JP2000331847A - Flux controlled electromagnetic apparatus - Google Patents

Flux controlled electromagnetic apparatus

Info

Publication number
JP2000331847A
JP2000331847A JP11142257A JP14225799A JP2000331847A JP 2000331847 A JP2000331847 A JP 2000331847A JP 11142257 A JP11142257 A JP 11142257A JP 14225799 A JP14225799 A JP 14225799A JP 2000331847 A JP2000331847 A JP 2000331847A
Authority
JP
Japan
Prior art keywords
magnetic
control
magnetic flux
core
winding
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
JP11142257A
Other languages
Japanese (ja)
Other versions
JP3439692B2 (en
Inventor
Hiromichi Sato
博道 佐藤
Mitsuru Maeda
満 前田
Takashi Ohinata
大日向  敬
Shigeaki Akatsuka
重昭 赤塚
Mineo Kawakami
峰夫 川上
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.)
Tohoku Electric Power Co Inc
Original Assignee
Tohoku Electric Power Co Inc
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 Tohoku Electric Power Co Inc filed Critical Tohoku Electric Power Co Inc
Priority to JP14225799A priority Critical patent/JP3439692B2/en
Publication of JP2000331847A publication Critical patent/JP2000331847A/en
Application granted granted Critical
Publication of JP3439692B2 publication Critical patent/JP3439692B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Abstract

PROBLEM TO BE SOLVED: To provide a flux controlled electromagnetic apparatus in which opposite laminated iron cores are in the same laminated direction as a laminated electromagnetic steel plate in a pair of cut-core contacts and which comprises an electromagnetic iron core without an insulating film. SOLUTION: Windows 16a and 16b through an iron core are formed on respective legs 11a and 11b in a two or three leg core formed of a laminated iron core. A primary winding 15 connected to an AC power supply and generating primary magnetic flux ϕ1 is wound around the core of each of the legs, and a control winding 14 connected to a control power supply and generating control magnetic flux in a magnetic circuit around the windows is wound around each of the windows. A common circuit of a magnetic circuit for primary magnetic flux due to the primary winding 15 and a magnetic circuit for control magnetic flux due to the control winding 14 is formed on each of windows in the cores, and permeability of the common circuit is adjusted by excited current of the control winding 14 to control the primary magnetic flux ϕ1.

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【発明の属する技術分野】この発明は、主巻線が形成す
る磁束の磁気回路と制御巻線が形成する磁束の磁気回路
が互いに共通磁路を形成し、共通磁路の透磁率を制御す
る可変リアクトル、可変変圧器等の磁束制御形電磁機器
に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a magnetic circuit of magnetic flux formed by a main winding and a magnetic circuit of magnetic flux formed by a control winding forming a common magnetic path with each other and controlling the magnetic permeability of the common magnetic path. The present invention relates to a magnetic flux control type electromagnetic device such as a variable reactor and a variable transformer.

【0002】[0002]

【従来の技術】磁束制御形の電磁機器の従来技術として
は、例えば、特公昭55―64474号公報、実公平8
―5534号公報等に記載された可変リアクトルが知ら
れており、その鉄心は、図14に示すように、一対のU
形カットコア12,13の両脚端面を互いに90度捩っ
て接触させた構造になっており、図示のように、巻線1
4で形成される磁束φ2と巻線15で形成される磁束φ
1が通る磁気回路が直交し、互いに一方の巻線の磁束は
他方の巻線と鎖交しないことが特徴である。磁束φ1と
φ2は一対の鉄心12,13の接触部で共通の磁路を形
成しているので、一方の巻線を制御巻線として直流励磁
することにより共通磁路の透磁率を調整でき、他方の主
巻線の磁束を制御できるものである。
2. Description of the Related Art For example, Japanese Patent Publication No. 55-64474, Japanese Utility Model Publication No.
A variable reactor described in Japanese Patent Application Laid-Open No. 5534/1993 is known.
The two cut end cores 12 and 13 have a structure in which both leg end faces are in contact with each other by being twisted by 90 degrees.
4 and the magnetic flux φ formed by the winding 15
1 is characterized in that the magnetic circuits passing through are orthogonal, and the magnetic flux of one winding does not interlink with the other winding. Since the magnetic fluxes φ1 and φ2 form a common magnetic path at the contact portion of the pair of iron cores 12 and 13, the DC permeability of the common magnetic path can be adjusted by DC-exciting one of the windings as a control winding. The magnetic flux of the other main winding can be controlled.

【0003】特公昭55−64474号公報のものは、
テレビ画面の糸巻歪補正用に用いられる可飽和リアクト
ルであり、高周波電流が通電するので鉄心にはフェライ
トが使用され、鉄心の端面間にはギャップを形成するた
めのスペーサが介装されている。
[0003] Japanese Patent Publication No. 55-64474 discloses
A saturable reactor used for correcting pincushion distortion of a television screen. Ferrite is used for an iron core because high-frequency current flows, and a spacer for forming a gap is interposed between end faces of the iron core.

【0004】実公平8−5534号公報のものは、電力
用の無効電力補償用の可変リアクトルであり、商用周波
の電流が通電するので積層鉄心が使用され、鉄心の端面
は制御の可変範囲を大にするためにできるだけ密着させ
るように構成される。
Japanese Utility Model Publication No. 8-5534 discloses a variable reactor for compensating for reactive power for electric power. Since a commercial frequency current flows, a laminated core is used, and the end face of the core has a variable control range. It is configured to be as close as possible to increase the size.

