EP0921540A1 - Fabrication process of a magnetic core of a soft magnetic nanocrystalline alloy and use in a differential circuit breaker - Google Patents
Fabrication process of a magnetic core of a soft magnetic nanocrystalline alloy and use in a differential circuit breaker Download PDFInfo
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- EP0921540A1 EP0921540A1 EP98402803A EP98402803A EP0921540A1 EP 0921540 A1 EP0921540 A1 EP 0921540A1 EP 98402803 A EP98402803 A EP 98402803A EP 98402803 A EP98402803 A EP 98402803A EP 0921540 A1 EP0921540 A1 EP 0921540A1
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- magnetic
- alloy
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- heat treatment
- magnetic core
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- 238000004519 manufacturing process Methods 0.000 title claims abstract description 13
- 229910045601 alloy Inorganic materials 0.000 title claims description 17
- 239000000956 alloy Substances 0.000 title claims description 17
- 238000000034 method Methods 0.000 title claims description 12
- 230000035699 permeability Effects 0.000 claims abstract description 21
- 238000010438 heat treatment Methods 0.000 claims abstract description 19
- 238000002425 crystallisation Methods 0.000 claims abstract description 16
- 230000008025 crystallization Effects 0.000 claims abstract description 16
- 229910052796 boron Inorganic materials 0.000 claims abstract description 11
- 229910052710 silicon Inorganic materials 0.000 claims abstract description 11
- 229910001004 magnetic alloy Inorganic materials 0.000 claims abstract description 10
- 229910052758 niobium Inorganic materials 0.000 claims abstract description 10
- 229910052735 hafnium Inorganic materials 0.000 claims abstract description 8
- 229910052720 vanadium Inorganic materials 0.000 claims abstract description 8
- 229910052726 zirconium Inorganic materials 0.000 claims abstract description 8
- 229910052804 chromium Inorganic materials 0.000 claims abstract description 7
- 229910052802 copper Inorganic materials 0.000 claims abstract description 7
- 229910052750 molybdenum Inorganic materials 0.000 claims abstract description 7
- 229910052715 tantalum Inorganic materials 0.000 claims abstract description 7
- 229910052719 titanium Inorganic materials 0.000 claims abstract description 7
- 229910052721 tungsten Inorganic materials 0.000 claims abstract description 7
- 229910052742 iron Inorganic materials 0.000 claims abstract description 6
- 229910052748 manganese Inorganic materials 0.000 claims abstract description 5
- 238000011282 treatment Methods 0.000 claims description 12
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical compound [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 claims description 11
- 239000010955 niobium Substances 0.000 claims description 10
- 239000010703 silicon Substances 0.000 claims description 10
- ZOXJGFHDIHLPTG-UHFFFAOYSA-N Boron Chemical compound [B] ZOXJGFHDIHLPTG-UHFFFAOYSA-N 0.000 claims description 9
- GUCVJGMIXFAOAE-UHFFFAOYSA-N niobium atom Chemical compound [Nb] GUCVJGMIXFAOAE-UHFFFAOYSA-N 0.000 claims description 9
- VYZAMTAEIAYCRO-UHFFFAOYSA-N Chromium Chemical compound [Cr] VYZAMTAEIAYCRO-UHFFFAOYSA-N 0.000 claims description 7
- RYGMFSIKBFXOCR-UHFFFAOYSA-N Copper Chemical compound [Cu] RYGMFSIKBFXOCR-UHFFFAOYSA-N 0.000 claims description 7
- ZOKXTWBITQBERF-UHFFFAOYSA-N Molybdenum Chemical compound [Mo] ZOKXTWBITQBERF-UHFFFAOYSA-N 0.000 claims description 7
- RTAQQCXQSZGOHL-UHFFFAOYSA-N Titanium Chemical compound [Ti] RTAQQCXQSZGOHL-UHFFFAOYSA-N 0.000 claims description 7
- QCWXUUIWCKQGHC-UHFFFAOYSA-N Zirconium Chemical compound [Zr] QCWXUUIWCKQGHC-UHFFFAOYSA-N 0.000 claims description 7
- 239000010949 copper Substances 0.000 claims description 7
- VBJZVLUMGGDVMO-UHFFFAOYSA-N hafnium atom Chemical compound [Hf] VBJZVLUMGGDVMO-UHFFFAOYSA-N 0.000 claims description 7
- GUVRBAGPIYLISA-UHFFFAOYSA-N tantalum atom Chemical compound [Ta] GUVRBAGPIYLISA-UHFFFAOYSA-N 0.000 claims description 7
- LEONUFNNVUYDNQ-UHFFFAOYSA-N vanadium atom Chemical compound [V] LEONUFNNVUYDNQ-UHFFFAOYSA-N 0.000 claims description 7
- 239000011651 chromium Substances 0.000 claims description 6
- 239000011733 molybdenum Substances 0.000 claims description 6
- 239000010936 titanium Substances 0.000 claims description 6
- WFKWXMTUELFFGS-UHFFFAOYSA-N tungsten Chemical compound [W] WFKWXMTUELFFGS-UHFFFAOYSA-N 0.000 claims description 6
- 239000010937 tungsten Substances 0.000 claims description 6
