JPH03201412A - Magnetic material for earth leakage breaker consisting of crystallite base alloy - Google Patents
Magnetic material for earth leakage breaker consisting of crystallite base alloyInfo
- Publication number
- JPH03201412A JPH03201412A JP2091962A JP9196290A JPH03201412A JP H03201412 A JPH03201412 A JP H03201412A JP 2091962 A JP2091962 A JP 2091962A JP 9196290 A JP9196290 A JP 9196290A JP H03201412 A JPH03201412 A JP H03201412A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic
- core
- earth leakage
- flux density
- iron
- 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.)
- Granted
Links
- 229910045601 alloy Inorganic materials 0.000 title claims abstract description 17
- 239000000956 alloy Substances 0.000 title claims abstract description 17
- 239000000696 magnetic material Substances 0.000 title claims description 5
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical compound [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 claims abstract description 30
- 229910052742 iron Inorganic materials 0.000 claims abstract description 15
- 230000004907 flux Effects 0.000 claims abstract description 13
- 239000000463 material Substances 0.000 claims description 14
- 239000002245 particle Substances 0.000 claims description 5
- 230000001419 dependent effect Effects 0.000 claims 1
- 239000011162 core material Substances 0.000 abstract description 33
- 239000013081 microcrystal Substances 0.000 abstract 3
- 239000000203 mixture Substances 0.000 abstract 1
- PXHVJJICTQNCMI-UHFFFAOYSA-N Nickel Chemical compound [Ni] PXHVJJICTQNCMI-UHFFFAOYSA-N 0.000 description 6
- 230000035699 permeability Effects 0.000 description 5
- 238000007710 freezing Methods 0.000 description 4
- 230000008014 freezing Effects 0.000 description 4
- 230000003068 static effect Effects 0.000 description 4
- ZOXJGFHDIHLPTG-UHFFFAOYSA-N Boron Chemical compound [B] ZOXJGFHDIHLPTG-UHFFFAOYSA-N 0.000 description 3
- 238000000137 annealing Methods 0.000 description 3
- 229910052796 boron Inorganic materials 0.000 description 3
- 238000004519 manufacturing process Methods 0.000 description 3
- 229910052759 nickel Inorganic materials 0.000 description 3
- 229910052710 silicon Inorganic materials 0.000 description 3
- 239000010703 silicon Substances 0.000 description 3
- RYGMFSIKBFXOCR-UHFFFAOYSA-N Copper Chemical compound [Cu] RYGMFSIKBFXOCR-UHFFFAOYSA-N 0.000 description 2
- 239000010941 cobalt Substances 0.000 description 2
- 229910017052 cobalt Inorganic materials 0.000 description 2
- GUTLYIVDDKVIGB-UHFFFAOYSA-N cobalt atom Chemical compound [Co] GUTLYIVDDKVIGB-UHFFFAOYSA-N 0.000 description 2
- 238000001816 cooling Methods 0.000 description 2
- 229910052802 copper Inorganic materials 0.000 description 2
- 239000010949 copper Substances 0.000 description 2
- 238000010438 heat treatment Methods 0.000 description 2
- 239000002184 metal Substances 0.000 description 2
- 229910052751 metal Inorganic materials 0.000 description 2
- 229910052758 niobium Inorganic materials 0.000 description 2
- 239000010955 niobium Substances 0.000 description 2
- 229910000889 permalloy Inorganic materials 0.000 description 2
- IOMKFXWXDFZXQH-UHFFFAOYSA-N (6-oxo-7,8,9,10-tetrahydrobenzo[c]chromen-3-yl) 3-chloro-4-[3-[(2-methylpropan-2-yl)oxycarbonylamino]propanoyloxy]benzoate Chemical compound C1=C(Cl)C(OC(=O)CCNC(=O)OC(C)(C)C)=CC=C1C(=O)OC1=CC=C(C2=C(CCCC2)C(=O)O2)C2=C1 IOMKFXWXDFZXQH-UHFFFAOYSA-N 0.000 description 1
- 229910000640 Fe alloy Inorganic materials 0.000 description 1
- 229910001030 Iron–nickel alloy Inorganic materials 0.000 description 1
- 239000002178 crystalline material Substances 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 239000000835 fiber Substances 0.000 description 1
- 229910052735 hafnium Inorganic materials 0.000 description 1
- UGKDIUIOSMUOAW-UHFFFAOYSA-N iron nickel Chemical compound [Fe].[Ni] UGKDIUIOSMUOAW-UHFFFAOYSA-N 0.000 description 1
