WO2013099258A1 - 方向性電磁鋼板 - Google Patents
方向性電磁鋼板 Download PDFInfo
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- WO2013099258A1 WO2013099258A1 PCT/JP2012/008366 JP2012008366W WO2013099258A1 WO 2013099258 A1 WO2013099258 A1 WO 2013099258A1 JP 2012008366 W JP2012008366 W JP 2012008366W WO 2013099258 A1 WO2013099258 A1 WO 2013099258A1
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- steel sheet
- magnetic domain
- grain
- oriented electrical
- electrical steel
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- 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
- H01F1/16—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 in the form of sheets
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- C—CHEMISTRY; METALLURGY
- C21—METALLURGY OF IRON
- C21D—MODIFYING THE PHYSICAL STRUCTURE OF FERROUS METALS; GENERAL DEVICES FOR HEAT TREATMENT OF FERROUS OR NON-FERROUS METALS OR ALLOYS; MAKING METAL MALLEABLE, e.g. BY DECARBURISATION OR TEMPERING
- C21D1/00—General methods or devices for heat treatment, e.g. annealing, hardening, quenching or tempering
- C21D1/34—Methods of heating
- C21D1/38—Heating by cathodic discharges
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- C—CHEMISTRY; METALLURGY
- C21—METALLURGY OF IRON
- C21D—MODIFYING THE PHYSICAL STRUCTURE OF FERROUS METALS; GENERAL DEVICES FOR HEAT TREATMENT OF FERROUS OR NON-FERROUS METALS OR ALLOYS; MAKING METAL MALLEABLE, e.g. BY DECARBURISATION OR TEMPERING
- C21D8/00—Modifying the physical properties by deformation combined with, or followed by, heat treatment
- C21D8/12—Modifying the physical properties by deformation combined with, or followed by, heat treatment during manufacturing of articles with special electromagnetic properties
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- C—CHEMISTRY; METALLURGY
- C21—METALLURGY OF IRON
- C21D—MODIFYING THE PHYSICAL STRUCTURE OF FERROUS METALS; GENERAL DEVICES FOR HEAT TREATMENT OF FERROUS OR NON-FERROUS METALS OR ALLOYS; MAKING METAL MALLEABLE, e.g. BY DECARBURISATION OR TEMPERING
- C21D8/00—Modifying the physical properties by deformation combined with, or followed by, heat treatment
- C21D8/12—Modifying the physical properties by deformation combined with, or followed by, heat treatment during manufacturing of articles with special electromagnetic properties
- C21D8/1277—Modifying the physical properties by deformation combined with, or followed by, heat treatment during manufacturing of articles with special electromagnetic properties involving a particular surface treatment
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- C—CHEMISTRY; METALLURGY
- C21—METALLURGY OF IRON
- C21D—MODIFYING THE PHYSICAL STRUCTURE OF FERROUS METALS; GENERAL DEVICES FOR HEAT TREATMENT OF FERROUS OR NON-FERROUS METALS OR ALLOYS; MAKING METAL MALLEABLE, e.g. BY DECARBURISATION OR TEMPERING
- C21D8/00—Modifying the physical properties by deformation combined with, or followed by, heat treatment
- C21D8/12—Modifying the physical properties by deformation combined with, or followed by, heat treatment during manufacturing of articles with special electromagnetic properties
- C21D8/1294—Modifying the physical properties by deformation combined with, or followed by, heat treatment during manufacturing of articles with special electromagnetic properties involving a localized treatment
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- C—CHEMISTRY; METALLURGY
- C22—METALLURGY; FERROUS OR NON-FERROUS ALLOYS; TREATMENT OF ALLOYS OR NON-FERROUS METALS
- C22C—ALLOYS
- C22C38/00—Ferrous alloys, e.g. steel alloys
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- C—CHEMISTRY; METALLURGY
- C22—METALLURGY; FERROUS OR NON-FERROUS ALLOYS; TREATMENT OF ALLOYS OR NON-FERROUS METALS
- C22C—ALLOYS
- C22C38/00—Ferrous alloys, e.g. steel alloys
- C22C38/001—Ferrous alloys, e.g. steel alloys containing N
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- C—CHEMISTRY; METALLURGY
- C22—METALLURGY; FERROUS OR NON-FERROUS ALLOYS; TREATMENT OF ALLOYS OR NON-FERROUS METALS
- C22C—ALLOYS
- C22C38/00—Ferrous alloys, e.g. steel alloys
- C22C38/02—Ferrous alloys, e.g. steel alloys containing silicon
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- C—CHEMISTRY; METALLURGY