- PWHULOQIROXLJO-UHFFFAOYSA-N Manganese Chemical compound [Mn] PWHULOQIROXLJO-UHFFFAOYSA-N 0.000 claims description 5
- 239000011572 manganese Substances 0.000 claims description 4
- 239000000203 mixture Substances 0.000 claims description 4
- 239000000126 substance Substances 0.000 claims description 4
- 239000012535 impurity Substances 0.000 claims description 2
- WPBNNNQJVZRUHP-UHFFFAOYSA-L manganese(2+);methyl n-[[2-(methoxycarbonylcarbamothioylamino)phenyl]carbamothioyl]carbamate;n-[2-(sulfidocarbothioylamino)ethyl]carbamodithioate Chemical compound [Mn+2].[S-]C(=S)NCCNC([S-])=S.COC(=O)NC(=S)NC1=CC=CC=C1NC(=S)NC(=O)OC WPBNNNQJVZRUHP-UHFFFAOYSA-L 0.000 claims description 2
- 229910000808 amorphous metal alloy Inorganic materials 0.000 abstract 2
- 229910000521 B alloy Inorganic materials 0.000 abstract 1
- NFCWKPUNMWPHLM-UHFFFAOYSA-N [Si].[B].[Fe] Chemical compound [Si].[B].[Fe] NFCWKPUNMWPHLM-UHFFFAOYSA-N 0.000 abstract 1
- XUIMIQQOPSSXEZ-UHFFFAOYSA-N Silicon Chemical compound [Si] XUIMIQQOPSSXEZ-UHFFFAOYSA-N 0.000 description 8
- 238000000137 annealing Methods 0.000 description 4
- 230000035945 sensitivity Effects 0.000 description 4
- 229910001030 Iron–nickel alloy Inorganic materials 0.000 description 2
- 230000005284 excitation Effects 0.000 description 2
- 230000015572 biosynthetic process Effects 0.000 description 1
- 238000005266 casting Methods 0.000 description 1
- 239000013078 crystal Substances 0.000 description 1
- 239000006185 dispersion Substances 0.000 description 1
- 238000012423 maintenance Methods 0.000 description 1
- 238000010791 quenching Methods 0.000 description 1
- 230000000171 quenching effect Effects 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
- H01F1/15341—Preparation processes therefor
-
- 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
- H01F1/15333—Amorphous metallic alloys, e.g. glassy metals containing nanocrystallites, e.g. obtained by annealing
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F41/00—Apparatus or processes specially adapted for manufacturing or assembling magnets, inductances or transformers; Apparatus or processes specially adapted for manufacturing materials characterised by their magnetic properties
- H01F41/02—Apparatus or processes specially adapted for manufacturing or assembling magnets, inductances or transformers; Apparatus or processes specially adapted for manufacturing materials characterised by their magnetic properties for manufacturing cores, coils, or magnets
- H01F41/0206—Manufacturing of magnetic cores by mechanical means
- H01F41/0213—Manufacturing of magnetic circuits made from strip(s) or ribbon(s)
- H01F41/0226—Manufacturing of magnetic circuits made from strip(s) or ribbon(s) from amorphous ribbons
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- 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
Definitions
- the present invention relates to a magnetic core of magnetic alloy soft nanocrystalline usable, in particular, for the manufacture of a circuit breaker AC class differential.
- Class AC circuit breakers are circuit breakers differentials sensitive to sinusoidal fault currents. They include in particular a soft magnetic alloy magnetic core for which seeks both high ⁇ magnetic permeability and very good stability in temperature of this magnetic permeability. Magnetic core size given, the sensitivity of the RCD is all the better as the magnetic permeability is high; this permeability must be stable in the range operating temperature of the earth leakage circuit breaker (generally - 25 ° C at + 100 ° C) so as to obtain good operational safety.
- the magnetic cores for RCD class AC circuit breakers are made of a soft magnetic alloy of the Fe-Ni 20-80 type, stabilized by annealing. This technique has the disadvantage of not making it possible to reliably obtain maximum magnetic permeabilities of impedance ⁇ z substantially greater than 300,000, which limits the possibilities of reducing the size of the magnetic cores, and therefore, the size of earth leakage circuit breakers.
- Nanocrystalline soft magnetic alloys of the type comprising more than 60 atoms% of iron, copper, silicon, boron and an element chosen from titanium, niobium, zirconium, hafnium, vanadium, tantalum, chromium, molybdenum, tungsten and manganese have the advantage of making it possible to obtain maximum magnetic permeabilities of impedance ⁇ z greater than 300,000, which would make it possible to manufacture magnetic cores for differential circuit breakers of class AC of substantially reduced size .