- 230000005415 magnetization Effects 0.000 description 1
- 238000005259 measurement Methods 0.000 description 1
- 150000002739 metals Chemical class 0.000 description 1
- GUCVJGMIXFAOAE-UHFFFAOYSA-N niobium atom Chemical compound [Nb] GUCVJGMIXFAOAE-UHFFFAOYSA-N 0.000 description 1
- 229910052715 tantalum Inorganic materials 0.000 description 1
- 230000036962 time dependent Effects 0.000 description 1
- 229910052721 tungsten Inorganic materials 0.000 description 1
- 229910052726 zirconium Inorganic materials 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F1/00—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties
- H01F1/01—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials
- H01F1/03—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity
- H01F1/12—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of soft-magnetic materials
- H01F1/14—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of soft-magnetic materials metals or alloys
- H01F1/147—Alloys characterised by their composition
- H01F1/153—Amorphous metallic alloys, e.g. glassy metals
- H01F1/15308—Amorphous metallic alloys, e.g. glassy metals based on Fe/Ni
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01H—ELECTRIC SWITCHES; RELAYS; SELECTORS; EMERGENCY PROTECTIVE DEVICES
- H01H83/00—Protective switches, e.g. circuit-breaking switches, or protective relays operated by abnormal electrical conditions otherwise than solely by excess current
- H01H83/14—Protective switches, e.g. circuit-breaking switches, or protective relays operated by abnormal electrical conditions otherwise than solely by excess current operated by imbalance of two or more currents or voltages, e.g. for differential protection
- H01H83/144—Protective switches, e.g. circuit-breaking switches, or protective relays operated by abnormal electrical conditions otherwise than solely by excess current operated by imbalance of two or more currents or voltages, e.g. for differential protection with differential transformer
Landscapes
- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Chemical & Material Sciences (AREA)
- Dispersion Chemistry (AREA)
- Soft Magnetic Materials (AREA)
- Hard Magnetic Materials (AREA)
- Transformers For Measuring Instruments (AREA)
- Analogue/Digital Conversion (AREA)
- Driving Mechanisms And Operating Circuits Of Arc-Extinguishing High-Tension Switches (AREA)
Abstract
Description
【発明の詳細な説明】
[lll上上利用分野]
この発明は、微結晶鉄ベース合金から成る漏電遮断器用
磁石材料に関する。DETAILED DESCRIPTION OF THE INVENTION [Top Field of Application] This invention relates to a magnet material for earth leakage circuit breakers comprising a microcrystalline iron-based alloy.
[従来の技術]
漏電遮断器は長年にわたり人体及び機械の保護のために
用いられている。漏電遮断器の重要な構成部品は差動変
流器として働く軟磁性磁心である0機械保護用漏電遮断
器のための引き外し電流は約300〜500 m Aの
範囲にある。これに反して人体保護用漏電遮断器の場合
には引き外し電流は30mAにすぎない、ヒルツインゲ
ル(Hilzinger )及びポル(Boi1) c
7)論文「結晶質及び非晶質軟磁性金属(Weichm
agnetischekristalline und
amorphe Metalle ) J 、 xレ
クトロニク(Elektronik) 、第22巻、1
987年には、磁心に対する要求とこのために使用され
る材料とが記載されている。?a1心材料は高い最大透
磁率又は小さい磁界強度の際の十分な磁束密度のほかに
、特に全使用範囲にわたり磁気特性の温度依存性を小さ
くしなければならない、30mA漏電遮断器に対しては
主として約77%ニッケルを含む結晶質ニッケル・鉄合
金(パーマロイ形)が使用される。この材料の飽和値は
約0.8Tである。しかしながら材料の磁気特性の温度
依存性を小さくするためには、パーマロイ合金の場合に
は補助的な費用のかかる焼きなましが必要である。それ
により漏電遮断器用磁心の製造は費用がかかり高価とな
る。焼きなましの必要性はファイア y (Pfeif
er )及びポル(Rol1)の論文、アイトリプルイ
ー トランザクションズ(IEEETransacti
ons) 、磁気掌編、第MAG−5巻、第3号、19
69年9月、第365〜370ページに詳細に述べられ
ている。[Prior Art] Earth leakage circuit breakers have been used for many years to protect humans and machinery. The key component of the earth leakage circuit breaker is a soft magnetic core that acts as a differential current transformer.The tripping current for a machine protection earth leakage circuit breaker is in the range of about 300-500 mA. On the other hand, in the case of earth leakage circuit breakers for personal protection, the tripping current is only 30 mA.