- C22—METALLURGY; FERROUS OR NON-FERROUS ALLOYS; TREATMENT OF ALLOYS OR NON-FERROUS METALS
- C22C—ALLOYS
- C22C38/00—Ferrous alloys, e.g. steel alloys
- C22C38/04—Ferrous alloys, e.g. steel alloys containing manganese
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- C—CHEMISTRY; METALLURGY
- C22—METALLURGY; FERROUS OR NON-FERROUS ALLOYS; TREATMENT OF ALLOYS OR NON-FERROUS METALS
- C22C—ALLOYS
- C22C38/00—Ferrous alloys, e.g. steel alloys
- C22C38/06—Ferrous alloys, e.g. steel alloys containing aluminium
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- C—CHEMISTRY; METALLURGY
- C22—METALLURGY; FERROUS OR NON-FERROUS ALLOYS; TREATMENT OF ALLOYS OR NON-FERROUS METALS
- C22C—ALLOYS
- C22C38/00—Ferrous alloys, e.g. steel alloys
- C22C38/60—Ferrous alloys, e.g. steel alloys containing lead, selenium, tellurium, or antimony, or more than 0.04% by weight of sulfur
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- C—CHEMISTRY; METALLURGY
- C21—METALLURGY OF IRON
- C21D—MODIFYING THE PHYSICAL STRUCTURE OF FERROUS METALS; GENERAL DEVICES FOR HEAT TREATMENT OF FERROUS OR NON-FERROUS METALS OR ALLOYS; MAKING METAL MALLEABLE, e.g. BY DECARBURISATION OR TEMPERING
- C21D2201/00—Treatment for obtaining particular effects
- C21D2201/05—Grain orientation
Definitions
- the present invention relates to a grain-oriented electrical steel sheet suitable for an iron core material such as a transformer.
- the grain-oriented electrical steel sheet is mainly used as an iron core of a transformer, and is required to have excellent magnetization characteristics, particularly low iron loss. To that end, it is important to highly align the secondary recrystallized grains in the steel sheet with the (110) [001] orientation (Goss orientation) and to reduce impurities in the product. Furthermore, since there is a limit to the control of crystal orientation and the reduction of impurities, technology that introduces non-uniformity to the surface of the steel sheet by a physical method, subdivides the width of the magnetic domain, and reduces iron loss, That is, magnetic domain fragmentation technology has been developed.
- Patent Document 1 proposes a technique for narrowing the magnetic domain width and reducing iron loss by irradiating a final product plate with a laser and introducing a high dislocation density region into the steel sheet surface layer.
- Patent Document 2 proposes a technique for controlling the magnetic domain width by electron beam irradiation.
- the present invention relates to a method for enabling reduction of noise generated by the iron core when the iron core is laminated on a transformer iron core or the like in a grain-oriented electrical steel sheet in which iron loss is reduced by magnetic domain subdivision processing.
- the purpose is to propose.
- the noise of the transformer is mainly caused by magnetostriction behavior that occurs when the magnetic steel sheet is magnetized.
- the steel sheet in an electrical steel sheet containing about 3% by mass of Si, the steel sheet generally extends in the magnetized direction.
- a linear strain having a certain angle from the orthogonal direction or the orthogonal direction is applied to the rolling direction of the steel sheet with a continuous laser or an electron beam, a reflux magnetic domain is generated in the strain portion.
- the change in the magnetic domain structure when the steel plate is magnetized is already due to magnetostriction.
- the steel sheet does not expand or contract due to the change of magnetostriction.
- the change in the magnetic domain structure when the steel plate is magnetized adds to the generation and disappearance of the return magnetic domain in addition to the domain wall motion of the 180 ° magnetic domain.
- the reflux magnetic domain extends in the sheet width direction
- the steel sheet exhibits expansion and contraction due to changes in magnetostriction in the rolling direction, the sheet width direction, and the sheet thickness direction due to generation and disappearance of the reflux magnetic domain. Therefore, if the amount of the return magnetic domain in the steel sheet is different, it is considered that the magnetostriction caused by magnetization and the noise when laminated as a transformer core also change.