- These magnetic cores are obtained by casting the alloy in the form of an amorphous ribbon, which is wound to form a torus, then subjected to a thermal crystallization treatment intended to give the alloy a nanocrystalline structure.
- magnetic cores of this type have insufficient temperature stability: at 100 ° C, the magnetic permeability is more than 40% lower than the magnetic permeability at 25 ° C; they cannot therefore be used for the manufacture of miniaturized residual current devices.
- the object of the present invention is to remedy this drawback by proposing a means for manufacturing a magnetic core usable in a Class AC circuit breaker with reduced dimensions.
- the subject of the invention is a process for the manufacture of a magnetic core made of nanocrystalline soft magnetic alloy whose chemical composition comprises more than 60 atoms% of iron, from 10 to 20 atoms% of silicon, from 0, 1 to 2 atom% of copper, 5 to 20 atom% of boron, 0.1 to 10 atom% of at least one element chosen from titanium, niobium, zirconium, hafnium, vanadium, tantalum , chromium, molybdenum, tungsten and manganese, as well as impurities resulting from the production; the sum of the silicon and boron contents being less than 30 atom%; the nanocrystalline alloy being obtained by a heat treatment of crystallization of the alloy in the amorphous state; the magnetic core having a maximum magnetic permeability of impedance ⁇ z at 50 Hertz, at 25 ° C, greater than 350,000, this maximum magnetic permeability of impedance ⁇ z varying by less than 25% over the temperature range between - 25
- the heat treatment under transverse magnetic field is carried out at a temperature between 200 ° C and 350 ° C.
- the chemical composition of the magnetic alloy soft nanocrystalline contains from 10 to 17 atoms% of silicon, from 0.5 to 1.5 atoms % copper, 5 to 14 atoms% boron and 2 to 4% of at least one element taken among titanium, niobium, zirconium, hafnium, vanadium, tantalum, chromium, molybdenum, tungsten and manganese.
- thermal relaxation treatment can consist of maintaining at a temperature between 250 ° C and 480 ° C for a time between 0.1 and 10 hours.
- the magnetic core obtained by this process can advantageously be used for the manufacture of a class-current differential circuit breaker AC.
- the sum of the silicon and boron contents should preferably remain less than 30 at% and, better still, remain less than 25 at%.
- the crystallization annealing consists of maintaining at a temperature higher than the start of crystallization temperature and lower than the temperature from the onset of secondary phases which deteriorate the properties magnetic.
- the crystallization annealing temperature is understood between 500 ° C and 600 ° C, but it can be optimized for each ribbon, by example, by determining by tests the temperature which leads to permeability maximum magnetic.
- the heat treatment carried out under magnetic field is carried out at a temperature between 150 ° C and 400 ° C, and preferably between 200 ° C and 300 ° C.
- the magnetic field is applied in the form of a succession of slots.
- One slot corresponds to one period during which the applied magnetic field is maximum, followed by a period during which it is zero or very weak (less than 10% of the magnetic field reached during treatment).
- the applied magnetic field can be continuous or alternating, in the latter case the intensity of the magnetic field is peak intensity (maximum intensity reached at each alternation).
- the intensity of magnetic field can be constant throughout the period of application of the field (rectangular slots) or variable. All slots can be from same intensity or on the contrary of variable intensity from one niche to another.
- the heat treatment can end at the end of the field application period magnetic of the last slot; the main thing is that the treatment involves minus two periods during which the magnetic field is applied separated by a period during which the magnetic field is not applied.
- the inventors have in fact found that by doing so, the stability in temperature the magnetic properties of the magnetic core were very significantly improved.
- a magnetic core whose maximum magnetic permeability of impedance ⁇ z at 50 Hertz, for an alternating magnetic excitation field of 8 mA / cm (peak value), at 25 ° C is greater than 350,000 , or even 400,000, this magnetic permeability varying by less than 25% between - 25 ° C and + 100 ° C.
- Such a magnetic core can be used in a class AC circuit breaker. Due to its high magnetic permeability, at equal sensitivity of the circuit breaker, the section of the core can be significantly reduced compared to the section of a magnetic core made of Fe-Ni alloy according to the prior art.
- the treatment temperature was 200 ° C
- the treatment temperature was 300 ° C.
- the maximum magnetic permeability of impedance ⁇ z measured at 50 Hz in a maximum excitation field of 8 mA / cm (peak value) at 25 ° C, at - 25 ° C , at + 80 ° C and at + 100 ° C, the ratio ⁇ / ⁇ representing the variations of ⁇ z with respect to its value at 25 ° C.
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- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Chemical & Material Sciences (AREA)
- Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Dispersion Chemistry (AREA)
- Manufacturing & Machinery (AREA)
- Crystallography & Structural Chemistry (AREA)
- Inorganic Chemistry (AREA)
- Materials Engineering (AREA)
- Soft Magnetic Materials (AREA)
Abstract
Description
La présente invention concerne un noyau magnétique en alliage magnétique doux nanocristallin utilisable, notamment, pour la fabrication d'un disjoncteur différentiel de la classe AC.The present invention relates to a magnetic core of magnetic alloy soft nanocrystalline usable, in particular, for the manufacture of a circuit breaker AC class differential.
