JPH0199204A - Magnetic core - Google Patents
Magnetic coreInfo
- Publication number
- JPH0199204A JPH0199204A JP25617287A JP25617287A JPH0199204A JP H0199204 A JPH0199204 A JP H0199204A JP 25617287 A JP25617287 A JP 25617287A JP 25617287 A JP25617287 A JP 25617287A JP H0199204 A JPH0199204 A JP H0199204A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic core
- magnetic
- members
- winding
- section
- 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
- 238000004804 winding Methods 0.000 claims abstract description 30
- 239000000696 magnetic material Substances 0.000 claims abstract description 6
- 239000000463 material Substances 0.000 claims abstract description 4
- 230000004907 flux Effects 0.000 abstract description 8
- 238000009826 distribution Methods 0.000 abstract description 6
- 239000002075 main ingredient Substances 0.000 abstract 1
- 239000011162 core material Substances 0.000 description 45
- 229910000976 Electrical steel Inorganic materials 0.000 description 6
- 238000004519 manufacturing process Methods 0.000 description 3
- 239000004696 Poly ether ether ketone Substances 0.000 description 2
- 230000020169 heat generation Effects 0.000 description 2
- 230000035699 permeability Effects 0.000 description 2
- 229920002530 polyetherether ketone Polymers 0.000 description 2
- 229910045601 alloy Inorganic materials 0.000 description 1
- 239000000956 alloy Substances 0.000 description 1
- 230000003321 amplification Effects 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 239000003822 epoxy resin Substances 0.000 description 1
- 238000003780 insertion Methods 0.000 description 1
- 230000037431 insertion Effects 0.000 description 1
- 238000010030 laminating Methods 0.000 description 1
- 239000006247 magnetic powder Substances 0.000 description 1
- 230000005415 magnetization Effects 0.000 description 1
- 238000012986 modification Methods 0.000 description 1
- 230000004048 modification Effects 0.000 description 1
- 238000003199 nucleic acid amplification method Methods 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
- 238000010791 quenching Methods 0.000 description 1
- 230000000171 quenching effect Effects 0.000 description 1
- 229920005989 resin Polymers 0.000 description 1
- 239000011347 resin Substances 0.000 description 1
- 238000005245 sintering Methods 0.000 description 1
- 230000009466 transformation Effects 0.000 description 1
Landscapes
- Soft Magnetic Materials (AREA)
Abstract
Description
【発明の詳細な説明】
[発明の目的]
(産業上の利用分野)
本発明は、高周波高電圧の変成に用いられる高周波変圧
器や、高周波のパルス発生に用いられるマグアンプ等の
パルス電圧発生器におけるチョーク等の磁路を形成する
ための磁心に関する。[Detailed Description of the Invention] [Object of the Invention] (Industrial Application Field) The present invention relates to a high-frequency transformer used for high-frequency high-voltage transformation, and a pulse voltage generator such as a mag-amp used for high-frequency pulse generation. The present invention relates to a magnetic core for forming a magnetic path in a choke or the like.
(従来の技術)
従来、変圧器等の磁心としは、硅素鋼板製のものが主に
用いられている。また、最近では、Fe。(Prior Art) Conventionally, magnetic cores of transformers and the like have mainly been made of silicon steel plates. Also, recently, Fe.
Si、 3. Co等からなる合金の急冷組織である非
晶質(アモルファス)テープ(リボン)を積層して磁心
を構成することも行われている。Si, 3. A magnetic core is also constructed by laminating amorphous tapes (ribbons), which are rapidly solidified alloys made of Co or the like.
非晶質テープを用いた磁心は、高透磁率を有し、低電流
損、無方向性磁化特性である等の特質から、高周波特性
が良好で、低発熱性、すなわち、低電力損、低ノイズ信
号増幅性という電気的にも優れた特性を発揮する。Magnetic cores using amorphous tape have high magnetic permeability, low current loss, and non-directional magnetization characteristics, so they have good high frequency characteristics and low heat generation, that is, low power loss and low It also exhibits excellent electrical characteristics such as noise signal amplification.
ざらに、近年非晶質材料を用いて線状の磁心材料を形成
することも容易になりつつある。In recent years, it has become easier to form linear magnetic core materials using amorphous materials.
