JPH0262044B2 - - Google Patents
Info
- Publication number
- JPH0262044B2 JPH0262044B2 JP23899987A JP23899987A JPH0262044B2 JP H0262044 B2 JPH0262044 B2 JP H0262044B2 JP 23899987 A JP23899987 A JP 23899987A JP 23899987 A JP23899987 A JP 23899987A JP H0262044 B2 JPH0262044 B2 JP H0262044B2
- Authority
- JP
- Japan
- Prior art keywords
- winding
- core
- shunt
- series
- magnetic
- 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
- 238000004804 winding Methods 0.000 claims description 122
- 230000004907 flux Effects 0.000 claims description 31
- 238000009738 saturating Methods 0.000 claims description 2
- 238000007599 discharging Methods 0.000 claims 1
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical compound [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 description 16
- 230000007935 neutral effect Effects 0.000 description 6
- 239000000463 material Substances 0.000 description 4
- RYGMFSIKBFXOCR-UHFFFAOYSA-N Copper Chemical compound [Cu] RYGMFSIKBFXOCR-UHFFFAOYSA-N 0.000 description 3
- 229910052802 copper Inorganic materials 0.000 description 3
- 239000010949 copper Substances 0.000 description 3
- 229910052742 iron Inorganic materials 0.000 description 3
- 230000000694 effects Effects 0.000 description 2
- 229910000976 Electrical steel Inorganic materials 0.000 description 1
- 230000002238 attenuated effect Effects 0.000 description 1
- 230000008878 coupling Effects 0.000 description 1
- 238000010168 coupling process Methods 0.000 description 1
- 238000005859 coupling reaction Methods 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 238000010030 laminating Methods 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 229920006395 saturated elastomer Polymers 0.000 description 1
Landscapes
- Coils Or Transformers For Communication (AREA)
- Amplifiers (AREA)
Description
【発明の詳細な説明】
〔発明の対象〕
本発明は磁気増幅器に関し、とくに、小形軽量
の磁気増幅器の改良に関する。DETAILED DESCRIPTION OF THE INVENTION [Object of the Invention] The present invention relates to magnetic amplifiers, and more particularly to improvements in small and lightweight magnetic amplifiers.
従来、可飽和リアクトル形の磁気増幅器が提案
されているが、従来の磁気増巾器は定格容量の増
加に比例して鉄および銅等の使用材料が増大し
て、寸法重量が著しく大きくなり、極めて高価で
あつた。しかも、出力電圧の波形歪みが大きいた
めに、バルキーで高価な外部フイルターを必要と
していた。
Conventionally, saturable reactor type magnetic amplifiers have been proposed, but conventional magnetic amplifiers use materials such as iron and copper that increase in proportion to the increase in rated capacity, resulting in significantly large dimensions and weight. It was extremely expensive. Moreover, the large waveform distortion of the output voltage required a bulky and expensive external filter.
本発明の目的は出力波形が良好な小形軽量の磁
気増幅器を提供することにある。
An object of the present invention is to provide a small and lightweight magnetic amplifier with a good output waveform.
本発明の他の目的は小さな自己容量で大きな負
荷容量がとれ、使用材料が少なく、鉄損、銅損を
著しく軽減した、高効率の磁気増幅器を提供する
ことにある。 Another object of the present invention is to provide a highly efficient magnetic amplifier that has a large load capacity with a small self-capacity, uses less material, and significantly reduces iron loss and copper loss.
本発明の磁気増幅器は第1直列巻線とこの第1
直列巻線に直列接続された分路巻線とこの分路巻
線とは異なる極性で分路巻線に直列接続された第
2直列巻線とを有する第1可飽和鉄心を備えた主
磁束ループ路と、前記分路巻線と前記第2直列巻
線との間に配置されて前記主磁束ループ路の一部
をバイパスさせるためのエアギヤツプを備えた少
くとも1つの磁気分路鉄心と、前記磁気分路鉄心
と前記第2直列巻線との間の前記第1可飽和鉄心
の一部とその延長部とに磁気的に結合された第2
可飽和鉄心を備えた補助磁速ループ路と、前記第
1可飽和鉄心の前記延長部に巻装され、前記第2
可飽和鉄心を介して前記第1可飽和鉄心の前記一
部を磁気飽和させて前記第1直列巻線と前記分路
巻線の磁束を前記磁気分路鉄心にシフトさせるた
めの制御巻線とを備えたことを特徴とする。
The magnetic amplifier of the present invention includes a first series winding and a first series winding.