Les disjoncteurs différentiels de la classe AC sont des disjoncteurs différentiels sensibles à des courants de défaut sinusoïdaux. Ils comportent notamment un noyau magnétique en alliage magnétique doux pour lequel on recherche à la fois une perméabilité magnétique µ élevée et une très bonne stabilité en température de cette perméabilité magnétique. A taille de noyau magnétique donnée, la sensibilité du disjoncteur différentiel est d'autant meilleure que la perméabilité magnétique est élevée ; cette perméabilité doit être stable dans la plage de température de fonctionnement du disjoncteur différentiel (en général de - 25 °C à + 100 °C) de façon a obtenir une bonne sûreté de fonctionnement.Class AC circuit breakers are circuit breakers differentials sensitive to sinusoidal fault currents. They include in particular a soft magnetic alloy magnetic core for which seeks both high µ magnetic permeability and very good stability in temperature of this magnetic permeability. Magnetic core size given, the sensitivity of the RCD is all the better as the magnetic permeability is high; this permeability must be stable in the range operating temperature of the earth leakage circuit breaker (generally - 25 ° C at + 100 ° C) so as to obtain good operational safety.
Les noyau magnétiques pour disjoncteurs différentiels de la classe AC sont fabriqués en alliage magnétique doux du type Fe-Ni 20-80, stabilisé par un recuit. Cette technique présente l'inconvénient de ne pas permettre d'obtenir de façon fiable des perméabilités magnétiques maximales d'impédance µz sensiblement supérieures à 300 000, ce qui limite les possibilités de réduction de la dimension des noyaux magnétiques, et donc, de la dimension des disjoncteurs différentiels.The magnetic cores for RCD class AC circuit breakers are made of a soft magnetic alloy of the Fe-Ni 20-80 type, stabilized by annealing. This technique has the disadvantage of not making it possible to reliably obtain maximum magnetic permeabilities of impedance μ z substantially greater than 300,000, which limits the possibilities of reducing the size of the magnetic cores, and therefore, the size of earth leakage circuit breakers.
Les alliages magnétiques doux nanocristallins du type comprenant plus de 60 atomes % de fer, du cuivre, du silicium, du bore et un élément pris parmi le titane, le niobium, le zirconium, le hafnium, le vanadium, le tantale, le chrome, le molybdène, le tungstène et le manganèse ont l'avantage de permettre d'obtenir des perméabilités magnétiques maximales d'impédance µz supérieures à 300 000, ce qui permettrait de fabriquer des noyaux magnétiques pour disjoncteurs différentiels de la classe AC de dimension sensiblement réduite. Ces noyaux magnétiques sont obtenus en coulant l'alliage sous forme d'un ruban amorphe, qui est enroulé pour former un tore, puis soumis à un traitement thermique de cristallisation destiné à conférer à l'alliage une structure nanocristalline. Mais, les noyaux magnétiques de ce type ont une stabilité en température insuffisante : à 100 °C, la perméabilité magnétique est inférieure de plus de 40 % à la perméabilité magnétique à 25 °C ; ils ne peuvent donc pas être utilisés pour la fabrication de disjoncteurs différentiels miniaturisés.Nanocrystalline soft magnetic alloys of the type comprising more than 60 atoms% of iron, copper, silicon, boron and an element chosen from titanium, niobium, zirconium, hafnium, vanadium, tantalum, chromium, molybdenum, tungsten and manganese have the advantage of making it possible to obtain maximum magnetic permeabilities of impedance μ z greater than 300,000, which would make it possible to manufacture magnetic cores for differential circuit breakers of class AC of substantially reduced size . These magnetic cores are obtained by casting the alloy in the form of an amorphous ribbon, which is wound to form a torus, then subjected to a thermal crystallization treatment intended to give the alloy a nanocrystalline structure. However, magnetic cores of this type have insufficient temperature stability: at 100 ° C, the magnetic permeability is more than 40% lower than the magnetic permeability at 25 ° C; they cannot therefore be used for the manufacture of miniaturized residual current devices.
Le but de la présente invention est de remédier à cet inconvénient en proposant un moyen pour fabriquer un noyau magnétique utilisable dans un disjoncteur différentiel de la classe AC de dimensions réduites.The object of the present invention is to remedy this drawback by proposing a means for manufacturing a magnetic core usable in a Class AC circuit breaker with reduced dimensions.
