JPS6015908A - Magnetic core - Google Patents
Magnetic coreInfo
- Publication number
- JPS6015908A JPS6015908A JP12274483A JP12274483A JPS6015908A JP S6015908 A JPS6015908 A JP S6015908A JP 12274483 A JP12274483 A JP 12274483A JP 12274483 A JP12274483 A JP 12274483A JP S6015908 A JPS6015908 A JP S6015908A
- Authority
- JP
- Japan
- Prior art keywords
- core
- magnetic
- soft magnetic
- magnetic core
- shaped
- 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
- H01F27/255—Magnetic cores made from particles
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F38/00—Adaptations of transformers or inductances for specific applications or functions
- H01F38/02—Adaptations of transformers or inductances for specific applications or functions for non-linear operation
- H01F38/023—Adaptations of transformers or inductances for specific applications or functions for non-linear operation of inductances
Landscapes
- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Physics & Mathematics (AREA)
- Nonlinear Science (AREA)
- Coils Or Transformers For Communication (AREA)
Abstract
Description
【発明の詳細な説明】 本発明はET型磁心の改良に関するものである。[Detailed description of the invention] The present invention relates to improvements in ET type magnetic cores.
従来チョークコイル用磁心や高周波1〜ランス用磁心と
しては主に、フエライ1〜等のElコアやEEココア用
いられていた。Conventionally, as magnetic cores for choke coils and magnetic cores for high frequency lances, El cores such as Ferrai 1 and EE cocoa have been mainly used.
しかながら、これらの磁心はコアが飽和に近づくまでは
透磁率がほぼ一定の線形特性を示づ゛ため、スイッチン
グ電源の平滑用チョークとしては十分な特性ではなかっ
た。すなわち、この様な通常の線形特性の磁心ではチョ
ーク用磁心として用いた場合、低電流でもインダクタン
スが大きくならず、負荷電流が小さい場合に出力電圧が
上昇してしまい問題どなる。このため通常は出力電圧の
変動をJ5ざえる回路を作りこの問題を解決していた。However, these magnetic cores exhibit linear characteristics in which magnetic permeability is approximately constant until the core approaches saturation, and therefore, these cores do not have sufficient characteristics as smoothing chokes for switching power supplies. That is, when a magnetic core with such normal linear characteristics is used as a choke core, the inductance does not increase even at low currents, and the output voltage increases when the load current is small, causing problems. For this reason, this problem is usually solved by creating a circuit that reduces output voltage fluctuations.
従って部品の増加によ−るコストの上昇1部品の増加に
よる電源の大型化などの問題、効率の低下などの点で好
ましいとはいえなかった。Therefore, it is not desirable in terms of problems such as an increase in cost due to the increase in the number of parts, an increase in the size of the power supply due to the increase in the number of parts, and a decrease in efficiency.
このような目的にはコイルに流れる電流が小ざい場合に
インダクタンスが大きく、ある電流以上から磁心が飽和
する電流まではインダクタンスがほぼ一定C直流重E特
性の良い磁心が必要である。For this purpose, a magnetic core with good DC, heavy, and E characteristics is required, which has a large inductance when the current flowing through the coil is small, and whose inductance is approximately constant from a certain current level up to a current at which the magnetic core is saturated.
これを解決するため、ElコアやEEココアは接合面に
段差をつりギレップを形成した磁心の提案がなされCい
る。In order to solve this problem, proposals have been made for magnetic cores such as El cores and EE cocoas that have a step formed on the joint surface to form a gill.
しかしながらこれを行なうためには、接合面の一部を精
度良くけする必要があり、工数が犬となり技術的にも1
η難な面がある。またフェライトなどの]アでは飽和磁
束密度が低く低電流側で十分な直rAL重畳特性が得ら
れない。However, in order to do this, it is necessary to sharpen a part of the joint surface with high precision, which requires a lot of man-hours and is technically 1
There are some difficult aspects. Furthermore, materials such as ferrite have a low saturation magnetic flux density, and sufficient direct rAL superimposition characteristics cannot be obtained on the low current side.
このため、巻線の増加、コアの大型化などの問題がある
。Therefore, there are problems such as an increase in the number of windings and an increase in the size of the core.
本発明は上記従来技術の欠点を改良し、直流重畳特性に
優れた非線形のインダクタンス特性を示す磁心を提供す
ることを目的とする。SUMMARY OF THE INVENTION An object of the present invention is to improve the drawbacks of the prior art described above and provide a magnetic core that exhibits nonlinear inductance characteristics with excellent DC superimposition characteristics.
