JP6559930B2 - Simple evaluation method for dust cores - Google Patents

Simple evaluation method for dust cores Download PDF

Info

Publication number
JP6559930B2
JP6559930B2 JP2014087107A JP2014087107A JP6559930B2 JP 6559930 B2 JP6559930 B2 JP 6559930B2 JP 2014087107 A JP2014087107 A JP 2014087107A JP 2014087107 A JP2014087107 A JP 2014087107A JP 6559930 B2 JP6559930 B2 JP 6559930B2
Authority
JP
Japan
Prior art keywords
eddy current
current loss
inductance
dust core
insulation
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.)
Active
Application number
JP2014087107A
Other languages
Japanese (ja)
Other versions
JP2015207652A (en
Inventor
三谷 宏幸
宏幸 三谷
北条 啓文
啓文 北条
祐司 谷口
祐司 谷口
里美 佐藤
里美 佐藤
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.)
Kobe Steel Ltd
Original Assignee
Kobe Steel Ltd
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 Kobe Steel Ltd filed Critical Kobe Steel Ltd
Priority to JP2014087107A priority Critical patent/JP6559930B2/en
Publication of JP2015207652A publication Critical patent/JP2015207652A/en
Application granted granted Critical
Publication of JP6559930B2 publication Critical patent/JP6559930B2/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Landscapes

  • Measurement Of Resistance Or Impedance (AREA)
  • Investigating Or Analyzing Materials By The Use Of Magnetic Means (AREA)
  • Soft Magnetic Materials (AREA)

Description

本発明は、絶縁皮膜で被覆された軟磁性粉末を圧縮成形してなる圧粉磁心の絶縁皮膜による絶縁性および耐熱性を評価する圧粉磁心の簡易評価方法に関するものである。   The present invention relates to a dust core simple evaluation method for evaluating insulation and heat resistance of a dust core formed by compression-molding soft magnetic powder coated with an insulation film.

交流で使用されるモーターにおけるステータやロータなどの電磁気部品の磁心、特にハイブリッド自動車などのインバータやコンバータの昇圧回路に使用されるリアクトルなどには、近年、軟磁性粉末を圧縮成形してなる圧粉磁心が用いられることが多くなってきている。   In recent years, magnetic cores of electromagnetic parts such as stators and rotors in motors used in alternating current, especially reactors used in boosters for inverters and converters in hybrid vehicles, etc., have recently been compressed by compacting soft magnetic powder. Magnetic cores are increasingly used.

この圧粉磁心の原料粉末には絶縁皮膜で被覆された軟磁性粉末が用いられている。絶縁皮膜は圧粉磁心の渦電流損を抑制するために原料粉末の表面に形成されており、この絶縁皮膜による絶縁性が不十分であると鉄損の一つである渦電流損が増大してしまう。また、絶縁皮膜による耐熱性が不十分であっても歪取り焼鈍後に渦電流損が増大してしまう。   A soft magnetic powder coated with an insulating film is used as the raw material powder for the dust core. The insulation film is formed on the surface of the raw material powder to suppress the eddy current loss of the powder magnetic core. If the insulation by this insulation film is insufficient, eddy current loss, which is one of iron loss, increases. End up. Further, even if the heat resistance due to the insulating film is insufficient, eddy current loss increases after strain relief annealing.

図2に示すように、圧粉磁心において発生する渦電流損には、軟磁性粉末1すなわち粒子内で発生する粒子内渦電流損6と、複数の粒子にまたがって発生する粒子間渦電流損7がある。粒子内渦電流損6は不可避な損失であるが、粒子間渦電流損7の方は、軟磁性粉末1を絶縁皮膜2で被覆することで抑制することができる損失である。このように、絶縁皮膜2は、渦電流損のうちでも粒子間渦電流損7を抑制するために原料粉末である軟磁性粉末1の表面を被覆するようにして形成される。   As shown in FIG. 2, the eddy current loss generated in the powder magnetic core includes soft magnetic powder 1, that is, an intra-particle eddy current loss 6 generated in a particle and an inter-particle eddy current loss generated across a plurality of particles. There are seven. The intra-particle eddy current loss 6 is an inevitable loss, but the inter-particle eddy current loss 7 is a loss that can be suppressed by covering the soft magnetic powder 1 with the insulating film 2. Thus, the insulating film 2 is formed so as to cover the surface of the soft magnetic powder 1 that is the raw material powder in order to suppress the interparticle eddy current loss 7 among the eddy current losses.

しかしながら、絶縁皮膜2による絶縁性或いは断熱性が不十分であると、粒子間渦電流が発生してしまい、この渦電流が発生すると渦電流損が急激に増大するため、軟磁性粉末1を被覆する絶縁皮膜2を確実に形成することが圧粉磁心を作製するにあたり特に重要な条件となる。   However, if the insulation or heat insulation by the insulating film 2 is insufficient, an inter-particle eddy current is generated, and when this eddy current is generated, the eddy current loss increases rapidly, so that the soft magnetic powder 1 is coated. The reliable formation of the insulating film 2 is a particularly important condition for producing a dust core.

このようなことから、圧粉磁心を製造するにあたっては、軟磁性皮膜1を被覆する絶縁皮膜2が粒子間渦電流損7を抑制できる程度に絶縁性および耐熱性を有していることを調べることが不可欠であるといえるが、現在は渦電流損を直接測定することで、圧粉磁心の絶縁皮膜による絶縁性および耐熱性を評価することが一般的である。   For this reason, in manufacturing the dust core, it is examined that the insulating film 2 covering the soft magnetic film 1 has insulation and heat resistance to such an extent that the interparticle eddy current loss 7 can be suppressed. However, it is common to evaluate the insulation and heat resistance of the dust core by measuring the eddy current loss directly.