A cet effet, l'invention a pour objet un procédé pour la fabrication d'un noyau magnétique en alliage magnétique doux nanocristallin dont la composition chimique comprend plus de 60 atomes % de fer, de 10 à 20 atomes % de silicium, de 0,1 à 2 atomes % de cuivre, de 5 à 20 atomes % de bore, de 0,1 à 10 atomes % d'au moins un élément pris parmi le titane, le niobium, le zirconium, le hafnium, le vanadium, le tantale, le chrome, le molybdène, le tungstène et le manganèse, ainsi que des impuretés résultant de l'élaboration; la somme des teneurs en silicium et en bore étant inférieure à 30 atomes %; l'alliage nanocristallin étant obtenu par un traitement thermique de cristallisation de l'alliage à l'état amorphe; le noyau magnétique ayant une perméabilité magnétique maximale d'impédance µz à 50 Hertz, à 25 °C, supérieure à 350 000, cette perméabilité magnétique maximale d'impédance µz variant de moins de 25 % sur la plage de température comprise entre - 25 °C et + 100 °C. Selon ce procédé, on effectue sur le noyau magnétique un traitement thermique sous champ magnétique transverse à une température comprise entre 150 °C et 400 °C, le champ magnétique étant appliqué sous forme de créneaux.To this end, the subject of the invention is a process for the manufacture of a magnetic core made of nanocrystalline soft magnetic alloy whose chemical composition comprises more than 60 atoms% of iron, from 10 to 20 atoms% of silicon, from 0, 1 to 2 atom% of copper, 5 to 20 atom% of boron, 0.1 to 10 atom% of at least one element chosen from titanium, niobium, zirconium, hafnium, vanadium, tantalum , chromium, molybdenum, tungsten and manganese, as well as impurities resulting from the production; the sum of the silicon and boron contents being less than 30 atom%; the nanocrystalline alloy being obtained by a heat treatment of crystallization of the alloy in the amorphous state; the magnetic core having a maximum magnetic permeability of impedance µ z at 50 Hertz, at 25 ° C, greater than 350,000, this maximum magnetic permeability of impedance µ z varying by less than 25% over the temperature range between - 25 ° C and + 100 ° C. According to this method, heat treatment is carried out on the magnetic core under a transverse magnetic field at a temperature between 150 ° C and 400 ° C, the magnetic field being applied in the form of slots.
De préférence, le traitement thermique sous champ magnétique transverse est effectué à une température comprise entre 200 °C et 350 °C.Preferably, the heat treatment under transverse magnetic field is carried out at a temperature between 200 ° C and 350 ° C.
De préférence également, la composition chimique de l'alliage magnétique doux nanocristallin comprend de 10 à 17 atomes % de silicium, de 0,5 à 1,5 atomes % de cuivre, de 5 à 14 atomes % de bore et de 2 à 4 % d'au moins un élément pris parmi le titane, le niobium, le zirconium, le hafnium, le vanadium, le tantale, le chrome, le molybdène, le tungstène et le manganèse.Also preferably, the chemical composition of the magnetic alloy soft nanocrystalline contains from 10 to 17 atoms% of silicon, from 0.5 to 1.5 atoms % copper, 5 to 14 atoms% boron and 2 to 4% of at least one element taken among titanium, niobium, zirconium, hafnium, vanadium, tantalum, chromium, molybdenum, tungsten and manganese.
Avant d'effectuer le traitement thermique de cristallisation de l'alliage à l'état amorphe, on peut effectuer sur l'alliage à l'état amorphe un traitement thermique de relaxation à une température inférieure à la température de début de cristallisation de l'alliage à l'état amorphe. Par exemple, le traitement thermique de relaxation peut consister en un maintien à une température comprise entre 250 °C et 480 °C pendant un temps compris entre 0,1 et 10 heures.Before carrying out the heat treatment of crystallization of the alloy in the state amorphous, one can carry out on the alloy in the amorphous state a heat treatment of relaxation at a temperature below the temperature at the start of crystallization of the alloy in the amorphous state. For example, thermal relaxation treatment can consist of maintaining at a temperature between 250 ° C and 480 ° C for a time between 0.1 and 10 hours.
Le noyau magnétique obtenu par ce procédé peut, avantageusement, être utilisé pour la fabrication d'un disjoncteur différentiel à propre courant de la classe AC.The magnetic core obtained by this process can advantageously be used for the manufacture of a class-current differential circuit breaker AC.
L'invention va maintenant être décrite de façon plus précise, mais non limitative, et illustrée par des exemples.The invention will now be described in more detail, but not limiting, and illustrated by examples.
Pour fabriquer un noyau magnétique en alliage magnétique doux nanocristallin, on coule l'alliage sous forme d'un ruban amorphe, puis on enroule un segment de ruban de longueur appropriée autour d'un mandrin de façon à former une bobine torique de section rectangulaire ou carrée. La bobine qui va constituer le noyau magnétique est alors soumise à un traitement thermique de cristallisation destiné à déstabiliser la structure amorphe et à provoquer la formation de cristaux dont la taille est inférieure à 100 nanomètres, voire inférieure à 20 nanomètres, et, ainsi, obtenir une structure appelée « nanocristalline ». Ce traitement est, ensuite, complété par un traitement thermique sous champ magnétique transverse, c'est à dire, sous un champ magnétique parallèle à l'axe du noyau. L'alliage est du type décrit notamment dans les demandes de brevet européen EP 0 271 657 et EP 0 299 498. Il est constitué principalement de fer en une teneur supérieure à 60 atomes %, et contient en outre :
- de 0,1 à 2 at %, et de préférence, de 0,5 à 1,5 at % de cuivre ;
- de 10 à 20 at %, et de préférence, moins de 17 at % de silicium ;
- de 5 à 20 at %, et de préférence, moins de 14 at % de bore ;
- de 0,1 à 10 at % d'au moins un élément pris parmi le titane, le niobium, le zirconium, le hafnium, le vanadium, le tantale, le chrome, le molybdène, le tungstène et le manganèse ; de préférence de 2 et 4 at % de niobium .