7) Paper “Crystalline and Amorphous Soft Magnetic Metals (Weichm
agnetischekristalline und
amorphe Metalle) J, x Elektronik, Volume 22, 1
987 describes the requirements for magnetic cores and the materials used for them. ? In addition to a high maximum magnetic permeability or a sufficient magnetic flux density at low magnetic field strengths, the a1 core material must also have a low temperature dependence of the magnetic properties over the entire range of use, especially for 30 mA ground fault circuit breakers. A crystalline nickel-iron alloy (permalloy type) containing approximately 77% nickel is used. The saturation value of this material is approximately 0.8T. However, in order to reduce the temperature dependence of the magnetic properties of the material, additional and expensive annealing is necessary in the case of permalloy alloys. This makes the production of earth fault circuit breaker cores expensive and expensive. The need for annealing is due to fire
er) and Pol (Rol1), IEEE Transacti
ons), Magnetic Handbook, Vol. MAG-5, No. 3, 19
It is described in detail in September 1969, pages 365-370.
結晶質材料のほかに既に漏電遮断器用非晶質材料が提案
されている。小さい磁化力が要求されるために30mA
用1m電遣断器に対してはコバルトを多く含む合金だけ
が問題となり、その飽和(iは0.55〜0.7Tの範
囲にある。しかしながらポル及びヒルツインゲルの前記
論文に記載のように、非晶質材料を使用する場合に温度
依存性に関する高い要求において問題が生じる。In addition to crystalline materials, amorphous materials for earth leakage circuit breakers have already been proposed. 30mA because a small magnetizing force is required
For commercial 1 m disconnectors, only cobalt-rich alloys are a problem, and their saturation (i is in the range 0.55 to 0.7 T). , problems arise when using amorphous materials with high demands regarding temperature dependence.
[発明が解決しようとする課題]
この発明の課題は、飽和磁束密度が高いと同時に磁気特
性の温度依存性が小さい漏電遮断器用磁心材料を提供す
ることにある。[Problems to be Solved by the Invention] An object of the present invention is to provide a magnetic core material for an earth leakage circuit breaker that has a high saturation magnetic flux density and at the same time has a small temperature dependence of magnetic properties.
[課題を解決するための手段]
この課題はこの発明に基づき、60原子%以上の鉄台イ
■量を有し、その組織の50%以上が1100n未満の
粒度の微結晶粒子から成り、t、t”r以上の飽和磁束
密度及び0.7未満の残留磁気比B r / B sを
有する鉄ベース合金を磁心材料として使用することによ
り解決される。ここでB、は残留磁気であり、BSは飽
和磁束密度である。[Means for Solving the Problem] This problem is based on the present invention, and has an iron base grain content of 60 atomic % or more, 50% or more of its structure consists of microcrystalline grains with a grain size of less than 1100 nm, and t , t”r or more and a remanence ratio B r /B s less than 0.7, as the magnetic core material, where B is the remanence; BS is the saturation magnetic flux density.
この種の微結晶鉄ベース合金は欧州特許出願公開FJ2
71B57号公報から知られている。これは特に鉄のほ
かに主として0.1〜3原子%の銅、0.1〜30原子
%のNb、 W 、 Ta、 Zr、Hf、 Ti、N
oのような別の金属、30原子%以下のケイ素及び25
原子%以下のホウ素を含む合金であり。This kind of microcrystalline iron-based alloy is available in European Patent Application Publication FJ2
It is known from Publication No. 71B57. In particular, in addition to iron, it mainly contains 0.1-3 at.% copper, 0.1-30 at.% Nb, W, Ta, Zr, Hf, Ti, N.
another metal such as o, up to 30 atom % silicon and 25
It is an alloy containing less than atomic percent of boron.
その際ホウ素とケイ素との合計含有量は5〜30原子%
の範囲にある。鉄は部分的にコバルト及び/又はニッケ
ルにより置き替えることができる。この材料はその良好
な磁気高周波特性に基づき高周波変成器、チョーク及び
磁石に使用するために提案されている。欧州特許出願公
開第299498号公報から微結晶鉄ベース合金から成
る磁心が知られており、この磁心は透磁率の時間依存性
変化が非常に少ない。チョーク、フィルタ及び高周波変
成器における磁心の前記公報に記載の用途に対して、0
.3以下又は0.7以上の残留磁気比を有する磁心が用
いられる。更に吉沢、山内、中機及び杉原の論文、ジャ
ーナル オブ アプライド フィジックス(Journ
al of AppliedPhysics ) 、?
