JPS62239511A - Stationary induction apparatus - Google Patents
Stationary induction apparatusInfo
- Publication number
- JPS62239511A JPS62239511A JP8213586A JP8213586A JPS62239511A JP S62239511 A JPS62239511 A JP S62239511A JP 8213586 A JP8213586 A JP 8213586A JP 8213586 A JP8213586 A JP 8213586A JP S62239511 A JPS62239511 A JP S62239511A
- Authority
- JP
- Japan
- Prior art keywords
- coil
- iron core
- magnetic field
- iron
- iron loss
- 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
- 230000006698 induction Effects 0.000 title claims abstract description 10
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical compound [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 claims abstract description 89
- 229910052742 iron Inorganic materials 0.000 abstract description 30
- 238000000034 method Methods 0.000 abstract description 4
- 230000005284 excitation Effects 0.000 abstract description 3
- 230000015572 biosynthetic process Effects 0.000 abstract 2
- 230000004907 flux Effects 0.000 description 9
- 238000010586 diagram Methods 0.000 description 4
- 238000004804 winding Methods 0.000 description 4
- 238000000137 annealing Methods 0.000 description 3
- 230000000694 effects Effects 0.000 description 3
- 238000010438 heat treatment Methods 0.000 description 3
- 239000000463 material Substances 0.000 description 3
- 238000011282 treatment Methods 0.000 description 3
- 230000002159 abnormal effect Effects 0.000 description 2
- 229910000976 Electrical steel Inorganic materials 0.000 description 1
- 239000003795 chemical substances by application Substances 0.000 description 1
- 229910001004 magnetic alloy Inorganic materials 0.000 description 1
- 230000005381 magnetic domain Effects 0.000 description 1
- 230000005415 magnetization Effects 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 230000002250 progressing effect Effects 0.000 description 1
- 238000007670 refining Methods 0.000 description 1
- 230000003068 static effect Effects 0.000 description 1
- 229910000859 α-Fe Inorganic materials 0.000 description 1
Landscapes
- Regulation Of General Use Transformers (AREA)
Abstract
Description
【発明の詳細な説明】
[発明の目的]
(産業上の利用分野)
本発明は変圧器及びリアクトルなどの静止形誘導機器に
関する。DETAILED DESCRIPTION OF THE INVENTION [Object of the Invention] (Field of Industrial Application) The present invention relates to stationary induction equipment such as transformers and reactors.
(従来の技術)
最近、静止形誘導機器においては、非晶質磁性合金いわ
ゆるアモルファスから成る薄帯を高周波鉄心として採用
することが考えられており、実用化がすすんで来ている
。このアモルファス薄帯は固有抵抗が比較的高いことか
ら高周波領域において鉄損が小さいことや、鉄をベース
としたアモルファスでは、特に飽和磁束密度とキュリ一
点とが高いことにより、鉄心の小形化及び高効率化に極
めて有効である。(Prior Art) Recently, in stationary induction devices, it has been considered to use a ribbon made of an amorphous magnetic alloy as a high-frequency iron core, and its practical use is progressing. This amorphous ribbon has a relatively high specific resistance, so iron loss is small in the high frequency range, and iron-based amorphous ribbons have a particularly high saturation magnetic flux density and Curie point, making it possible to miniaturize and increase the iron core. It is extremely effective in increasing efficiency.
ところで、鉄系アモルファスを鉄心に用いる場合には、
高周波領域での鉄損特性を低くするために、種々の処理
がなさている。By the way, when using iron-based amorphous for the iron core,
Various treatments have been used to reduce iron loss characteristics in the high frequency range.
(1)その一つとしては焼鈍といった熱処理を行なうよ
うにしている。この焼鈍の有用性は、アモルファスの製
作時における超急冷熱処理による歪みを除去し、これに
よりヒステリシス損失を減少させると共に、磁区の細分
化を図って磁壁付近の局所的な異常渦電流損失を減少さ
せるためにある。この異常渦電流損失は高周波領域の鉄
損に与える影響が大である。(1) One of the methods is to perform heat treatment such as annealing. The usefulness of this annealing is that it removes the distortion caused by the ultra-rapid heat treatment during amorphous manufacturing, thereby reducing hysteresis loss, and reducing local abnormal eddy current loss near the domain wall by refining the magnetic domain. It's for a purpose. This abnormal eddy current loss has a large effect on iron loss in the high frequency region.
