JPS6047730B2 - reactor - Google Patents

reactor

Info

Publication number
JPS6047730B2
JPS6047730B2 JP56054545A JP5454581A JPS6047730B2 JP S6047730 B2 JPS6047730 B2 JP S6047730B2 JP 56054545 A JP56054545 A JP 56054545A JP 5454581 A JP5454581 A JP 5454581A JP S6047730 B2 JPS6047730 B2 JP S6047730B2
Authority
JP
Japan
Prior art keywords
magnetic
reactor
magnetic flux
magnetic core
shielding device
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
Application number
JP56054545A
Other languages
Japanese (ja)
Other versions
JPS57169219A (en
Inventor
捷敏 東
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric Corp
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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP56054545A priority Critical patent/JPS6047730B2/en
Publication of JPS57169219A publication Critical patent/JPS57169219A/en
Publication of JPS6047730B2 publication Critical patent/JPS6047730B2/en
Expired legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F27/00Details of transformers or inductances, in general
    • H01F27/34Special means for preventing or reducing unwanted electric or magnetic effects, e.g. no-load losses, reactive currents, harmonics, oscillations, leakage fields
    • H01F27/36Electric or magnetic shields or screens
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F27/00Details of transformers or inductances, in general
    • H01F27/34Special means for preventing or reducing unwanted electric or magnetic effects, e.g. no-load losses, reactive currents, harmonics, oscillations, leakage fields
    • H01F27/36Electric or magnetic shields or screens
    • H01F27/363Electric or magnetic shields or screens made of electrically conductive material

Landscapes

  • Engineering & Computer Science (AREA)
  • Power Engineering (AREA)
  • Regulation Of General Use Transformers (AREA)

Description

【発明の詳細な説明】 この発明は、リアクトル特に車両に搭載されるリアクト
ルの漏洩磁束による誘導障害を抑えるための磁気シール
ドに関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a magnetic shield for suppressing induction disturbances caused by leakage magnetic flux of a reactor, particularly a reactor mounted on a vehicle.

一般にリアクトルにおける磁束は、第1図に示す如く磁
芯1−1の周辺では、Φ、のような磁芯による対称な分
布をしている。
In general, the magnetic flux in the reactor has a symmetrical distribution around the magnetic core 1-1, as shown in FIG. 1, as Φ.

従つて例えばA点に信号検知用センサ等があると、リア
クトルの漏洩磁束によつて誘導障害を受ける。
Therefore, for example, if a signal detection sensor or the like is located at point A, the leakage magnetic flux of the reactor will cause an induction disturbance.

この誘導障害を抑えるために従来は第2図に示すように
シールド装置2をリアクトルのコイル1の外側に配設し
ていた。このシールド装置2は製作の容易さや構造の強
化のために通常磁心1−1に対称的にコイルを取りまい
て円筒形、または箱形にアルミ板または銅板のような非
磁性で導電性の高い材料で構成されていた。従つて直流
磁束シールド装置2の影響を受けないが、脈動磁界は、
シールド装置2でブ上ツクされ、Φ。
In order to suppress this induced disturbance, conventionally a shield device 2 was disposed outside the coil 1 of the reactor as shown in FIG. This shielding device 2 is usually made of a non-magnetic and highly conductive material such as an aluminum plate or a copper plate in a cylindrical or box shape, with a coil symmetrically surrounding the magnetic core 1-1 for ease of manufacture and strengthening of the structure. It was made up of materials. Therefore, it is not affected by the DC magnetic flux shielding device 2, but the pulsating magnetic field is
Bookmarked by shield device 2, Φ.

のように磁路長が延長される。磁束Φは、起磁力をAT
)磁気抵抗をRとした場合、Φ=−となる。
The magnetic path length is extended as follows. The magnetic flux Φ is the magnetomotive force AT
) If magnetic resistance is R, then Φ=-.

空心リアクトルではRは磁路長に比例的に大きくなるの
で、第2図のものではシールド装置2によつて磁路長が
長くなり、A点に影響を及ぼす磁束は減少する。
In an air-core reactor, R increases in proportion to the magnetic path length, so in the one shown in FIG. 2, the magnetic path length is increased by the shield device 2, and the magnetic flux affecting point A is reduced.

しかしこのような装置では、磁路長が長くなるだけの効
果はあるが、その効果を顕著にするためにはシールド装
置を磁心方向に長大化しなければならず、装置が大形化
する欠点があつた。この発明はこのような従来のものの
欠点を除去しようとするもので、シールド装置を磁芯に
対し一て非対称に構成しリアクトル周辺の必要な位置で
の磁束密度を減少させようとするものである。
However, in such a device, although the effect is simply that the magnetic path length is lengthened, the shielding device must be made longer in the direction of the magnetic core in order to make the effect noticeable, which has the disadvantage of increasing the size of the device. It was hot. This invention attempts to eliminate such drawbacks of the conventional system by configuring the shield device asymmetrically with respect to the magnetic core to reduce the magnetic flux density at necessary positions around the reactor. .

以下第3図〜第6図にもとづいてこの発明の原理ならび
に各実施例を説明する。即ち第3図イに示す如く磁芯に
対称な状態でシノールド装置2を設けた場合の磁束Φに
比べ、第3図口に示す如く磁芯に対して非対称な状態で
シールド装置を設けたものでは、シールド装置の無い部
分で磁気抵抗が小さくなるので、磁束が増大し、磁芯部
での磁束密度が高くなり、磁芯部所要夕ATが増大する
The principle of this invention and each embodiment will be explained below based on FIGS. 3 to 6. That is, compared to the magnetic flux Φ when the sinold device 2 is installed in a symmetrical state with respect to the magnetic core as shown in FIG. In this case, the magnetic resistance decreases in the area where there is no shielding device, so the magnetic flux increases, the magnetic flux density in the magnetic core increases, and the required AT of the magnetic core increases.