【0005】[0005]

【発明が解決しようとする課題】上述のように、巻鉄心
で形成された電力用の一対のU形カットコアを直交磁路
に対応してカット面を互いに90度捩って接触させる場
合、電磁鋼板の積層端面は互いに直交して接触するた
め、積層電磁鋼板の端部が接触面で♯状に直交して接触
し、相互に絶縁されている電磁鋼板を短絡し、図15に
Ieにて示すように、♯状の接触部を通じて積層鉄心を
流れる渦電流路が形成されることになる。
As described above, when a pair of U-shaped cut cores for electric power formed of a wound iron core are brought into contact with each other so that the cut surfaces are twisted by 90 degrees with respect to the orthogonal magnetic path, Since the laminated end faces of the electromagnetic steel sheets contact each other at right angles to each other, the ends of the laminated electromagnetic steel sheets contact at right angles to each other at the contact surface, and short-circuit the mutually insulated electromagnetic steel sheets. As shown, an eddy current path flowing through the laminated core through the を 通 じ て -shaped contact portion is formed.

【0006】鉄心端面はできるだけ密着させなければな
らないが、この渦電流路の形成を防ぐために、従来、絶
縁フィルムを介して接触させている。このため、絶縁フ
ィルムに相当するギャップが介在することになり、それ
よる磁気特性の劣化が避けられず、制御の可変範囲が減
少するという問題があった。
[0006] The end faces of the iron core must be as close as possible, but in order to prevent the formation of this eddy current path, they are conventionally brought into contact via an insulating film. For this reason, a gap corresponding to the insulating film is interposed, which inevitably deteriorates the magnetic characteristics, and causes a problem that the variable range of control is reduced.

【0007】さらに、両カットコアの一方は直流励磁さ
れる制御巻線が巻回され、他方は商用周波数で励磁され
る主巻線が巻回されるため、接触部には繰返し叩くよう
な磁気吸引力が加わることになり、この連続する振動応
力に十分な耐久性のある絶縁フィルムを確保することが
難しいと言う問題があった。
Further, one of the two cut cores is wound with a control winding which is excited by a direct current, and the other is wound with a main winding which is excited at a commercial frequency. Attraction force is applied, and there is a problem that it is difficult to secure an insulating film having sufficient durability against the continuous vibration stress.

【0008】カットコアの接触部で、絶縁フィルムを叩
くように加わる繰返し応力により、フィルムの一部が損
傷し部分的に渦電流路が形成されると、渦電流による加
熱が絶縁フィルムの劣化をさらに拡大する。絶縁フィル
ムの劣化の拡大により、渦電流路はさらに拡大し、絶縁
フィルムの損傷が広がると接触面にギャップが形成され
ることになり、鉄心の過熱と共に接触面の振動の増大等
により障害が益々拡大することが懸念された。
[0008] When a part of the film is damaged and a eddy current path is partially formed by the repetitive stress applied to hit the insulating film at the contact portion of the cut core, heating by the eddy current causes deterioration of the insulating film. Expand further. Due to the deterioration of the insulation film, the eddy current path further expands, and if the damage of the insulation film spreads, a gap will be formed in the contact surface. There was concern that it would expand.

【0009】なお、鉄心にフェライトを用い、ギャップ
形成用のスペーサを介在させる高周波用の場合は、この
ような問題は生じないが、電力用電磁装置にフェライト
の使用は適さず、ギャップを設けると、可変制御範囲が
小さくなると言う問題が生じる。
In the case of a high-frequency type in which a ferrite is used for an iron core and a gap forming spacer is interposed, such a problem does not occur. However, the use of ferrite is not suitable for a power electromagnetic device. The problem that the variable control range becomes small arises.

【0010】本発明は、上述のごとき実状に鑑みて提案
されもので、第1、第2(前述の一対のカットコア)の
鉄心の接触部において、対向する積層鉄心の電磁鋼板の
積層方向を同方向とし、絶縁フィルムを必要としない電
磁鉄心で構成した磁束制御形電磁機器を提供すること、
また、第1、第2の積層鉄心が端面で衝合することが無
く、端面を叩くような振動を回避する電磁鉄心を提供す
ること、さらには、主巻線の電流歪の原因となる高調波
の発生を防止する電磁鉄心を提供すること、を目的とし
てなされたものである。
[0010] The present invention has been proposed in view of the above-described situation. In the first and second (the above-mentioned pair of cut cores) core contact portions, the lamination direction of the electromagnetic steel plates of the opposing laminated iron cores is changed. To provide a magnetic flux control type electromagnetic device configured with an electromagnetic core that does not require an insulating film in the same direction,
Further, the present invention provides an electromagnetic iron core that prevents the first and second laminated iron cores from abutting at the end faces and avoiding vibrations hitting the end faces, and further provides harmonics that cause current distortion of the main winding. An object of the present invention is to provide an electromagnetic core that prevents generation of waves.

【0011】[0011]

【課題を解決するための手段】本発明は、積層鉄心で構
成された二脚又は三脚の電磁鉄心の各脚に、磁心を貫通
する窓部を形成し、前記各脚の磁心に、単相又は三相電
源に接続され主磁束を発生する主巻線を巻装し、前記窓
部のそれぞれに、制御電源に接続され窓部の周囲に沿う
磁気回路に制御磁束を発生する制御巻線を巻装し、磁心
の窓部に主巻線による主磁束の磁気回路と制御巻線によ
る制御磁束の磁気回路との共通磁路を形成し、制御巻線
の励磁電流により当該共通磁路の透磁率を調整して主磁
束を制御することを特徴としたものである。
SUMMARY OF THE INVENTION According to the present invention, a window is formed in each leg of a two-legged or three-legged electromagnetic core composed of a laminated core, and a window is formed through the core. Alternatively, a main winding that is connected to a three-phase power supply and generates a main magnetic flux is wound, and a control winding that is connected to a control power supply and generates a control magnetic flux in a magnetic circuit along the periphery of the window is wound around each of the windows. A common magnetic path is formed between the magnetic circuit of the main magnetic flux by the main winding and the magnetic circuit of the control magnetic flux by the control winding in the window of the magnetic core. The main magnetic flux is controlled by adjusting the magnetic susceptibility.