- the inventors focused on the volume fraction of the return magnetic domain contained in the steel sheet and investigated the influence on the iron loss and the noise of the transformer.
- the factor of magnetostriction generated in the rolling direction of the steel sheet is the generation of the reflux magnetic domain as described above.
- the magnetization in the return magnetic domain has a direction orthogonal to the magnetization of the 180 ° magnetic domain, and the steel sheet shrinks.
- the reflux magnetic domain is present at a volume fraction of ⁇ , the change in magnetostriction in the rolling direction relative to the state without the reflux magnetic domain is proportional to ⁇ 100 ⁇ .
- ⁇ 100 is a magnetostriction constant of 23 ⁇ 10 ⁇ 6 in the [100] direction.
- the ideal electrical steel sheet has [001] orientation of all crystal grains parallel to the rolling direction and the magnetization of the 180 ° magnetic domain is also parallel to the rolling direction. Has a deviation angle. For this reason, magnetization rotation in the 180 ° magnetic domain occurs due to magnetization in the rolling direction, and magnetostriction in the rolling direction occurs. At this time, the magnetostriction change in the rolling direction due to the magnetization rotation is proportional to ⁇ 100 (1-cos 2 ⁇ ), compared to the case where the magnetization of the 180 ° magnetic domain is parallel to the rolling direction. When the magnetostriction in the rolling direction is measured by exciting the steel plate, a mixture of the above two factors is observed.
- the inventors evaluated the volume fraction of the return magnetic domain from the magnetostriction measurement under the saturation magnetic flux density. Under the saturation magnetic flux density, all the magnetic domains of the steel plate are 180 ° magnetic domains, and when the magnetic flux density approaches 0 (zero) due to the alternating magnetic field, a reflux magnetic domain is generated and magnetostriction occurs.
- the volume fraction ⁇ of the reflux magnetic domain was determined by the following equation (A) using the difference ⁇ PP between the maximum value and the minimum value of magnetostriction at this time.
- the volume fraction of the reflux magnetic domain of the steel plate was calculated, and W 17/50 measurement and noise measurement of the transformer core were performed using a single plate magnetic tester (SST). These measurement results are shown in FIG.
- the volume fraction of the reflux magnetic domain was calculated using the above method, and the magnetostriction in the rolling direction was measured using a laser Doppler vibrometer at a frequency of 50 Hz and a saturation magnetic flux density.
- W 17/50 is the iron loss at a frequency of 50 Hz and a maximum magnetic flux density of 1.7 T.
- the excitation conditions for the transformer core are a frequency of 50 Hz and a maximum magnetic flux density of 1.7T.
- the sample is a grain oriented electrical steel sheet having a thickness of 0.23 mm and satisfies B 8 ⁇ 1.930T.
- the strain was introduced by irradiating the steel plate surface with a continuous laser beam under various conditions in which the laser beam output was 100 W, the scanning speed was 10 m / s, and the beam diameter on the steel plate surface was changed.
- the beam diameter can be changed by changing the diameter of the laser beam incident on the condensing lens to focus the laser beam on the surface of the steel plate surface and its surrounding area. .
- the inventors have found that as the beam diameter is increased, the volume fraction of the reflux magnetic domain introduced into the sample decreases, and the noise of the iron core also decreases accordingly.
- W 17/50 is the beam diameter, becomes minimum at close to the minimum value of the beam diameter possible with a laser irradiation apparatus, when enlarging the beam diameter, W 17/50 was found to tend to deteriorate.
- W 17/50 is more deteriorated than 0.720W / kg, good magnetic properties were not obtained.
- the decrease in the volume fraction of the return magnetic domain due to the beam diameter expansion means a decrease in the strain introduced into the steel sheet. Therefore, it is considered that such a deterioration in the magnetic properties is due to the weakening of the magnetic domain subdivision effect.
- the inventors have excellent B 8, and the amount of introduced distortion, and the volume fraction of the reflux magnetic domain generated in the distortion part in a range of from less than 3.00% 1.00% or more, transformers
- the present inventors have provided a grain-oriented electrical steel sheet excellent in noise characteristics and magnetic characteristics suitable as an iron core or the like.