この磁芯部での所要ATの増大のために、A点近傍を通
る磁束Φ2は小さくなり、イの場合の磁束Φ、>Φ2な
る関係が成立する。従つて第4図に示す如く、リアクト
ルのコイル1に対してA点に近接する部分は磁芯方向に
長く、A点から遠い部分は短く構成されたシールド装置
2で、シールドしたものでは磁束は磁路長の短いA点に
遠い部分に集まり、A点に近い部分はΦ2の如く少なく
なる。
Due to the increase in the required AT in the magnetic core portion, the magnetic flux Φ2 passing near point A becomes smaller, and the relationship of magnetic flux Φ>Φ2 in case A is established. Therefore, as shown in FIG. 4, the shielding device 2 is configured such that the part of the reactor coil 1 that is close to point A is long in the direction of the magnetic core, and the part that is far from point A is short. It gathers in the part far from point A where the magnetic path length is short, and the part close to point A becomes smaller like Φ2.

なお、第5図に示す如くシールド装置2を磁心に対して
片側即ちA点側にのみ配置してもよい。
Incidentally, as shown in FIG. 5, the shield device 2 may be arranged only on one side with respect to the magnetic core, that is, on the point A side.

また第6図に示す如く目的の個所の誘導障害を抑えるた
めのシールド装置2の他に、目的の個所から遠い部分に
磁性部材3を配置し、全体の磁束をより増大させて、目
的の個所の近傍の漏洩脈動磁束を抑えるようにしてもよ
い。上記のようにこの発明によるリアクトルは、非磁性
で導電性の高い材料でなる磁気シールド装置をコイルの
磁芯に対して非対称に配置したもので、リアクトル周辺
の目的の個所での脈動磁束を減少させ、誘導障害を効果
的に抑えることができる。
In addition, as shown in FIG. 6, in addition to the shielding device 2 for suppressing induction disturbances at the target location, a magnetic member 3 is placed at a portion far from the target location to further increase the overall magnetic flux. It may be possible to suppress leakage pulsating magnetic flux in the vicinity of . As mentioned above, the reactor according to the present invention has a magnetic shielding device made of a non-magnetic and highly conductive material arranged asymmetrically with respect to the magnetic core of the coil, thereby reducing pulsating magnetic flux at a desired location around the reactor. This can effectively suppress induction disturbances.

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

第1図および第2図は従来のリアクトルを示す側断面図
、第3図はこの発明の原理を説明するための側断面図、
第4図〜第6図はこの発明の各実施例を示す側断面図で
ある。 図中、1はコイル、2はシールド装置、3は磁性部材で
ある。
1 and 2 are side sectional views showing a conventional reactor, and FIG. 3 is a side sectional view for explaining the principle of the present invention.
4 to 6 are side sectional views showing each embodiment of the present invention. In the figure, 1 is a coil, 2 is a shield device, and 3 is a magnetic member.

Claims (1)

【特許請求の範囲】 1 コイル、このコイルの磁芯に対して非対称に配置さ
れた非磁性で導電性の高い材料でなる磁気シールド装置
を備えたリアクトル。 2 磁気シールド装置は磁芯方向に長さが異つている特
許請求の範囲第1項記載のリアクトル。 3 磁気シールド装置は磁芯に対して一方側にのみ配置
されている特許請求の範囲第1項記載のリアクトル。 4 磁芯に対して他方側には磁性部材が配置されている
特許請求の範囲第3項記載のリアクトル。
[Claims] 1. A reactor equipped with a coil and a magnetic shielding device made of a non-magnetic and highly conductive material arranged asymmetrically with respect to the magnetic core of the coil. 2. The reactor according to claim 1, wherein the magnetic shielding device has different lengths in the direction of the magnetic core. 3. The reactor according to claim 1, wherein the magnetic shielding device is arranged only on one side with respect to the magnetic core. 4. The reactor according to claim 3, wherein a magnetic member is disposed on the other side with respect to the magnetic core.
JP56054545A 1981-04-09 1981-04-09 reactor Expired JPS6047730B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56054545A JPS6047730B2 (en) 1981-04-09 1981-04-09 reactor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56054545A JPS6047730B2 (en) 1981-04-09 1981-04-09 reactor

Publications (2)

Publication Number Publication Date
JPS57169219A JPS57169219A (en) 1982-10-18
JPS6047730B2 true JPS6047730B2 (en) 1985-10-23

Family

ID=12973643

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56054545A Expired JPS6047730B2 (en) 1981-04-09 1981-04-09 reactor

Country Status (1)

Country Link
JP (1) JPS6047730B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN106252047A (en) * 2016-08-29 2016-12-21 苏州腾冉电气设备股份有限公司 A kind of low magnetism leakage air reactor

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB8332177D0 (en) * 1983-12-01 1984-01-11 Oxford Magnet Tech Magnet system

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN106252047A (en) * 2016-08-29 2016-12-21 苏州腾冉电气设备股份有限公司 A kind of low magnetism leakage air reactor
CN106252047B (en) * 2016-08-29 2018-02-02 苏州腾冉电气设备股份有限公司 A kind of low magnetism leakage air reactor

Also Published As

Publication number Publication date
JPS57169219A (en) 1982-10-18

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