564巻、第10号、1988年、第6047〜604
9ページから、チ3.−クコイルに使用するための微結
晶鉄ベース合金から成る磁心が知られている。この論文
には飽和磁束密度の温度依存性についての測定fメと、
氷点以上の温度に対する透磁率とが記載されている。At that time, the total content of boron and silicon is 5 to 30 at%
within the range of Iron can be partially replaced by cobalt and/or nickel. This material has been proposed for use in high frequency transformers, chokes and magnets due to its good magnetic high frequency properties. From European Patent Application No. 299,498 a magnetic core is known consisting of a microcrystalline iron-based alloy, which magnetic core exhibits a very low time-dependent change in magnetic permeability. For the use of magnetic cores in chokes, filters and high frequency transformers as described in the above publication, 0
.. A magnetic core having a remanence ratio of 3 or less or 0.7 or more is used. Furthermore, papers by Yoshizawa, Yamauchi, Nakaki, and Sugihara, Journal of Applied Physics (Journal
al of Applied Physics),?
Volume 564, No. 10, 1988, Nos. 6047-604
From page 9, CH3. - Cores made of microcrystalline iron-based alloys for use in coils are known. This paper includes measurements of the temperature dependence of saturation magnetic flux density,
The magnetic permeability at temperatures above the freezing point is described.
[作用効果]
驚くべきことに微結晶鉄ベース合金が、漏電遮断器の使
用範囲である一25℃の温度までの氷点下の温度におい
ても、磁気特性の温度依存性が極めて小さいということ
が発見された。氷点を超える場合の磁気特性の小さい温
度依存性は、漏電遮断器に磁心材料として使用するため
には不十分であり、更に従来漏電遮断器のために使用さ
れた材料から知られているように(第4図参照)、氷点
下の温度の場合の小さい温度依存性に対するあかしとは
ならない、既にファイファ及びポルの論文に記載のよう
に、従来の技術に基づくニッケル・鉄合金も比較的高い
温度の場合には透磁率の低下は比較的小さいが、これに
反して低い温度の場合には透磁率の低下が著しい。[Operation and Effect] Surprisingly, it has been discovered that the temperature dependence of the magnetic properties of microcrystalline iron-based alloys is extremely small even at sub-zero temperatures of -25°C, which is the range of temperatures in which earth leakage circuit breakers are used. Ta. The small temperature dependence of the magnetic properties above the freezing point is not sufficient for use as core material in earth leakage circuit breakers, and furthermore, as is known from the materials conventionally used for earth leakage circuit breakers. (see Figure 4), does not provide evidence for a small temperature dependence in the case of sub-zero temperatures.As already mentioned in the paper by Pfeiffer and Pol, the nickel-iron alloys based on the prior art are also At low temperatures, the decrease in magnetic permeability is relatively small; on the other hand, at low temperatures, the decrease in magnetic permeability is significant.
漏電遮断器のためのこの発明に基づく微結晶磁心は、非
常に良好な軟磁性特性を有し、またこの特性の温度依存
性は小さい、このことは丸いヒステリシスループを有す
るすなわち0.4以上0.7未満の残留磁気比を有する
磁心に対し特に成立する。この合金の製造は経済的であ
る。なぜならば磁気特性の温度依存性を小さくするため
の補助的な特殊の焼きなましが必要でないからである。The microcrystalline magnetic core according to the invention for earth leakage circuit breakers has very good soft magnetic properties and the temperature dependence of these properties is small, which means that it has a round hysteresis loop, i.e. This holds especially true for magnetic cores with a remanence ratio of less than .7. The production of this alloy is economical. This is because no special supplementary annealing is required to reduce the temperature dependence of the magnetic properties.
環状磁心はパルスレベル制御に対するばかりでなく重畳
された小さい直流磁界に対しても非常に良好な安定性を
示す。The toroidal core exhibits very good stability not only to pulse level control but also to small superimposed DC magnetic fields.
[実施例]
次にこの発明に基づ〈磁石材料の複数の実施例の特性を
示すグラフにより、この発明の詳細な説明する。[Examples] Next, the present invention will be explained in detail using graphs showing the characteristics of a plurality of examples of magnetic materials based on the present invention.
fらなヒステリシスループを有する環状テープコアばか
りでなく丸いヒステリシスループを有する環状テープコ
アが作られた。30mA漏電遮断器に使用するために、
特に0.4〜0.7の範囲の残留磁気比を有する材料が
有利であることが判明した。微結晶テープは、−回の熱
処理工程と続いて0.4に7分以上の冷却速度による冷
却とにより、元来非晶質のテープを結晶化することによ
り製作された。An annular tape core with a round hysteresis loop as well as an annular tape core with a round hysteresis loop were made. For use in 30mA earth leakage circuit breakers,
Materials with a remanence ratio in the range from 0.4 to 0.7 have proven particularly advantageous. The microcrystalline tape was fabricated by crystallizing the originally amorphous tape by - heat treatment steps followed by cooling with a cooling rate of 0.4 to 7 minutes or more.