渦電流損を測定するためには、図4に示すように、リング状の圧粉磁心試験片3を作製し、その圧粉磁心試験片3に巻き線8を施すことで測定用サンプルとして渦電流損を測定している。しかしながら、測定用サンプルの作製には、リング状の圧粉磁心試験片3と巻き線8が短絡しないように、圧粉磁心試験片3の表面上に絶縁性の材料である綿テープやビニルテープなどを巻き回した上で、巻き線8を施す必要がある。また、巻き線8には、励磁用巻き線8aと検出用巻き線8bの2種の巻き線8があり、この励磁用巻き線8aと検出用巻き線8bが短絡しないように、巻き線8も絶縁材料で被覆する必要があって、渦電流損を測定するための測定用サンプルの準備が非常に煩雑であるというのが現状である。   In order to measure the eddy current loss, as shown in FIG. 4, a ring-shaped dust core test piece 3 is prepared, and the winding core 8 is applied to the dust core test piece 3 to obtain a vortex as a measurement sample. Current loss is measured. However, for the production of the measurement sample, cotton tape or vinyl tape, which is an insulating material, is provided on the surface of the dust core test piece 3 so that the ring-shaped dust core test piece 3 and the winding 8 are not short-circuited. It is necessary to wind winding 8 after winding. In addition, the winding 8 includes two types of windings 8 of an excitation winding 8a and a detection winding 8b, and the winding 8 is prevented from short-circuiting the excitation winding 8a and the detection winding 8b. However, it is necessary to coat with an insulating material, and the present situation is that preparation of a measurement sample for measuring eddy current loss is very complicated.

このように、現在実施されている従来からの渦電流損の測定方法では、測定用サンプルの準備に、巻き線を施したり絶縁材料で被覆したりするといった非常に煩雑な作業を伴うため、必要最低限でしか測定が行われていないことが多いのが現状であり、軟磁性皮膜を被覆する絶縁皮膜による絶縁性および耐熱性を評価するための簡易的な評価方法の開発が待ち望まれている。   As described above, the conventional methods for measuring eddy current loss that are currently being carried out require a very complicated operation such as winding or covering with an insulating material to prepare a measurement sample. At present, the measurement is often performed at the minimum, and the development of a simple evaluation method for evaluating the insulation and heat resistance of the insulating film covering the soft magnetic film is awaited. .

また、特許文献1には、インダクタンス素子においては、周波数変化に対するインダクタンスの変化(周波数特性)を安定させることが必要であることが記載されており、また、特許文献2には、絶縁皮膜により被覆された軟磁性粉末に関する技術が記載されており、その効果として、軟磁性粉末粒子間のギャップを十分保つことで良好な直流重畳特性が得られる。更に直流重畳特性はインダクタンスの低下率で評価されることが記載されている。   Patent Document 1 describes that in an inductance element, it is necessary to stabilize an inductance change (frequency characteristic) with respect to a frequency change, and Patent Document 2 is covered with an insulating film. As a result, good direct current superposition characteristics can be obtained by maintaining a sufficient gap between the soft magnetic powder particles. Furthermore, it is described that the direct current superimposition characteristic is evaluated by the rate of decrease in inductance.

特開平9−35937号公報JP-A-9-35937 特開2013−138159号公報JP 2013-138159 A

本発明は、上記従来の問題を解決せんとしてなされたもので、圧粉磁心の絶縁皮膜による絶縁性および耐熱性を、渦電流損を直接測定するのではなく簡易な方法で容易に評価することができる圧粉磁心の簡易評価方法を提供することを課題とするものである。   The present invention has been made as a solution to the above-mentioned conventional problems, and it is possible to easily evaluate the insulation and heat resistance of a dust core by an insulating method rather than directly measuring eddy current loss. It is an object of the present invention to provide a simple evaluation method of a dust core that can be used.

本発明の圧粉磁心の簡易評価方法は、絶縁皮膜で被覆された軟磁性粉末を圧縮成形してなる圧粉磁心における前記絶縁皮膜による絶縁性および耐熱性を評価する圧粉磁心の簡易評価方法において、棒状の圧粉磁心試験片をコイルの中に挿入し、前記圧粉磁心試験片に、10Hz〜1MHzの範囲で、且つ100倍以上の差の2種類の異なる周波数の交流電流(以下、単に電流という。)をそれぞれ流すことで、各周波数における前記圧粉磁心試験片のインダクタンスを測定し、その2種類の周波数間でのインダクタンスの低下率から、前記絶縁皮膜による絶縁性および耐熱性を評価することを特徴とする圧粉磁心の簡易評価方法である。   The simple evaluation method of a dust core of the present invention is a simple evaluation method of a dust core for evaluating the insulation and heat resistance of the insulation core in a dust core formed by compression molding a soft magnetic powder coated with an insulation film. In the above, a rod-shaped dust core test piece is inserted into a coil, and alternating currents of two different frequencies (hereinafter, Inductance of the dust core test piece at each frequency is measured by flowing each current), and the insulation and heat resistance by the insulating film are determined from the rate of decrease in inductance between the two frequencies. It is a simple evaluation method of a dust core characterized by evaluating.