【0012】[0012]

【発明の実施の形態】図1は、本発明を単相機器に適用
した場合の実施例を説明するための斜視図で、図中、1
1は閉磁路を構成する鉄心であり、11a,11bがそ
の二脚の鉄心(磁心)である。15は単相電源に接続さ
れる主巻線であり、主磁束φ1が二脚磁心11a,11
bを通る磁気回路に生じる。鉄心11の両脚の磁心11
a,11bを貫通して窓16a,16bが形成され、該
窓を画成する両側辺部16x,16yに切込み17a,
17bが形成される。両窓16a,16bを通って制御
巻線14が巻回され、制御磁束φ2が窓部の周囲に沿う
磁気回路に生じる。図示のように、主磁束φ1と制御磁
束φ2が通る磁気回路は直交しており、両巻線により生
じる主磁束又は制御磁束が他方の制御巻線又は主巻線と
鎖交しない。
DESCRIPTION OF THE PREFERRED EMBODIMENTS FIG. 1 is a perspective view for explaining an embodiment in which the present invention is applied to a single-phase device.
Numeral 1 denotes an iron core constituting a closed magnetic circuit, and 11a and 11b denote iron cores (magnetic cores) of the two legs. Reference numeral 15 denotes a main winding connected to a single-phase power supply.
occurs in the magnetic circuit passing through b. Magnetic core 11 of both legs of iron core 11
a, 11b, windows 16a, 16b are formed, and cuts 17a, 16y are formed in both side portions 16x, 16y defining the windows.
17b is formed. The control winding 14 is wound through the windows 16a and 16b, and a control magnetic flux φ2 is generated in a magnetic circuit along the periphery of the window. As shown, the magnetic circuits through which the main magnetic flux φ1 and the control magnetic flux φ2 pass are orthogonal to each other, and the main magnetic flux or control magnetic flux generated by both windings does not interlink with the other control winding or main winding.

【0013】上記の鉄心構造により、主磁束φ1と制御
磁束φ2に対し、両脚の磁心11a,11bの窓形成部
11m,11nは共通の磁路になっており、制御巻線の
励磁電流により、当該磁路の透磁率を調整することによ
り主磁束を制御することができる。この制御により、主
巻線のインダクタンスを制御することができ、可変リア
クトルを構成できる。また、主巻線を一次巻線として2
次巻線を設ければ、2次巻線の電圧を制御することがで
き、可変変圧器を構成できる。窓部を画成する側辺16
x,16yに形成された切込み17a,17bは、共通
磁路11m,11nの磁束に対する透磁率の変化の直線
性を改善し、主巻線の電流の歪を軽減する。閉磁路鉄心
11は、帯状の電磁鋼板を巻回して形成することがで
き、電磁鉄心は一体に構成される。また、閉磁路鉄心を
ロ字形の打抜き電磁鋼板を積重ねて形成することもで
き、この場合も、電磁鉄心は一体に構成できる。ただ、
この場合、制御磁束が一部で鋼板を貫通するが、制御電
流が直流の場合には渦電流損を考慮する必要がないので
問題はない。
With the above-described iron core structure, the window forming portions 11m and 11n of the magnetic cores 11a and 11b of the two legs form a common magnetic path for the main magnetic flux φ1 and the control magnetic flux φ2. The main magnetic flux can be controlled by adjusting the magnetic permeability of the magnetic path. With this control, the inductance of the main winding can be controlled, and a variable reactor can be configured. The main winding is used as a primary winding and
If the secondary winding is provided, the voltage of the secondary winding can be controlled, and a variable transformer can be configured. Side 16 that defines the window
The cuts 17a and 17b formed in x and 16y improve the linearity of the change of the magnetic permeability with respect to the magnetic flux of the common magnetic paths 11m and 11n, and reduce the current distortion of the main winding. The closed magnetic circuit core 11 can be formed by winding a band-shaped electromagnetic steel plate, and the electromagnetic core is integrally formed. In addition, the closed magnetic circuit core can be formed by stacking square-shaped punched electromagnetic steel sheets. In this case, the electromagnetic core can be formed integrally. However,
In this case, a part of the control magnetic flux penetrates the steel plate. However, when the control current is DC, there is no problem because it is not necessary to consider the eddy current loss.

