Nanocristalline magnetic glass-covered wires and process for their production

Abstract: The invention refers to nanocrystalline magnetic glass-covered wires and to a process for their production. The wires consist of a metallic nanocrystalline core with diameters by the order of 10 -6 m having compositions based on transition metals and metalloids and other additional metals, and a glass cover having the thickness of the wall by the same order of magnitude. The nanocrystalline wires present high or medium saturation induction, nearly zero magnetostriction and values of the coercive field and of the magnetic permeability in function of the requested applications. The nanocrystalline glass-covered wires are used in electronics and electrotechnics to achieve inductive coils, mini-transformers, magnetic shields, devices working on the basis of the correlation between the magnetic properties of the metallic core and the optical properties of the glass cover.

Description: TECHNICAL FIELD The invention refers to nanocrystalline magnetic glass-covered wires with applications in electrotechnics and electronics and to a process for their production. BACKGROUND ART There are known ribbon and wire shaped amorphous materials obtained by rapid quenching from the melt and nanocrystalline magnetic materials obtained by thermal treatment of the amorphous ones with adequate compositions ( US patents nos. 4.501.316 and 4 . 523 . 626 ). Thus, amorphous magnetic wires with diameters ranging from 60 µm to 180 µm are obtained by the in-rotating-water spinning method and nanocrystalline magnetic wires are obtained by controlled thermal treatments of the above mentioned amorphous ones with adequate compositions. The disadvantage of these wires consists in the fact that they cannot be obtained directly from the melt in amorphous state with diameters less than 60 µm. Amorphous magnetic wires having diameters of minimum 30 µm are obtained by succesive cold-drawings of the above mentioned amorphous magnetic wires followed by stress relief thermal treatment. The disadvantages of these wires consists in the fact that by repeated drawings and annealing stages can be obtained amorphous magnetic wires having no less than 30 µm in diameter and that their magnetic and mechanical properties are unfavourably affected by the mechanical treatments. There are also known metallic glass-covered wires in crystalline state as well as some glass-covered amorphous alloys obtained by the glass- coated melt spinning method ( T.Goto, T.Toyama, "The preparation of ductile high strength Fe-base filaments using the methods of glass-coated melt spinning", Journal of Materials Science 20 (1985) pp. 1883-1888 ). The disadvantage of these wires consists in the fact that they do not present appropriate magnetic properties and behaviour for applications in electronics and electrotechnics to achieve magnetic sensors and actuators, but only properties that make them useful as metallic catalysts, composite materials, electrical conductors. Also known are amorphous magnetic wires covered by glass having the composition of the metallic core alloy Fe 65 B 15 Si 15 C 5 , Fe 60 B 15 Si 15 Cr 10 and Fe 40 Ni 40 P 14 B 6 ( Horia Chiriac et al . "Magnetic behavior of the amorphous wires covered by glass, Journal of Applied Physics, vol 75, no.10, 15.05.1994, pp. 6949-6951 ) with diameters of the metallic core ranging between 5 and 30 µm, coercive fields between 239 and 462 A/m and magnetization between 0.16 and 0.32 T. It is also mentioned a method for their obtaining based on the Taylor method, indicating as steps: the sealing of the glass tube, the heating of the seal and the drawing of a fibre from the heated end. The products disclosed in this document have very limited magnetic properties. There are also known amorphous glass-covered wires of compositions (Fe 80 Co 20 ) 75 B 15 Si 10 and Fe 65 B 15 Si 15 C 5 ( A.P.Zhukov et al ., "The magnetization process in thin and ultra-thin Fe-rich amorphous wires ) having diameters of the metallic core of 10 and 15 µm respectively, thickness of the glass cover of 2.5µm and coercive field of 65 and 140 A/m respectively. DISCLOSURE OF THE INVENTION The technical problem solved by this invention consists in the obtaining of nanocrystalline magnetic wires covered by glass, having controlled dimensional and compositional characteristics with adequate magnetic properties for different application categories, using a thermal treatment process with very specific parameters. For applications as minitransformers and inductive coils, that implies high values of the saturation magnetization and of the magnetic permeability are adequate nanocrystalline magnetic glass-covered wires according to the invention with diameters of the metallic core ranging between 5 and 25 µm and thickness of the glass cover ranging between 1 and 15 µm, of compositions based on Fe, containing 20 atomic % or less Si, 7 up to 35 atomic % B and 25 atomic % or less from one or more metals selected from the group Cu, Nb, V, Ta, W, Zr and Hf. The nanocrystalline magnetic glass-covered wires according to the invention are obtained from amorphpous magnetic glass-covered wires using a special thermal treatment. The process of producing amorphous magnetic glass covered wires, according to the invention, allows to obtain wires with the above mentioned dimensional and compositional characteristics directly by rapid quenching from the melt and consists in melting the metallic alloy which is introduced in a glass tube till the glass becomes soft, drawing the glass tube together with the molten alloy which is stretched to form a glass-coated metallic filament, which is coiled on a winding drum ensuring a high cooling rate necessary to obtain the metallic wire in amorphous state, in the following conditions: the temperature of the molted metal ranging between 900° C and 1500° C; the diameter of the glass tube ranging between 3 and 15 mm and the thickness of the glass wall ranging between 0.1 and 2 mm; the glass tube, containing the molten alloy, moves down with a uniform feed-in speed ranging between 5 x 10 -6 and 170 x 10 -6 m/s; the vacuum or the inert gas atmosphere level in the glass tube, above the molten alloy, ranging between 50 and 200 N/m 2 ; the drawing speed of the wire ranging between 0.5 and 10 m/s; the flow capacity of the cooling liquid through which the wire passes ranging between 10 -5 and 2 x 10 -5 m 3 /s. To ensure the continuity of the process and also to obtain continuous glass-covered wires of good quality and having the requested dimensions it is necessary that the employed materials and the process parameters to fulfill the following conditions: the high purity alloy is prepared in an arc furnace or in an induction furnace using pure components (at least 99 % purity) bulk shaped or powders bond together by pressing and then heating in vacuum or inert atmosphere (depending on the reactivity of the employed components); during the glass-coated melt spinning process an inert gas is introduced in the glass tube to avoid oxidation of the alloy; the employed glass must be compatible with the metal or the alloy at the drawing temperature in order to avoid the process of glass-metal difusion; the thermal expansion coefficient of the glass must be equal or slightly smaller than that of the employed metal or alloy to avoid the fragmentation of the alloy during the solidification process due to the internal stresses. The advantages of the wires according to the invention consist in the following: they can be used in a large field of applications based on their magnetic properties and behaviour; they can be used in devices based on the correlation between the magnetic properties of the metallic core and the optical properties of the glass cover, this application being facilitated by the intimate contact between the metallic core and the glass cover; they can be used in devices which involve suitable magnetic properties of the metallic core together with corrosion resistance, and the electrical insulation offered by the glass cover. The advantage of the producing process according to the invention is that it allows to obtain at low costs nanocrystalline magnetic glass-covered wires having very small diameters of the metallic core. BEST MODE FOR CARRYING OUT THE INVENTION In order to more completely understand the present invention, the following 5 examples are presented. Example 1. An amorphous glass-covered wire was produced using an alloy of composition Fe 73.5 Cu 1 Nb 3 B 9.5 Si 13 prepared in argon atmosphere from pure components in the shape of powders bond by pressing and heating in vacuum. The glass tube has 10 mm external diameter, 0.6 mm thickness of the glass wall and 50 cm length. In the glass tube are introduced and melted 10 g of the mentioned alloy, the melt temperature being 1200 ± 50° C. The process parameters are maintained at constant values of: 6.5 x 10 -6 m/s feed-in speed of the glass tube, 0.8 m/s peripheral speed of the winding drum, and 18 x 10 -6 m 3 /s flow capacity of the cooling liquid. The resulted positive magnetostrictive amorphous magnetic glass-covered wire of composition Fe 73.5 Cu 1 Nb 3 B 9.5 Si 13 having 22 µm diameter of the metallic core and 4 µm thickness of the glass cover, presents the following magnetic characteristics: large Barkhausen jump (M r /M s = 0.80); saturation induction (B s = 1.11 T); positive saturation magnetostriction (λ s = +4 x 10 -6 ); switching field (H* = 140 A/m). These wires are used either for magnetic sensors measuring mechanical quantities, or as precursors for nanocrystalline glas-covered wires. A special thermal treatment is applied to the amorphous magnetic wire of composition Fe 73.5 Cu 1 Nb 3 B 9.5 Si 13 prepared as described above. The special character of the thermal treatment refers to the strict correlation between the temperature and the duration of the thermal treatment. The magnetic amorphous glass-covered wire having the above mentioned composition is introduced into an electric furnace, in argon atmosphere and is thermally treated at 550° C for 1 hour. In this way one obtains a magnetic glass-covered wire having nanocrystalline structure that presents the following magnetic characteristics: does not present large Barkhausen jump (M r /M s = 0.2); saturation induction (B s = 1.25 T); almost zero saturation magnetization (λ s = -0.1 x 10 -6 ). These wires are used in inductive coils, mini-transformers, and magnetic shields. The magnetic measurements were performed using a fluxmetric method and the amorphous state was checked by X-ray diffraction.