しかしながら、テープ状の非晶質軟磁性体を積層した磁
心の場合、この磁心の断面は必然的に角型となり、一方
、この磁心に巻回するコイルの巻回状態は本質的に円形
となるため、このような磁心及びコイルにより変圧器や
チョークコイルを形成した場合、磁心とコイルとの間に
磁束空隙が生じ易いという問題がある。However, in the case of a magnetic core made of laminated tape-shaped amorphous soft magnetic material, the cross section of this magnetic core is inevitably square, whereas the winding state of the coil wound around this magnetic core is essentially circular. Therefore, when a transformer or a choke coil is formed using such a magnetic core and coil, there is a problem in that a magnetic flux gap is likely to occur between the magnetic core and the coil.
また、磁心の断面が角型である限り、コイルをいかに円
形に近く巻回しても磁心における磁束分布は、その中央
部、周辺部において一様とはならず、この不均一な磁束
分布のため高周波特性を阻害するという問題点がおる。In addition, as long as the cross section of the magnetic core is square, no matter how close to a circle the coil is wound, the magnetic flux distribution in the magnetic core will not be uniform in the center and periphery, and due to this non-uniform magnetic flux distribution. There is a problem that high frequency characteristics are inhibited.
一方、小型、小電力用の磁心の場合、非晶質テープの巻
始め、巻終り部分をテーバ状にしておき、完成した磁心
の断面が円形を呈するようにすることも可能で、このよ
うな形状の磁心を用いた小型変圧器、小型チョークコイ
ルも実用化されている。On the other hand, in the case of small-sized, low-power magnetic cores, it is also possible to make the amorphous tape tapered at the beginning and end of the winding so that the cross section of the completed magnetic core has a circular shape. Small transformers and small choke coils using shaped magnetic cores have also been put into practical use.
しかし、大型、大電力用の磁心に上述した構成を適用し
た場合、非晶質テープの廃棄部分が多くなり、経済性の
点で問題がある。However, when the above-described configuration is applied to a large-sized, high-power magnetic core, a large amount of the amorphous tape is discarded, which poses an economical problem.
ざらに、非晶質磁性体の粉末の焼結により、断面が円形
の磁心を形成することも可能であるが、この場合には、
透磁率が著しく低下し磁束損失や発熱等が多大でおる等
磁気的電気的特性の点で実用向きではない。It is also possible to form a magnetic core with a circular cross section by sintering amorphous magnetic powder, but in this case,
It is not suitable for practical use due to its magnetic and electrical characteristics, such as a marked decrease in magnetic permeability and large amounts of magnetic flux loss and heat generation.
また、硅素鋼板について言及すると、磁気的に優秀な軟
磁性体でおる硅素鋼は、Siを多くすればするほど機械
的特性が劣化し、展性が悪く延性が殆どないため割れや
すい。したがって、このような硅素鋼は、厚さ50μm
程度の板状のものが最善であり、線状にすることは不可
能で、必然的に線状の硅素鋼製の磁心を製造することは
できなかった。Also, referring to silicon steel sheets, silicon steel is a soft magnetic material with excellent magnetic properties, but the more Si it contains, the worse its mechanical properties are, and its malleability is poor and it has almost no ductility, so it is easily broken. Therefore, such silicon steel has a thickness of 50 μm.
It is best to have a plate-like core, and it is impossible to make it into a wire, so it was inevitably impossible to manufacture a wire-like silicon steel magnetic core.
(発明が解決しようとする問題点)
上述したように非晶質テープを用いた磁心の場合、電磁
気的特性、経済性の点で不十分であり、また、硅素鋼製
の磁心の場合、機械的特性の点で満足し得るものを得ら
れないという問題がある。(Problems to be Solved by the Invention) As mentioned above, magnetic cores using amorphous tape are insufficient in terms of electromagnetic properties and economical efficiency, and magnetic cores made of silicon steel are mechanically unstable. There is a problem in that it is not possible to obtain satisfactory physical characteristics.
そこで、本発明は、電磁気的特性及び機械的特性の双方
が優れた磁心を提供することを目的とするものである。Therefore, an object of the present invention is to provide a magnetic core that is excellent in both electromagnetic properties and mechanical properties.
[発明の構成]
(問題点を解決するための手段)
本発明の磁心は、線状部材を集合して形成した断面が半
円形状の磁心部材を組合せて断面円形状の巻線巻回部を
形成したものである。[Structure of the Invention] (Means for Solving the Problems) The magnetic core of the present invention has a winding portion having a circular cross section by combining magnetic core members each having a semicircular cross section formed by collecting linear members. was formed.