【0014】図2は、巻線の巻装を容易にするため、鉄
心11を2つのカットコア11x,11yに分割し、カ
ットコア11x,11yのカット面を接触して、図1に
示した鉄心11を構成するものであるが、その場合に、
カット面における両コアの電磁鋼板の積層方向を同一方
向とし、従来構造のように接触面で電磁鋼板が直交して
接触することを無くし、積層鉄心に流れる渦電流流路が
形成されることのないようにしたものである。図3は、
この場合の巻線の巻装の1例を示す図で、図3(A)は
カットコア11yに制御巻線14及び主巻線15を巻回
した時の様子を示す斜視図、図3(B)は、図3(A)
のようにして巻線を巻回したカットコア11yにカット
コア11xを接触させた時の構成を示す。
FIG. 2 shows the iron core 11 divided into two cut cores 11x and 11y in order to facilitate winding of the winding, and the cut surfaces of the cut cores 11x and 11y are brought into contact with each other, as shown in FIG. It constitutes the iron core 11, in which case,
The lamination direction of the magnetic steel sheets of both cores on the cut surface is made the same direction, eliminating the perpendicular contact of the electromagnetic steel sheets on the contact surface as in the conventional structure, and forming an eddy current flow path flowing through the laminated iron core. It is not to be. FIG.
FIG. 3A is a diagram showing an example of winding of the winding in this case, and FIG. 3A is a perspective view showing a state where the control winding 14 and the main winding 15 are wound around the cut core 11y. FIG. 3 (A)
The configuration when the cut core 11x is brought into contact with the cut core 11y on which the winding is wound as described above.

【0015】図4は、前記カットコア11x又は11y
を作成する場合の例を示す図で、まず、図4(A)に示
すように、矩形の短片に窓部に対応する凹所wを形成し
た打抜き電磁鋼板11zの長辺を適宜調整し、次いで、
図4(B)に示すように、曲折し、その後、積層して対
を形成し、それらを対向接触して構成する例を示す。な
お、打抜き電磁鋼板の形状を様々に変えることで鉄心の
形状を自由に設定できることは明らかである。
FIG. 4 shows the cut core 11x or 11y.
First, as shown in FIG. 4A, a long side of a punched electromagnetic steel sheet 11z having a rectangular short piece formed with a recess w corresponding to a window portion is appropriately adjusted as shown in FIG. Then
As shown in FIG. 4 (B), an example is shown in which a pair is formed by bending and then laminating, and they are brought into facing contact with each other. It is clear that the shape of the iron core can be freely set by changing the shape of the punched electromagnetic steel sheet in various ways.

【0016】図5は、図4に示したようにして積層した
窓部の電磁鋼板の積層構造を示し(図5(A)は、一体
構成とする前の構成、図5(B)は、一体構成とした後
の構成を示し、(a2),(b2)はそれぞれ(a1),
(b1)の接触部の構成を拡大して示す)、図5(A)
に示すように、電磁鋼板の接触部を櫛形に積層し、この
櫛形積層鉄心の櫛形端部を互いに重ねて接触部を形成し
て、図5(B)に示すように、一体型構成と同様の構成
とする。
FIG. 5 shows the laminated structure of the electromagnetic steel sheets of the window portion laminated as shown in FIG. 4 (FIG. 5 (A) is a structure before being integrated, and FIG. (A 2 ) and (b 2 ) are (a 1 ) and (b 2 ), respectively.
FIG. 5 (A) is an enlarged view of the configuration of the contact portion (b 1 ).
As shown in FIG. 5, the contact portions of the electromagnetic steel sheets are laminated in a comb shape, and the comb-shaped ends of the comb-shaped laminated iron core are overlapped with each other to form a contact portion, as shown in FIG. Configuration.

【0017】図6は、三相機器用の実施例を説明するも
ので、閉磁路鉄心11には三脚の磁心11a,11b,
11cを有する。三脚の磁心には、それぞれ三相電源に
接続される主巻線15a,15b,15cが巻回され
る、主磁束φ1a,φ1b,φ1cが各磁心を通る磁気
回路に生じる。鉄心11の三脚の各磁心11a,11
b,11cのそれぞれを貫通して窓16a,16b,1
6cが形成される。それぞれの窓を通って制御巻線14
が巻回され、制御磁束φ2a,φ2b,φ2cがそれぞ
れの窓の周囲に沿う磁気回路に生じ、主磁束の磁気回路
と制御磁束の磁気回路は互いに直交している。
FIG. 6 illustrates an embodiment for a three-phase device, in which a closed magnetic circuit core 11 includes three cores 11a, 11b, and 11b.
11c. Main magnetic fluxes φ1a, φ1b, φ1c are wound around the magnetic core of the tripod, and the main magnetic fluxes φ1a, φ1b, φ1c are generated in a magnetic circuit passing through the respective magnetic cores. Each magnetic core 11a, 11 of the tripod of the iron core 11
b, 11c through each of the windows 16a, 16b, 1
6c is formed. Control winding 14 through each window
Are wound, and control magnetic fluxes φ2a, φ2b, φ2c are generated in magnetic circuits along the periphery of each window, and the magnetic circuit of the main magnetic flux and the magnetic circuit of the control magnetic flux are orthogonal to each other.

【0018】各磁心の窓部形成部11m,11n,11
oはそれぞれ主磁束φ1a,φ1b,φ1cと制御磁束
φ2a,φ2b,φ2cの共通磁路となり、制御巻線の
励磁電流の制御により当該磁路の透磁率を調整し、主磁
束を制御することができ、三相可変リアクトル、又は三
相可変変圧器を構成することができる。17は、窓の側
辺部に形成した切込みであり、前述の通り主巻線の電流
歪を軽減する。
Window portions 11m, 11n, 11 of each magnetic core
o is a common magnetic path of the main magnetic fluxes φ1a, φ1b, φ1c and the control magnetic fluxes φ2a, φ2b, φ2c, respectively. By controlling the exciting current of the control winding, the permeability of the magnetic path can be adjusted to control the main magnetic flux. It is possible to configure a three-phase variable reactor or a three-phase variable transformer. Reference numeral 17 denotes a notch formed in a side portion of the window, which reduces current distortion of the main winding as described above.