また、本発明の圧粉磁心の簡易評価方法は、前記圧粉磁心試験片の電気抵抗と鉄損を予め測定しておき、前記電気抵抗と、前記鉄損から求めた渦電流損、および前記インダクタンスの低下率との関係から検量線を求め、前記インダクタンスの低下率の閾値を決定することで、前記絶縁皮膜による絶縁性および耐熱性を評価することが好ましい。   Further, in the simple evaluation method of the dust core of the present invention, the electrical resistance and the iron loss of the dust core test piece are measured in advance, the electrical resistance, the eddy current loss obtained from the iron loss, and the It is preferable to evaluate the insulation and heat resistance of the insulating film by obtaining a calibration curve from the relationship with the inductance reduction rate and determining the threshold value of the inductance reduction rate.

本発明の圧粉磁心の簡易評価方法によると、圧粉磁心の絶縁皮膜による絶縁性および耐熱性を、準備に非常に煩雑な作業を伴う測定用サンプルを用いて渦電流損を直接測定するのではなく、単純な棒状の圧粉磁心試験片を螺旋状に巻かれたコイルの中に挿入してインダクタンスを測定するという簡易な方法により容易に評価することができる。   According to the simple evaluation method of a dust core of the present invention, the insulation and heat resistance of an insulation film of a dust core can be directly measured using a measurement sample that involves a very complicated operation for preparation. Instead, it can be easily evaluated by a simple method of measuring inductance by inserting a simple bar-shaped dust core test piece into a spirally wound coil.

本発明の圧粉磁心の簡易評価方法を適用してインダクタンスを測定している状態を示す斜視図である。It is a perspective view which shows the state which is measuring the inductance by applying the simple evaluation method of the dust core of this invention. 軟磁性粉末の粒子内で発生する粒子内渦電流損と、複数の粒子にまたがって発生する粒子間渦電流損を示す説明図である。It is explanatory drawing which shows the intra-particle eddy current loss which generate | occur | produces in the particle | grains of a soft magnetic powder, and the inter-particle eddy current loss which generate | occur | produces over several particle | grains. 圧粉磁心におけるインダクタンスと周波数の関係を示すグラフ図である。It is a graph which shows the relationship between the inductance and frequency in a dust core. リング状の圧粉磁心試験片を用いて渦電流損を測定している状態を示す斜視図である。It is a perspective view which shows the state which is measuring the eddy current loss using a ring-shaped dust core test piece. 実施例で測定した圧粉磁心試験片の電気抵抗と渦電流損の関係を示すグラフ図である。It is a graph which shows the relationship between the electrical resistance of a powder magnetic core test piece measured in the Example, and an eddy current loss. 実施例で測定した圧粉磁心試験片の電気抵抗とインダクタンスの低下率の関係を示すグラフ図である。It is a graph which shows the relationship between the electrical resistance of the powder magnetic core test piece measured in the Example, and the decreasing rate of an inductance. 実施例で測定した圧粉磁心試験片のインダクタンスの低下率と渦電流損の関係を示すグラフ図である。It is a graph which shows the relationship between the fall rate of the inductance of a powder magnetic core test piece measured in the Example, and an eddy current loss.

工業的に圧粉磁心を生産するには、絶縁処理工程の検査や、絶縁皮膜が十分な絶縁性や耐熱性を備えていることを評価する製品検査が必要である。圧粉磁心の絶縁皮膜による絶縁性および耐熱性を評価するにあたって、従来からの渦電流損を直接測定する方法では、測定用サンプルの準備作業に、巻き線を施したり絶縁材料で被覆したりするという非常に煩雑な準備作業を伴っていたため、本発明者らは、圧粉磁心の絶縁皮膜による絶縁性および耐熱性の評価を、単純な構成の試験片を用いて簡易な方法により評価できる方法を見出すことを目的として、鋭意、研究、実験等の検討を実施した。   In order to produce a dust core industrially, it is necessary to inspect the insulation treatment process and to inspect the product to evaluate that the insulating film has sufficient insulation and heat resistance. In the conventional method of directly measuring eddy current loss when evaluating the insulation and heat resistance of a dust core insulation film, the sample is prepared by winding or covering with an insulating material. The present inventors have been able to evaluate the insulation and heat resistance of the dust core with an insulating film by a simple method using a test piece having a simple structure. With the aim of finding out, we studied diligently, research and experimentation.

その結果、棒状の圧粉磁心試験片を、螺旋状や渦巻状に巻かれたコイルの中に挿入して、圧粉磁心試験片に一定の条件を満足する2種類の異なる周波数の電流をそれぞれ流すことで、それぞれの周波数における前記圧粉磁心試験片のインダクタンスを測定して、その2種類の周波数間でのインダクタンスの低下率を求め、そのインダクタンスの低下率から、圧粉磁心の絶縁皮膜による絶縁性および耐熱性を簡易な方法で容易に評価することができることを見出し、本発明を完成した。   As a result, a rod-shaped dust core test piece is inserted into a spirally or spirally wound coil, and two different frequency currents satisfying certain conditions are applied to the dust core test piece, respectively. By measuring the inductance of the powder magnetic core test piece at each frequency, the inductance reduction rate between the two types of frequencies is obtained, and from the inductance reduction rate, the insulation core of the powder magnetic core is used. The inventors have found that insulation and heat resistance can be easily evaluated by a simple method, and completed the present invention.