- 0.1 to 2 at%, and preferably 0.5 to 1.5 at% copper;
- from 10 to 20 at%, and preferably, less than 17 at% of silicon;
- from 5 to 20 at%, and preferably less than 14 at% boron;
- from 0.1 to 10 at% of at least one element taken from titanium, niobium, zirconium, hafnium, vanadium, tantalum, chromium, molybdenum, tungsten and manganese; preferably 2 and 4 at% niobium.
La somme des teneurs en silicium et en bore doit, de préférence, rester inférieure à 30 at % et, mieux encore, rester inférieure à 25 at %.The sum of the silicon and boron contents should preferably remain less than 30 at% and, better still, remain less than 25 at%.
Le recuit de cristallisation consiste en un maintien à une température supérieure à la température de début de cristallisation et inférieure à la température de début d'apparition des phases secondaires qui détériorent les propriétés magnétiques. En général, la température de recuit de cristallisation est comprises entre 500 °C et 600 °C, mais elle peut être optimisée pour chaque ruban, par exemple, en déterminant par des essais la température qui conduit à la perméabilité magnétique maximale.The crystallization annealing consists of maintaining at a temperature higher than the start of crystallization temperature and lower than the temperature from the onset of secondary phases which deteriorate the properties magnetic. In general, the crystallization annealing temperature is understood between 500 ° C and 600 ° C, but it can be optimized for each ribbon, by example, by determining by tests the temperature which leads to permeability maximum magnetic.
Le traitement thermique effectué sous champ magnétique est effectué à une température comprise entre 150 °C et 400 °C, et de préférence entre 200 °C et 300 °C. Pendant le maintien en température, le champ magnétique est appliqué sous forme d'une succession de créneaux. Un créneau correspond à une période pendant laquelle le champ magnétique appliqué est maximal, suivi d'une période pendant la quelle il est nul ou très faible (inférieur à 10 % du champ magnétique maximal atteint pendant le traitement). Le champ magnétique appliqué peut être continu ou alternatif, dans ce dernier cas, l'intensité du champ magnétique est l'intensité de crête (intensité maximale atteinte à chaque alternance). L'intensité du champ magnétique peut être constante pendant toute la période d'application du champ (créneaux rectangulaires) ou variable. Tous les créneaux peuvent être de même intensité ou au contraire d'intensité variable d'un créneau à l'autre. Le traitement thermique peut se terminer à la fin de la période d'application du champ magnétique du dernier créneau ; l'essentiel étant que le traitement comporte au moins deux périodes pendant lesquelles le champ magnétique est appliqué séparées par une période pendant laquelle le champ magnétique n'est pas appliqué. Les inventeurs ont, en effet, constaté qu'en procédant ainsi, la stabilité en température des propriétés magnétiques du noyau magnétique étaient très sensiblement améliorées.The heat treatment carried out under magnetic field is carried out at a temperature between 150 ° C and 400 ° C, and preferably between 200 ° C and 300 ° C. During temperature maintenance, the magnetic field is applied in the form of a succession of slots. One slot corresponds to one period during which the applied magnetic field is maximum, followed by a period during which it is zero or very weak (less than 10% of the magnetic field reached during treatment). The applied magnetic field can be continuous or alternating, in the latter case the intensity of the magnetic field is peak intensity (maximum intensity reached at each alternation). The intensity of magnetic field can be constant throughout the period of application of the field (rectangular slots) or variable. All slots can be from same intensity or on the contrary of variable intensity from one niche to another. The heat treatment can end at the end of the field application period magnetic of the last slot; the main thing is that the treatment involves minus two periods during which the magnetic field is applied separated by a period during which the magnetic field is not applied. The inventors have in fact found that by doing so, the stability in temperature the magnetic properties of the magnetic core were very significantly improved.