a main flux comprising a first saturable iron core having a shunt winding connected in series with the series winding and a second series winding connected in series with the shunt winding with a polarity different from the shunt winding; at least one magnetic shunt core comprising a loop path and an air gap disposed between the shunt winding and the second series winding to bypass a portion of the main flux loop path; a second magnetically coupled portion of the first saturable core and an extension thereof between the magnetic shunt core and the second series winding;
an auxiliary magnetic velocity loop path having a saturable iron core;
a control winding for magnetically saturating the part of the first saturable core via the saturable core to shift the magnetic flux of the first series winding and the shunt winding to the magnetic shunt core; It is characterized by having the following.
本発明による磁気増幅器の望ましい実施例を第
1〜5図を参照しながら説明する。
A preferred embodiment of the magnetic amplifier according to the present invention will be described with reference to FIGS. 1-5.
第1図において、磁気増幅器10は主磁束ルー
プ路を構成する第1コア部12aと第2コア部1
2bと、主磁束ループ路の1部をバイパスさせる
ための磁気分路鉄心14とを有し、第1可飽和鉄
心として作用する、第1巻鉄心12を備える。第
1巻鉄心12の第1コア部12a上に第1直列巻
線16と分路巻線18が巻装され、一方、第2コ
ア部12b上に第2直列巻線20が巻装される。
第1直列巻線16は高圧端子Uと中圧端子uとの
間に接続され、分路巻線18は第1直列巻線16
に同一極性で直列接続される。分路巻線18の下
端部は第1中性点V1に接続される。第2直列巻
線20は分路巻線18の下端部と第2中性点V2
との間において第1直列巻線16とは逆極性で接
続される。第2コア部12bの少くとも一部の磁
気飽和状態を変えて、磁気分路鉄心14の磁束密
度を制御するために第2可飽和鉄心として作用す
る第2巻鉄心22と、制御巻線24とが設けられ
ている。 In FIG. 1, a magnetic amplifier 10 includes a first core portion 12a and a second core portion 1 that constitute a main magnetic flux loop path.
2b and a magnetic shunt core 14 for bypassing a portion of the main magnetic flux loop path, the first volume core 12 acts as a first saturable core. A first series winding 16 and a shunt winding 18 are wound on the first core part 12a of the first core 12, and a second series winding 20 is wound on the second core part 12b. .
The first series winding 16 is connected between the high voltage terminal U and the medium voltage terminal U, and the shunt winding 18 is connected to the first series winding 16.
connected in series with the same polarity. The lower end of the shunt winding 18 is connected to the first neutral point V 1 . The second series winding 20 connects the lower end of the shunt winding 18 with the second neutral point V 2
The first series winding 16 is connected with the opposite polarity between the first series winding 16 and the first series winding 16 . A second winding core 22 that acts as a second saturable core to control the magnetic flux density of the magnetic shunt core 14 by changing the magnetic saturation state of at least a portion of the second core portion 12b, and a control winding 24. is provided.