(II)他の処理方式としては、種々あるが、例えば特
開昭59−148314号には、焼鈍時に圧縮力を加え
ることにより、10%程度の鉄損の改善を図るようにし
たものもある。(II) There are various other treatment methods, but for example, Japanese Patent Application Laid-Open No. 148314/1983 proposes a method that improves iron loss by about 10% by applying compressive force during annealing. .
(発明が解決しようとする問題点)
しかしながら、鉄損の減少を図るについて、上述したよ
うに種々の処理がなされているが、いずれも鉄損の低減
に限界があり、静止形誘導機器においては、さらに鉄損
を減少させることが要求されている。斯様な問題は鉄心
にアモルファス以外の材料からなるものを用いた場合に
も少ならからずいえることであった。(Problems to be Solved by the Invention) However, although various treatments have been carried out to reduce iron loss as described above, all of them have a limit to the reduction of iron loss, and in static induction equipment, , it is required to further reduce iron loss. Such problems also occur to some extent when iron cores made of materials other than amorphous are used.
そこで本発明の目的は、鉄心の鉄損を実質的に低減でき
て、鉄心の小形化及び高効率化をさらに図り得る静止形
誘導機器を提供するにある。SUMMARY OF THE INVENTION Accordingly, an object of the present invention is to provide a stationary induction device that can substantially reduce iron loss of an iron core, and further improve the size and efficiency of the iron core.
[発明の構成]
(問題点を解決するための手段)
本発明は、−次コイル及び二次コイルを巻回した鉄心に
直流磁界形成用コイルを巻回し、誘導機器使用時、この
直流磁界形成用コイルに直流電流を通電するようにした
ものである。[Structure of the Invention] (Means for Solving the Problems) The present invention provides for winding a coil for forming a DC magnetic field around an iron core around which a secondary coil and a secondary coil are wound, and when using an induction device, forming a DC magnetic field. A direct current is passed through the coil for use.
(作用)
直流磁界形成用コイルに直流を通電すると、鉄心は直流
磁界で励磁され、−次コイルに基づく交流励磁によって
発生するところの鉄損が低減し、以て動作時における鉄
損を低減できて、実質的な鉄損の低減を図るものである
。(Function) When direct current is applied to the coil for forming a direct current magnetic field, the iron core is excited by the direct current magnetic field, reducing the iron loss that would occur due to alternating current excitation based on the -order coil, thereby reducing iron loss during operation. This aims to substantially reduce iron loss.
(実施例) 以下本発明の一実施例につき図面を参照して説明する。(Example) An embodiment of the present invention will be described below with reference to the drawings.
まず第1図においては、全体を原理的に表わしており、
同図において、1は分割鉄心1a、lbから成る鉄心で
あり、これは例えばアライド社製アモルファス2605
S3Aというアモルファスの薄帯を連続的に巻回して成
る。分割鉄心1a、lbはその鉄心断面積を一方の分割
鉄心1aの断面積がA1他方の分割鉄心1bのそれがA
゛となるように設定しである。この鉄心1には共通に一
次コイル2及び二次コイル3が巻回されている。機器使
用時、−次コイル2に交流型#、4が人力されると、二
次コイル3に接続された負荷5に電力が供給される。6
は2個の分割コイル6a、6bからなる直流磁界形成用
コイルであり、これらは、鉄心1の分割鉄心1a、lb
にそれぞれ巻回されて直列に接続されており、その巻数
をN、If”とするとAN−A″N′となるように設定
しである。この直流磁界形成用コイル6は直流tli#
i7が印加されるようになっていると共に、その印加電
圧を調整するための可変抵抗8が接続されている。尚、
この場合、交流励磁は5 KHz。First of all, Figure 1 shows the whole in principle,
In the figure, 1 is an iron core consisting of split iron cores 1a and 1b, which is made of, for example, Amorphous 2605 manufactured by Allied Co., Ltd.
It is made by continuously winding an amorphous ribbon called S3A. The cross-sectional areas of the divided cores 1a and lb are as follows: One of the divided cores 1a has a cross-sectional area of A1, and the other of the divided cores 1b has a cross-sectional area of A.
The settings are as follows. A primary coil 2 and a secondary coil 3 are commonly wound around this iron core 1. When the device is in use, when AC type #, 4 is manually applied to the secondary coil 2, power is supplied to the load 5 connected to the secondary coil 3. 6
is a DC magnetic field forming coil consisting of two divided coils 6a and 6b, and these are the divided iron cores 1a and lb of the iron core 1.