微結晶のテープの製造方法は原理的に前記欧州特許出願
公開公報から知られている。微結晶粒子の粒度はすべて
の実施例において常に25nm未満であった。実施例の
磁心は73.5原子%の鉄のほかに更にl原子%の銅、
3原子%のニオブ、13.5原子%のケイ素及び9原子
%のホウ素を含んでいた。完成された環状テープコアは
φ19×φ15X5mmの寸法を有していた。環状テー
プコアではそれぞれ、f4 (50Hz)及び静的磁束
密度偏移Δ13stat及び動的磁束密度偏移ΔBdV
nのヒステリシスループ及び磁化曲線が、正弦波、半波
整流及び全波整流電流の場合に室温で測定された。更に
静的及び動的磁束密度偏移及び50Hzでのル4の温度
依存性が測定された。A method for producing microcrystalline tapes is known in principle from the aforementioned European Patent Application Publication No. 2003-210002. The grain size of the microcrystalline particles was always less than 25 nm in all examples. In addition to 73.5 atom % of iron, the magnetic core of the example also contains 1 atom % of copper,
It contained 3 at.% niobium, 13.5 at.% silicon and 9 at.% boron. The completed annular tape core had dimensions of φ19×φ15×5 mm. f4 (50Hz) and static magnetic flux density deviation Δ13stat and dynamic magnetic flux density deviation ΔBdV, respectively, for the annular tape core.
Hysteresis loops and magnetization curves of n were measured at room temperature for sinusoidal, half-wave rectified and full-wave rectified currents. Furthermore, the static and dynamic magnetic flux density excursions and the temperature dependence of L4 at 50 Hz were measured.
例 1 :
磁界を用いない熱処理が実施された磁心は0.65の残
留磁気比を有していた(丸いヒステリシスループ)。第
1図にはこの磁心のほぼ静的なヒステリシスループが示
されている。Example 1: A magnetic core subjected to a heat treatment without a magnetic field had a remanence ratio of 0.65 (round hysteresis loop). FIG. 1 shows the nearly static hysteresis loop of this core.
第2図は官、ΔBstat、ΔBdyn及び磁界強度間
の関係を示す。丸いヒステリシスループをイIするこの
発明に基づく磁心の磁束密度Bは、既に10mA/cm
の磁界強度の場合に0.5Tの値に達し、従って従来の
技術に基づく漏電遮断器用磁石材料の値を超える。また
この発明に基づく磁心は静的及び動的磁束密度偏移に対
する高い値を右する。第3図a)〜C)にはこの発明に
基づく磁心の磁気特性の温度依存性が示されている。こ
の温度依存性は、−258C〜+80’Cの実際の用途
に対し必要な全温度範囲にわたり変動の小さい非常に高
い不変性を有する。FIG. 2 shows the relationship between ΔBstat, ΔBdyn, and magnetic field strength. The magnetic flux density B of the magnetic core according to the invention with a round hysteresis loop is already 10 mA/cm.
For a magnetic field strength of , a value of 0.5 T is reached, thus exceeding the value of magnet materials for earth leakage circuit breakers according to the prior art. The magnetic core according to the invention also exhibits high values for static and dynamic flux density excursions. FIGS. 3a) to 3c) show the temperature dependence of the magnetic properties of the magnetic core according to the invention. This temperature dependence has very high constancy with small variations over the entire temperature range required for practical applications from -258C to +80'C.
比較のために第4図には従来の技術に基づ〈合金に対す
る磁気特性の温度依存性が示されている。この合金は商
品名ウルトラパームF80(7)もとに漏電遮断器用に
販売されている高ニッケル金石合金である。この合金も
氷点以上の温度に対しては磁石値のまさに良好な不変性
を有する。しかしながら氷点下の温度に対しては大きい
変動を生じる。For comparison, FIG. 4 shows the temperature dependence of magnetic properties for alloys based on the prior art. This alloy is a high nickel goldstone alloy sold for earth leakage circuit breakers under the trade name Ultrapalm F80(7). This alloy also has a very good constancy of the magnetic value to temperatures above the freezing point. However, large fluctuations occur for temperatures below freezing.
例 2 :
横磁界の中で熱処理が実施された磁心では0.1の残留
磁気比が測定された(平らなヒステリシスループ)。こ
の磁心は同様に、第5図a)〜C)に示すような温度変
化の際の磁気特性の良好な不変性を有する。しかし丸い
ヒステリシスループを有する磁心の場合よりこの変動は
大きかった。Example 2: A remanence ratio of 0.1 was measured for a core heat treated in a transverse magnetic field (flat hysteresis loop). This magnetic core likewise has a good constancy of the magnetic properties upon temperature changes, as shown in FIGS. 5a) to 5c). However, this variation was larger than in the case of the magnetic core with round hysteresis loop.
