JPS6233728B2 - - Google Patents
Info
- Publication number
- JPS6233728B2 JPS6233728B2 JP56081304A JP8130481A JPS6233728B2 JP S6233728 B2 JPS6233728 B2 JP S6233728B2 JP 56081304 A JP56081304 A JP 56081304A JP 8130481 A JP8130481 A JP 8130481A JP S6233728 B2 JPS6233728 B2 JP S6233728B2
- Authority
- JP
- Japan
- Prior art keywords
- iron
- silicon steel
- phase transformer
- highly oriented
- magnetic flux
- 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
Links
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F27/00—Details of transformers or inductances, in general
- H01F27/24—Magnetic cores
- H01F27/245—Magnetic cores made from sheets, e.g. grain-oriented
Landscapes
- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Soft Magnetic Materials (AREA)
- Manufacturing Cores, Coils, And Magnets (AREA)
Description
【発明の詳細な説明】
本発明は、鉄損失を低減することを目的として
微小歪が付与された電気鉄板を積層して構成され
た中央脚鉄を有する三相変圧器鉄心に関するもの
である。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a three-phase transformer core having a central leg iron constructed by laminating electrical iron plates to which minute strains are applied for the purpose of reducing iron loss.
従来、この種の鉄心としては、例えば、添付図
面第1図に示すようなものがあつた。すなわち図
において符号1及び2は外側脚鉄、3は中央脚
鉄、4及び5は上継鉄、6及び7は下継鉄で、所
定の形状に切断された電気鉄板を積層して形成さ
れている。ここで、実線は最上層の鉄心素片を示
し、点線はその次の層の最上層と異なつた部分を
示すものである。これらの電気鉄板としては、一
般的に一方向性ケイ素鋼板が使用されるが、一方
向性ケイ素鋼板の進歩はめざましく、近年では、
さらに一方向への配向性を高めた高配向性ケイ素
鋼板が使用されるようになつた。高配向性ケイ素
鋼板は、従来の一方向性ケイ素鋼板より圧延方向
の配向性が向上しているため、圧延方向に磁化し
た場合の磁気特性は向上する。しかし、それに反
して圧延方向よりずれた方向の磁気特性は悪くな
る。従つて、三相変圧器鉄心にこの高配向性ケイ
素鋼板を用いた場合には、一方向性ケイ素鋼板を
用いた場合より変圧器鉄心全体の鉄損失は低下す
るものの、鉄損失のビルデイングフアクターが極
度に悪くなるという欠点があつた。これは、一つ
には高配向性ケイ素鋼板の場合には、従来の一方
向性ケイ素鋼板に比較して中央脚鉄3の磁束波形
の歪が大きくなるためである。第2図にこのよう
な中央脚鉄3の磁束波形の例を示す。図におい
て、曲線aは高配向性ケイ素鋼板を使用した場合
の磁束波形を、また、曲線bは従来の一方向性ケ
イ素鋼板を使用した場合の磁束波形を示すもので
ある。いま、両者を比較すると、高配向性ケイ素
鋼板を使用した場合の磁束波形aは台形に近い形
状を示してあり、磁束波形の歪の大きいことがわ
かる。この磁束波形の歪は、三相励磁において中
央脚鉄3が励磁されていない状態での中央脚鉄3
への磁束の流入に起因しており、従来の一方向性
ケイ素鋼板に比較して高配向性ケイ素鋼板の方が
この傾向が大きいことを示している。第3図は、
外側脚鉄1及び2が励磁されており、且つ、中央
脚鉄3が励磁されていない状態の等ベクトルポテ
ンシヤル線8を有限要素法を用いて解析した図で
あつて、これによると中央脚鉄3への磁束の流入
が認められる。磁束波形の歪は、鉄損失成分の内
のうず電流損失成分を増大させるものである。ま
た、高配向性ケイ素鋼板の場合には、従来の一方
向性ケイ素鋼板に比較して、磁区幅が大きいた
め、全鉄損失に対して、うず電流損失の占める割
合が大きい。このことも高配向性ケイ素鋼板の鉄
損失のビルデイングフアクターを悪くする原因と
なつている。次に第4図は、高配向性ケイ素鋼板
を用いた三相変圧器鉄心と従来の一方向性ケイ素
鋼板を用いた三相変圧器鉄心との各脚鉄及び継鉄
における鉄損失のビルデイングフアクターを有限
要素法を用いて解析した結果であつて、このビル
デイングフアクターを示す数値の上段は高配向性
ケイ素鋼板の場合を、また、下段は従来の一方向
性ケイ素鋼板の場合を、それぞれの場所において
示すものである。なお、この図は三相変圧器鉄心
の上半分のみを示している。このように、高配向
性ケイ素鋼板を用いた三相変圧器鉄心は、中央脚