Par ce procédé on obtient un noyau magnétique dont la perméabilité magnétique maximale d'impédance µz à 50 Hertz, pour un champ magnétique d'excitation alternatif de 8 mA/cm (valeur de crête), à 25 °C est supérieur à 350 000, voire 400 000, cette perméabilité magnétique variant de moins de 25 % entre - 25 °C et + 100 °C. Un tel noyau magnétique peut être utilisé dans un disjoncteur différentiel de la classe AC. Du fait de sa forte perméabilité magnétique, à sensibilité égale du disjoncteur, la section du noyau peut être sensiblement réduite par rapport à la section d'un noyau magnétique en alliage Fe-Ni selon l'art antérieur.By this process we obtain a magnetic core whose maximum magnetic permeability of impedance µ z at 50 Hertz, for an alternating magnetic excitation field of 8 mA / cm (peak value), at 25 ° C is greater than 350,000 , or even 400,000, this magnetic permeability varying by less than 25% between - 25 ° C and + 100 ° C. Such a magnetic core can be used in a class AC circuit breaker. Due to its high magnetic permeability, at equal sensitivity of the circuit breaker, the section of the core can be significantly reduced compared to the section of a magnetic core made of Fe-Ni alloy according to the prior art.
En complément des traitements thermiques qui viennent d'être décrit, on peut, avant le traitement thermique de cristallisation, effectuer sur le noyau un traitement thermique de relaxation à une température inférieure à la température de début de cristallisation de la bande amorphe, et, de préférence, comprise entre 250°C et 480 °C. Ce recuit de relaxation a pour avantage de réduire encore la sensibilité des propriétés magnétiques des noyaux à la température, de réduire la dispersion des propriétés magnétiques de noyaux fabriqués en série et de réduire la sensibilité des propriétés magnétiques aux contraintes.In addition to the heat treatments which have just been described, it is possible, before the crystallization heat treatment, carry out a treatment on the core thermal relaxation at a temperature below the start temperature of crystallization of the amorphous band, and preferably between 250 ° C and 480 ° C. This relaxation annealing has the advantage of further reducing the sensitivity of magnetic properties of cores at temperature, reduce the dispersion of magnetic properties of mass-produced cores and reduce the sensitivity of magnetic properties under stress.
A titre d'exemple, à partir d'un ruban en alliage Fe73,5Si13,5B9Cu1Nb3, (73,5
at % de fer, 13,5 at % de silicium, etc.), de 20 µm d'épaisseur et 10 mm de largeur
obtenus par trempe directe sur une roue refroidie, on a fabriqué trois séries A, B, C
de noyaux magnétiques qui ont été soumises toutes les trois à un traitement de
cristallisation de 3 heures à 530 °C (sans traitement de relaxation). A titre de
comparaison, la première série A de noyaux n'a pas été soumise à un traitement
thermique sous champ magnétique transverse. Conformément à l'invention, les deux
autres séries B et C ont été soumises à un traitement thermique sous champ
magnétique transverse appliqué sous forme de créneaux : 3 périodes de 5 mn sous
champ magnétique séparées l'une de l'autre par des périodes de 15 mn sans champ
magnétique. Pour l'une des séries, B , la température de traitement était de 200 °C,
et pour l'autre, C , la température de traitement était de 300 °C. Sur les trois séries
de noyaux magnétiques on a mesuré la perméabilité magnétique maximale
d'impédance µz mesurée à 50 Hz dans un champ d'excitation maximale de 8 mA/cm
(valeur de crête) à 25 °C, à - 25 °C, à + 80 °C et à + 100 °C, le rapport Δµ/µ
représentant les variations de µz par rapport à sa valeur à 25 °C. Les résultats ont
été les suivants :
Ces exemples montrent bien que si la série A a une perméabilité magnétique excellente, sa stabilité en température est insuffisante. Par contre, les exemples B et C ont des perméabilité plus faibles, mais néanmoins très satisfaisantes, et présentent une bonne stabilité en température de la perméabilité magnétique.These examples clearly show that if the series A has magnetic permeability excellent, its temperature stability is insufficient. On the other hand, examples B and C have lower permeability, but nevertheless very satisfactory, and exhibit good temperature stability of magnetic permeability.
