JPS60152012A - Transformer - Google Patents
TransformerInfo
- Publication number
- JPS60152012A JPS60152012A JP59008325A JP832584A JPS60152012A JP S60152012 A JPS60152012 A JP S60152012A JP 59008325 A JP59008325 A JP 59008325A JP 832584 A JP832584 A JP 832584A JP S60152012 A JPS60152012 A JP S60152012A
- Authority
- JP
- Japan
- Prior art keywords
- core
- ferromagnetic material
- eddy current
- transformer
- delta
- 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
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
Landscapes
- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Hard Magnetic Materials (AREA)
- Soft Magnetic Materials (AREA)
Abstract
Description
【発明の詳細な説明】 く技iホ■分野〉 本発明はトランスに関するものである。[Detailed description of the invention] Technical field The present invention relates to a transformer.
〈従来技術〉
従来のトランスは、鉄等の強磁性体を磁気回路用コアと
して用いており、そのためトランスの重量が■く、又、
うず電流による損失や発熱を考慮する必要があった。<Prior art> Conventional transformers use a ferromagnetic material such as iron as the core for the magnetic circuit, and as a result, the weight of the transformer is small.
It was necessary to consider loss and heat generation due to eddy current.
〈発明の目的〉
本発明は、このような点に鑑みてなされ、トランスのコ
アとして有機物強磁性体を用いることで軽量化を計り、
しかも絶縁体であるためうず電流もほとんど流れず、損
失や発熱の考慮の必要がな、い1−ランスを提供するこ
とを目的とする。<Object of the Invention> The present invention was made in view of the above points, and aims to reduce the weight by using an organic ferromagnetic material as the core of the transformer.
Moreover, since it is an insulator, almost no eddy current flows, and there is no need to consider loss or heat generation.
〈実施例〉 以下図面に従って本発明の一実施例を説明する。<Example> An embodiment of the present invention will be described below with reference to the drawings.
第1図において、1は例えばAClooVの交流電圧が
印加される一次側コイル、2は一次側コイ/l/1との
巻線比に従って所定の出力’tri:圧が+1yり出さ
れる二次側コイルである。3は一次側コイル1と二次側
コイ/Ly2の間で磁気回路を形成するコアで、有機物
強磁性体からなる。この有機物強磁性体としては、例え
ばピリジン環の縮合ポリマーの鉄誘導体がある。In Fig. 1, 1 is a primary coil to which an AC voltage of AClooV is applied, for example, and 2 is a secondary coil to which a predetermined output 'tri:pressure of +1y is output according to the winding ratio with the primary coil/l/1. It is a coil. A core 3 forms a magnetic circuit between the primary coil 1 and the secondary coil/Ly2, and is made of an organic ferromagnetic material. Examples of this organic ferromagnetic material include iron derivatives of pyridine ring condensation polymers.
コイ/v1,2が巻かれているコア3ば、−次側コイl
し1からの交流−次入力に応じて、第2図に示されるよ
うな磁束の交流変化を生じる。この時、コア3は閉じた
磁気回路を形成しているので、磁束はほとんど外にもれ
ない。そして、二次側コイ/l/2が巻いである部分も
磁束は交流的に変化する3゜すると、MAXWELLの
方程式
%式%
)
に従って、二次側コイ/L/2には一次、二次の巻線比
に応じた父’UE ’=L圧が生じる。Core 3 on which coil/v1, 2 is wound, - next side coil l
In response to the alternating current input from 1, an alternating current change in magnetic flux as shown in FIG. 2 occurs. At this time, since the core 3 forms a closed magnetic circuit, almost no magnetic flux leaks out. Then, the magnetic flux also changes in an alternating current manner in the part where the secondary coil /l/2 is wound.If 3 degrees, then according to MAXWELL's equation, the secondary coil /l/2 has primary and secondary coils. UE'=L pressure is generated depending on the winding ratio.