本発明の要点は、E型コア等の中央脚とその両側の脚の
間に板状の軟磁性体を配置し、その上にI型コアを配置
したことにある。The gist of the present invention is that a plate-shaped soft magnetic material is arranged between a central leg such as an E-shaped core and the legs on both sides thereof, and an I-shaped core is arranged thereon.
軟磁性体どして、強磁性薄帯を用いると低磁場の透vJ
1率の周波数依存性を小さくできるため好ましい。更に
ア上ルファス薄帯を使用した場合は打ち扱きホトエッチ
ラミネ−1・後切断する等により容易に成形でさ、高周
波特性も優れフエライ1〜等より飽和磁束密度が高いた
め、直流重畳特性を改善できより好ましい結果を得るこ
とができる。When a ferromagnetic ribbon is used as a soft magnetic material, the transmission vJ of low magnetic field is
This is preferable because the frequency dependence of the 1 rate can be reduced. Furthermore, when Arufus thin strip is used, it can be easily formed by photo-etch lamination 1 and then cutting, and it also has excellent high frequency characteristics and has a higher saturation magnetic flux density than Ferrai 1~ etc., so it has excellent DC superimposition characteristics. can be improved and more favorable results can be obtained.
また、脚の部分に配置する軟磁性体とI型コアの間に非
磁性のスペーサーを配置することにより直流重畳特性を
任意に変えることが可能である。Further, by arranging a non-magnetic spacer between the soft magnetic material arranged in the leg portion and the I-shaped core, it is possible to arbitrarily change the DC superposition characteristic.
脚の部分に配置する軟磁性体は全部の脚でなく、2つの
脚近傍に配置しただけでも良い。The soft magnetic material placed in the leg portions may not be placed on all the legs, but may be placed only near two legs.
更に、非線形である直流重畳特性はI型コアに晶を入れ
たり、脚に配置する軟磁性体の幅をE型。Furthermore, the DC superimposition characteristic, which is non-linear, is achieved by adding a crystal to the I-shaped core and changing the width of the soft magnetic material placed in the legs to an E-shaped core.
I型コアの幅より小さくすることによ・〕ても任意に変
えられる。It can also be changed arbitrarily by making it smaller than the width of the I-type core.
強磁↑4薄帯の代わりにスパッタリングや蒸着等の方法
で軟磁性膜を形成し、同一の構造としたものも同じ効果
が得られ本発明の範囲に含まれるのは明らかである。E
型コア、(型コアの形状と類似のものを用いた場合も本
発明の範囲に含まれるのは明らかである。It is clear that the same effect can be obtained by forming a soft magnetic film by a method such as sputtering or vapor deposition in place of the ferromagnetic ↑4 thin ribbon, and the same effect is obtained and it is within the scope of the present invention. E
It is clear that the scope of the present invention also includes the use of a mold core (similar in shape to the mold core).
本発明による磁心は特にスイッチング電源の出力型iA
コ平滑用チョークに用いた場合その効果が著しい。The magnetic core according to the invention is particularly suitable for output type iA switching power supplies.
The effect is remarkable when used in smoothing chalk.
以下、本発明を実施例に従って31明する。Hereinafter, the present invention will be explained based on 31 examples.
実施例1
第1図ぼ本発明の磁心の実施例の一部を示した口である
。図に示すように本発明による磁心は、)Jライト等か
らなるE型磁心1と)型磁心2お、j、び板状の軟磁性
体3から溝底されている。Embodiment 1 FIG. 1 shows a portion of an embodiment of the magnetic core of the present invention. As shown in the figure, the magnetic core according to the present invention includes an E-type magnetic core 1 made of J-light or the like, an )-type magnetic core 2, and a plate-shaped soft magnetic body 3.
(21)は軟磁性1ホ3と「型磁心1,1型磁心2を直
接重ね合せた場合であり、磁気特性の違いからヂョーク
コイル等に用いた場合、低電流時のインダクタンスが上
昇し非線形特性となる。(21) is a case where the soft magnetic 1-hole 3 and the ``type magnetic core 1 and 1-type magnetic core 2 are directly superimposed, and due to the difference in magnetic properties, when used in a jog coil, etc., the inductance at low current increases and the nonlinear characteristics becomes.