Claims: Nanocrystalline magnetic glass-covered wires characterized in the fact that they consist of a metallic core with diameters ranging between 3 and 25 µm and a glass cover with the thickness ranging between 1 and 15 µm, the nanocrystalline magnetic wires having compositions based on Fe, containing 20 atomic % or less Si, 7 up to 35 atomic % B and 25 atomic % or less of one or more metals selected from the group Co, Ta, Nb, V, Cu, W, Zr and Hf, having saturation induction ranging between 0.7 and 1.25 T, almost zero magnetostriction, coercive field between 20 and 2500 A/m and relative magnetic permeability ranging between 100 and 12000. A process of producing nanocrystalline magnetic glass-covered wires defined in claim 1 characterized in the fact that magnetic amorphous glass-covered wires are thermally treated in vacuum or in inert atmosphere, in an electric furnace at temperatures smaller than the crystallization temperature of the amorphous alloy ranging between 480°C and 550°C for a given time ranging between 10 and 10 5 seconds.

Inventors: BARARIU FIRUTA, CHIRIAC HORIA, OVARI TIBOR ADRIAN, POP GHEORGHE, BARARIU, FIRUTA, CHIRIAC, HORIA, OVARI, TIBOR ADRIAN, POP, GHEORGHE
Applicants: INST DE FIZICA TEHNICA, INSTITUTUL DE FIZICA TEHNICA
Application year: 1996
Main classification: H01F1
IPC codes: H01F1