- the gist configuration of the present invention is as follows. (1) Periodically in the rolling direction of the steel sheet, linear distortion extending in the direction perpendicular to the rolling direction of the steel sheet to an angle of 30 ° or less, with an iron loss W 17/50 of 0.720 W / kg or less A directional electrical steel sheet having a magnetic flux density B 8 of 1.930 T or more, wherein a volume occupied by the reflux magnetic domain generated in the strain portion is 1.00% or more and 3.00% or less of a total magnetic domain volume in the steel sheet. Oriented electrical steel sheet with excellent noise characteristics.
- the noise suppression is 1.930T or more magnetic flux density B 8 is required.
- the magnetic flux density B 8 is less than 1.930 T, the rotational motion of the magnetic domain is indispensable in order to make the magnetization parallel to the exciting magnetic field in the magnetization process, but such magnetization rotation causes a large change in magnetostriction, resulting in transformer noise. Increase. Further, when the direction, interval, or region of the strain to be applied is changed, the obtained iron loss reduction effect changes.
- the irradiation direction is a direction transverse to the rolling direction, preferably 60 ° to 90 ° with respect to the rolling direction (the angle formed with the direction perpendicular to the rolling is within 30 °), and this irradiation is 3 to 15 mm in the rolling direction. Perform at regular intervals.
- the amount of strain introduced can be evaluated by measuring the magnetostriction in the rolling direction under an alternating magnetic field that gives a saturation magnetic flux density, and calculating the volume fraction of the return magnetic domain by the above equation (A).
- the magnetostriction is preferably measured by a method using a laser Doppler vibrometer or a strain gauge by preparing a single electromagnetic steel sheet.
- the irradiation conditions when using a continuous laser beam are preferably in the range of 100 to 10000 W / mm 2 , although the beam diameter is 0.1 mm to 1 mm and the power density depends on the scanning speed.
- the focused diameter of the laser beam if a thin beam with a minimum diameter of 0.1 mm or less determined by the equipment configuration of the laser irradiation device is directly irradiated onto the surface of the steel plate as it is, the amount of strain introduced increases and the reflux magnetic domain increases. As a result, the volume fraction increases and the noise in the transformer core increases. Therefore, the volume fraction of the return magnetic domain is adjusted by changing the diameter of the laser beam incident on the converging lens for laser convergence.
- the beam diameter on the steel sheet surface is increased to about twice the minimum diameter.
- the condensing diameter is too large, the effect of subdividing the magnetic domain is diminished and the improvement of the iron loss is suppressed. Therefore, it is desirable to increase the condensing diameter to about 5 times.
- a semiconductor laser-excited fiber laser or the like is effective as the excitation source.
- the irradiation conditions when using an electron beam are preferably an acceleration voltage of 10 to 200 kV and a beam current of 0.005 to 10 mA.
- the volume fraction of the return magnetic domain can be adjusted by adjusting the beam current amount. Although it depends on the acceleration voltage, when the current exceeds this range, the amount of distortion introduced increases and the noise in the transformer core increases.
- the grain- oriented electrical steel sheet is not particularly limited as long as it has the characteristics that the iron loss W 17/50 is 0.720 W / kg or less and the magnetic flux density B 8 is 1.930 T or more.
- the component composition containing 1 type or 2 types or more of% is suitable.
- this cold-rolled sheet for grain-oriented electrical steel sheets is decarburized and subjected to primary recrystallization annealing, and then an annealing separator containing MgO as a main component is applied, and final annealing including secondary recrystallization process and purification process is performed.
- a grain-oriented electrical steel sheet having a forsterite film was obtained.
- an insulating coat composed of 60% colloidal silica and aluminum phosphate was applied to the grain-oriented electrical steel sheet and baked at 800 ° C.
- magnetic domain subdivision treatment was performed by irradiating a continuous fiber laser perpendicular to the rolling direction.
- a three-phase transformer core was manufactured by stacking the sample as a bevel with a width of 100 mm and a thickness of 15 mm, and using a condenser microphone, noise at a maximum magnetic flux density of 1.7 T and a frequency of 50 Hz was measured. At that time, A scale correction is performed as auditory correction.
- the volume fraction of the return magnetic domain is out of the scope of the invention, and the noise is also deteriorated.
- the beam diameter is too large, the volume fraction of the return magnetic domain is within the range of the invention and the noise characteristics are good, but W 17/50 is high.