(1))は2つに分割した軟磁性体3aを配置した場合
であり、(a )と同様、非線形特性が得られ分割した
軟磁性体どうしの間隔を変えることにより、直流重畳特
性を任意に変えることができる。(1)) is a case where a soft magnetic body 3a divided into two is arranged, and as in (a), nonlinear characteristics are obtained, and by changing the interval between the divided soft magnetic bodies, the DC superposition characteristic can be adjusted arbitrarily. can be changed to
(C)は軟磁性体とI型磁心の間に非磁性のスペーサー
を入れた場合であり、やはり非線形特性が得られる。ス
ペーサーの厚みにより直流重畳特性を任意に変えること
が可能となる。(d )は幅が■型磁心、E型磁心の幅
より小さい軟磁性体3bを配置した揚台であり、幅を変
えることにより直流重畳特性を変えることができる。(
e )は1つの脚に非磁性のスペーサー4a、中央脚と
反ヌ4側の間に軟磁1ff一体3Gを配置した場合、<
f)はI型磁心に溝5を入れた場合、(g)はE型磁心
の脚の間のI型磁心の下側に軟磁性1ホ3dを配置した
場合、(h)は2つ以上に分割したI型コア2aを配置
し1ζ場合であり、どの構造も非線形1°j性を示す。(C) is a case in which a nonmagnetic spacer is inserted between the soft magnetic material and the I-type magnetic core, and nonlinear characteristics can also be obtained. The DC superposition characteristics can be changed arbitrarily by changing the thickness of the spacer. (d) is a platform on which a soft magnetic material 3b whose width is smaller than the width of the ■-shaped magnetic core and the E-shaped magnetic core is arranged, and by changing the width, the DC superposition characteristics can be changed. (
e) When a non-magnetic spacer 4a is placed on one leg and a soft magnetic 1ff integral 3G is placed between the center leg and the opposite side 4, <
f) is when the groove 5 is placed in the I-type magnetic core, (g) is when the soft magnetic 1-hole 3d is placed below the I-type magnetic core between the legs of the E-type magnetic core, and (h) is when two or more This is the case where an I-shaped core 2a divided into 1ζ is arranged, and all structures exhibit nonlinear 1°j property.
実施例2
第2図は本発明の磁心の直流重畳特性の1例を示した図
である。比較のため軟磁性2体を配置しない場合の直流
重畳特性も示す。Embodiment 2 FIG. 2 is a diagram showing an example of the DC superposition characteristics of the magnetic core of the present invention. For comparison, the DC superposition characteristics when two soft magnetic bodies are not arranged are also shown.
図から明らかなようにコイルに流れる電流が小さい場合
のインダクタンスが上昇しており、スイッチング電源の
平滑用チョークの磁心として17ら優れているのがわか
る。As is clear from the figure, the inductance increases when the current flowing through the coil is small, and it can be seen that No. 17 is superior as a magnetic core for a smoothing choke in a switching power supply.
本発明により、低電流時のインダクタンスが改善され、
かつ従来のコアより直流重畳特性が優れており作製も容
易なためその効果は著しい。According to the present invention, inductance at low current is improved,
Moreover, the DC superimposition characteristics are superior to conventional cores, and the fabrication is easy, so the effect is remarkable.
1図は本発明の磁心の実施例の一部を示した図、第2図
は本発明の直流重畳特性の1例を示した図である。
第 1 図
第2 回
IDc (A)FIG. 1 is a diagram showing a part of an embodiment of the magnetic core of the present invention, and FIG. 2 is a diagram showing an example of the DC superposition characteristic of the present invention. Figure 1 2nd IDc (A)
Claims (1)
磁性体を配置し、イの上にI型コアを配置したことを特
徴とする磁心。 2、E型コア等の脚の部分に配置づる板状の軟磁性体に
強磁性薄帯を積層したものあるいは一枚単独で用いたこ
とを特徴とする特許請求の範囲第1項記載の磁心。 3、強磁性薄帯どしてアモルファス薄帯を用いたことを
特徴とする特許請求の範囲第2項記載の磁心。 4、脚の部分に配置する軟磁性1ホとI型コアの間に非
磁性のスペーサーを配置したことを特徴とする特WF請
求の範囲第1項、第2項ならびに第3項記載の磁心。 5.1型コアの中央に溝を入れたことを特徴とする14
訂請求の範囲第1項、第2項、第3項ならびに第4項記
載の磁心。 6、軟磁性体の幅をE型、I型コアの幅より小さくした
ことを特徴とする特許請求の範囲第1項。 第2項、第3項、ならびに第4項記載の磁心。 7、■型コアを切断し配置したことを特徴とする特許請
求の範囲第1項、第2項、第3項、第4項ならびに第6
項記載の磁心。 8、スイッチング電源の出力電流事情用チョークに用い
たことを特徴とする特許請求の範囲第1項。 第2項、第3項、第4項、第5項、第6項ならびに第7
項記載の磁心。[Claims] 1. A magnetic core characterized in that a plate-shaped soft magnetic material is arranged between a central leg of an E-shaped core and the legs on both sides thereof, and an I-shaped core is arranged above A. 2. A magnetic core according to claim 1, characterized in that a ferromagnetic ribbon is laminated on a plate-shaped soft magnetic material arranged in the leg portion of an E-shaped core or the like, or a single ferromagnetic ribbon is used alone. . 3. The magnetic core according to claim 2, characterized in that an amorphous ribbon is used as the ferromagnetic ribbon. 4. The magnetic core according to claim 1, 2, and 3, characterized in that a non-magnetic spacer is arranged between the soft magnetic 1-hole and the I-shaped core arranged in the leg part. . 14 characterized by having a groove in the center of the 5.1 type core.