尚、インダクタンスLは周波数を上げていくとある周波数に達したところから低下することが知られており、例えば、図3に示すように、絶縁性や耐熱性が悪い圧粉磁心Aは、絶縁性や耐熱性が高い圧粉磁心Bに比べ、低い周波数からインダクタンスLが低下してしまう。一定の条件を満足する低周波数fと高周波数fの電流を圧粉磁心試験片3に流すことでそれぞれのインダクタンスLを測定し、その低下率を評価することで、対象の圧粉磁心が十分な絶縁性および耐熱性を有しているかどうかを評価することができる。 It is known that the inductance L decreases from a certain frequency when the frequency is increased. For example, as shown in FIG. 3, a dust core A having poor insulation and heat resistance is insulated. As compared with the dust core B having high heat resistance and heat resistance, the inductance L decreases from a low frequency. Each inductance L is measured by flowing currents of a low frequency f 1 and a high frequency f 2 that satisfy a certain condition through the powder magnetic core test piece 3, and the rate of decrease thereof is evaluated. It can be evaluated whether or not has sufficient insulation and heat resistance.

以下、本発明を添付図面に示す実施形態に基づいて更に詳細に説明する。   Hereinafter, the present invention will be described in more detail based on embodiments shown in the accompanying drawings.

図1は本発明の圧粉磁心の簡易評価方法を適用し、圧粉磁心試験片3を用いてコイル4につないだLCRメータ5でインダクタンスを測定している状態を示している。棒状に圧縮成形した圧粉磁心試験片3を、螺旋状或いは渦巻状に巻かれたコイル4の中心に挿入し、その状態で後述する所定の2種類の異なる周波数の電流を、それぞれ圧粉磁心試験片3に順に流し、コイル4につないだLCRメータ5でそれぞれのインダクタンスLを測定する。測定した2種類の異なる周波数f、fでのインダクタンスLf,Lfをもとに、(Lf−Lf)/Lf×100という式からインダクタンスLの低下率を求める(図3を参照)。詳しくは実施例で説明するが、インダクタンスLの低下率から渦電流損を想定することができる。圧粉磁心試験片3に流す2種類の周波数の電流の詳細については後述する。因みに、インダクタンスLの低下率が小さい場合は電気抵抗が大きく、インダクタンスLの低下率が大きい場合は電気抵抗が小さいということができる。 FIG. 1 shows a state where an inductance is measured by an LCR meter 5 connected to a coil 4 using a dust core test piece 3 by applying the dust core simple evaluation method of the present invention. A powder magnetic core test piece 3 compression-molded into a rod shape is inserted into the center of a coil 4 wound in a spiral shape or a spiral shape, and in this state, currents of two different frequencies which will be described later are respectively supplied to the powder magnetic core. The respective inductances L are measured with an LCR meter 5 connected in sequence to the test piece 3 and connected to the coil 4. Based on the measured inductances Lf 1 and Lf 2 at two different frequencies f 1 and f 2 , the reduction rate of the inductance L is obtained from the equation (Lf 1 −Lf 2 ) / Lf 1 × 100 (FIG. 3). See). Although details will be described in the embodiment, eddy current loss can be assumed from the rate of decrease of the inductance L. Details of the two types of currents flowing through the dust core test piece 3 will be described later. Incidentally, it can be said that when the decrease rate of the inductance L is small, the electrical resistance is large, and when the decrease rate of the inductance L is large, the electrical resistance is small.

尚、圧粉磁心試験片3の形状は棒状であれば、角柱状、円柱状、短冊状等どのような形状であっても構わない。また、圧粉磁心試験片3は通常の圧粉磁心と同様に、図2に示すような絶縁皮膜2で被覆された軟磁性粉末1を圧縮成形することで作製する。   In addition, as long as the shape of the powder magnetic core test piece 3 is a rod shape, it may be any shape such as a prismatic shape, a cylindrical shape, a strip shape, or the like. Moreover, the dust core test piece 3 is produced by compression-molding the soft magnetic powder 1 covered with the insulating film 2 as shown in FIG. 2 in the same manner as a normal dust core.

軟磁性粉末1は、強磁性体の金属粉末であり、具体例としては、純鉄粉、鉄基合金粉末(Fe−Al合金、Fe−Si合金、センダスト、パーマロイ等)、アモルファス粉末等を挙げることができる。このような軟磁性粉末1は、例えば、アトマイズ法によって、微粒子とした後に還元し、その後、粉砕すること等によって製造することができる。   The soft magnetic powder 1 is a ferromagnetic metal powder. Specific examples thereof include pure iron powder, iron-based alloy powder (Fe—Al alloy, Fe—Si alloy, Sendust, Permalloy, etc.), amorphous powder, and the like. be able to. Such a soft magnetic powder 1 can be manufactured, for example, by reducing the fine particles by an atomizing method, and then reducing the fine particles.