【0019】三相鉄心においても巻鉄心、積層鉄心、さ
らにカットコアの接合、曲折鋼板の積層により形成でき
ることは明らかである。直交磁路形電磁装置は、主磁束
の磁束が制御巻線と鎖交しないので、制御巻線に誘起電
圧が生ぜず、制御回路に主回路に起因する電圧が加わら
ないことが特徴である。そこで、主磁束φ1の磁気回路
と制御磁束φ2の磁気回路の共通磁路に制御磁束φ2を
形成するための制御巻線を、図7に示すように、磁心に
設けた窓の両枠部20,21のそれぞれに同一巻数巻回
して形成することができる。この場合、前記両枠部に巻
回した制御巻線にはそれぞれ主磁束によって誘起電圧が
生じるが両巻線は同一巻回数であり、それぞれの誘起電
圧は等しく、かつ、両巻線は極性が逆に接続されている
ので誘起電圧は打消され、制御巻線の端子に誘起電圧が
生じることはない。
It is apparent that the three-phase core can be formed by winding a core, a laminated core, a cut core, and laminating bent steel plates. The orthogonal magnetic path type electromagnetic device is characterized in that since the magnetic flux of the main magnetic flux does not interlink with the control winding, no induced voltage is generated in the control winding, and a voltage due to the main circuit is not applied to the control circuit. Therefore, as shown in FIG. 7, a control winding for forming the control magnetic flux φ2 in a common magnetic path of the magnetic circuit of the main magnetic flux φ1 and the magnetic circuit of the control magnetic flux φ2 is connected to both frame portions 20 of the window provided on the magnetic core, as shown in FIG. , 21 with the same number of turns. In this case, an induced voltage is generated by the main magnetic flux in each of the control windings wound around the two frame portions, but the two windings have the same number of turns, the induced voltages are equal, and the two windings have polarities. Since the connection is reversed, the induced voltage is canceled, and no induced voltage is generated at the terminal of the control winding.

【0020】上記の場合、図1の場合と同様な制御が可
能であり、このように制御巻線を巻装する場合は、二脚
磁心の一方の磁心に窓を形成すれば良い。三相機器の場
合も、上記と同様に制御磁束φ2a,φ2b,φ2cを
形成する制御巻線を、三脚磁心の各磁心に形成した窓の
両窓枠部20,21にそれぞれ同一回数巻回することが
できる。
In the above case, the same control as in the case of FIG. 1 can be performed. When the control winding is wound in this manner, a window may be formed in one of the two leg magnetic cores. In the case of a three-phase device as well, control windings for forming control magnetic fluxes φ2a, φ2b, φ2c are wound the same number of times around the window frames 20, 21 of the windows formed on the respective magnetic cores of the tripod core in the same manner as described above. be able to.

【0021】なお、前記実施例の説明では、両窓枠の磁
路が磁気的に対称的であることを前提に、窓枠部の制御
巻線の巻回数を同一とする旨説明したが、要は両巻線に
誘起する電圧を打消すように構成することであり、窓枠
部の磁気回路が磁気的に対称的でなければ前記の巻回数
が異なってくることは明らかである。
In the description of the above embodiment, the number of turns of the control winding of the window frame portion is set to be the same on the assumption that the magnetic paths of both window frames are magnetically symmetric. The point is that the voltage induced in both windings is cancelled, and it is clear that the number of windings differs if the magnetic circuit of the window frame is not magnetically symmetric.

【0022】図8は、本発明の電磁鉄心を用いた可変リ
アクトルの電力系統への使用例を示すもので、可変リア
クトルを構成する主巻線15に電力用コンデンサCを並
列接続して、電力系統に並列に挿入し、制御巻線14の
励磁電流を制御することにより、系統に生じる遅相から
進相の無効電力を連続的に補償するようにしたものであ
る。
FIG. 8 shows an example of the use of a variable reactor using an electromagnetic core according to the present invention in a power system. A power capacitor C is connected in parallel to a main winding 15 constituting the variable reactor, and By inserting in parallel to the system and controlling the exciting current of the control winding 14, the reactive power from the late phase to the early phase generated in the system is continuously compensated.

【0023】図9は、同じく、可変リアクトルの各相の
主巻線に15に並列にコンデンサCを接続して、電力系
統の送電線の各相に直列に挿入し、制御巻線の励磁電流
を制御することにより送電線路のインピーダンスを誘導
性インピーダンスから容量性インピーダンスに連続的に
調整し、電力系統における受電電圧又は送電電圧の移相
制御に適用した例を示す。
FIG. 9 also shows that the capacitor C is connected in parallel to the main winding of each phase of the variable reactor 15 and inserted in series with each phase of the transmission line of the power system, and the exciting current of the control winding is changed. In this example, the impedance of the transmission line is continuously adjusted from the inductive impedance to the capacitive impedance by controlling the power transmission line, and applied to the phase shift control of the receiving voltage or the transmitting voltage in the power system.

【0024】図10は、可変リアクトルを送電線路に直
列に挿入し、送電線の過大電流を検出した場合に、制御
巻線の励磁電流の制御により主巻線のリアクトルを増加
させて電流を制限する、限流リアクトルとした適用例を
示す。
FIG. 10 shows that a variable reactor is inserted in a transmission line in series, and when an excessive current of the transmission line is detected, the reactor of the main winding is increased by controlling the exciting current of the control winding to limit the current. The following is an application example of a current limiting reactor.