第2〜3図において、第1巻鉄心12は主磁束
ループ路を構成するセンター・レツグ26とアウ
ター・レツグ28,30を備える。センター・レ
ツグ26は磁気分路鉄心14により区分された第
1コア部12aと第2コア部12bを備える。さ
らに、センター・レツグ26はアウター・レツグ
28,30の外側に延びる延長部、すなわち、第
3コア部12cを備える。センター・レツグ26
は第1巻鉄心12の上に配置されて、固定具3
2,34で互いに固定されて一体化される。第
2,3,5図より明らかなように、磁気分路鉄心
14は多枚数のケイ素鋼板を積層した断面C形状
の鉄心からなる。磁気分路鉄心14の溝14aは
センター・レツグ26と磁気的に結合するように
配置してある。磁気分路鉄心14の端部14b,
14cは第1直列巻線16および分路巻線18の
コイルブロツクと第2直列巻線20のコイルブロ
ツクとの間で一定のエアギヤツプに相当する所要
の厚みの間装物36,38を挟んで第1巻鉄心1
2のアウター・レツグ28,30上に配置され、
固定具40,42によつてアウター・レツグ2
8,30に固定されて、各鉄心は一体化される。
磁気分路鉄心14は主磁束ループ路の磁束の一部
を高リラクタンスをなすギヤツプ(間装物36,
38により形成される)を介してアウター・レツ
グ28,30に分路されて後述の如く出力電圧を
調整するとともに、高調波を減衰させ、出力電圧
の波形歪みを少なくするように機能する。第2巻
鉄心22は磁気分路鉄心14の下側において、す
なわち、第1直列巻線16および分路巻線18の
コイルブロツクと第2直列巻線20のコイルブロ
ツクとの間でセンター・レツグ26の第2コア部
12bの上部と第3コア部12cの下端部の上に
配置されて、固定具44,46によつて各鉄心は
一体化されて磁気的に結合される。このように、
第2巻鉄心22は第1巻鉄心12の下半部とオー
バーラツプするように配置され、第1可飽和鉄心
の一部を磁気飽和させて第2直列巻線20の磁束
が第1直列巻線16と分路巻線18の磁束に作用
しないようにするとともに、第1直列巻線16と
分路巻線18の磁束を磁気分路鉄心14にシフト
させるように起能する。第1直列巻線16および
分路巻線18、第2直列巻線20ならびに制御巻
線24はそれぞれセンター・レツグ26の第1〜
第3コア部12a,12b,12c上に巻かれ
て、ほぼ同一平面内に配置される。さらに、各巻
線の上面と下面は第2巻鉄心22の上面と第1巻
鉄心12の下面とにそれぞれ整列するように配置
される。すなわち、第1直列巻線16と分路巻線
18のコイル・ブロツクと第2直列巻線20から
なるコイル・ブロツクと、制御巻線24のコイ
ル・ブロツクはセンター・レツグ26、第1、第
2巻鉄心12,22の厚み内にほぼ配置される。
センター・レツグ26の第3コア部12Cは第1
巻鉄心12の外側に延びていて、制御巻線24は
センター・レツグ26の下端部12c上に巻かれ
ている。第2巻鉄心22は第2直列巻線20のコ
イル・ブロツクと制御巻線24のコイル・ブロツ
クを囲んでいる。第2,3図において第2巻鉄心
22の上部と下部はそれぞれ固定具44,46に
よりセンター・レツグ26とともに補助磁束ルー
プ路を構成し、制御巻線24に高流制御電流が供
給されたときに制御巻線24の磁束の通路として
機能する。すなわち、制御巻線24の磁束はセン
ター・レツグ26の第2コア部12bを部分的に
磁気飽和させ、もつて第1直列巻線16および分
路巻線18の磁束を主磁束ループから磁気分路鉄
心14を介してアウター・レツグ28,30にシ
フトさせる。 2 and 3, the first volume core 12 includes a center leg 26 and outer legs 28, 30 that constitute a main magnetic flux loop path. The center leg 26 includes a first core portion 12a and a second core portion 12b separated by the magnetic shunt core 14. Additionally, the center leg 26 includes an extension, or third core portion 12c, extending outwardly from the outer legs 28,30. center leg 26
is placed on the first core 12, and the fixture 3
2 and 34 to be fixed to each other and integrated. As is clear from FIGS. 2, 3, and 5, the magnetic shunt core 14 is composed of a C-shaped cross-sectional core made by laminating a large number of silicon steel plates. Groove 14a of magnetic shunt core 14 is arranged to magnetically couple with center leg 26. end portion 14b of magnetic shunt core 14;
14c is arranged between the coil blocks of the first series winding 16 and the shunt winding 18 and the coil block of the second series winding 20, with inserts 36 and 38 having a required thickness corresponding to a constant air gap sandwiched therebetween. Volume 1 iron core 1
placed on the outer legs 28, 30 of 2;
The outer leg 2 is fixed by the fixing devices 40 and 42.