鉄3の鉄損失のビルデイングフアクターが極度に
悪くなるため、高配向性ケイ素鋼板の低鉄損失特
性が生かせず、経済的にも不利になるという欠点
があつた。 Conventionally, this type of iron core has been, for example, as shown in FIG. 1 of the accompanying drawings. That is, in the figure, numerals 1 and 2 are outer leg irons, 3 is center leg iron, 4 and 5 are upper yoke irons, and 6 and 7 are lower yoke irons, which are formed by laminating electrical iron plates cut into a predetermined shape. ing. Here, the solid line indicates the core piece of the top layer, and the dotted line indicates the portion of the next layer that is different from the top layer. Unidirectional silicon steel sheets are generally used as these electrical iron plates, but progress in unidirectional silicon steel sheets has been remarkable, and in recent years,
Furthermore, highly oriented silicon steel sheets with improved orientation in one direction have come into use. Since the highly oriented silicon steel sheet has improved orientation in the rolling direction compared to conventional unidirectional silicon steel sheets, its magnetic properties when magnetized in the rolling direction are improved. However, on the other hand, the magnetic properties in directions deviated from the rolling direction become worse. Therefore, when this highly oriented silicon steel sheet is used in the core of a three-phase transformer, the iron loss of the entire transformer core is lower than when a unidirectional silicon steel sheet is used, but the building factor of iron loss is The drawback was that it became extremely bad. One reason for this is that in the case of a highly oriented silicon steel plate, the distortion of the magnetic flux waveform of the central leg iron 3 is greater than that in a conventional unidirectional silicon steel plate. FIG. 2 shows an example of the magnetic flux waveform of such a central leg iron 3. In the figure, curve a shows the magnetic flux waveform when a highly oriented silicon steel plate is used, and curve b shows the magnetic flux waveform when a conventional unidirectional silicon steel plate is used. Now, when comparing the two, it can be seen that the magnetic flux waveform a when a highly oriented silicon steel plate is used has a shape close to a trapezoid, indicating that the distortion of the magnetic flux waveform is large. This distortion of the magnetic flux waveform is caused by the distortion of the central leg iron 3 when the central leg iron 3 is not excited during three-phase excitation.