A magnetic core according to claims 1, 2, 3, and 4. 6. Claim 1, characterized in that the width of the soft magnetic material is smaller than the width of the E-type and I-type cores. The magnetic core according to Items 2, 3, and 4. 7. Claims 1, 2, 3, 4, and 6 characterized in that the ■-shaped core is cut and arranged.
Magnetic core described in section. 8. Claim 1, characterized in that it is used as a choke for output current conditions of a switching power supply. Sections 2, 3, 4, 5, 6 and 7
Magnetic core described in section.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP12274483A JPS6015908A (en) | 1983-07-06 | 1983-07-06 | Magnetic core |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP12274483A JPS6015908A (en) | 1983-07-06 | 1983-07-06 | Magnetic core |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS6015908A true JPS6015908A (en) | 1985-01-26 |
Family
ID=14843521
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP12274483A Pending JPS6015908A (en) | 1983-07-06 | 1983-07-06 | Magnetic core |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS6015908A (en) |
Cited By (18)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH01130517U (en) * | 1988-02-29 | 1989-09-05 | ||
WO1994007300A1 (en) * | 1992-09-24 | 1994-03-31 | Kabushiki Kaisha Toshiba | Snubber circuit, switching power-supply, and saturable inductor used for them |
US5748013A (en) * | 1995-10-24 | 1998-05-05 | Thomson-Csf | Combined magnetic core |
WO2009114873A1 (en) * | 2008-03-14 | 2009-09-17 | Volterra Semiconductor Corporation | Voltage converter inductor having a nonlinear inductance value |
US7746209B1 (en) | 2002-12-13 | 2010-06-29 | Volterra Semiconductor Corporation | Method for making magnetic components with N-phase coupling, and related inductor structures |
US7893806B1 (en) | 2002-12-13 | 2011-02-22 | Volterra Semiconductor Corporation | Method for making magnetic components with N-phase coupling, and related inductor structures |
US7898379B1 (en) | 2002-12-13 | 2011-03-01 | Volterra Semiconductor Corporation | Method for making magnetic components with N-phase coupling, and related inductor structures |
US7965165B2 (en) | 2002-12-13 | 2011-06-21 | Volterra Semiconductor Corporation | Method for making magnetic components with M-phase coupling, and related inductor structures |
US7994888B2 (en) | 2009-12-21 | 2011-08-09 | Volterra Semiconductor Corporation | Multi-turn inductors |
US8102233B2 (en) | 2009-08-10 | 2012-01-24 | Volterra Semiconductor Corporation | Coupled inductor with improved leakage inductance control |
JP2012054549A (en) * | 2010-08-31 | 2012-03-15 | Samsung Electro-Mechanics Co Ltd | Transformer with integrated inductor |
US8174348B2 (en) | 2009-12-21 | 2012-05-08 | Volterra Semiconductor Corporation | Two-phase coupled inductors which promote improved printed circuit board layout |
US8237530B2 (en) | 2009-08-10 | 2012-08-07 | Volterra Semiconductor Corporation | Coupled inductor with improved leakage inductance control |
US8299885B2 (en) | 2002-12-13 | 2012-10-30 | Volterra Semiconductor Corporation | Method for making magnetic components with M-phase coupling, and related inductor structures |
US8330567B2 (en) | 2010-01-14 | 2012-12-11 | Volterra Semiconductor Corporation | Asymmetrical coupled inductors and associated methods |
CN102820125A (en) * | 2011-06-06 | 2012-12-12 | 株式会社丰田自动织机 | Magnetic core |
CN102930957A (en) * | 2012-09-27 | 2013-02-13 | 江苏锴博材料科技有限公司 | Variable-inductance inductive iron core |
CN104810137A (en) * | 2014-01-28 | 2015-07-29 | Tdk株式会社 | Reactor |
-
1983
- 1983-07-06 JP JP12274483A patent/JPS6015908A/en active Pending
Cited By (28)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH01130517U (en) * | 1988-02-29 | 1989-09-05 | ||