8 and 30, each core is integrated.
The magnetic shunt core 14 transfers a part of the magnetic flux of the main magnetic flux loop path to a gap (intermediate 36,
38) to the outer legs 28, 30 to regulate the output voltage as described below and to attenuate harmonics and reduce waveform distortion of the output voltage. The second winding core 22 has a center leg on the underside of the magnetic shunt core 14, that is, between the coil blocks of the first series winding 16 and shunt winding 18 and the coil block of the second series winding 20. The iron cores are arranged on the upper part of the second core part 12b and the lower end part of the third core part 12c of 26, and the respective iron cores are integrated and magnetically coupled by the fixtures 44 and 46. in this way,
The second volume core 22 is arranged so as to overlap the lower half of the first volume core 12, and magnetically saturates a part of the first saturable core so that the magnetic flux of the second series winding 20 is transferred to the first series winding. 16 and shunt winding 18, and causes the magnetic flux of first series winding 16 and shunt winding 18 to be shifted to magnetic shunt core 14. The first series winding 16 and the shunt winding 18, the second series winding 20 and the control winding 24 are connected to the first to fourth windings of the center leg 26, respectively.
It is wound on the third core parts 12a, 12b, and 12c and arranged in substantially the same plane. Furthermore, the upper surface and the lower surface of each winding are arranged so as to be aligned with the upper surface of the second-volume core 22 and the lower surface of the first-volume core 12, respectively. That is, the coil block consisting of the first series winding 16, the shunt winding 18, the second series winding 20, and the control winding 24 are connected to the center leg 26, the first It is arranged approximately within the thickness of the two-turn iron cores 12 and 22.
The third core portion 12C of the center leg 26 is
Extending outside the wound core 12, the control winding 24 is wound onto the lower end 12c of the center leg 26. A second core 22 surrounds the coil block of the second series winding 20 and the control winding 24. In FIGS. 2 and 3, the upper and lower parts of the second core 22 constitute an auxiliary magnetic flux loop path with the center leg 26 by fixtures 44 and 46, respectively, and when a high current control current is supplied to the control winding 24, It functions as a path for the magnetic flux of the control winding 24. That is, the magnetic flux of the control winding 24 partially magnetically saturates the second core portion 12b of the center leg 26, causing the magnetic flux of the first series winding 16 and the shunt winding 18 to be magnetically separated from the main magnetic flux loop. It is shifted to the outer legs 28, 30 via the road core 14.
第1直列巻線16と分路巻線18はセンター・
レツグ26の第1コア部12a上に巻かれて単巻
変圧器を構成し、第2直列巻線20が第2コア1
2b上に第1直列巻線16とは逆極性で換かれ
て、いわゆる、差動結合される。 The first series winding 16 and the shunt winding 18 are connected to the center
The second series winding 20 is wound on the first core part 12a of the leg 26 to constitute an autotransformer.
2b, the first series winding 16 has a polarity opposite to that of the first series winding 16, and is so-called differentially coupled.
上記構成において、中圧端子uと第1中性端子
V1を交流電流に接続して、高圧端子Uと第2中
性点端子V2とを負荷に接続すると、第1、第2
直列巻線16,20に大電流が流れ、分路巻線1
8には入力電流と出力電流と差電流が流れる。 In the above configuration, the intermediate voltage terminal u and the first neutral terminal
When V 1 is connected to an alternating current and high voltage terminal U and second neutral terminal V 2 are connected to a load, the first and second
A large current flows through the series windings 16 and 20, and the shunt winding 1
8, an input current, an output current, and a difference current flow.
