JPH0584046B2 - - Google Patents
Info
- Publication number
- JPH0584046B2 JPH0584046B2 JP58124411A JP12441183A JPH0584046B2 JP H0584046 B2 JPH0584046 B2 JP H0584046B2 JP 58124411 A JP58124411 A JP 58124411A JP 12441183 A JP12441183 A JP 12441183A JP H0584046 B2 JPH0584046 B2 JP H0584046B2
- Authority
- JP
- Japan
- Prior art keywords
- divided bodies
- reactor
- conductor
- magnetic core
- annular 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 - Lifetime
Links
- 239000004020 conductor Substances 0.000 claims description 28
- 239000000843 powder Substances 0.000 claims description 12
- 239000000203 mixture Substances 0.000 claims description 4
- 229920005989 resin Polymers 0.000 claims description 3
- 239000011347 resin Substances 0.000 claims description 3
- 238000000748 compression moulding Methods 0.000 claims description 2
- 239000002184 metal Substances 0.000 claims description 2
- 229910052751 metal Inorganic materials 0.000 claims description 2
- 229920001187 thermosetting polymer Polymers 0.000 claims description 2
- 229920001169 thermoplastic Polymers 0.000 claims 1
- 239000004416 thermosoftening plastic Substances 0.000 claims 1
- 230000000694 effects Effects 0.000 description 6
- 239000006247 magnetic powder Substances 0.000 description 5
- 229910045601 alloy Inorganic materials 0.000 description 4
- 239000000956 alloy Substances 0.000 description 4
- 239000002245 particle Substances 0.000 description 4
- 229910000859 α-Fe Inorganic materials 0.000 description 3
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical compound [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 description 2
- 239000000696 magnetic material Substances 0.000 description 2
- 229920006122 polyamide resin Polymers 0.000 description 2
- 229910000838 Al alloy Inorganic materials 0.000 description 1
- RYGMFSIKBFXOCR-UHFFFAOYSA-N Copper Chemical compound [Cu] RYGMFSIKBFXOCR-UHFFFAOYSA-N 0.000 description 1
- 229910017061 Fe Co Inorganic materials 0.000 description 1
- 229910017082 Fe-Si Inorganic materials 0.000 description 1
- 229910017133 Fe—Si Inorganic materials 0.000 description 1
- 229910001030 Iron–nickel alloy Inorganic materials 0.000 description 1
- 229910000990 Ni alloy Inorganic materials 0.000 description 1
- 229910000676 Si alloy Inorganic materials 0.000 description 1
- 229910002796 Si–Al Inorganic materials 0.000 description 1
- 229910000831 Steel Inorganic materials 0.000 description 1
- 238000001816 cooling Methods 0.000 description 1
- 239000000498 cooling water Substances 0.000 description 1
- 229910052802 copper Inorganic materials 0.000 description 1
- 239000010949 copper Substances 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
- 239000003822 epoxy resin Substances 0.000 description 1
- 230000005284 excitation Effects 0.000 description 1
- 238000010438 heat treatment Methods 0.000 description 1
- 238000009413 insulation Methods 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 238000000465 moulding Methods 0.000 description 1
- 229920005668 polycarbonate resin Polymers 0.000 description 1
- 239000004431 polycarbonate resin Substances 0.000 description 1
- 229920000647 polyepoxide Polymers 0.000 description 1
- 229920001225 polyester resin Polymers 0.000 description 1
- 239000004645 polyester resin Substances 0.000 description 1
- 239000004065 semiconductor Substances 0.000 description 1
- 239000010959 steel Substances 0.000 description 1
- 238000005728 strengthening Methods 0.000 description 1
- 230000003746 surface roughness Effects 0.000 description 1
- 229920005992 thermoplastic resin Polymers 0.000 description 1
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
- H01F27/255—Magnetic cores made from particles
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F37/00—Fixed inductances not covered by group H01F17/00
Landscapes
- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Coils Or Transformers For Communication (AREA)
- General Induction Heating (AREA)
Description
【発明の詳細な説明】
〔発明の技術分野〕
本発明は、1つまたは複数の環状磁心を導体に
外装してなる大電流用のリアクトルに関する。DETAILED DESCRIPTION OF THE INVENTION [Technical Field of the Invention] The present invention relates to a reactor for large currents, which is formed by surrounding one or more annular magnetic cores with a conductor.