This is due to the inflow of magnetic flux into the unidirectional silicon steel sheet, and this tendency is greater in the highly oriented silicon steel sheet than in the conventional unidirectional silicon steel sheet. Figure 3 shows
This is a diagram obtained by analyzing the equivector potential line 8 using the finite element method when the outer leg irons 1 and 2 are energized and the center leg iron 3 is not energized. An inflow of magnetic flux into 3 is observed. Distortion of the magnetic flux waveform increases the eddy current loss component of the iron loss components. Further, in the case of a highly oriented silicon steel sheet, the magnetic domain width is larger than that of a conventional unidirectional silicon steel sheet, so that the eddy current loss accounts for a large proportion of the total iron loss. This also causes a worsening of the iron loss building factor of the highly oriented silicon steel sheet. Next, Figure 4 shows the building graph of iron loss in each leg and yoke of a three-phase transformer core using highly oriented silicon steel sheets and a conventional three-phase transformer core using unidirectional silicon steel sheets. These are the results of analyzing the actor using the finite element method. The upper row of numerical values indicating this building factor is for the case of highly oriented silicon steel sheet, and the lower row is for the case of conventional unidirectional silicon steel sheet. This is shown at the location. Note that this figure shows only the upper half of the three-phase transformer core. In this way, three-phase transformer cores using highly oriented silicon steel sheets have an extremely poor building factor for iron loss in the central leg iron 3, making it impossible to take advantage of the low iron loss characteristics of highly oriented silicon steel sheets. However, it also had the disadvantage of being economically disadvantageous.
本発明は、上記のような三相変圧器における従
来の欠点を除去した鉄損失を低減して中央脚鉄の
鉄損失のビルデイングフアクターを改善し、これ
によつて、省エネルギー、省コストな三相電磁誘
導機器鉄心である三相変圧器鉄心を提供すること
を、その目的とするものである。 The present invention eliminates the conventional drawbacks in three-phase transformers, reduces iron loss, and improves the building factor of iron loss in the central leg iron, thereby creating an energy-saving and cost-saving three-phase transformer. The purpose is to provide a three-phase transformer core that is a phase electromagnetic induction equipment core.
本発明はこの目的を達成するために、三相変圧
器鉄心の中央脚鉄以外の部位には高透磁率、低鉄
損失の高配向性ケイ素鋼板を適用し、中央脚鉄に
は圧延方向に対して直角方向に線状の微小歪を付
与して低透磁率、低鉄損失とした高配向性ケイ素
鋼板を積層して構成したことを特徴とするもので
ある。 In order to achieve this object, the present invention applies a highly oriented silicon steel plate with high magnetic permeability and low iron loss to the parts of the three-phase transformer core other than the central leg iron, and the central leg iron It is characterized by being constructed by laminating highly oriented silicon steel plates with low magnetic permeability and low iron loss by applying linear minute strain in the direction perpendicular to the other.
この微小歪を付与することによる作用につい
て、次に説明しておく。 The effect of applying this minute strain will be explained next.
線状の微小歪を付与した高配向性ケイ素鋼板
は、鉄損失成分の内、ヒステリシス損は増加させ
ず、磁区を細分化させて、うず電流損を低下させ
ることにより、鉄損失を低減させている。この場
合、微小歪を付与していることから透磁率は低下
している。すなわち、鋼板に歪を付与するという
ことは、鋼板に機械的な内部応力を残すことであ
り、透磁率の低下となる。この透磁率の低下は、
一般的に、この内部応力に起因する反磁場による
静磁エネルギーを緩和するために形成される還流
磁区及び反転磁区の形成によるものと説明されて
いる。 Highly oriented silicon steel sheet with linear microstrain does not increase hysteresis loss among iron loss components, but subdivides magnetic domains to reduce eddy current loss, thereby reducing iron loss. There is. In this case, the magnetic permeability is reduced because minute strain is applied. That is, applying strain to a steel plate means that mechanical internal stress remains in the steel plate, resulting in a decrease in magnetic permeability. This decrease in magnetic permeability is
Generally, it is explained that this is due to the formation of a reflux magnetic domain and a reversal magnetic domain, which are formed to relieve the magnetostatic energy due to the demagnetizing field caused by this internal stress.