磁気増幅器10の自己容量を小さくして装置の
小形化を図るために、第1直列巻線16と分路巻
線18との巻線比を大きく選択する。たとえば、
中圧端子uと第1中性端子V1に100〔V〕の交流
電源を接続して、高圧端子Uと第2中性端子V2
を負荷に接続する目的で磁気増幅器10を設計す
るときは入力電圧100Vに対して出力電圧が1%
上昇して101Vとなるように第1直列巻線16の
巻線n1と分路巻線18の巻線n2を選択する。つぎ
に、第2直列巻線20の巻線n3は調整したい出力
電圧の変動範囲に応じて定める。すなわち、出力
電圧を101〜90.9〔V〕の10%の範囲内で変化させ
る場合には第2直列巻線20の巻線n3は下記の式
で定める。 In order to reduce the self-capacitance of the magnetic amplifier 10 and thereby downsize the device, the winding ratio between the first series winding 16 and the shunt winding 18 is selected to be large. for example,
Connect a 100 [V] AC power supply to the medium voltage terminal U and the first neutral terminal V 1 , and connect the high voltage terminal U and the second neutral terminal V 2
When designing the magnetic amplifier 10 for the purpose of connecting the
Winding n 1 of the first series winding 16 and winding n 2 of the shunt winding 18 are selected to increase to 101V. Next, the winding n3 of the second series winding 20 is determined according to the variation range of the output voltage to be adjusted. That is, when changing the output voltage within a range of 10% from 101 to 90.9 [V], the winding n3 of the second series winding 20 is determined by the following formula.
n3=(n1+n2)×E0−E′0/E0
上記式において、E0は最大出力電圧101〔V〕
に相当し、E′0は最少出力電圧90.9〔V〕に相当す
る。 n 3 = (n 1 + n 2 ) × E 0 −E′ 0 /E 0 In the above formula, E 0 is the maximum output voltage 101 [V]
E′ 0 corresponds to the minimum output voltage of 90.9 [V].
第1,2図において、制御巻線24に直流制御
電流が供給されないときは、第1直列巻線16と
分路巻線18および分路巻線18に差動結合され
た第2直列巻線20により生じた磁束がセンタ
ー・レツグ26からアウター・レツグ28,30
を通過して、センター・レツグ26に循還する。
このとき、第1直列巻線16と分路巻線18の生
ずる磁束φ1と第2直列巻線20の生ずる磁束φ2
とは逆方向になつているから、相互磁束全体とし
ては、差になつて作用する。したがつて、このと
きの出力電圧は最少のE′0となる。 1 and 2, when no DC control current is supplied to the control winding 24, the first series winding 16, the shunt winding 18, and the second series winding differentially coupled to the shunt winding 18 The magnetic flux generated by 20 is transferred from the center leg 26 to the outer legs 28, 30.
and circulates to the center leg 26.
At this time, the magnetic flux φ 1 generated by the first series winding 16 and the shunt winding 18 and the magnetic flux φ 2 generated by the second series winding 20
Since they are in opposite directions, the mutual magnetic flux as a whole acts as a difference. Therefore, the output voltage at this time is the minimum E′ 0 .
つぎに、制御巻線24をDC電源(図示せず)
に接続して、第2巻鉄心22を介してセンター・
レツグ26の第2、第3コア部12b,12cを
磁気飽和させると、第1直列巻線16と分路巻線
18の生ずる磁束φ1は磁気分路鉄心14にシフ
トされる。このとき、磁束φ1は第1コア部12
a,アウター・レツグ28,30および磁気分路
鉄心14を介して循還し、端子U,V2間の出力
電圧は最大のE0となる。制御巻線24に供給さ
れるDC電流を少なくすると、それに応じて出力
電圧は低下する。このように、センター・レツグ
26の第2、第3コア部12b,12cの磁気飽
和状態を可動制御することにより、第1直列巻線
16と分路巻線18に対する第2直列巻線の差動
結合状態を変化させて磁気分路鉄心14にシフト
れる第1直列巻線16および分路巻線18の磁束
を制御し、端子U,V2間の出力電圧を可変制御
できる。 Next, connect the control winding 24 to a DC power source (not shown).
to the center via the second volume iron core 22.
When the second and third core portions 12b and 12c of the leg 26 are magnetically saturated, the magnetic flux φ 1 generated by the first series winding 16 and the shunt winding 18 is shifted to the magnetic shunt core 14. At this time, the magnetic flux φ 1 is
a, circulates through the outer legs 28, 30 and the magnetic shunt core 14, and the output voltage between the terminals U, V2 is at a maximum E0 . When the DC current supplied to the control winding 24 is reduced, the output voltage is reduced accordingly. In this way, by movably controlling the magnetic saturation states of the second and third core portions 12b and 12c of the center leg 26, the difference between the second series winding 16 and the shunt winding 18 can be adjusted. The magnetic flux of the first series winding 16 and the shunt winding 18 shifted to the magnetic shunt core 14 is controlled by changing the dynamic coupling state, and the output voltage between the terminals U and V 2 can be variably controlled.