従来より、半導体素子を用いた電力変換装置等
に用いられる大電流用のリアクトルであつて、比
較的小インダクタンスのものとして、たとえば第
1図に示すリアクトルがある。
2. Description of the Related Art Conventionally, there is a reactor shown in FIG. 1, for example, as a large current reactor with a relatively small inductance used in power converters and the like using semiconductor elements.
このリアクトルは、図に示す如く、表面に絶縁
処理が施された棒状の導体1と、この導体1に順
次外装されて軸方向に直列配置された複数の環状
磁心2と、上記導体1の両端部に取り付けられた
端子3とで構成されている。 As shown in the figure, this reactor consists of a rod-shaped conductor 1 whose surface is insulated, a plurality of annular magnetic cores 2 that are sequentially sheathed around this conductor 1 and arranged in series in the axial direction, and both ends of the conductor 1. It consists of a terminal 3 attached to the section.
このようなリアクトルは環状磁心の数、形状お
よび大きさ等で容易にインダクタンスを調整で
き、構造が単純であるうえ、サージ電流に対する
導体の機械的強度が高いなどの利点がある。 Such a reactor has advantages such as the inductance can be easily adjusted by adjusting the number, shape, size, etc. of the annular magnetic cores, the structure is simple, and the conductor has high mechanical strength against surge currents.
ところで、このようなリアクトルでは、導体1
に環状磁心2を嵌合させる際の作業性を考慮し
て、導体1の外径と環状磁心2の内径とに僅かの
隙間を持たせている。しかしながら、この隙間は
導体1から環状磁心2へ与えられる励磁力を弱
め、所望のインダクタンスを得るための環状磁心
の必要体積を増加させる結果をもたらす。 By the way, in such a reactor, conductor 1
In consideration of workability when fitting the annular magnetic core 2 to the annular magnetic core 2, a slight gap is provided between the outer diameter of the conductor 1 and the inner diameter of the annular magnetic core 2. However, this gap weakens the excitation force applied from the conductor 1 to the annular magnetic core 2, resulting in an increase in the required volume of the annular magnetic core to obtain a desired inductance.
そこで、このような不具合を解消するため、電
磁鋼板またはフエライト等からなる環状磁心を直
径方向に2分割し、得られた分割体(カツトコ
ア)を導体に外装した後、再び衝き合わせてリア
クトルを構成することが行われている。これによ
つて磁心の導体への装着を容易にし、同時に導体
と磁心との密着性をも高めることが可能となる。
しかしながら、このようなカツトコアを用いて上
記の密着性を確保するためには、特別にカツトコ
アを締結するための締結部材が必要となり、却つ
て装置が大型化するという問題があつた。 Therefore, in order to solve this problem, we divided the annular magnetic core made of electromagnetic steel plate or ferrite into two in the diametrical direction, covered the resulting divided bodies (cut cores) with conductors, and then brought them together again to form a reactor. things are being done. This makes it possible to easily attach the magnetic core to the conductor, and at the same time to improve the adhesion between the conductor and the magnetic core.
However, in order to ensure the above-mentioned adhesion using such a cut core, a special fastening member for fastening the cut core is required, which has the problem of increasing the size of the device.
また、上記の分割面での接合状態も芳しくな
く、磁気抵抗が増大して所望のインダクタンスを
得ることができないという問題もあつた。また、
特にフエライト等では磁歪が顕著であり、分割面
での騒音が問題となることもあつた。 Further, the bonding condition at the above-mentioned dividing plane was not good, and there was also the problem that the magnetic resistance increased, making it impossible to obtain the desired inductance. Also,
In particular, magnetostriction is noticeable in ferrite, etc., and noise at the split surface sometimes becomes a problem.
本発明は、かかる点に鑑みてなされたものであ
り、その目的とするところは、環状磁心を複数の
分割体で構成しながらも、特に締結部材を必要と
することなく導体と磁心および分割体と分割体の
高い密着性を確保でき、もつて外形の小型化、構
造の簡単化が図れるリアクトルを提供することに
ある。
The present invention has been made in view of the above, and an object of the present invention is to form a conductor, a magnetic core, and the divided bodies without particularly requiring a fastening member, even though the annular magnetic core is composed of a plurality of divided bodies. It is an object of the present invention to provide a reactor which can ensure high adhesion between the divided bodies and the reactor, which can have a smaller external size and a simpler structure.