【0025】図11は、単相の可変リアクトルを送電系
統に接続された変圧器の中性点の接地回路に消弧リアク
トルとして挿入し、中性点の電圧と中性点の電流の位相
を検出し、可変リアクトルのインダクタンスを常に系統
の浮遊容量との共振点に合調するように制御巻線の励磁
電流を制御するものである。
FIG. 11 shows that a single-phase variable reactor is inserted as an arc-extinguishing reactor into a neutral-point grounding circuit of a transformer connected to a power transmission system, and the phase of the neutral-point voltage and the neutral-point current is changed. This is to detect and control the exciting current of the control winding so that the inductance of the variable reactor is always tuned to the resonance point with the stray capacitance of the system.

【0026】図12は、可変リアクトルを誘導電動機の
交流電源回路に直列に接続した、起動電流抑制回路への
適用例を示す。可変リアクトルは制御電流無しの状態で
最大であるため起動時の励磁突入電流は抑制される。可
変リアクトルの減少制御は誘導電動機の起動信号を条件
に開始し、回転信号に応じた制御信号により可変リアク
トルを最小まで減じ、最終的にはリアクトルの端子を短
絡する制御を行う。なお同様の制御を誘導発電機の交流
形統連系時の併入電流抑制にも適用できることは明らか
である。
FIG. 12 shows an example of application to a starting current suppressing circuit in which a variable reactor is connected in series to an AC power supply circuit of an induction motor. Since the variable reactor is maximum without a control current, the inrush current at startup is suppressed. The control for reducing the variable reactor is started on the condition of the start signal of the induction motor, the variable reactor is reduced to a minimum by a control signal corresponding to the rotation signal, and finally, the terminal of the reactor is short-circuited. It is clear that the same control can be applied to the suppression of the inrush current when the induction generator is connected to the AC type.

【0027】図13は、可変リアクトルを巻線形誘導電
動機の二次回路に接続し、二次回路に誘起される電圧に
よる電流を調整する回路への適用例を示しており、調速
機などからの信号を検出することにより誘導電動機のす
べりなどからトルク制御を、そして誘導機起動信号によ
り起動電流抑制制御を行うことができる。なお、同様の
制御を誘導発電機においても適用できることは明らかで
ある。
FIG. 13 shows an example of application to a circuit in which a variable reactor is connected to a secondary circuit of a wound induction motor and a current is adjusted by a voltage induced in the secondary circuit. , The torque control can be performed from the slip of the induction motor, and the starting current suppression control can be performed by the induction motor starting signal. It is clear that the same control can be applied to the induction generator.

【0028】なお、以上には、可変リアクトルへの適用
例を中心に説明したが、主巻線が巻回された磁心に2次
巻線を巻回することにより可変変圧器を構成できること
は明らかなことである。
Although the description has been made mainly of the application to the variable reactor, it is apparent that the variable transformer can be formed by winding the secondary winding around the magnetic core around which the main winding is wound. That is what.

【0029】[0029]

【発明の効果】以上のように、従来構造では、カットコ
アの接触面で電磁鋼板の端面が直交して接触することに
よる渦電流流路の形成を避けるための絶縁フィルムの介
在が必須であり、それによる磁気特性の劣化が避けられ
ず、また耐久性のある絶縁フィルムの確保が現状では極
め困難であったが、本発明により、積層鉄心により一体
構造の鉄心の構成が可能となり、接触部がなく絶縁フィ
ルムを要せず、磁気特性の劣化が避けられ、渦電流によ
る障害の発生もない電力用磁束制御形電磁機器を構成す
ることができる。
As described above, in the conventional structure, the interposition of the insulating film for avoiding the formation of the eddy current flow path due to the perpendicular contact of the end faces of the magnetic steel sheet at the contact surface of the cut core is essential. However, the deterioration of magnetic properties due to this is inevitable, and it is extremely difficult at present to secure a durable insulating film. However, according to the present invention, it is possible to form a monolithic iron core by using a laminated iron core. This eliminates the need for an insulating film, avoids deterioration of magnetic properties, and can be used to configure a magnetic flux control type electromagnetic device for electric power that does not cause any trouble due to eddy current.

【0030】また、カットコアの接触による構成とする
場合でも、カットコアの接触面において電磁鋼板の積層
方向は同方向であり、渦電流流路が形成されることは無
く、絶縁フィルムの介在を必要とせず、絶縁フィルムの
介在に伴う磁気特性の劣化を避けることができる。
[0030] Even when the cut core is configured to be in contact, the lamination direction of the electromagnetic steel sheets is the same on the contact surface of the cut core, no eddy current flow path is formed, and the insulating film is interposed. It is not necessary, and it is possible to avoid deterioration of magnetic properties due to the interposition of the insulating film.

【0031】上述のように、本発明により現状では確保
が困難であった絶縁フィルムを必要としないことから、
電力分野における可変リアクトル、可変変圧器、電力結
合装置等の磁束制御形電磁機器として広範囲な適用が可
能になる。
As described above, since the present invention does not require an insulating film which was difficult to secure at present,
It can be widely applied as a magnetic flux control type electromagnetic device such as a variable reactor, a variable transformer, and a power coupling device in the electric power field.

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

【図1】 本発明を適用した一体構成の単相磁束制御形
電磁機器の説明図である。
FIG. 1 is an explanatory diagram of an integrated single-phase magnetic flux control type electromagnetic device to which the present invention is applied.