以上より明らかなように、本発明による磁気増
幅器はつぎのような効果をもたらす。
As is clear from the above, the magnetic amplifier according to the present invention provides the following effects.
本発明の磁気増幅器では自己容量の極めて小さ
な構造を採用したために、大幅な小形軽量化と低
価格化が図れる。しかも、磁気増幅器の使用材料
が著しく少なくなり、鉄損、銅損が少なくなるた
めに、高効率である。すなわち、鉄心の全長が短
くなつて磁気抵抗が減少し、全体の所要資材が減
り、損失の発生源が著しく減少するため、高効率
である。さらに、本発明の構造では単一の制御巻
線の採用を可能にして各巻鉄心と各巻線とを同一
平面内に配置したために、磁気増幅器の超薄形化
とコンパクト化が達成される。なお、センター・
レツグと各巻鉄心とは固定具により一体化したた
め、製造、組立が簡単である。さらに、主磁束ル
ープ路にエアギヤツプを介して磁気分路を設けた
ために、高調波を減衰させて出力電圧の波形歪み
を改善する効果がある。 Since the magnetic amplifier of the present invention employs a structure with extremely small self-capacitance, it can be significantly reduced in size, weight, and cost. Furthermore, the magnetic amplifier uses significantly less material, and iron loss and copper loss are reduced, resulting in high efficiency. That is, the overall length of the iron core is shortened, reducing magnetic reluctance, reducing overall material requirements, and significantly reducing sources of loss, resulting in high efficiency. Further, in the structure of the present invention, it is possible to employ a single control winding and each winding core and each winding are arranged in the same plane, so that the magnetic amplifier can be made ultra-thin and compact. In addition, the center
Since the leg and each core are integrated with a fixture, manufacturing and assembly are easy. Furthermore, since a magnetic shunt is provided in the main magnetic flux loop path via an air gap, harmonics are attenuated and waveform distortion of the output voltage is improved.
第1図は本発明による磁気増幅器の望ましい実
施例の結線図、第2図は第1図の磁気増幅器の平
面図、第3図は第2図の磁気増幅器の右側図、第
4図は第2図の磁気増幅器の底面図、第5図は第
2図のV−V線の断面図をそれぞれ示す。
12……第1巻鉄心、16……第1直列巻線、
18……分路巻線、20……第2直列巻線、22
……第2巻鉄心、24……制御巻線、26……セ
ンター・レツグ、28,30……アウター・レツ
グ。
FIG. 1 is a wiring diagram of a preferred embodiment of the magnetic amplifier according to the present invention, FIG. 2 is a plan view of the magnetic amplifier of FIG. 1, FIG. 3 is a right side view of the magnetic amplifier of FIG. 2, and FIG. FIG. 2 shows a bottom view of the magnetic amplifier, and FIG. 5 shows a sectional view taken along line V-V in FIG. 2, respectively. 12...First volume iron core, 16...First series winding,
18...Shunt winding, 20...Second series winding, 22
... Second volume iron core, 24 ... Control winding, 26 ... Center leg, 28, 30 ... Outer leg.