(作 用)
上記構成の磁心は、線状部材を集合して形成した断面半
円形状の磁心部材の組合せにより、巻線巻回部の断面形
状を円形としたものであるから、この巻線巻回部に巻線
を巻回し通電することにより誘起される磁束の分布が均
一となり電磁気特性が良好となる。(Function) In the magnetic core having the above configuration, the cross-sectional shape of the winding portion is circular due to the combination of magnetic core members having a semicircular cross section formed by collecting wire members. By winding the winding around the winding portion and energizing it, the distribution of magnetic flux induced becomes uniform, resulting in good electromagnetic characteristics.
また、巻線巻回部が線状部材の集合であるため、機械的
特性も良好となる。Furthermore, since the wire winding portion is a collection of linear members, the mechanical properties are also good.
(実施例)
以下に本発明の詳細な説明する。第1図及び第2図に示
す磁心1は、断面が半円形状で、かつ全体形状が長円形
状の2個の非晶質線材製の磁心部材2A、2Bを有して
いる。そして、両磁心部材2A、2Bの直線状部分を接
合し、これにより断面が円形となった部分を巻線巻回部
3として用いるようになっている。(Example) The present invention will be described in detail below. The magnetic core 1 shown in FIGS. 1 and 2 has two magnetic core members 2A and 2B made of amorphous wire, each having a semicircular cross section and an elliptical overall shape. Then, the straight portions of both magnetic core members 2A and 2B are joined, and the portion having a circular cross section is used as the winding portion 3.
このような磁心1の製造例を、第3図乃至第6図をも参
照して説明する。An example of manufacturing such a magnetic core 1 will be described with reference to FIGS. 3 to 6.
まず、第3図(a)、(b)に示すような半円状の巻線
領域5を外周に沿って形成した巻枠4を用意する。この
巻枠4は第3図(a)において上下対称形状の上部枠4
Aと下部枠4Bとを突き合せることにより構成している
。First, a winding frame 4 having a semicircular winding region 5 formed along its outer periphery as shown in FIGS. 3(a) and 3(b) is prepared. This winding frame 4 is an upper frame 4 having a vertically symmetrical shape in FIG. 3(a).
It is constructed by butting A and the lower frame 4B.
次に第4図(a)に示すように巻枠4の巻線領域5に、
線径10乃至200μmの非晶質軟磁性体製の線材6を
巻回し、第4図(b)に示すように半円状の巻線領域5
の全域を線材6で巻き尽す。Next, as shown in FIG. 4(a), in the winding area 5 of the winding frame 4,
A wire rod 6 made of an amorphous soft magnetic material with a wire diameter of 10 to 200 μm is wound, and a semicircular winding area 5 is formed as shown in FIG. 4(b).
Wrap the entire area with the wire rod 6.
この線材6は、近年の技術進歩により、非晶質軟磁性体
の急冷加工により製造することが可能となり、その強度
が大きく、抗張力も大きいことが知られているものであ
る。Due to recent technological advances, this wire rod 6 can be manufactured by quenching an amorphous soft magnetic material, and is known to have high strength and high tensile strength.
次に、第4図(b)の状態で巻線領域5内の線材6に対
しエポキシ樹脂、ポリエステル樹脂、ポリエーテルエー
テルケトン(PEEK)樹脂等を含浸させ巻回状態の線
材6を固定化した後、前記2個の上部枠4A、下部枠4
Bを分割状態で除去すれば第5図及び第6図に示す磁心
部材2Aを得ることができる。Next, in the state shown in FIG. 4(b), the wire rod 6 in the winding area 5 was impregnated with epoxy resin, polyester resin, polyether ether ketone (PEEK) resin, etc., and the wire rod 6 in the wound state was fixed. After that, the two upper frames 4A and the lower frame 4
If B is removed in a divided state, a magnetic core member 2A shown in FIGS. 5 and 6 can be obtained.
そして、この磁心部材2Aと、上述した製造工程で全く
同様に製造した別の磁心部材2Bとを、両者の直線状部
分を接合するようにして突き合せれば、第1図及び第2
図に示すように断面が円形の巻線巻回部3を有する磁心
1を得ることができる。Then, if this magnetic core member 2A and another magnetic core member 2B manufactured in exactly the same manner in the above-mentioned manufacturing process are butted together so that their linear portions are joined, the results shown in FIGS.
As shown in the figure, a magnetic core 1 having a wire winding portion 3 having a circular cross section can be obtained.