本発明に係るリアクトルは、その環状磁心が、
周方向に複数に分さ割れた分割体の集合によつて
構成され、かつその分割体に形成された溝および
突条の嵌合結合によつて、各分割体が一体的に結
合されている。そして、上記溝および突条は分割
体の軸方向への相対的なスライドによつて、上記
分割体の接合部分の密着度を高めるくさび作用を
発揮するように設けられている。
In the reactor according to the present invention, the annular magnetic core is
It is composed of a set of divided bodies divided into a plurality of parts in the circumferential direction, and each divided body is integrally connected by the fitting connection of grooves and protrusions formed in the divided bodies. . The grooves and the protrusions are provided so as to exhibit a wedge effect that increases the degree of adhesion between the joined portions of the divided bodies by relative sliding of the divided bodies in the axial direction.
本発明によれば、環状磁心を複数の分割体で構
成しているので、磁心の導体への外装作業が極め
てスムーズに行えることになる。
According to the present invention, since the annular magnetic core is composed of a plurality of divided bodies, the exterior work of the magnetic core to the conductor can be performed extremely smoothly.
そして、これら分割体は、分割体に形成された
突条と溝とのくさび作用によつて、互いの接合部
分の密着度を高めることができるので、分割体相
互の磁気的結合の強化を図れるとともに、導体と
分割体との密着性をも高めることが可能となる。
この結果、所望のインダクタンスを得るための必
要磁心体積を小さく設定することができる。しか
も、分割体相互を締結部材を用いることなく連結
できるので、全体の小型化、構造の簡単化を図れ
るという多大なる効果を奏する。 These divided bodies can increase the degree of adhesion between the joints of each other due to the wedge action between the protrusions and grooves formed on the divided bodies, thereby strengthening the magnetic coupling between the divided bodies. At the same time, it is possible to improve the adhesion between the conductor and the divided body.
As a result, the required magnetic core volume to obtain the desired inductance can be set small. Moreover, since the divided bodies can be connected to each other without using a fastening member, there is a great effect that the overall size can be reduced and the structure can be simplified.
以下、本発明の詳細を図示の実施例に基づき説
明する。
Hereinafter, details of the present invention will be explained based on illustrated embodiments.
第2図は本発明の一実施例に係るリアクトルの
外観を示した斜視図である。 FIG. 2 is a perspective view showing the appearance of a reactor according to an embodiment of the present invention.
本実施例に係るリアクトルは、表面が絶縁層で
覆われた棒状導体1と、この導体1に順次外装さ
れて軸方向に直列配置された複数の環状磁心4
と、上記導体1の両端部に取付けられた端子3と
で構成されている。環状磁心4は分割体5,6を
嵌合結合させて形成されたもので、分割体5,6
は、たとえば平均粒子53μmのFe−1.5%Si合金磁
性粉と半硬化性エポキシ樹脂粉末とを体積比にし
て85:15で混合して得た混合体を金型にて
600MPaの圧力で圧縮成形して形成されている。
そして、分割体5には第3図aに示す如く両端面
7,8に軸方向に延びる溝9,10がそれぞれ設
けられており、また、分割体6にも同図bに示す
如く両端面11,12に軸方向に延びる突条1
3,14が設けられている。溝9,10は、それ
ぞれ同一形状に形成されており、その幅が全体的
に軸方向に進むにしたがつて徐々に狭くなる形状
で、かつ開口面の幅より底面の幅の方が広い形状
に形成されている。突条13,14は、上記溝
9,10に対応した形状、つまり、その幅が全体
的に軸方向に進むにしたがつて徐々に狭くなる形
状で、かつ先端の幅より基端の幅の方が狭い形状
に形成されている。 The reactor according to this embodiment includes a rod-shaped conductor 1 whose surface is covered with an insulating layer, and a plurality of annular magnetic cores 4 which are sequentially sheathed around the conductor 1 and arranged in series in the axial direction.
and terminals 3 attached to both ends of the conductor 1. The annular magnetic core 4 is formed by fitting and connecting the divided bodies 5 and 6.
For example, a mixture obtained by mixing Fe-1.5% Si alloy magnetic powder with an average particle size of 53 μm and semi-hardened epoxy resin powder at a volume ratio of 85:15 is molded.
It is formed by compression molding at a pressure of 600MPa.