Claims (1)
された分路巻線とこの分路巻線とは異なる極性で
分路巻線に直列接続された第2直列巻線とを有す
る第1可飽和鉄心を備えた主磁束ループ路と、前
記分路巻線と前記第2直列巻線との間に配置され
て前記主磁束ループ路の一部をバイパスさせるた
めのエアギヤツプを備えた少くとも1つの磁気分
路鉄心と、前記磁気分路鉄心と前記第2直列巻線
との間の前記第1可飽和鉄心の一部とその延長部
とに磁気的に結合された第2可飽和鉄心を備えた
補助磁束ループ路と、前記第1可飽和鉄心の前記
延長部に巻装され、前記第2可飽和鉄心を介して
前記第1可飽和鉄心の前記一部を磁気飽和させて
前記第1直列巻線と前記分路巻線の磁束を前記磁
気分路鉄心にシフトさせるための制御巻線とを備
えた磁気増幅器。 2 前記第1可飽和鉄心がセンター・レツグとア
ウター・レツグを有する第1巻鉄心を備え、前記
補助磁束ループ路が前記センター・レツグ上に前
記第2直列巻線と前記制御巻線を囲むように配置
された第2巻鉄心とを備え、前記センター・レツ
グが前記第1巻鉄心の外方に延びる前記延長部を
備えたことを特徴とする特許請求の範囲第1項記
載の磁気増幅器。 3 前記第1巻鉄心と前記センター・レツグとを
固定する第1の固定具と、前記第2巻鉄心と前記
センター・レツグとを固定する第2の固定具とを
さらに備えたことを特徴とする特許請求の範囲第
2項記載の磁気増幅器。 4 前記センター・レツグの一方の側に前記第1
巻鉄心が配置され、前記センター・レツグの他方
側に前記第2巻鉄心が配置されたことを特徴とす
る特許請求の範囲第2項ないし第3項記載の磁気
増幅器。 5 前記第1直列巻線および前記分路巻線と、前
記第2直列巻線と、前記制御巻線とがほぼ同一平
面内に配置されたことを特徴とする特許請求の範
囲第4項記載の磁気増幅器。 6 前記第1直列巻線および分路巻線と、前記第
2直列巻線と、前記制御巻線とが前記センター・
レツグと前記第1および第2巻鉄心との厚み内に
ほぼ配置されたことを特徴とする特許請求の範囲
第5項記載の磁気増幅器。[Claims] 1. A first series winding, a shunt winding connected in series to the first series winding, and a second series winding connected in series to the shunt winding with a polarity different from that of the shunt winding. a main magnetic flux loop path including a first saturable core having a series winding; and a main magnetic flux loop path disposed between the shunt winding and the second series winding to bypass a portion of the main magnetic flux loop path. at least one magnetic shunt core with an air gap for magnetically discharging a portion of the first saturable core and an extension thereof between the magnetic shunt core and the second series winding. an auxiliary magnetic flux loop path having a coupled second saturable core; and an auxiliary magnetic flux loop path wound around the extension of the first saturable core and connected to the first saturable core via the second saturable core. a control winding for magnetically saturating the first series winding and shifting the magnetic flux of the shunt winding to the magnetic shunt core. 2. The first saturable core includes a first-turn core having a center leg and an outer leg, and the auxiliary flux loop path surrounds the second series winding and the control winding on the center leg. 2. The magnetic amplifier according to claim 1, further comprising: a second-volume core disposed in the center leg, and wherein said center leg includes said extension portion extending outward from said first-volume core. 3, further comprising a first fixture for fixing the first volume core and the center leg, and a second fixture for fixing the second volume core and the center leg. A magnetic amplifier according to claim 2. 4. On one side of the center leg, the first
4. The magnetic amplifier according to claim 2, wherein a wound core is disposed, and the second wound core is disposed on the other side of the center leg. 5. The first series winding, the shunt winding, the second series winding, and the control winding are arranged in substantially the same plane. magnetic amplifier. 6. The first series winding and shunt winding, the second series winding, and the control winding are connected to the center winding.
6. The magnetic amplifier according to claim 5, wherein the magnetic amplifier is disposed substantially within the thickness of the leg and the first and second cores.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP23899987A JPS6482810A (en) | 1987-09-25 | 1987-09-25 | Magnetic amplifier |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP23899987A JPS6482810A (en) | 1987-09-25 | 1987-09-25 | Magnetic amplifier |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6482810A JPS6482810A (en) | 1989-03-28 |
| JPH0262044B2 true JPH0262044B2 (en) | 1990-12-21 |
Family
ID=17038395
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP23899987A Granted JPS6482810A (en) | 1987-09-25 | 1987-09-25 | Magnetic amplifier |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6482810A (en) |
-
1987
- 1987-09-25 JP JP23899987A patent/JPS6482810A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS6482810A (en) | 1989-03-28 |
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