WO1994007300A1 (en) * | 1992-09-24 | 1994-03-31 | Kabushiki Kaisha Toshiba | Snubber circuit, switching power-supply, and saturable inductor used for them |
US5745353A (en) * | 1992-09-24 | 1998-04-28 | Kabushiki Kaisha Toshiba | Snubber circuit that suppresses surge and rush current flowing to a switching element of a self excitation-type flyback power supply |
US5748013A (en) * | 1995-10-24 | 1998-05-05 | Thomson-Csf | Combined magnetic core |
US8350658B1 (en) | 2002-12-13 | 2013-01-08 | Volterra Semiconductor Corporation | Method for making magnetic components with N-phase coupling, and related inductor structures |
US7772955B1 (en) | 2002-12-13 | 2010-08-10 | Volterra Semiconductor Corporation | Method for making magnetic components with N-phase coupling, and related inductor structures |
US7864016B1 (en) | 2002-12-13 | 2011-01-04 | Volterra Semiconductor Corporation | Method for making magnetic components with N-phase coupling, and related inductor structures |
US7893806B1 (en) | 2002-12-13 | 2011-02-22 | Volterra Semiconductor Corporation | Method for making magnetic components with N-phase coupling, and related inductor structures |
US7898379B1 (en) | 2002-12-13 | 2011-03-01 | Volterra Semiconductor Corporation | Method for making magnetic components with N-phase coupling, and related inductor structures |
US7965165B2 (en) | 2002-12-13 | 2011-06-21 | Volterra Semiconductor Corporation | Method for making magnetic components with M-phase coupling, and related inductor structures |
US8299885B2 (en) | 2002-12-13 | 2012-10-30 | Volterra Semiconductor Corporation | Method for making magnetic components with M-phase coupling, and related inductor structures |
US7746209B1 (en) | 2002-12-13 | 2010-06-29 | Volterra Semiconductor Corporation | Method for making magnetic components with N-phase coupling, and related inductor structures |
US8294544B2 (en) | 2008-03-14 | 2012-10-23 | Volterra Semiconductor Corporation | Method for making magnetic components with M-phase coupling, and related inductor structures |
US9627125B2 (en) | 2008-03-14 | 2017-04-18 | Volterra Semiconductor LLC | Voltage converter inductor having a nonlinear inductance value |
US8836463B2 (en) | 2008-03-14 | 2014-09-16 | Volterra Semiconductor Corporation | Voltage converter inductor having a nonlinear inductance value |
WO2009114873A1 (en) * | 2008-03-14 | 2009-09-17 | Volterra Semiconductor Corporation | Voltage converter inductor having a nonlinear inductance value |
US8237530B2 (en) | 2009-08-10 | 2012-08-07 | Volterra Semiconductor Corporation | Coupled inductor with improved leakage inductance control |
US8102233B2 (en) | 2009-08-10 | 2012-01-24 | Volterra Semiconductor Corporation | Coupled inductor with improved leakage inductance control |
US8174348B2 (en) | 2009-12-21 | 2012-05-08 | Volterra Semiconductor Corporation | Two-phase coupled inductors which promote improved printed circuit board layout |
US7994888B2 (en) | 2009-12-21 | 2011-08-09 | Volterra Semiconductor Corporation | Multi-turn inductors |
US8330567B2 (en) | 2010-01-14 | 2012-12-11 | Volterra Semiconductor Corporation | Asymmetrical coupled inductors and associated methods |
JP2012054549A (en) * | 2010-08-31 | 2012-03-15 | Samsung Electro-Mechanics Co Ltd | Transformer with integrated inductor |
CN102820125A (en) * | 2011-06-06 | 2012-12-12 | 株式会社丰田自动织机 | Magnetic core |
JP2012253264A (en) * | 2011-06-06 | 2012-12-20 | Toyota Industries Corp | Magnetic core |
US9041500B2 (en) | 2011-06-06 | 2015-05-26 | Kabushiki Kaisha Toyota Jidoshokki | Magnetic core |
CN102930957A (en) * | 2012-09-27 | 2013-02-13 | 江苏锴博材料科技有限公司 | Variable-inductance inductive iron core |
CN104810137A (en) * | 2014-01-28 | 2015-07-29 | Tdk株式会社 | Reactor |
US9455080B2 (en) | 2014-01-28 | 2016-09-27 | Tdk Corporation | Reactor |
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