従つて、透磁率は、以上の理由により低下する
が、内部応力に起因していることから、当然のこ
とながら、微小歪の間隔(物理的な距離)に依存
している。この微小歪の間隔が10mmを越えるよう
なものであれば、透磁率の低下はわずかである
が、例えば、5mm位であれば約30%も低下する。
このように、透磁率の低下の度合いは付与する微
小歪の間隔によつて異なる。従つて、線状の微小
歪を付与した高配向性ケイ素鋼板は、透磁率の低
下した低鉄損失材料すなわちうず電流損の小さい
材料といえる。 Therefore, the magnetic permeability decreases for the above reasons, but since it is caused by internal stress, it naturally depends on the interval (physical distance) between the minute strains. If the distance between the microstrains exceeds 10 mm, the magnetic permeability decreases only slightly, but if the distance is about 5 mm, for example, the permeability decreases by about 30%.
In this way, the degree of decrease in magnetic permeability varies depending on the interval between the applied microstrains. Therefore, a highly oriented silicon steel sheet with linear microstrain can be said to be a low iron loss material with reduced magnetic permeability, that is, a material with small eddy current loss.
このことは、三相電磁誘導機器鉄心の中央脚鉄
に使用するには都合が良い。すなわち、中央脚鉄
では、中央脚鉄が励磁されていない場合の磁束の
進入のため磁束が歪むが、磁束が歪むと、その高
調波成分のため素材のうず電流損が増加する。こ
れを防止するには、磁束の進入を防ぐために、中
央脚鉄の透磁率を低く、すなわち、磁気抵抗を大
きくし、かつ、磁束波形が歪んでも、鉄損失が増
加しない、すなわち、うず電流損成分の低い材料
を使用することが好ましい。 This is convenient for use in the central leg iron of a three-phase electromagnetic induction equipment core. That is, in the center leg iron, the magnetic flux is distorted due to the intrusion of the magnetic flux when the center leg iron is not excited, but when the magnetic flux is distorted, the eddy current loss in the material increases due to its harmonic components. To prevent this, in order to prevent magnetic flux from entering, the permeability of the central leg iron should be made low, that is, the magnetic resistance should be made large, and even if the magnetic flux waveform is distorted, iron loss will not increase, that is, eddy current loss. It is preferable to use materials with low constituents.
また、より低鉄損失効果を出すために、元の素
材自身の鉄損失も低いことが好ましい。 Furthermore, in order to achieve a lower iron loss effect, it is preferable that the iron loss of the original material itself is also low.
上記の作用等を勘案して、本発明は構成されて
いる。 The present invention has been constructed in consideration of the above effects and the like.
以下、本発明をその一実施例を示す添付図面に
基づいて説明する。 DESCRIPTION OF THE PREFERRED EMBODIMENTS The present invention will be described below with reference to the accompanying drawings showing one embodiment thereof.
第5図は、中央脚鉄11を、磁化方向と直角に
線状の微小歪12が付与された電気鉄板を積層し
て構成した三相変圧器鉄心の一例である。このこ
とは、一方向性ケイ素鋼板に、圧延方向と直角方
向に適当な線状の微小歪を付与すると、その180
゜磁区が細分化されるために、鉄損失、特に、そ
の成分であるうず電流損失が低減すると言われて
おり、この効果は、特に、磁区幅の大きい高配向
性ケイ素鋼板に著しいことを利用するものであつ
て、この線状の微小歪が付与された電気鉄板を、
歪波磁束の発生する中央脚鉄11として積層し構
成することによつて、基本波磁束によるうず電流
損失を低減させるだけでなく、歪波磁束の高調波
成分によるうず電流損失も低減させるものであ
る。また、圧延方向(磁化方向)と直角方向に付
与された線状の微小歪のために、上記のことから
例えばその微小歪の間隔を5〜10mmとすると、透
磁率が25%小さくなるため、中央脚鉄11が励磁
されていない状態の中央脚鉄11への磁束の流入
が減少し、中央脚鉄11の磁束波形の歪が緩和さ
れる。この結果、一方向性ケイ素鋼板、特に高配
向性ケイ素鋼板を用いた三相変圧器鉄心の中央脚
鉄の鉄損失のビルデイングフアクターが改善され
る。第6図には、中央脚鉄11に線状の微小歪が
付与された高配向性ケイ素鋼板を積層して形成し
た場合の鉄損失のビルデイングフアクターの計算
結果を示すものであつて、その中央脚鉄11の鉄
損失のビルデイングフアクターは、第4図に示す
従来の高配向性ケイ素鋼板によつて構成されたも
のに対して、ほぼ7.5%改善されている。 FIG. 5 shows an example of a three-phase transformer core in which the central leg iron 11 is constructed by laminating electric iron plates to which a linear minute strain 12 is applied perpendicular to the magnetization direction. This means that when a suitable linear microstrain is applied to a unidirectional silicon steel sheet in the direction perpendicular to the rolling direction, the 180