第1VgJはこの発明に基づく磁石材料の一実施例のB
−H曲線を示した図、第2図は第1図と同じ材料のfl
(50Hz)、Δ13stat、ΔBdyn −H特性
をグラフで示した図、第3図a)〜C)は第2図に示す
μa (50H2)、Δ13 s t a t 。
ΔB d、nの温度依存性をグラフで示した図、第4図
は一従来例の第3図と同様な温度依存性をグラフで示し
た図、第5図a)〜C)は別の実施例の第3図a)〜C
)と同様な温度依存性をグラフで示した図である。
繊束免炙ITJ
繊輪LITノ
μ4〜
(l ICXλフノ
20
0
20406080
t rocノ
00The first VgJ is B of an embodiment of the magnet material based on this invention.
-H curve, Figure 2 is the fl of the same material as Figure 1.
(50Hz), Δ13stat, ΔBdyn -H characteristics as a graph, FIG. 3 a) to C) are μa (50H2), Δ13 stat shown in FIG. Figure 4 is a graph showing the temperature dependence of ΔB d, n. Figure 4 is a graph showing the same temperature dependence as Figure 3 for a conventional example. Figure 5 a) to C) is a graph for another example. Figure 3 a) to C of the example
) is a diagram illustrating the same temperature dependence as a graph. Fiber bundle release ITJ Senwa LIT noμ4~ (l ICXλfuno200 20406080 t rocno00
Claims (1)
%以上が100nm未満の粒度の微結晶粒子から成り、
1.1T以上の飽和磁束密度及び0.7未満の残留磁気
比Br/Bsを有する微結晶鉄ベース合金から成ること
を特徴とする漏電遮断器用磁石材料。 2)残留磁気比が0.4以上であることを特徴とする請
求項1記載の磁石材料。 3)動作点での磁束密度偏移の温度依存性変化が、−2
5℃ないし+800℃の温度領域 で室温に対し±10%未満であることを特徴とする請求
項1記載の磁石材料。 4)微結晶粒子が25nm未満の粒度を有することを特
徴とする請求項1記載の磁石材料。[Scope of Claims] 1) Having an iron content of 60 atomic % or more, and having an iron content of 50 atomic % or more,
% or more consists of microcrystalline particles with a particle size of less than 100 nm,
A magnet material for an earth leakage circuit breaker, characterized in that it is made of a microcrystalline iron-based alloy having a saturation magnetic flux density of 1.1 T or more and a remanence ratio Br/Bs of less than 0.7. 2) The magnetic material according to claim 1, having a remanence ratio of 0.4 or more. 3) The temperature-dependent change in magnetic flux density deviation at the operating point is -2
The magnetic material according to claim 1, characterized in that the magnetic material exhibits a temperature difference of less than ±10% with respect to room temperature in a temperature range of 5°C to +800°C. 4) Magnet material according to claim 1, characterized in that the microcrystalline particles have a particle size of less than 25 nm.
Applications Claiming Priority (2)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| DE3911480A DE3911480A1 (en) | 1989-04-08 | 1989-04-08 | USE OF A FINE CRYSTALLINE IRON BASE ALLOY AS A MAGNETIC MATERIAL FOR FAULT CURRENT CIRCUIT BREAKERS |
| DE3911480.5 | 1989-04-08 |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH03201412A true JPH03201412A (en) | 1991-09-03 |
| JP2563097B2 JP2563097B2 (en) | 1996-12-11 |
Family
ID=6378191
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP2091962A Expired - Lifetime JP2563097B2 (en) | 1989-04-08 | 1990-04-06 | Magnetic core material for earth leakage circuit breaker composed of microcrystalline iron-based alloy |
Country Status (5)
| Country | Link |
|---|---|
| EP (1) | EP0392204B1 (en) |
| JP (1) | JP2563097B2 (en) |
| AT (1) | ATE145089T1 (en) |
| DE (2) | DE3911480A1 (en) |
| ES (1) | ES2094125T3 (en) |
Families Citing this family (19)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| DE4210748C1 (en) * | 1992-04-01 | 1993-12-16 | Vacuumschmelze Gmbh | Current transformers for pulse current sensitive residual current circuit breakers, residual current circuit breakers with such a current transformer, and method for heat treatment of the iron alloy strip for its magnetic core |
| ES2091368T3 (en) * | 1992-06-16 | 1996-11-01 | Siemens Ag | WRONG CURRENT PROTECTION SWITCH. |
| ATE149755T1 (en) * | 1993-06-25 | 1997-03-15 | Siemens Ag | LEAD CURRENT DETECTION DEVICE WITH HIGH SENSITIVITY |
