (A≧2B). Therefore, from FIGS. 3 and 4, if the weight of the iron core made of amorphous metal magnetic material is A', Δ'uni 10091111. (5) 4 Therefore, by substituting A≧2B into equation (5), we get A', that is, A'≧tan... (6) 2B-42, and the iron core weight A' is the input KVA value B. It will be about 1/2.

ところで、(1)式より周波数を高くすれば、鉄芯重量
は低減することが可能であるが、第6図に示すように、
周波数が高くなると、やはり鉄損が増加するので、(1
)武道りには鉄芯断面積を低減することができない。
By the way, the weight of the iron core can be reduced by increasing the frequency according to equation (1), but as shown in Figure 6,
As the frequency increases, the iron loss also increases, so (1
) It is not possible to reduce the cross-sectional area of the iron core in martial arts.

したがって、周波数を高くしだ率に対して、鉄損が増加
する率が少い範囲内で、周波数を設定する必要が生じて
くる。
Therefore, it becomes necessary to set the frequency within a range in which the rate at which the iron loss increases is small relative to the rate at which the frequency is increased.

すなわち、商用周波数fo時の鉄芯の鉄損CWA9 )
値をPloとし、第2図の周波数変換回路6により供給
される電源の周波数1時の鉄芯の鉄損(w/k17)値
をPiとすれば、鉄芯の磁束密度が一定の場合には、 の式が成り立つときのみ、鉄芯の断面積を減らすことが
可能である。また、鉄芯の断面積を同じとすれば の式が成り立つところまで、周波数fを高くすることが
できる。
In other words, the iron loss of the iron core at commercial frequency fo (CWA9)
If the value is Plo, and Pi is the iron loss (w/k17) value of the iron core when the frequency of the power supply supplied by the frequency conversion circuit 6 in Fig. 2 is 1, then when the magnetic flux density of the iron core is constant, It is possible to reduce the cross-sectional area of the iron core only when the formula holds true. Furthermore, the frequency f can be increased to the point where the equation holds if the cross-sectional areas of the iron cores are the same.

ある。第7図より、 の式が成り立つのは、はぼ周波数fが15 kHz以下
のところであることがわかる。
be. From FIG. 7, it can be seen that the equation holds true when the frequency f is 15 kHz or less.

(9) したがって(7)式より、鉄芯の磁束密度を一定とすれ
ば、周波数fが15 kHz ’!での範囲であれば、
第3図、第4図より非晶質金属の磁性材料を使用するこ
とにより、硅素鋼板を使用した時に比べて、鉄芯の重量
は約174以下の値を確保することが可能である。すな
わち(6)式より、A′≦旦が成り立つ溶接用絶縁変圧
器を製作することが可能となり、入力KVA値の1/2
以下の鉄芯重量(kl? )値という小形軽量化が可能
となる。
(9) Therefore, from equation (7), if the magnetic flux density of the iron core is constant, the frequency f is 15 kHz'! If it is within the range of
As shown in FIGS. 3 and 4, by using an amorphous metal magnetic material, it is possible to secure the weight of the iron core to be approximately 174 mm or less compared to when a silicon steel plate is used. In other words, from equation (6), it is possible to manufacture an insulating transformer for welding where A'≦tan holds, and 1/2 of the input KVA value.
It is possible to reduce the size and weight with the following iron core weight (kl?) value.

また、周波数fを15 kHz以上とした場合、すの式
が成り立つ範囲において、硅素鋼板に比べて非晶質金属
磁性材料の鉄芯を用いた場合の鉄芯型−X 2.74=
0.68 となり、硅素鋼板に比べて68係の鉄芯重量で製作する
ことが可能である。したがって、ここで(7)式に(6
)式を代入すると、 の式が成り立つ範囲内であれば、従来の硅素鋼板を鉄芯
に使用した溶接用絶縁変圧器の鉄芯重量より小形軽量と
することが可能であり、したがって、アーク溶接機の小
形軽量化が可能となる。
Furthermore, when the frequency f is set to 15 kHz or higher, within the range where the equation holds true, the iron core type -X 2.74=
0.68, and it is possible to manufacture the iron core with a weight of 68 mm compared to silicon steel plate. Therefore, here, in equation (7), (6
) If the formula holds true, it is possible to make the core smaller and lighter than the core weight of a conventional welding insulating transformer that uses a silicon steel plate for the core, and therefore arc welding This allows the machine to be made smaller and lighter.

(発明の効果) 以上に詳述したように、本発明は溶接用絶縁質≦1を満
足するよう周波数fの値を定め、かつA≦−を満足する
よう鉄芯の重量Aと定格人力Bを定めたことにより鉄芯
の重量を著しく低減させることかでき、とくに周波数f
が比較的低い領域例えば15 kHz以下においてその
効果はとくに顕著である。
(Effects of the Invention) As detailed above, the present invention determines the value of the frequency f so that the welding insulation quality≦1, and the weight A of the iron core and the rated human power B so that A≦− is satisfied. By determining this, the weight of the iron core can be significantly reduced, especially when the frequency
The effect is particularly remarkable in a region where the frequency is relatively low, for example, below 15 kHz.