また、この軟磁性粉末1の表面を被覆する絶縁皮膜2としては、リン酸系化成被膜等のリン酸を主成分とする皮膜やクロム系化成皮膜などの無機物、或いは低融点ガラス皮膜や、樹脂を用いて形成した皮膜を採用することが好ましい。樹脂としては、例えば、シリコーン樹脂、フェノール樹脂、エポキシ樹脂、フェノキシ樹脂、ポリアミド樹脂、ポリイミド樹脂、ポリフェニレンサルファイド樹脂、スチレン樹脂、アクリル樹脂、スチレン/アクリル樹脂、エステル樹脂、ウレタン樹脂、ポリエチレンなどのオレフィン樹脂、カーボネート樹脂、ケトン樹脂、フッ化メタクリレートやフッ化ビニリデンなどのフッ素樹脂、PEEKなどのエンジニアリングプラスチックまたはその変性品などを皮膜として用いることができる。   Further, as the insulating film 2 covering the surface of the soft magnetic powder 1, an inorganic material such as a phosphoric acid-based chemical film such as a phosphoric acid-based chemical film or a chromium-based chemical film, a low-melting glass film, a resin It is preferable to employ a film formed using. Examples of the resin include olefin resins such as silicone resin, phenol resin, epoxy resin, phenoxy resin, polyamide resin, polyimide resin, polyphenylene sulfide resin, styrene resin, acrylic resin, styrene / acrylic resin, ester resin, urethane resin, and polyethylene. Carbonate resins, ketone resins, fluororesins such as fluorinated methacrylate and vinylidene fluoride, engineering plastics such as PEEK, or modified products thereof can be used as the film.

先に説明したように本発明の圧粉磁心の簡易評価方法では、圧粉磁心試験片3に2種類の所定の周波数の電流を流すが、その周波数は、10Hz〜1MHzの範囲で、且つ100倍以上の差の2種類の異なる周波数とする。リアクトルなどに用いられる圧粉磁心試験片3に流す電流の周波数は、圧粉磁心の使用周波数帯域および装置の構成上、10Hz〜1MHzの範囲が妥当な範囲である。しかしながら、圧粉磁心試験片3に流す2種類の電流の周波数の差が小さすぎると、インダクタンスの低下率から渦電流損を想定し、絶縁皮膜による絶縁性および耐熱性を評価することが難しくなってしまったり不可能になったりするので、圧粉磁心試験片3に流す2種類の電流の周波数の差は100倍以上の差とする。尚、上限は特に記載していないが、圧粉磁心試験片3に流す電流の周波数は10Hz〜1MHzの範囲であるので、10万倍である。   As described above, in the dust core simple evaluation method of the present invention, two kinds of currents of a predetermined frequency are passed through the dust core test piece 3, and the frequency ranges from 10 Hz to 1 MHz, and 100 Two different frequencies with a difference of twice or more are used. The range of 10 Hz to 1 MHz is an appropriate range for the frequency of the current flowing through the powder magnetic core test piece 3 used for the reactor and the like in terms of the frequency band of the powder magnetic core used and the configuration of the apparatus. However, if the difference between the frequencies of the two kinds of currents flowing through the dust core test piece 3 is too small, it is difficult to evaluate the insulation and heat resistance of the insulating film, assuming eddy current loss from the rate of decrease in inductance. The frequency difference between the two types of currents flowing through the dust core test piece 3 is 100 times or more. In addition, although the upper limit is not specifically described, since the frequency of the current passed through the dust core test piece 3 is in the range of 10 Hz to 1 MHz, it is 100,000 times.

また、本発明の圧粉磁心の簡易評価方法は、棒状の圧粉磁心試験片3をコイル4の中心に挿入するという簡単な方法で試験体をセットするだけで試験の事前準備ができ、図4に示す従来からのリング状の圧粉磁心試験材を用いた試験のように、圧粉磁心試験材に絶縁材料を巻き回した上で巻き線を施し、また、巻き線にも絶縁材料で被覆するという非常に煩雑な準備作業を必要としないため、本発明は作業効率に優れた評価方法といえる。   Moreover, the simple evaluation method of the dust core of the present invention can be prepared in advance by simply setting the test body by inserting the rod-like dust core test piece 3 into the center of the coil 4. As in the test using the conventional ring-shaped dust core test material shown in Fig. 4, the insulating material is wound around the dust core test material, and then the winding is applied. The present invention can be said to be an evaluation method excellent in work efficiency because it does not require a very complicated preparation work of covering.

尚、圧粉磁心は搭載される製品や材料によって、使用する周波数帯やインダクタンスの絶対値やインダクタンスの低下率が異なる。従って、インダクタンンスの低下率と渦電流損の関係を予め評価した上で、検量線を作成し、インダクタンスの閾値を設定することが望ましい。   Note that the dust core has different frequency bands to be used, the absolute value of the inductance, and the rate of decrease of the inductance depending on the product or material to be mounted. Therefore, it is desirable to create a calibration curve and set the inductance threshold after evaluating the relationship between the inductance drop rate and eddy current loss in advance.

また、本発明の圧粉磁心の簡易評価方法は、閉回路で行う測定でないため、磁心以外の空間にまで磁束が漏れることが想定される。そのため、測定用のコイル4の周辺には磁性体が存在することは好ましくなく、少なくともコイル4の周辺50cm以内には磁性体が存在しないことを要件とする。   Moreover, since the simple evaluation method of the dust core of the present invention is not a measurement performed in a closed circuit, it is assumed that the magnetic flux leaks to a space other than the magnetic core. For this reason, it is not preferable that a magnetic material exists around the measurement coil 4, and it is a requirement that no magnetic material exists within at least 50 cm around the coil 4.

以下、実施例を挙げて本発明をより具体的に説明するが、本発明はもとより下記実施例によって制限を受けるものではなく、本発明の趣旨に適合し得る範囲で適宜変更を加えて実施することも可能であり、それらは何れも本発明の技術的範囲に含まれる。   EXAMPLES Hereinafter, the present invention will be described more specifically with reference to examples. However, the present invention is not limited by the following examples, and the present invention is implemented with appropriate modifications within a range that can meet the gist of the present invention. These are all included in the technical scope of the present invention.