The windings are respectively wound and connected in series, and the number of turns is set to be AN-A''N', where N and If'' are the winding numbers. This DC magnetic field forming coil 6 is a DC magnetic field forming coil 6.
i7 is applied, and a variable resistor 8 is connected to adjust the applied voltage. still,
In this case, the AC excitation is 5 KHz.
動作磁束密度は0.1、Q、3.0.4Tである。The operating magnetic flux density is 0.1, Q, 3.0.4T.
上記構成の本実施例において、機器使用時、交流電源4
を一次コイル2に与えると共に、直流電源7を直流磁界
形成用コイル6に与えると、第2図に示す特性が得られ
る。この第2図において、磁束密度を0.ITとし、横
軸には直流磁界(A/cm)、一方の縦軸には鉄損(W
/kg) 、他方の縦軸には騒音(dB)をとり、特性
線Jは鉄損変化を、又、特性線には騒音変化を夫々示し
ている。In this embodiment with the above configuration, when using the device, the AC power supply 4
When the voltage is applied to the primary coil 2 and the DC power source 7 is applied to the DC magnetic field forming coil 6, the characteristics shown in FIG. 2 are obtained. In this FIG. 2, the magnetic flux density is set to 0. IT, the horizontal axis is the DC magnetic field (A/cm), and the vertical axis is the iron loss (W
/kg), and the other vertical axis shows the noise (dB), the characteristic line J shows the iron loss change, and the characteristic line shows the noise change.
この場合、直流磁界形成用コイル6のうち一方の分割鉄
心1aに巻回された分割コイル6aと他方の分割鉄心1
bに巻回された分割コイル6bとにおいて、誘起される
電圧は絶対値が略等しく且つ位相が逆となるため、可変
抵抗8と直流電源7との端子間には電圧は発生せず、従
って負荷とはならない。面して、直流磁界形成用コイル
6に直流電源7により直流電流Iが流れ、これにより分
割鉄心1a、lbには夫々、N I/L、N−I/Lの
磁界が発生する(L:磁路長)。この磁界がO12〜1
. 6 (A/am)に収まるように可変抵抗8を調整
することで、鉄心1の鉄損を、磁界が0(A / cm
)の時の25%まで低減できる。In this case, the divided coil 6a wound around one divided core 1a of the DC magnetic field forming coil 6 and the other divided core 1
In the split coil 6b wound around the split coil 6b, the induced voltages have approximately the same absolute value and opposite phases, so no voltage is generated between the terminals of the variable resistor 8 and the DC power supply 7, and therefore It is not a load. Direct current I flows through the direct current magnetic field forming coil 6 from the direct current power source 7, thereby generating magnetic fields of N I/L and N-I/L in the divided iron cores 1a and lb, respectively (L: magnetic path length). This magnetic field is O12~1
.. By adjusting the variable resistor 8 so that the magnetic field falls within 0 (A/cm), the iron loss of the iron core 1 can be reduced to 0 (A/cm).
) can be reduced to 25%.
このように鉄損の低減を図り得るから、鉄心1の小形化
及び高効率化を図ることができる。Since iron loss can be reduced in this way, the iron core 1 can be made smaller and more efficient.
又、第2図から分るように、0. 25 (A/cm)
付近の直流磁界を得るように可変抵抗8等をシ!j節す
れば、騒音の低減を図ることができる。Also, as can be seen from Figure 2, 0. 25 (A/cm)
Set variable resistor 8 etc. to obtain a nearby DC magnetic field! Noise reduction can be achieved by setting the j section.
第3図は磁束密度が0.3T、0.4Tの時の鉄損特性
を示しており、特性線J1は磁束密度か0.3Tの場合
の鉄損特性を示し、特性線J2は磁束密度0.4Tの場
合の鉄損特性を示す。この第3図の場合、低鉄損が得ら
れる直流磁界領域が狭くなっているが、磁束密度が0.
7T以下であれば低鉄損の達成は図り得るものである。Figure 3 shows the iron loss characteristics when the magnetic flux density is 0.3T and 0.4T, the characteristic line J1 shows the iron loss characteristics when the magnetic flux density is 0.3T, and the characteristic line J2 shows the iron loss characteristics when the magnetic flux density is 0.3T. The iron loss characteristics in the case of 0.4T are shown. In the case of FIG. 3, the DC magnetic field region where low core loss can be obtained is narrow, but the magnetic flux density is 0.