| DE4423622A1 (en) * | 1994-07-06 | 1996-01-11 | Vacuumschmelze Gmbh | Total current transformer for electronic protective devices |
| DE59503192D1 (en) * | 1994-09-19 | 1998-09-17 | Siemens Ag | DIFFERENTIAL CURRENT PROTECTION SWITCH WITH SPECIAL CORE MATERIAL |
| FR2733374B1 (en) | 1995-04-18 | 1997-06-06 | Schneider Electric Sa | DIFFERENTIAL PROTECTION DEVICE SENSITIVE TO PULSED CURRENTS |
| DE59707700D1 (en) * | 1996-03-18 | 2002-08-22 | Siemens Ag | Residual current circuit breaker with energy storage circuit |
| DE19702371A1 (en) * | 1997-01-23 | 1998-07-30 | Siemens Ag | Residual current device |
| FR2772182B1 (en) * | 1997-12-04 | 2000-01-14 | Mecagis | METHOD FOR MANUFACTURING A NANOCRYSTALLINE SOFT MAGNETIC ALLOY MAGNETIC CORE AND USE IN AN AC CLASS DIFFERENTIAL CIRCUIT BREAKER |
| FR2772181B1 (en) * | 1997-12-04 | 2000-01-14 | Mecagis | METHOD FOR MANUFACTURING A NANOCRYSTALLINE SOFT MAGNETIC ALLOY MAGNETIC CORE FOR USE IN A CLASS A DIFFERENTIAL CIRCUIT BREAKER AND MAGNETIC CORE OBTAINED |
| EP1154539A1 (en) * | 2000-05-10 | 2001-11-14 | Siemens Aktiengesellschaft | Fault current breaker with summation transformer |
| DE10134056B8 (en) | 2001-07-13 | 2014-05-28 | Vacuumschmelze Gmbh & Co. Kg | Process for the production of nanocrystalline magnetic cores and apparatus for carrying out the process |
| ATE401655T1 (en) * | 2005-02-25 | 2008-08-15 | Magnetec Gmbh | RESIDUAL CURRENT SWITCH AND MAGNETIC CORE FOR A RESIDUAL CURRENT SWITCH |
| DE102007034532A1 (en) | 2007-07-24 | 2009-02-05 | Vacuumschmelze Gmbh & Co. Kg | Magnetic core, process for its production and residual current circuit breaker |
| EP2416329B1 (en) | 2010-08-06 | 2016-04-06 | Vaccumschmelze Gmbh & Co. KG | Magnetic core for low-frequency applications and manufacturing process of a magnetic core for low-frequency applications |
| DE102010060740A1 (en) * | 2010-11-23 | 2012-05-24 | Vacuumschmelze Gmbh & Co. Kg | Soft magnetic metal strip for electromechanical components |
| US8699190B2 (en) | 2010-11-23 | 2014-04-15 | Vacuumschmelze Gmbh & Co. Kg | Soft magnetic metal strip for electromechanical components |
| JP5886024B2 (en) * | 2011-12-19 | 2016-03-16 | 株式会社東芝 | Magnetic resonance imaging system |
| DE102015211487B4 (en) | 2015-06-22 | 2018-09-20 | Vacuumschmelze Gmbh & Co. Kg | METHOD FOR PRODUCING A NANOCRYSTALLINE MAGNETIC CORE |
Citations (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS6439347A (en) * | 1987-08-06 | 1989-02-09 | Hitachi Metals Ltd | Fe-based soft magnetic alloy |
Family Cites Families (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CA1341105C (en) * | 1987-07-14 | 2000-10-03 | Yoshihito Yoshizawa | Magnetic core made of fe-base soft magnetic alloy and use thereof |
| JPH0680611B2 (en) * | 1987-10-23 | 1994-10-12 | 日立金属株式会社 | Magnetic core |
-
1989
- 1989-04-08 DE DE3911480A patent/DE3911480A1/en not_active Withdrawn
-
1990
- 1990-03-14 EP EP90104798A patent/EP0392204B1/en not_active Expired - Lifetime
- 1990-03-14 ES ES90104798T patent/ES2094125T3/en not_active Expired - Lifetime
- 1990-03-14 DE DE59010553T patent/DE59010553D1/en not_active Expired - Lifetime
- 1990-03-14 AT AT90104798T patent/ATE145089T1/en not_active IP Right Cessation
- 1990-04-06 JP JP2091962A patent/JP2563097B2/en not_active Expired - Lifetime
Patent Citations (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS6439347A (en) * | 1987-08-06 | 1989-02-09 | Hitachi Metals Ltd | Fe-based soft magnetic alloy |
Also Published As
| Publication number | Publication date |
|---|---|
| DE3911480A1 (en) | 1990-10-11 |
| ATE145089T1 (en) | 1996-11-15 |
| JP2563097B2 (en) | 1996-12-11 |