It is said that iron loss, especially eddy current loss, which is a component of iron loss, is reduced because the magnetic domains are subdivided, and this effect is particularly noticeable in highly oriented silicon steel sheets with large magnetic domain widths. The electric iron plate to which this linear microstrain has been applied is
By laminating and configuring the central leg iron 11 where distorted wave magnetic flux is generated, it is possible to reduce not only eddy current loss due to fundamental wave magnetic flux but also eddy current loss due to harmonic components of distorted wave magnetic flux. be. In addition, due to the linear microstrain applied in the direction perpendicular to the rolling direction (magnetization direction), from the above, if the spacing between the microstrains is set to 5 to 10 mm, the magnetic permeability will decrease by 25%. The inflow of magnetic flux into the center leg iron 11 in a state where the center leg iron 11 is not excited is reduced, and the distortion of the magnetic flux waveform of the center leg iron 11 is alleviated. As a result, the building factor of iron loss in the central leg iron of a three-phase transformer core using a unidirectional silicon steel plate, particularly a highly oriented silicon steel plate, is improved. FIG. 6 shows the calculation results of the building factor of iron loss when the center leg iron 11 is formed by laminating highly oriented silicon steel plates to which linear microstrain is applied. The building factor of iron loss of the center leg iron 11 is improved by approximately 7.5% compared to that constructed from the conventional highly oriented silicon steel plate shown in FIG.
なお、上記実施例においては、いわゆるスクラ
ツプレス鉄心の中央脚鉄11を線状の微小歪12
の付与された鉄気鉄板を積層したものによつて構
成されたものの例を示したが、必ずしもこれに限
るものでなく、第7図に示すような鉄心の中央脚
鉄3′に、第8図に示す実施例のように、このよ
うな線状の微小歪22を中央脚鉄21に付与した
電気鉄板を積層して構成しても良く、この場合に
おいても、その効果は、上記実施例と同等の効果
を奏することができるものである。 In the above embodiment, the center leg iron 11 of the so-called scrap press iron core is subjected to linear minute strain 12.
Although we have shown an example of a structure made of laminated iron plates with a As in the embodiment shown in the figure, it may be constructed by laminating electric iron plates in which such a linear minute strain 22 is applied to the central leg iron 21. In this case as well, the effect is the same as that of the above embodiment. It is possible to achieve the same effect as.
以上のように、本発明によれば、三相変圧器鉄
心の中央脚鉄を、微小歪の付与された電気鉄板、
特に、高配向性ケイ素鋼板を積層したものによつ
て構成したために、三相変圧器鉄心の鉄損失のビ
ルデイングフアクターが改善され、従つて、特性
の良い変圧器が経済的に製作できる効果を、本発
明は有している。 As described above, according to the present invention, the central leg iron of the three-phase transformer iron core is formed of an electrical iron plate to which minute strain has been applied.
In particular, since the construction is made of laminated highly oriented silicon steel sheets, the building factor of iron loss in the three-phase transformer core is improved, and therefore a transformer with good characteristics can be manufactured economically. , the present invention has.