The divided body 5 is provided with grooves 9 and 10 extending in the axial direction on both end surfaces 7 and 8, respectively, as shown in FIG. Projections 1 extending in the axial direction at 11 and 12
3 and 14 are provided. The grooves 9 and 10 are each formed in the same shape, the width of which gradually narrows as it advances in the axial direction, and the width of the bottom surface is wider than the width of the opening surface. is formed. The protrusions 13 and 14 have a shape corresponding to the grooves 9 and 10, that is, a shape whose overall width gradually becomes narrower as it advances in the axial direction, and whose width is smaller at the base end than at the tip end. It is formed into a narrower shape.
しかして、対をなす分割体5,6を導体1に添
設して、溝9と突条14とを、また溝10と突条
13とを第4図に示すように嵌合させ、この状態
で分割体5,6を相対的に軸方向にスライドさせ
ることによつて上記分割体5と6とを連結させて
1つの環状磁心4を組立て、以下同様の手順で所
望数の環状磁心4を導体1の外周に装着した後、
たとえば150℃、15分間の熱処理を施こし接合面
を一体化させてリアクトルを形成したものとなつ
ている。 Then, the pair of divided bodies 5 and 6 are attached to the conductor 1, and the groove 9 and the protrusion 14 are fitted together, and the groove 10 and the protrusion 13 are fitted together as shown in FIG. By sliding the divided bodies 5 and 6 relatively in the axial direction in this state, the divided bodies 5 and 6 are connected to assemble one annular magnetic core 4 , and the desired number of annular magnetic cores 4 is assembled by following the same procedure. After attaching to the outer circumference of conductor 1,
For example, a reactor is formed by applying heat treatment at 150°C for 15 minutes to integrate the joint surfaces.
このような構成であると、分割体5,6を導体
1に添設して溝と突条とを嵌合させればよいの
で、導体1への環状磁心4の取付けが極めて容易
となる。また、分割体5と6とを結合させる際
に、第4図中点線矢印方向に相対的にスライドさ
せると、分割体5に形成された溝10,9の側壁
24,25と、分割体6に形成された突条13,
14の側壁26,27とが摺動し、この結果、上
記側壁24,25および側壁26,27の軸方向
に対してなす角度によつて、上記分割体5,6
は、図中実線矢印で示すように互いに密着する方
向に移動する。したがつて分割体5,6の接合面
および分割体5,6と導体1との接合面が強力に
密接されて分割体相互が結合されることになる。 With such a configuration, the annular magnetic core 4 can be attached to the conductor 1 very easily since it is only necessary to attach the divided bodies 5 and 6 to the conductor 1 and fit the grooves and the protrusions. Furthermore, when the divided bodies 5 and 6 are joined together, if the divided bodies 5 and 6 are slid relative to each other in the direction of the dotted line arrow in FIG. The protrusion 13 formed in
As a result, the side walls 24, 25 and the side walls 26, 27 form an angle with respect to the axial direction, so that the divided bodies 5, 6
move in a direction in which they come into close contact with each other, as shown by the solid line arrows in the figure. Therefore, the joint surfaces of the divided bodies 5, 6 and the joint surfaces of the divided bodies 5, 6 and the conductor 1 are strongly brought into close contact, and the divided bodies are bonded to each other.
それに加えて、分割体5と分割体6との接合面
積が単に平面同士を衝き合わせたものより、略突
条の側壁分だけ拡大されるため、接合部での磁気
抵抗を低く抑えることができ、結局、前述した効
果が得られる。 In addition, since the joint area between the dividing body 5 and the dividing body 6 is expanded by approximately the side wall of the protrusion compared to simply abutting planes, the magnetic resistance at the joint can be kept low. As a result, the above-mentioned effects can be obtained.
また、導体1と環状磁心4との密着性を高くと
ることができるので、たとえば導体1に銅パイプ
を用い、導体内部に冷却水を流通させて冷却を行
うようにしたリアクトルでは、その冷却効率を高
めることにもつながる。 In addition, since it is possible to maintain high adhesion between the conductor 1 and the annular magnetic core 4 , for example, in a reactor in which a copper pipe is used for the conductor 1 and cooling water is circulated inside the conductor, the cooling efficiency is improved. It also leads to increasing.
また、本実施例における分割体5,6は金型に
よる成形が可能な形状となつているので、生産性
も良好である。 Further, since the divided bodies 5 and 6 in this embodiment have a shape that can be molded with a mold, productivity is also good.