- the volume fraction of the closure domains are within the invention scope, and even those core loss also good, the B 8 is less than 1.930T steel is deteriorated noise of transformer core.
- the transformer in order to be suitable oriented electrical steel sheet as the core or the like, the magnetic flux density B 8, is important to within the range of all three are the invention of iron loss W 17/50 and the volume fraction of the closure domain is there.
- Example 2 The same sample as the electromagnetic steel plate before laser irradiation used in laser beam irradiation in Example 1 was irradiated with an electron beam with various beam currents under the conditions of an acceleration voltage of 60 kV and a beam speed of 30 m / s.
- the obtained sample was measured for the volume fraction of the reflux magnetic domain in the steel plate, W 17/50, and the noise of the transformer core.
- the measured noise of the transformer core is shown in Table 2 together with the beam current, B 8 , and volume fraction of the return magnetic domain.
- B 8 ⁇ 1.930T and the volume fraction of the return magnetic domain is within the specified range by lowering the beam current, the noise is reduced to 36 dBA or less.
- the volume fraction of the return magnetic domain exceeds the range of the invention.
- noise increases, and when the current density is decreased, the volume fraction of the return magnetic domain falls below the range of the invention. 17/50 has deteriorated.
- the volume fraction invention range closure domains, and also W 17/50 is equal to or less than 0.720W / kg, the B 8 ⁇ what is 1.930T is noise greater than 36 dBA, electronic also in the beam irradiation, the magnetic flux density B 8, by keeping the range of all three are the invention of iron loss W 17/50 and the volume fraction of the closure domains, compatible for the first time the magnetic properties and noise characteristics.
Abstract
Description
そのためには、鋼板中の二次再結晶粒を(110)[001]方位(ゴス方位)に高度に揃えることや製品中の不純物を低減することが重要である。さらに、結晶方位の制御や不純物の低減には限界があることから、鋼板の表面に対して物理的な手法で不均一性を導入し、磁区の幅を細分化して鉄損を低減する技術、すなわち磁区細分化技術が開発されている。
たとえば、特許文献1には、最終製品板にレーザを照射し、鋼板表層に高転位密度領域を導入することにより、磁区幅を狭くし鉄損を低減する技術が提案されている。また、特許文献2には、電子ビームの照射により磁区幅を制御する技術が提案されている。
ところで、連続レーザあるいは電子ビーム等で鋼板の圧延方向に対し、直交方向あるいは直交方向から一定の角度を持った線状の歪を与えると、この歪部分に還流磁区が発生する。この鋼板中の還流磁区が一切存在せず、かつ鋼板の磁区構造が圧延方向を向く180°磁区のみで構成される理想的な場合、鋼板を磁化した時の磁区構造の変化は、既に磁歪によって圧延方向に伸びきった180°磁区の磁壁移動のみで完結し、それ故磁歪の変化による鋼板の伸縮は発生しない。しかし、鋼板中に還流磁区が存在すると、鋼板を磁化した時の磁区構造の変化は、180°磁区の磁壁移動に、還流磁区の生成・消滅が加わる。ここで、還流磁区は板幅方向に伸長するため、還流磁区の生成・消滅によって鋼板は圧延方向および板幅方向・板厚方向への磁歪の変化による伸縮を示す。従って、鋼板中の還流磁区の量が異なると、磁化によって生じる磁歪、および変圧器鉄心として積層した時の騒音も変化することが考えられる。