【図2】 図1に示した単相電磁鉄心をカットコア構成
とした本発明の電磁鉄心の説明図である。
FIG. 2 is an explanatory diagram of an electromagnetic core of the present invention in which the single-phase electromagnetic core shown in FIG. 1 has a cut core configuration.

【図3】 カットコア構成とした場合の巻線巻装の説明
図である。
FIG. 3 is an explanatory diagram of winding winding in the case of a cut core configuration.

【図4】 打抜き鋼板の積層で本発明の電磁鉄心を形成
する場合の説明図である。
FIG. 4 is an explanatory diagram in the case where the electromagnetic iron core of the present invention is formed by laminating stamped steel sheets.

【図5】 積層鉄心の接触部の説明図である。FIG. 5 is an explanatory view of a contact portion of a laminated core.

【図6】 本発明を適用した三相磁束制御形電磁機器の
説明図である。
FIG. 6 is an explanatory diagram of a three-phase magnetic flux control type electromagnetic device to which the present invention is applied.

【図7】 本発明の単相磁束制御形電磁機器の別の実施
例の説明図である。
FIG. 7 is an explanatory diagram of another embodiment of the single-phase magnetic flux control type electromagnetic device of the present invention.

【図8】 本発明を無効電力補償装置に適用した例を示
す図である。
FIG. 8 is a diagram showing an example in which the present invention is applied to a reactive power compensator.

【図9】 本発明を移相器に適用した例を示す図であ
る。
FIG. 9 is a diagram showing an example in which the present invention is applied to a phase shifter.

【図10】 本発明を限流装置に適用した例を示す図で
ある。
FIG. 10 is a diagram showing an example in which the present invention is applied to a current limiting device.

【図11】 本発明を消弧リアクトルに適用した例を示
す図である。
FIG. 11 is a diagram showing an example in which the present invention is applied to an arc extinguishing reactor.

【図12】 本発明を誘導機の起動電流抑制回路に適用
した例を示す図である。
FIG. 12 is a diagram showing an example in which the present invention is applied to a starting current suppressing circuit of an induction machine.

【図13】 本発明を巻線形誘導機の速度調整,トルク
調整,起動電流抑制回路に適用した例を示す図である。
FIG. 13 is a diagram showing an example in which the present invention is applied to a speed adjustment, torque adjustment, and starting current suppression circuit of a wound-type induction machine.

【図14】 従来の直交磁路形電磁装置の鉄心を示す図
である。
FIG. 14 is a diagram illustrating an iron core of a conventional orthogonal magnetic path type electromagnetic device.

【図15】 従来の鉄心の説明図である。FIG. 15 is an explanatory diagram of a conventional iron core.

【符号の説明】[Explanation of symbols]

11…鉄心(磁心)、11a,11b,11c…磁心の
脚部、11m,11n,11o…磁心脚部の窓部構成
部、12,13…U形カットコア、14…制御巻線、1
5,15a,15b,15c…主巻線、16,16a,
16b,16c…脚部に設けた窓、16x、16y…窓
部を画成する側辺、17,17a,17b…切込み、2
0,21…窓部の両枠部。
11: iron core (magnetic core), 11a, 11b, 11c: magnetic core leg, 11m, 11n, 11o: magnetic core leg window component, 12, 13: U-shaped cut core, 14: control winding, 1
5, 15a, 15b, 15c ... main winding, 16, 16a,
16b, 16c: windows provided on the legs, 16x, 16y: sides defining the windows, 17, 17a, 17b ... cuts, 2
0, 21: Both frame portions of the window portion.

─────────────────────────────────────────────────────
────────────────────────────────────────────────── ───

【手続補正書】[Procedure amendment]

【提出日】平成12年2月17日(2000.2.1
7)
[Submission date] February 17, 2000 (2000.2.1
7)

【手続補正1】[Procedure amendment 1]

【補正対象書類名】明細書[Document name to be amended] Statement

【補正対象項目名】0013[Correction target item name] 0013

【補正方法】変更[Correction method] Change

【補正内容】[Correction contents]

【0013】上記の鉄心構造により、主磁束φ1と制御
磁束φ2に対し、両脚の磁心11a,11bの窓形成部
11m,11nは共通の磁路になっており、制御巻線の
励磁電流により、当該磁路の透磁率を調整することによ
り主磁束を制御することができる。この制御により、主
巻線のインダクタンスを制御することができ、可変リア
クトルを構成できる。また、主巻線を一次巻線として2
次巻線を設ければ、2次巻線の電圧を制御することがで
き、可変変圧器を構成できる。窓部を画成する側辺16
x,16yに形成された切込み17a,17bは、共通
磁路11m,11nの磁束に対する透磁率の変化の直線
性を改善し、主巻線の電流の歪を軽減する。閉磁路鉄心
11は、帯状の電磁鋼板を巻回して形成することがで
き、電磁鉄心は一体に構成される。また、閉磁路鉄心を
ロ字形の打抜き電磁鋼板を積重ねて形成することもで
き、この場合も、電磁鉄心は一体に構成できる
With the above-described iron core structure, the window forming portions 11m and 11n of the magnetic cores 11a and 11b of the two legs form a common magnetic path for the main magnetic flux φ1 and the control magnetic flux φ2. The main magnetic flux can be controlled by adjusting the magnetic permeability of the magnetic path. With this control, the inductance of the main winding can be controlled, and a variable reactor can be configured. The main winding is used as a primary winding and
If the secondary winding is provided, the voltage of the secondary winding can be controlled, and a variable transformer can be configured. Side 16 that defines the window
The cuts 17a and 17b formed in x and 16y improve the linearity of the change of the magnetic permeability with respect to the magnetic flux of the common magnetic paths 11m and 11n, and reduce the current distortion of the main winding. The closed magnetic circuit core 11 can be formed by winding a band-shaped electromagnetic steel plate, and the electromagnetic core is integrally formed. In addition, the closed magnetic circuit core can be formed by stacking square-shaped punched electromagnetic steel sheets. In this case, the electromagnetic core can be formed integrally .