なお、本実施例では一方の分割体5には溝のみ
を、また他方の分割体6には突条のみを形成した
が、たとえば第5図に示す如く分割体30の一方
の端面に溝31を形成し、他方の端面には突条3
2を形成するようにしても良い。分割体をこのよ
うな形状にすれば、金型が一種類しか必要とせ
ず、より経済的である。 In this embodiment, only grooves were formed in one of the divided bodies 5, and only protrusions were formed in the other divided body 6, but for example, as shown in FIG. is formed, and a protrusion 3 is formed on the other end surface.
2 may be formed. If the divided body has such a shape, only one type of mold is required, which is more economical.
また、環状磁心は円形状に限定されるものでは
なく、たとえば第6図に示すように角形の分割体
33から構成されるものであつてもよい。 Further, the annular magnetic core is not limited to a circular shape, but may be composed of rectangular divided bodies 33, as shown in FIG. 6, for example.
さらに、分割体の溝および突条の形状について
も、上記した形状のものに限定されるものではな
い。つまり、分割体相互の機械的結合強度が確保
でき、両分割体の軸方向のスライドに伴なうくさ
び作用が働いて両者の接合部分の密着度および導
体外周面への密着度を増加させ得る形状であれば
よい。また、環状磁心を3つ以上の分割体で構成
するようにしてもよい。さらに分割体の材質につ
いても、特に前記実施例で述べたものに限らず、
フエライト等であつても良い。圧粉磁性体を用い
る場合には、たとえば鉄粉、Fe−Si合金粉、Fe
−Ni合金粉、Fe−Si−Al合金粉、Fe−Co合金
粉、Ni粉、Fe−Al合金粉等の軟質磁性体粉末
と、ポリアミド樹脂、ポリエステル樹脂、ポリカ
ーボネート樹脂等の熱可塑性樹脂または半硬化状
態の熱硬化性樹脂とを混合させたものを用いるの
が良く、たとえば平均粒径44μmのFe−Ni合金粉
とポリアミド樹脂とを体積比にして8:2で混合
して得た混合体を、500MPaの圧力で成形するよ
うにしてもよい。このように磁性体粉末の平均粒
径が100μm以下であれば高周波特性および成形
後の表面粗度が良好なものとなり、磁性体粉末の
平均粒径が10μm以上であれば金属粉の取扱い上
なんら支障となることもない。また、圧粉磁性体
中の樹脂量が体積比で1.5%以上あれば磁心の強
度および磁性体粉末相互の絶縁性が良好となり、
本発明の効果を十分に発揮するリアクトルが得ら
れる。 Furthermore, the shapes of the grooves and protrusions of the divided body are not limited to those described above. In other words, the mechanical bonding strength between the divided bodies can be ensured, and the wedge effect that accompanies the sliding of both divided bodies in the axial direction can increase the degree of adhesion between the joints between the two bodies and the degree of closeness to the outer circumferential surface of the conductor. Any shape is fine. Alternatively, the annular magnetic core may be constructed of three or more divided bodies. Furthermore, the material of the dividing body is not limited to those specifically described in the above embodiments.
It may also be ferrite or the like. When using powder magnetic material, for example, iron powder, Fe-Si alloy powder, Fe
- Soft magnetic powders such as Ni alloy powder, Fe-Si-Al alloy powder, Fe-Co alloy powder, Ni powder, Fe-Al alloy powder, etc., and thermoplastic resins such as polyamide resin, polyester resin, polycarbonate resin, etc. It is best to use a mixture of thermosetting resin in a hardened state, such as a mixture obtained by mixing Fe-Ni alloy powder with an average particle size of 44 μm and polyamide resin at a volume ratio of 8:2. may be molded under a pressure of 500 MPa. In this way, if the average particle size of the magnetic powder is 100 μm or less, the high frequency characteristics and surface roughness after molding will be good, and if the average particle size of the magnetic powder is 10 μm or more, there will be no problems in handling the metal powder. It will not be a hindrance. In addition, if the amount of resin in the powder magnetic material is 1.5% or more by volume, the strength of the magnetic core and the mutual insulation of the magnetic powder will be good.
A reactor that fully exhibits the effects of the present invention can be obtained.