ここに、コア3の内部を考えると1
.1lD
r o t 11 ” i + −(アンペアの法則)
t
(II:磁場、 i:゛電流、D:′電束密度)から、
コア3の電気電導率をσとすると、!−σEとかける。Considering the inside of core 3, 1. 1lD r o t 11 ” i + − (Ampere's law)
From t (II: magnetic field, i: current, D: electric flux density),
If the electrical conductivity of core 3 is σ, then! Multiply by −σE.
このσEがうず電流であり、このコア3をl’ff)成
するイJ機物強磁性体が絶縁物であればσ−0であり、
うす電流は流れず、損失や発熱は少なくてすむ。If this σE is an eddy current and the ferromagnetic material forming the core 3 is an insulator, then σ-0,
No thin current flows, so there is less loss and heat generation.
また、上記したように閉じたコア3を用いれば、イa気
回路として外部への交流磁束もほとんどないである。Further, if the closed core 3 is used as described above, there is almost no alternating current magnetic flux to the outside as an a-air circuit.
〈発明の効果〉
以上のように本発明によれば、効率のよい、軽量で@熱
の少ない有用なトランスが提供できる。<Effects of the Invention> As described above, according to the present invention, a useful transformer that is efficient, lightweight, and generates little heat can be provided.
第1図は本発明の一実施例ケ示すIQi n’ji図、
第2図はコア内の磁束の流汎をljh+明する1ツ1で
ある3、1−次1111コイル、2・・−二次側コイル
、3・・・コア。FIG. 1 is an IQin'ji diagram showing one embodiment of the present invention;
Fig. 2 shows the distribution of magnetic flux in the core.3, 1-order 1111 coil, 2...-secondary side coil, 3...core.
Claims (1)
を特徴とするトランス。l A transformer characterized by using an organic ferromagnetic material for a magnetic circuit core.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59008325A JPS60152012A (en) | 1984-01-19 | 1984-01-19 | Transformer |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59008325A JPS60152012A (en) | 1984-01-19 | 1984-01-19 | Transformer |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPS60152012A true JPS60152012A (en) | 1985-08-10 |
Family
ID=11690022
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP59008325A Pending JPS60152012A (en) | 1984-01-19 | 1984-01-19 | Transformer |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS60152012A (en) |
Cited By (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0399367U (en) * | 1990-01-29 | 1991-10-17 | ||
| FR2703467A1 (en) * | 1993-03-29 | 1994-10-07 | Mecagis | Zero flux Hall effect current sensor particularly for motor vehicles and electric scooters. |
| US6501347B1 (en) | 1999-09-24 | 2002-12-31 | Ngk Spark Plug Co., Ltd. | Dielectric filter having forked auxiliary conductor |
| US6640419B2 (en) | 1999-06-04 | 2003-11-04 | Liaisons Electroniques-Mecaniques Lem S.A. | Method of making a magnetic circuit with coil |
-
1984
- 1984-01-19 JP JP59008325A patent/JPS60152012A/en active Pending
Cited By (7)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0399367U (en) * | 1990-01-29 | 1991-10-17 | ||
| FR2703467A1 (en) * | 1993-03-29 | 1994-10-07 | Mecagis | Zero flux Hall effect current sensor particularly for motor vehicles and electric scooters. |
| WO1994023305A1 (en) * | 1993-03-29 | 1994-10-13 | Mecagis | Electric current measuring device with a magnetic flux sensor, in particular for electric vehicles |
| US5734264A (en) * | 1993-03-29 | 1998-03-31 | Mecagis | Device for measuring electric current, including a sensor sensitive to magnetic flux and intended in particular for electrically propelled vehicles |
| US6640419B2 (en) | 1999-06-04 | 2003-11-04 | Liaisons Electroniques-Mecaniques Lem S.A. | Method of making a magnetic circuit with coil |
| US6987439B2 (en) | 1999-06-04 | 2006-01-17 | Liaisons Electroniques-Mecaniques Lem Sa | Magnetic circuit with coil |
| US6501347B1 (en) | 1999-09-24 | 2002-12-31 | Ngk Spark Plug Co., Ltd. | Dielectric filter having forked auxiliary conductor |
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