| EP0392204A3 (en) | 1992-04-08 |
| ES2094125T3 (en) | 1997-01-16 |
| EP0392204B1 (en) | 1996-11-06 |
| EP0392204A2 (en) | 1990-10-17 |
| DE59010553D1 (en) | 1996-12-12 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| JP2563097B2 (en) | Magnetic core material for earth leakage circuit breaker composed of microcrystalline iron-based alloy | |
| US4038073A (en) | Near-zero magnetostrictive glassy metal alloys with high saturation induction | |
| KR910003977B1 (en) | Fe-base soft magnetic alloy and method of producing same | |
| US4150981A (en) | Glassy alloys containing cobalt, nickel and iron having near-zero magnetostriction and high saturation induction | |
| CA1200407A (en) | Magnetic devices using amorphous alloys | |
| JP2007299838A (en) | Magnetic core for current transformer, current transformer using same, and electric power meter | |
| JPS5934781B2 (en) | Method for reducing magnetic hysteresis loss of soft magnetic amorphous alloy ribbon material | |
| Ido et al. | Magnetic properties of LaCo13‐based systems | |
| US4834816A (en) | Metallic glasses having a combination of high permeability, low coercivity, low ac core loss, low exciting power and high thermal stability | |
| JP2002541331A (en) | Magnetic glassy alloys for high frequency applications | |
| Williams et al. | Magnetic order in crystallographically ordered Pt4-y (MnxCr1-x) y alloys | |
| Fujii et al. | Effect of substitution of Zr on the magnetic properties of R2Co17 (R= Ce and Sm) | |
| JPH0338334B2 (en) | ||
| JPH01247557A (en) | Manufacture of hyperfine-crystal soft-magnetic alloy | |
| JP4843620B2 (en) | Iron-based high saturation magnetic induction amorphous alloy | |
| Hara et al. | Magnetic properties of Mn1− xNixAl | |
| JPS62179704A (en) | Fe-based amorphous core excellent in controlling magnetization characteristics | |
| Yu et al. | Temperature dependence of the magnetization of nanocrystalline Fe/sub 68.5/Co/sub 5/Nb/sub 3/CuSi/sub 13.5/B/sub 9/alloy | |
| Guo et al. | Structure, magnetic properties, and magnetostriction of Sm 0.88 Dy 0.12 (Fe 1− x M x) 2 (M= Mn, Al)(0⩽ x⩽ 0.2) | |
| JPH03271346A (en) | Soft magnetic alloy | |
| JPS6019125B2 (en) | Wound core material | |
| Thongmee et al. | Nanocrystalline Formation in Amorphous Fe 79 B 16 Si 5 and Fe 78 B 13 Si 9 Ribbons | |
| JPS6012423B2 (en) | Manufacturing method of low coercive force and high angularity amorphous alloy | |
| Wang et al. | Structure and magnetic properties of R2Fe17− xMnx compounds (R= Tb, Y) | |
| JPS5943838A (en) | Amorphous magnetic alloy |
Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| R250 | Receipt of annual fees |
Free format text: JAPANESE INTERMEDIATE CODE: R250 |
|
| R250 | Receipt of annual fees |
Free format text: JAPANESE INTERMEDIATE CODE: R250 |
|
| R250 | Receipt of annual fees |
Free format text: JAPANESE INTERMEDIATE CODE: R250 |
|
| FPAY | Renewal fee payment (event date is renewal date of database) |
Free format text: PAYMENT UNTIL: 20070919 Year of fee payment: 11 |
|
| FPAY | Renewal fee payment (event date is renewal date of database) |
Free format text: PAYMENT UNTIL: 20080919 Year of fee payment: 12 |
|
| FPAY | Renewal fee payment (event date is renewal date of database) |
Free format text: PAYMENT UNTIL: 20090919 Year of fee payment: 13 |
|
| FPAY | Renewal fee payment (event date is renewal date of database) |
Free format text: PAYMENT UNTIL: 20100919 Year of fee payment: 14 |
|
| EXPY | Cancellation because of completion of term | ||
| FPAY | Renewal fee payment (event date is renewal date of database) |
Free format text: PAYMENT UNTIL: 20100919 Year of fee payment: 14 |