軟磁性粉末として純鉄粉(神戸製鋼所製:マグメル(登録商標)ML35N)を用い、その表面に絶縁皮膜となるリン酸系化成皮膜を形成した。このリン酸系化成皮膜の形成には、リン酸系化成皮膜用処理液として、水:50質量部、NaHPO:30質量部、HPO:10質量部、(NHOH)・HSO:10質量部、Co(PO:10質量部を混合して原液とし、電気抵抗を変化させるために水で50倍まで適宜希釈して濃度を変えた処理液を用いた。純鉄粉100質量部に対して前記様々な濃度の処理液を5質量部混合して、大気中200℃で乾燥させることにより、純鉄粉の表面にリン酸系化成皮膜を形成した。 Pure iron powder (manufactured by Kobe Steel: Magmel (registered trademark) ML35N) was used as the soft magnetic powder, and a phosphoric acid-based chemical conversion film serving as an insulating film was formed on the surface thereof. In forming this phosphoric acid-based chemical conversion film, water: 50 parts by mass, NaH 2 PO 4 : 30 parts by mass, H 3 PO 4 : 10 parts by mass, (NH 2 OH) 2 · H 2 SO 4: 10 parts by mass, Co 3 (PO 4) 2 : 10 parts by weight and mixed to stock, varying concentrations were diluted appropriately to 50 times with water in order to change the electrical resistance process The liquid was used. The phosphoric acid-based chemical film was formed on the surface of the pure iron powder by mixing 5 parts by mass of the treatment liquid with various concentrations with respect to 100 parts by mass of the pure iron powder and drying in the atmosphere at 200 ° C.

その後、この絶縁皮膜を形成した軟磁性粉末を用いて圧粉成形することで、リング状の圧粉磁心試験片(φ45×φ33×5t:単位mm)と、角柱状の圧粉磁心試験片(12.7×31.75×5t:単位mm)を作製した。   Thereafter, the soft magnetic powder on which the insulating film is formed is compacted to form a ring-shaped dust core test piece (φ45 × φ33 × 5 t: unit mm) and a prismatic dust core test piece ( 12.7 × 31.75 × 5t: unit mm).

図4に示すようなリング状の圧粉磁心試験片3を用いて、その電気抵抗および鉄損(渦電流損)を測定すると共に、角柱状の圧粉磁心試験片3を用いてインダクタンスLを測定した。インダクタンスLの測定は、図1に示すように、筒にリッツ線を巻いた(巻き数100)コイル4の中心に角柱状の圧粉磁心試験片3を挿入し、コイル4にLCRメータ5をつなぎ、周波数100Hzと100kHzの電流をそれぞれ流した時のインダクタンスLをLCRメータ5で測定した。   The electrical resistance and iron loss (eddy current loss) are measured using a ring-shaped dust core test piece 3 as shown in FIG. 4, and the inductance L is measured using a prismatic dust core test piece 3. It was measured. As shown in FIG. 1, the inductance L is measured by inserting a prismatic dust core test piece 3 into the center of a coil 4 in which a litz wire is wound (number of turns 100), and an LCR meter 5 is inserted into the coil 4. The LCR meter 5 was used to measure the inductance L when currents having a frequency of 100 Hz and 100 kHz were passed.

100Hzの電流を流した際のインダクタンスL100Hzと、100kHzの電流を流した際のインダクタンスL100kHzとから、下記式をもとにインダクタンスLの低下率L(単位%)を求めた。
=(L100Hz−L100kHz)/L100Hz×100
From the inductance L 100 Hz when a current of 100 Hz was passed and the inductance L 100 kHz when a current of 100 kHz was passed, a reduction rate L D (unit%) of the inductance L was determined based on the following formula.
L D = (L 100 Hz− L 100 kHz ) / L 100 Hz × 100

前記した各測定で求めた電気抵抗(単位μΩ・m)と渦電流損(単位W/kg)の関係を図5に、電気抵抗(単位μΩ・m)とインダクタンスLの低下率(単位%)の関係を図6に、インダクタンスLの低下率(単位%)と渦電流損(単位W/kg)の関係を図7に、それぞれ示す。   FIG. 5 shows the relationship between the electrical resistance (unit μΩ · m) and the eddy current loss (unit W / kg) obtained in each measurement, and the reduction rate (unit%) of the electrical resistance (unit μΩ · m) and the inductance L. 6 shows the relationship between the rate of decrease in inductance L (unit%) and the eddy current loss (unit W / kg). FIG.

図5に示す電気抵抗と渦電流損の関係によると、電気抵抗がある程度小さくなると急激に渦電流損が増大することが分かる。また、図6に示す電気抵抗とインダクタンスLの低下率の関係も、図5に示す電気抵抗と渦電流損の関係と同様の傾向を示しており、図5と図6に図示した内容は、インダクタンスLの低下率と渦電流損には相関関係があることを示唆している。   According to the relationship between the electrical resistance and the eddy current loss shown in FIG. 5, it can be seen that the eddy current loss rapidly increases when the electrical resistance decreases to some extent. 6 also shows the same tendency as the relationship between the electrical resistance and eddy current loss shown in FIG. 5, and the contents shown in FIGS. This suggests that there is a correlation between the rate of decrease of inductance L and eddy current loss.