第1図は従来の三相変圧器鉄心を示す平面図、
第2図は第1図の三相変圧器鉄心の中央脚鉄の磁
束波形を示す曲線図、第3図は第1図の三相変圧
器鉄心の磁束分布を示す等ベクトルポテンシヤル
図、第4図は第1図の三相変圧器鉄心の鉄損失の
ビルデイングフアクターを示した説明図、第5図
は本発明の三相変圧器鉄心の一実施例を示す平面
図、第6図は第5図の三相変圧器鉄心の改善され
た鉄損失のビルデイングフアクターを示す説明
図、第7図は従来の他の三相変圧器鉄心を示す平
面図、第8図は本発明を従来の第7図の三相変圧
器鉄心に実施した平面図である。
図において、1,2は外側脚鉄、3,3′,1
1,21は中央脚鉄、4,5は上継鉄、6.7は
下継鉄、8は等ベクトルポテンシヤル線、12,
22は線状の微小歪である。
Figure 1 is a plan view showing the core of a conventional three-phase transformer.
Figure 2 is a curve diagram showing the magnetic flux waveform of the central leg iron of the three-phase transformer core in Figure 1, Figure 3 is an equivector potential diagram showing the magnetic flux distribution in the three-phase transformer core in Figure 1, and Figure 4 is an equivector potential diagram showing the magnetic flux distribution in the three-phase transformer core in Figure 1. The figure is an explanatory diagram showing the building factor of iron loss in the three-phase transformer core of Figure 1, Figure 5 is a plan view showing an embodiment of the three-phase transformer core of the present invention, and Figure 6 is the Fig. 5 is an explanatory diagram showing the improved iron loss building factor of the three-phase transformer core, Fig. 7 is a plan view showing another conventional three-phase transformer core, and Fig. 8 shows the present invention compared to the conventional three-phase transformer core. FIG. 8 is a plan view of the three-phase transformer core of FIG. 7; In the figure, 1 and 2 are outer leg irons, 3, 3', 1
1 and 21 are central leg irons, 4 and 5 are upper yoke irons, 6.7 are lower yoke irons, 8 is equal vector potential line, 12,
22 is a linear minute strain.
Claims (1)
して直角方向に線状の微小歪を付与した高配向性
ケイ素鋼板を積層して構成したことを特徴とする
三相変圧器鉄心。1. A three-phase transformer core, characterized in that the central leg iron of the three-phase transformer core is constructed by laminating highly oriented silicon steel plates to which linear microstrain is applied in a direction perpendicular to the rolling direction.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56081304A JPS57194507A (en) | 1981-05-26 | 1981-05-26 | Iron core of three-phase transformer |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56081304A JPS57194507A (en) | 1981-05-26 | 1981-05-26 | Iron core of three-phase transformer |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS57194507A JPS57194507A (en) | 1982-11-30 |
| JPS6233728B2 true JPS6233728B2 (en) | 1987-07-22 |
Family
ID=13742645
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP56081304A Granted JPS57194507A (en) | 1981-05-26 | 1981-05-26 | Iron core of three-phase transformer |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS57194507A (en) |
Families Citing this family (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN107275055A (en) * | 2017-05-12 | 2017-10-20 | 中科电力装备集团有限公司 | A kind of transformer iron-core structure |
| JP7427351B2 (en) * | 2017-12-05 | 2024-02-05 | 日本製鉄株式会社 | stacked iron core |
| CN109841400A (en) * | 2019-03-28 | 2019-06-04 | 广州增变电气有限公司 | A kind of assembly device and method of amorphous alloy transformer iron core |
| CN112550512B (en) * | 2020-12-09 | 2023-07-21 | 北京理工大学重庆创新中心 | A wheel-legged robot and its driving method |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5293917A (en) * | 1976-02-02 | 1977-08-08 | Hitachi Ltd | Three phase induction electrical apparatus iron core |
-
1981
- 1981-05-26 JP JP56081304A patent/JPS57194507A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS57194507A (en) | 1982-11-30 |
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