鉄芯重量Aと定格人力Bを設定することにより、鉄芯重
量を低減でき、とくに比較的高い周波数領域例えば15
 kHz以上においてより有効である。
By setting the iron core weight A and the rated manpower B, the iron core weight can be reduced, especially in a relatively high frequency range, e.g.
It is more effective at frequencies above kHz.

また、以上のように、溶接用絶縁変圧器が、小形軽量に
なれば、巻線の使用量も低減するので、巻線コストが安
価になると同時に、ロスが低減するので、省電力となり
、経済性に富んだアーク溶接機を提供することができる
In addition, as described above, if the welding insulation transformer becomes smaller and lighter, the amount of winding wire used will be reduced, which will reduce the winding cost and reduce loss, resulting in power savings and economical. It is possible to provide an arc welding machine with rich characteristics.

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

第1図は従来のアーク溶接機の構成例を示す。 第2図は周波数変換回路を有するアーク溶接機の構成例
を示す。 第3図および第4図は、硅素鋼と非晶質金属磁性材料の
鉄損の比較例を示す。 第5図は硅素鋼を鉄芯に使用した従来のアーク溶接機の
溶接用絶縁変圧器の鉄芯重量と定格入力容量(KVA 
)との関係の一例を示す。 第6図は非晶質金属磁性材料の鉄損と周波数の関係の一
例を示す。 第7図は第6図に示す非晶質金属磁性材料の鉄めて表示
した図を示す。 (13) 第1図 第2図 第5図 入力にVAB(にVA)− 第6図 磁木卵度(Tesla) − (−ウェーバ/m2)
FIG. 1 shows an example of the configuration of a conventional arc welding machine. FIG. 2 shows an example of the configuration of an arc welding machine having a frequency conversion circuit. FIGS. 3 and 4 show comparative examples of iron loss between silicon steel and amorphous metal magnetic material. Figure 5 shows the iron core weight and rated input capacity (KVA) of a welding insulation transformer for a conventional arc welding machine that uses silicon steel for the iron core.
) is shown below. FIG. 6 shows an example of the relationship between core loss and frequency of an amorphous metallic magnetic material. FIG. 7 shows a schematic diagram of the amorphous metal magnetic material shown in FIG. 6. (13) Figure 1 Figure 2 Figure 5 Input VAB (to VA) - Figure 6 Magnetic tree density (Tesla) - (-Weber/m2)

Claims (2)

【特許請求の範囲】[Claims] (1)溶接用絶縁変圧器の一次側に、周波数変換回路を
有し、商用周波数f (H2)よシ高い周波数f(Hz
)の電源を、前記溶接用絶縁変圧器に供給するように構
成したアーク溶接機において、前記溶接用絶縁変圧器の
鉄芯に非晶質金属磁性材料を用い、前記非晶質金属磁性
材料の磁束密度を一定としたなるようにfの値を定め、
かつ、前記溶接用絶縁変圧器の鉄芯の重量A (ky)
と、定格入力容量B(KVA)との関係が、A≦7とな
るよう如したことを特徴とするアーク溶接機。
(1) The primary side of the welding isolation transformer has a frequency conversion circuit, which converts the frequency f (Hz) higher than the commercial frequency f (H2).
) in an arc welding machine configured to supply a power source to the welding insulating transformer, an amorphous metal magnetic material is used for the iron core of the welding insulating transformer, and the amorphous metal magnetic material is The value of f is determined so that the magnetic flux density is constant,
and the weight A (ky) of the iron core of the welding insulation transformer.
and rated input capacity B (KVA) such that A≦7.
(2)溶接用絶縁変圧器の一次側に、周波数変換回路を
有し、商用周波数f(Hz)より高い周波数f(Hz 
)の電源を、前記溶接用絶縁変圧器に供給する(1) ように構成したアーク溶接機において、前記溶接用絶縁
変圧器の鉄芯に非晶質金属磁性材料を用い、前記非晶質
金属磁性材料の磁束密度を一定としたとなるようにfの
値を定め、かつ、前記溶接用絶うにしたことを特徴とす
るアーク溶接機。
(2) A frequency conversion circuit is provided on the primary side of the welding isolation transformer, and a frequency f (Hz) higher than the commercial frequency f (Hz) is provided.
) is supplied to the welding insulating transformer (1), in which an amorphous metal magnetic material is used for the iron core of the welding insulating transformer, An arc welding machine characterized in that the value of f is determined so that the magnetic flux density of the magnetic material is constant, and the arc welding machine is configured to be used for welding.
JP59119049A 1984-06-12 1984-06-12 Arc welder Granted JPS60263413A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP59119049A JPS60263413A (en) 1984-06-12 1984-06-12 Arc welder

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP59119049A JPS60263413A (en) 1984-06-12 1984-06-12 Arc welder

Publications (2)

Publication Number Publication Date
JPS60263413A true JPS60263413A (en) 1985-12-26
JPH0552651B2 JPH0552651B2 (en) 1993-08-06

Family

ID=14751637

Family Applications (1)

Application Number Title Priority Date Filing Date
JP59119049A Granted JPS60263413A (en) 1984-06-12 1984-06-12 Arc welder

Country Status (1)

Country Link
JP (1) JPS60263413A (en)

Also Published As

Publication number Publication date
JPH0552651B2 (en) 1993-08-06

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