第1図は従来のリアクトルの外観を示す斜視
図、第2図は本発明の一実施例に係るリアクトル
の外観を示す斜視図、第3図a,bは同リアクト
ルの環状磁心を構成する分割体を示した斜視図、
第4図は同分割体を嵌合する途中の状態を示す斜
視図、第5図および第6図は本発明の他の実施例
に係るリアクトルを構成する分割体を示す斜視図
である。
1…導体、2,4…環状磁心、3…端子、5,
6,30,33…分割体、9,10,31,34
…溝、13,14,32,35…突条。
Fig. 1 is a perspective view showing the external appearance of a conventional reactor, Fig. 2 is a perspective view showing the external appearance of a reactor according to an embodiment of the present invention, and Fig. 3 a and b are divisions forming the annular magnetic core of the reactor. A perspective view showing the body;
FIG. 4 is a perspective view showing the divided body in the middle of being fitted, and FIGS. 5 and 6 are perspective views showing the divided body constituting a reactor according to another embodiment of the present invention. 1... Conductor, 2, 4 ... Annular magnetic core, 3... Terminal, 5,
6, 30, 33...divided body, 9, 10, 31, 34
... Groove, 13, 14, 32, 35... Projection.
Claims (1)
磁心を装着してなるリアクトルにおいて、上記環
状磁心は環状に直列接続されて閉磁路を形成する
複数の分割体からなり、これら分割体の互いに接
合される接合端面部には隣接する上記分割体の軸
方向への相対的なスライドによつて互いが嵌合さ
れて上記隣接した分割体相互を機械的に連結する
とともに上記スライドに伴ない互いの接合部分の
密着度を増加させる軸方向に対する傾斜壁面を有
した突条および溝とが形成され隣接する分割体の
継手を構成してなることを特徴とするリアクト
ル。 2 上記分割体は、軟質磁性金属粉末と、熱可塑
性または半硬化状態にある熱硬化性樹脂との混合
体を圧縮成形して得たものであることを特徴とす
る特許請求の範囲第1項記載のリアクトル。[Claims] 1. A reactor comprising one or more annular magnetic cores attached to the outer periphery of a rod-shaped conductor, wherein the annular magnetic core is composed of a plurality of divided bodies connected in series in an annular shape to form a closed magnetic path. , the joint end surfaces of these divided bodies that are joined to each other are fitted into each other by relative sliding in the axial direction of the adjacent divided bodies, mechanically connecting the adjacent divided bodies to each other, and A reactor characterized in that a joint between adjacent divided bodies is formed with protrusions and grooves having wall surfaces inclined in the axial direction to increase the degree of adhesion between the mutually joined parts as the sliding occurs. 2. Claim 1, characterized in that the divided body is obtained by compression molding a mixture of soft magnetic metal powder and thermoplastic or semi-hardened thermosetting resin. Reactor listed.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58124411A JPS6016404A (en) | 1983-07-08 | 1983-07-08 | Reactor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58124411A JPS6016404A (en) | 1983-07-08 | 1983-07-08 | Reactor |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6016404A JPS6016404A (en) | 1985-01-28 |
| JPH0584046B2 true JPH0584046B2 (en) | 1993-11-30 |
Family
ID=14884801
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP58124411A Granted JPS6016404A (en) | 1983-07-08 | 1983-07-08 | Reactor |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6016404A (en) |
Families Citing this family (7)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0831383B2 (en) * | 1985-03-28 | 1996-03-27 | 株式会社東芝 | Large current reactor |
| JPH0234875Y2 (en) | 1986-08-29 | 1990-09-19 | ||
| JPH0760956B2 (en) * | 1987-02-19 | 1995-06-28 | 北川工業株式会社 | Noise absorber |
| JPH0614449Y2 (en) * | 1987-07-13 | 1994-04-13 | 北川工業株式会社 | Noise current absorber |
| DE8807359U1 (en) * | 1988-06-06 | 1989-10-12 | Siemens AG, 1000 Berlin und 8000 München | X-ray tubes |
| JP2004349617A (en) * | 2003-05-26 | 2004-12-09 | System Giken:Kk | Dust core for reactor |
| JP6811700B2 (en) * | 2017-11-29 | 2021-01-13 | 三菱電機株式会社 | Magnetic field adjustment current transformer |
-
1983
- 1983-07-08 JP JP58124411A patent/JPS6016404A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS6016404A (en) | 1985-01-28 |
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