───────────────────────────────────────────────────── フロントページの続き (72)発明者 大日向 敬 宮城県仙台市青葉区中山七丁目二番地一号 東北電力株式会社研究開発センター内 (72)発明者 赤塚 重昭 宮城県仙台市青葉区中山七丁目二番地一号 東北電力株式会社研究開発センター内 (72)発明者 川上 峰夫 宮城県仙台市青葉区中山七丁目二番地一号 東北電力株式会社研究開発センター内 Fターム(参考) 5E043 BA01  ──────────────────────────────────────────────────続 き Continued on the front page (72) Inventor Takashi Ohinata 7-2-1, Nakayama, Aoba-ku, Aoba-ku, Sendai, Miyagi Prefecture Inside the R & D Center of Tohoku Electric Power Co., Inc. (72) Inventor Shigeaki Akatsuka Nakayama, Aoba-ku, Sendai, Miyagi 1-chome 2-1-1, Tohoku Electric Power Co. R & D Center (72) Inventor Mineo Kawakami 7-2-1, Nakayama, Aoba-ku, Aoba-ku, Sendai City, Miyagi Prefecture F-term (reference) 5E043 BA01

Claims (5)

【特許請求の範囲】[Claims] 【請求項1】 積層鉄心で構成された二脚又は三脚の電
磁鉄心の各脚に、磁心を貫通する窓部を形成し、前記各
脚の磁心に、単相又は三相電源に接続され主磁束を発生
する主巻線を巻装し、前記窓部のそれぞれに、制御電源
に接続され窓部の周囲に沿う磁気回路に制御磁束を発生
する制御巻線を巻装し、磁心の窓部に主巻線による主磁
束の磁気回路と制御巻線による制御磁束の磁気回路との
共通磁路を形成し、制御巻線の励磁電流により当該共通
磁路の透磁率を調整し主磁束を制御する磁束制御形電磁
機器。
1. A window penetrating through a magnetic core is formed in each leg of a two-legged or three-legged electromagnetic core composed of a laminated core, and the magnetic core of each leg is connected to a single-phase or three-phase power source. A main winding for generating a magnetic flux is wound, and a control winding for generating a control magnetic flux is wound around a magnetic circuit connected to a control power supply along the periphery of the window in each of the window portions, and a window portion of a magnetic core is provided. A common magnetic path is formed between the magnetic circuit of the main magnetic flux by the main winding and the magnetic circuit of the control magnetic flux by the control winding, and the magnetic flux of the common magnetic path is adjusted by the excitation current of the control winding to control the main magnetic flux. Magnetic flux control type electromagnetic equipment.
【請求項2】 請求項1において、二脚磁心の一脚に窓
部を形成したことを特徴とする磁束制御形電磁機器。
2. A magnetic flux control type electromagnetic device according to claim 1, wherein a window is formed in one leg of the two-leg magnetic core.
【請求項3】 請求項1において、電磁鉄心の各脚に磁
心を貫通して形成する窓部は、各磁心の窓の開口中心が
略同軸上となるように形成することを特徴とする磁束制
御形電磁機器。
3. The magnetic flux according to claim 1, wherein the windows formed in each leg of the electromagnetic core so as to penetrate the magnetic core are formed such that the centers of the windows of the respective magnetic cores are substantially coaxial. Controlled electromagnetic devices.
【請求項4】 請求項1、2又は3において、各脚部に
形成された窓部を画成する脚部の側辺部に楔形の切込み
を形成したことを特徴とする磁束制御形電磁機器。
4. A magnetic flux control type electromagnetic device according to claim 1, wherein a wedge-shaped cut is formed in a side portion of the leg defining a window formed in each leg. .
【請求項5】 請求項1、2、3又は4において、磁心
を貫通して形成された窓部に巻装する制御巻線は、一対
の巻線を窓部の対向する枠部のそれぞれに巻装し、主磁
束によって両巻線に誘起する電圧を打消すように接続し
たことを特徴とする磁束制御形電磁機器。
5. The control winding according to claim 1, 2, 3 or 4, wherein the control winding wound around the window formed through the magnetic core comprises a pair of windings wound on each of the opposite frame portions of the window. A magnetic flux control type electromagnetic device characterized by being wound and connected so as to cancel out a voltage induced in both windings by a main magnetic flux.
JP14225799A 1999-05-21 1999-05-21 Magnetic flux control type electromagnetic equipment Expired - Lifetime JP3439692B2 (en)

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Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2005510076A (en) * 2001-11-21 2005-04-14 マグテック エーエス Device with controllable impedance
CN101986401A (en) * 2010-08-23 2011-03-16 吴江市变压器厂有限公司 Single-phase open core transformer
CN103219141A (en) * 2013-04-27 2013-07-24 福州大学 Alternating current inductor with controllable inductance value

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2005510076A (en) * 2001-11-21 2005-04-14 マグテック エーエス Device with controllable impedance
CN101986401A (en) * 2010-08-23 2011-03-16 吴江市变压器厂有限公司 Single-phase open core transformer
CN103219141A (en) * 2013-04-27 2013-07-24 福州大学 Alternating current inductor with controllable inductance value

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