If it is 7T or less, it is possible to achieve low iron loss.
尚、鉄心の祠質、熱処理条件、使用周波数、磁束密度に
よっても適正な直流磁界領域が異なるが、本実施例のよ
うに、可変抵抗8を調節することで、これに対処できる
。Note that the appropriate DC magnetic field range varies depending on the abrasive quality of the iron core, heat treatment conditions, operating frequency, and magnetic flux density, but this can be dealt with by adjusting the variable resistor 8 as in this embodiment.
上記実施例では、鉄心1の材料としてアモルファスを用
いたか、本発明者はけい素鋼、フェライトの′一部等の
他の材料を用いた鉄心の場合にも、鉄損の低減について
同様の傾向が示されることを実験的に確認している。In the above embodiment, amorphous was used as the material of the iron core 1, but the present inventors have found that the same tendency for reduction of iron loss can be observed in the case of iron cores made of other materials such as silicon steel or a portion of ferrite. It has been experimentally confirmed that this is shown.
[発明の効果]
本発明は以上の記述にて明らかなように、鉄心に直流磁
界を形成することで、鉄損の発生の少ない磁化領域で動
作させ得て、鉄心の鉄損を実質的に低減でき、鉄心の小
形化及び高効率化をさらに図り得るという優れた効果を
奏する。[Effects of the Invention] As is clear from the above description, the present invention can operate in a magnetization region where less iron loss occurs by forming a DC magnetic field in the iron core, and can substantially reduce the iron loss of the iron core. This has the excellent effect of further reducing the size of the iron core and increasing its efficiency.
図面は本発明の一実施例を示し、第1図は誘導機器を原
理的に表わす図、第2図は直流磁界−鉄損−騒音変化特
性図、第3図は第2図とは磁束密度が異なる場合の直流
磁界−鉄損変化特性図である。
図中、1は鉄心、2は一次コイル、3は二次コイル、6
は直流磁界形成用コイル、8は可変抵抗である。
代理人 弁理士 則 近 憲 (G同
三 俣 弘 文直充膳科 (A /cm
)
第 2 図
直流F1肱界 (A/cm )
第3図The drawings show one embodiment of the present invention, Fig. 1 is a diagram showing the principle of an induction device, Fig. 2 is a DC magnetic field-iron loss-noise change characteristic diagram, and Fig. 3 is a diagram showing the magnetic flux density in Fig. 2. FIG. 4 is a DC magnetic field-iron loss change characteristic diagram when the values are different. In the figure, 1 is the iron core, 2 is the primary coil, 3 is the secondary coil, 6
8 is a coil for forming a DC magnetic field, and 8 is a variable resistor. Agent: Patent Attorney Nori Chika (G.
Hiroshi Mimata Fuminao Mitsuru (A/cm)
) Fig. 2 DC F1 elbow field (A/cm) Fig. 3
Claims (1)
おいて、前記鉄心に直流磁界形成用コイルを巻回し、こ
の直流磁界形成用コイルに直流電流を通電するようにし
たことを特徴とする静止形誘導機器。1. A stationary device in which a primary coil and a secondary coil are wound around an iron core, wherein a DC magnetic field forming coil is wound around the iron core, and a DC current is passed through the DC magnetic field forming coil. shaped induction equipment.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP8213586A JPS62239511A (en) | 1986-04-11 | 1986-04-11 | Stationary induction apparatus |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP8213586A JPS62239511A (en) | 1986-04-11 | 1986-04-11 | Stationary induction apparatus |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS62239511A true JPS62239511A (en) | 1987-10-20 |
Family
ID=13765973
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP8213586A Pending JPS62239511A (en) | 1986-04-11 | 1986-04-11 | Stationary induction apparatus |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS62239511A (en) |
Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS50151335A (en) * | 1974-05-27 | 1975-12-05 | ||
JPS56115510A (en) * | 1980-02-19 | 1981-09-10 | Nippon Gakki Seizo Kk | Electric power source device |
-
1986
- 1986-04-11 JP JP8213586A patent/JPS62239511A/en active Pending
Patent Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS50151335A (en) * | 1974-05-27 | 1975-12-05 | ||
JPS56115510A (en) * | 1980-02-19 | 1981-09-10 | Nippon Gakki Seizo Kk | Electric power source device |
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