図7はインダクタンスLの低下率と渦電流損の関係を示すが、インダクタンスLの低下率が大きくなると渦電流損が増大しており、インダクタンスLの低下率と渦電流損には正の相関関係があることが分かる。また、インダクタンスLの低下率が3%以下では渦電流損の値は殆ど変化していないことから、この渦電流損の値が軟磁性粉末内で発生する不可避な損失の粒子内渦電流損であるといえる。すなわち、ML35Nの場合は、インダクタンスLの低下率が3%以下であれば、渦電流損は全て粒子内渦電流損であると見なすことができ、3%を閾値とすることで、絶縁皮膜による絶縁性および耐熱性を評価することができる。   FIG. 7 shows the relationship between the decrease rate of the inductance L and the eddy current loss. As the decrease rate of the inductance L increases, the eddy current loss increases, and a positive correlation exists between the decrease rate of the inductance L and the eddy current loss. I understand that there is. Further, since the value of the eddy current loss hardly changes when the decrease rate of the inductance L is 3% or less, the value of the eddy current loss is an inevitable loss in the particles, which is an inevitable loss generated in the soft magnetic powder. It can be said. That is, in the case of ML35N, if the rate of decrease of the inductance L is 3% or less, all eddy current loss can be regarded as intra-particle eddy current loss, and by setting 3% as a threshold, Insulation and heat resistance can be evaluated.

1…軟磁性粉末
2…絶縁皮膜
3…圧粉磁心試験片
4…コイル
5…LCRメータ
6…粒子内渦電流損
7…粒子間渦電流損
8…巻き線
8a…励磁用巻き線
8b…検出用巻き線
DESCRIPTION OF SYMBOLS 1 ... Soft magnetic powder 2 ... Insulating film 3 ... Powder magnetic core test piece 4 ... Coil 5 ... LCR meter 6 ... Intraparticle eddy current loss 7 ... Interparticle eddy current loss 8 ... Winding 8a ... Excitation winding 8b ... Detection Winding wire

Claims (2)

絶縁皮膜で被覆された軟磁性粉末を圧縮成形してなる圧粉磁心における前記絶縁皮膜による絶縁性または耐熱性を評価する圧粉磁心の簡易評価方法において、
棒状の圧粉磁心試験片をコイルの中に挿入し、
前記圧粉磁心試験片に、10Hz〜1MHzの範囲で、且つ100倍以上の差の2種類の異なる周波数の交流電流をそれぞれ流すことで、各周波数における前記圧粉磁心試験片のインダクタンスを測定し、その2種類の周波数間でのインダクタンスの低下率から、前記絶縁皮膜による絶縁性または耐熱性を評価することを特徴とする圧粉磁心の簡易評価方法。
In a simple evaluation method of a dust core for evaluating insulation or heat resistance of the insulation core in a dust core formed by compression molding a soft magnetic powder coated with an insulation film,
Insert a rod-shaped dust core test piece into the coil,
The inductance of the dust core test piece at each frequency is measured by flowing alternating currents of two different frequencies with a difference of 100 times or more in the range of 10 Hz to 1 MHz to the dust core test piece. A simple evaluation method for a dust core, wherein the insulation or heat resistance of the insulating film is evaluated from the rate of decrease in inductance between the two types of frequencies.
前記圧粉磁心試験片の電気抵抗と渦電流損を予め測定しておく工程と、
前記電気抵抗と前記渦電流損の関係、および、前記電気抵抗と前記インダクタンスの低下率の関係から前記インダクタンスの低下率と前記渦電流損の関係を示す検量線を作成する工程と、
前記検量線において、前記インダクタンスの低下率の増加に対して前記渦電流損の値が変化しない第1領域は、前記渦電流損が全て粒子内渦電流損であると見なし、前記インダクタンスの低下率が増加するに従って前記渦電流損も増加する第2領域は、前記渦電流損が前記粒子内渦電流損に加えて粒子間渦電流損も重畳されているものと見なす渦電流損評価工程と、
前記検量線の前記第1領域と前記第2領域が交わる位置の前記インダクタンスの低下率を前記インダクタンスの低下率の閾値と決定する閾値決定工程と、
を有し、
前記インダクタンスの低下率が前記閾値以下であるか超えているかにより、前記絶縁皮膜による絶縁性または耐熱性を評価する請求項1記載の圧粉磁心の簡易評価方法。
Families Ku step previously measured electric resistance and the eddy current loss of the powder magnetic core specimen,
Creating a calibration curve indicating the relationship between the decrease rate of the inductance and the eddy current loss from the relationship between the electrical resistance and the eddy current loss, and the relationship between the electrical resistance and the decrease rate of the inductance;
In the calibration curve, the first region where the value of the eddy current loss does not change with respect to the increase in the inductance reduction rate is considered that the eddy current loss is all in-particle eddy current loss, and the inductance reduction rate. The second region in which the eddy current loss increases as the eddy current loss increases, the eddy current loss evaluation step that considers that the eddy current loss is superimposed on the interparticle eddy current loss in addition to the intraparticle eddy current loss;
A threshold value determining step for determining a reduction rate of the inductance at a position where the first region and the second region of the calibration curve intersect as a threshold value of the reduction rate of the inductance;
Have
The simple evaluation method of a dust core according to claim 1, wherein the insulation or heat resistance of the insulating film is evaluated depending on whether the rate of decrease in inductance is equal to or less than the threshold value .
JP2014087107A 2014-04-21 2014-04-21 Simple evaluation method for dust cores Active JP6559930B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2014087107A JP6559930B2 (en) 2014-04-21 2014-04-21 Simple evaluation method for dust cores