そして、この磁心1の巻線巻回部3に対して第7図に示
すようコイル用巻線7A、7Bを施すことにより、高周
波用のトランスTとして用いることができる。By applying coil windings 7A and 7B to the winding portion 3 of this magnetic core 1 as shown in FIG. 7, it can be used as a high frequency transformer T.
このトランスTによれば、例えば一方のコイル用巻線7
Aに高周波電流を流すことにより生じる断面円形の記線
巻回部3の磁束分布が均一となり、これにより高周波は
特性が良好となる。According to this transformer T, for example, one coil winding 7
When a high frequency current is passed through A, the magnetic flux distribution of the line-marked winding portion 3 having a circular cross section becomes uniform, thereby providing good high frequency characteristics.
また、磁心1自体も強度が大きく抗張力も大きい線材6
を用いていることからその機械的特性も良好となる。In addition, the magnetic core 1 itself has a wire rod 6 with high strength and high tensile strength.
Since it is used, its mechanical properties are also good.
本発明は上述した実施例に限定されるものではなく、そ
の要旨の範囲内で種々の変形が可能である。The present invention is not limited to the embodiments described above, and various modifications can be made within the scope of the invention.
例えば上述した磁心1の代りに、この磁心を上下対称形
状に2分割しコイル用巻線を挿入し易くしたものを用い
ることもできる。For example, instead of the magnetic core 1 described above, it is also possible to use a magnetic core in which the magnetic core is divided into two vertically symmetrical shapes to facilitate insertion of coil windings.
[発明の効果]
以上詳述した本発明によれば、電磁気的及び機械的特性
に優れた磁心を提供することができる。[Effects of the Invention] According to the present invention described in detail above, a magnetic core with excellent electromagnetic and mechanical properties can be provided.
第1図は本発明の実施例を示す平面図、第2図は同上の
I−I線断面図、第3図(a)は巻枠の平面図、第3図
(b)は同上の■−■線断面図、第4図(a>は巻枠に
線材を巻回する状態を示す平面図、第4図(b)は巻枠
に線材を巻回し終った状態を示す断面図、第5図は磁心
部材の平面図、第6図は第5図の■−■線断面図、第7
図は本実施例の磁心によりトランスを構成した状態を示
す平面図である。
1・・・磁心、2A、2B・・・磁心部材、3・・・巻
線巻回部。
代理人 弁理士 則 近 憲 缶周
近 藤 猛CG)
第3図Fig. 1 is a plan view showing an embodiment of the present invention, Fig. 2 is a sectional view taken along the line I-I of the same, Fig. 3 (a) is a plan view of the winding frame, and Fig. 3 (b) is a plan view of the same -■ Line sectional view, Figure 4 (a> is a plan view showing the state in which the wire rod is wound around the winding frame, Figure 4 (b) is a cross-sectional view showing the state in which the wire rod is wound around the winding frame, Figure 5 is a plan view of the magnetic core member, Figure 6 is a cross-sectional view taken along the line ■-■ in Figure 5, and Figure 7 is a plan view of the magnetic core member.
The figure is a plan view showing a state in which a transformer is constructed using the magnetic core of this embodiment. DESCRIPTION OF SYMBOLS 1... Magnetic core, 2A, 2B... Magnetic core member, 3... Winding winding part. Agent Patent Attorney Nori Chika Ken Shu
Takeshi Kondo CG) Figure 3
Claims (2)
磁心部材を組合せて形成した断面円形状の巻線巻回部を
有することを特徴とする磁心。(1) A magnetic core characterized by having a wire winding portion having a circular cross section formed by combining magnetic core members in which linear members are assembled so as to have a semicircular cross section.
分とする軟磁性体の急冷組織である非結晶線材により形
成されるものである特許請求の範囲第1項記載の磁心。(2) The magnetic core according to claim 1, wherein the magnetic core member is formed of an amorphous wire material which is a quenched structure of a soft magnetic material mainly composed of Fe, Si, B, Co, etc.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP25617287A JPH0199204A (en) | 1987-10-13 | 1987-10-13 | Magnetic core |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP25617287A JPH0199204A (en) | 1987-10-13 | 1987-10-13 | Magnetic core |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH0199204A true JPH0199204A (en) | 1989-04-18 |
Family
ID=17288910
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP25617287A Pending JPH0199204A (en) | 1987-10-13 | 1987-10-13 | Magnetic core |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH0199204A (en) |
-
1987
- 1987-10-13 JP JP25617287A patent/JPH0199204A/en active Pending
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