Claims (6)
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
FR9715272 | 1997-12-04 | ||
FR9715272A FR2772182B1 (en) | 1997-12-04 | 1997-12-04 | METHOD FOR MANUFACTURING A NANOCRYSTALLINE SOFT MAGNETIC ALLOY MAGNETIC CORE AND USE IN AN AC CLASS DIFFERENTIAL CIRCUIT BREAKER |
Publications (2)
Publication Number | Publication Date |
---|---|
EP0921540A1 true EP0921540A1 (en) | 1999-06-09 |
EP0921540B1 EP0921540B1 (en) | 2006-05-24 |
Family
ID=9514142
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP98402803A Expired - Lifetime EP0921540B1 (en) | 1997-12-04 | 1998-11-13 | Fabrication process of a magnetic core of a soft magnetic nanocrystalline alloy and use in a differential circuit breaker |
Country Status (6)
Country | Link |
---|---|
EP (1) | EP0921540B1 (en) |
AT (1) | ATE327562T1 (en) |
DE (1) | DE69834615T2 (en) |
ES (1) | ES2262215T3 (en) |
FR (1) | FR2772182B1 (en) |
PL (1) | PL186805B1 (en) |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
FR2982409A1 (en) * | 2011-11-07 | 2013-05-10 | Schneider Electric Ind Sas | Method for manufacturing magnetic core for direct current sensor in differential circuit breaker, involves fixing layers with each other to form band, and forming core from band, where section of core is formed based on number of layers |
US8699190B2 (en) | 2010-11-23 | 2014-04-15 | Vacuumschmelze Gmbh & Co. Kg | Soft magnetic metal strip for electromechanical components |
CN112553545A (en) * | 2020-12-07 | 2021-03-26 | 国网河北省电力有限公司沧州供电分公司 | High-toughness and short-burst-resistant iron-based amorphous soft magnetic alloy and preparation method and application thereof |
Citations (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP0271657A2 (en) * | 1986-12-15 | 1988-06-22 | Hitachi Metals, Ltd. | Fe-base soft magnetic alloy and method of producing same |
EP0299498A1 (en) * | 1987-07-14 | 1989-01-18 | Hitachi Metals, Ltd. | Magnetic core and method of producing same |
EP0392204A2 (en) * | 1989-04-08 | 1990-10-17 | Vacuumschmelze GmbH | Use of a microcrystalline iron-based alloy as a magnetic material for a fault current-protective switch |
DE4019636A1 (en) * | 1989-07-01 | 1991-02-28 | James C M Li | METHOD FOR IMPROVING THE MAGNETIC PROPERTIES BY APPLYING AC OR PULSED CURRENT |
EP0563606A2 (en) * | 1992-04-01 | 1993-10-06 | Vacuumschmelze GmbH | Current transformer for earth-leakage circuit breakers which are sensitive to current pulses |
WO1996033505A1 (en) * | 1995-04-18 | 1996-10-24 | Schneider Electric S.A. | Current transformer, in particular for a fault current tripping device sensitive to pulsating currents and tripping device equipped with such a transformer |
-
1997
- 1997-12-04 FR FR9715272A patent/FR2772182B1/en not_active Expired - Fee Related
-
1998
- 1998-11-13 DE DE69834615T patent/DE69834615T2/en not_active Expired - Lifetime
- 1998-11-13 ES ES98402803T patent/ES2262215T3/en not_active Expired - Lifetime
- 1998-11-13 EP EP98402803A patent/EP0921540B1/en not_active Expired - Lifetime
- 1998-11-13 AT AT98402803T patent/ATE327562T1/en not_active IP Right Cessation
- 1998-12-04 PL PL98330100A patent/PL186805B1/en not_active IP Right Cessation
Patent Citations (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP0271657A2 (en) * | 1986-12-15 | 1988-06-22 | Hitachi Metals, Ltd. | Fe-base soft magnetic alloy and method of producing same |
EP0299498A1 (en) * | 1987-07-14 | 1989-01-18 | Hitachi Metals, Ltd. | Magnetic core and method of producing same |
EP0392204A2 (en) * | 1989-04-08 | 1990-10-17 | Vacuumschmelze GmbH | Use of a microcrystalline iron-based alloy as a magnetic material for a fault current-protective switch |
DE4019636A1 (en) * | 1989-07-01 | 1991-02-28 | James C M Li | METHOD FOR IMPROVING THE MAGNETIC PROPERTIES BY APPLYING AC OR PULSED CURRENT |
EP0563606A2 (en) * | 1992-04-01 | 1993-10-06 | Vacuumschmelze GmbH | Current transformer for earth-leakage circuit breakers which are sensitive to current pulses |
WO1996033505A1 (en) * | 1995-04-18 | 1996-10-24 | Schneider Electric S.A. | Current transformer, in particular for a fault current tripping device sensitive to pulsating currents and tripping device equipped with such a transformer |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US8699190B2 (en) | 2010-11-23 | 2014-04-15 | Vacuumschmelze Gmbh & Co. Kg | Soft magnetic metal strip for electromechanical components |
FR2982409A1 (en) * | 2011-11-07 | 2013-05-10 | Schneider Electric Ind Sas | Method for manufacturing magnetic core for direct current sensor in differential circuit breaker, involves fixing layers with each other to form band, and forming core from band, where section of core is formed based on number of layers |
CN112553545A (en) * | 2020-12-07 | 2021-03-26 | 国网河北省电力有限公司沧州供电分公司 | High-toughness and short-burst-resistant iron-based amorphous soft magnetic alloy and preparation method and application thereof |
Also Published As
Publication number | Publication date |
---|---|
FR2772182A1 (en) | 1999-06-11 |
ES2262215T3 (en) | 2006-11-16 |
PL186805B1 (en) | 2004-02-27 |
PL330100A1 (en) | 1999-06-07 |
EP0921540B1 (en) | 2006-05-24 |
DE69834615T2 (en) | 2007-04-26 |
ATE327562T1 (en) | 2006-06-15 |
DE69834615D1 (en) | 2006-06-29 |
FR2772182B1 (en) | 2000-01-14 |
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