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2014087107A JP6559930B2 (en) 2014-04-21 2014-04-21 Simple evaluation method for dust cores

Publications (2)

Publication Number Publication Date
JP2015207652A JP2015207652A (en) 2015-11-19
JP6559930B2 true JP6559930B2 (en) 2019-08-14

Family

ID=54604243

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2014087107A Active JP6559930B2 (en) 2014-04-21 2014-04-21 Simple evaluation method for dust cores

Country Status (1)

Country Link
JP (1) JP6559930B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP6595356B2 (en) * 2016-01-26 2019-10-23 株式会社東芝 Magnetic core member deterioration diagnosis device, magnetic core member deterioration diagnosis method, electrical equipment

Family Cites Families (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5846044B2 (en) * 1979-04-14 1983-10-14 日本金属株式会社 powder iron core
JPS57136159A (en) * 1981-02-18 1982-08-23 Aichi Steel Works Ltd Eddy current system metal internal defect finding method and device
JPS61243101A (en) * 1985-04-17 1986-10-29 Hitachi Metals Ltd Green compact magnetic core consisting of fe-ni
JPS6227674A (en) * 1985-07-29 1987-02-05 Hitachi Cable Ltd Method for measuring skin effect coefficient of conductor
JP2008013827A (en) * 2006-07-07 2008-01-24 Nec Tokin Corp Composite soft magnetic power and dust core using the same
JP4641299B2 (en) * 2006-10-02 2011-03-02 株式会社豊田中央研究所 Insulating film, magnetic core powder and powder magnetic core, and method for forming or manufacturing the same
JP2008096217A (en) * 2006-10-10 2008-04-24 Toyota Central R&D Labs Inc Method and apparatus for evaluating internal state of dust core component
JP2013138159A (en) * 2011-12-28 2013-07-11 Diamet:Kk Composite soft magnetic material and production method therefor

Also Published As

Publication number Publication date
JP2015207652A (en) 2015-11-19

Similar Documents

Publication Publication Date Title
Zhao et al. Evolution of the insulation matrix and influences on the magnetic performance of Fe soft magnetic composites during annealing
CN103098144B (en) The design apparatus of electric wire, coil, electric wire and motor
US9251946B2 (en) Compact
TWI546827B (en) Soft magnetic powder, method for producing soft magnetic component and component produced
Périgo et al. Magnetic properties of soft magnetic composites prepared with crystalline and amorphous powders
Laxminarayana et al. Study of AC magnetic properties and core losses of Fe/Fe3O4-epoxy resin soft magnetic composite
JP6194369B2 (en) High frequency wires and coils
EP3300089A1 (en) Dust core, method for producing said dust core, inductor provided with said dust core, and electronic/electrical device on which said inductor is mounted
EP2963656A1 (en) Inductor and method of manufacturing the same
CN103956259B (en) A kind of reactor design method based on visualized algorithm
JP6107804B2 (en) Coating liquid, dust core, powder for magnetic core and method for producing the same
JP2016054287A (en) Core and coil device using the same
JP2016181620A (en) Magnetic core for current transformer, current transformer and watthour meter
JP6062035B2 (en) Electric wires and coils
JP6559930B2 (en) Simple evaluation method for dust cores
JP2005213621A (en) Soft magnetic material and powder magnetic core
JP4909312B2 (en) Soft magnetic material for dust core and dust core
US11651892B2 (en) Method for producing composite magnetic body, magnetic powder, composite magnetic body and coil component
CN106575567A (en) Current transformer core, method for manufacturing same, and device equipped with said core
CN102426909A (en) Direct current resisting transformer based on composite magnetic core and manufacturing method thereof
CN102982958A (en) Zero temperature drift self-compensating Rogowski coil
CN105390226A (en) A core and a coil device using the core
JP2017168587A (en) Reactor
Manna et al. AC magnetic properties and core loss behavior of Fe–P soft magnetic sheets
JP2008143720A (en) Magnetite-iron composite powder, its manufacturing method and dust core

Legal Events

Date Code Title Description
RD02 Notification of acceptance of power of attorney

Free format text: JAPANESE INTERMEDIATE CODE: A7422

Effective date: 20160606

RD04 Notification of resignation of power of attorney

Free format text: JAPANESE INTERMEDIATE CODE: A7424

Effective date: 20160713

A621 Written request for application examination

Free format text: JAPANESE INTERMEDIATE CODE: A621

Effective date: 20160901

A977 Report on retrieval

Free format text: JAPANESE INTERMEDIATE CODE: A971007

Effective date: 20170630

A131 Notification of reasons for refusal

Free format text: JAPANESE INTERMEDIATE CODE: A131

Effective date: 20170801

A521 Written amendment

Free format text: JAPANESE INTERMEDIATE CODE: A523

Effective date: 20170925

A02 Decision of refusal

Free format text: JAPANESE INTERMEDIATE CODE: A02

Effective date: 20180403

A61 First payment of annual fees (during grant procedure)

Free format text: JAPANESE INTERMEDIATE CODE: A61

Effective date: 20190718

R150 Certificate of patent or registration of utility model

Ref document number: 6559930

Country of ref document: JP

Free format text: JAPANESE INTERMEDIATE CODE: R150