まず、鋼板の磁束密度B8と騒音との関係について調べた。すなわち、180°磁区内で磁化が圧延方向からずれていると、電磁鋼板を磁化した時に飽和磁化付近で磁化の回転が生じる。このような回転は圧延方向および板幅方向の伸縮を大きくし、磁歪の増大につながるため、変圧器鉄心における騒音の観点からは不利である。このことから、結晶粒の[001]方位が圧延方向に集積した高配向性のものが有利であり、発明者等はB8≧1.930Tであるときに、磁化の回転による変圧器鉄心の騒音増大を抑えられることを見出した。
また、理想的な電磁鋼板は全ての結晶粒の[001]方位が圧延方向と平行、かつ180°磁区の磁化も圧延方向と平行になるが、現実には結晶粒の方位は圧延方向からのずれ角をもつ。そのため、圧延方向への磁化によって180°磁区の磁化回転が生じ、圧延方向の磁歪が発生する。このとき、180°磁区の磁化が圧延方向と平行である場合に対して、磁化回転による圧延方向の磁歪変化はλ100(1-cos2θ)に比例する。鋼板を励磁して圧延方向の磁歪を測定すると、上記2つの要因が混在したものが観測される。ここで、B8≧1.930Tのとき、結晶粒の[001]方位のずれは圧延方向に対して4°以下であるが、磁化回転による磁歪への寄与は(6×10-4)λ100以下であり、3%Siを含む電磁鋼板の磁歪に比べて非常に小さい。従って、騒音特性に優れたB8≧1.930Tである鋼板においては、磁歪の要因として磁化の回転は無視することができ、還流磁区の体積分率の変化のみによって支配されていると考えて差し支えない。従って、圧延方向の磁歪を測定することによって、還流磁区の体積分率を評価することができる。
なお、ビーム径を変化させる方法としては、鋼板表面上でレーザビームを照射したい点およびその周辺領域にレーザを収束させるための、集光レンズに入射するレーザビームの径を変化させることで対応した。これにより、発明者らはビーム径を拡大していくと、試料に導入される還流磁区の体積分率は低下していき、それに伴って鉄心の騒音も減少していくことを見出した。
(1)鋼板の圧延直角方向と成す角度が30°以内の向きに延びる線状の歪を、該鋼板の圧延方向に周期的に有し、鉄損W17/50が0.720W/kg以下および磁束密度B8が1.930T以上の方向性電磁鋼板であって、前記歪部分に生じた、還流磁区の占める体積が、鋼板中の全磁区体積の1.00%以上3.00%以下であることを特徴とする騒音特性に優れた方向性電磁鋼板。
また、付与する歪の向きや間隔あるいは領域を変えると、得られる鉄損低減効果が変化する。適切な歪付与がなされない場合、鉄損が十分に低減されずに良好な磁気特性が得られなかったり、還流磁区の体積分率を制御しても磁歪が減少せず変圧器騒音を抑制できない場合がある。そこで、歪が適切に付与されて、鉄損W17/50が0.720W/kg以下である鋼板を使うことによって、還流磁区の制御による騒音低減効果を得ることができるようになる。
計測された変圧器鉄心の騒音を、ビーム電流、B8、還流磁区の体積分率とあわせて表2にまとめた。電子ビームにおいても、B8≧1.930Tかつ、ビーム電流を下げて還流磁区の体積分率が指定の範囲内にあるものは、騒音が36 dBA以下で低騒音化されている。
Claims (3)
- 鋼板の圧延直角方向と成す角度が30°以内の向きに延びる線状の歪を、該鋼板の圧延方向に周期的に有し、鉄損W17/50が0.720 W/kg以下および磁束密度B8が1.930T以上の方向性電磁鋼板であって、前記歪部分に生じた、還流磁区の占める体積が、鋼板中の全磁区体積の1.00%以上3.00%以下であることを特徴とする騒音特性に優れた方向性電磁鋼板。
- 前記線状の歪が、連続レーザビームの照射により導入されてなることを特徴とする請求項1に記載の方向性電磁鋼板。
- 前記線状の歪が、電子ビームの照射により導入されてなることを特徴とする請求項1に記載の方向性電磁鋼板。
Priority Applications (6)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
RU2014131034/02A RU2570250C1 (ru) | 2011-12-27 | 2012-12-27 | Текстурированный лист из электротехнической стали |
CN201280065085.0A CN104011246B (zh) | 2011-12-27 | 2012-12-27 | 取向性电磁钢板 |
KR1020147018637A KR101580837B1 (ko) | 2011-12-27 | 2012-12-27 | 방향성 전자 강판 |
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WO2022050053A1 (ja) | 2020-09-04 | 2022-03-10 | Jfeスチール株式会社 | 方向性電磁鋼板 |
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US9646749B2 (en) | 2017-05-09 |
EP2799574A1 (en) | 2014-11-05 |
CN104011246B (zh) | 2016-08-24 |
RU2570250C1 (ru) | 2015-12-10 |
EP2799574B1 (en) | 2017-02-01 |
KR20140109409A (ko) | 2014-09-15 |
US20140352849A1 (en) | 2014-12-04 |
JPWO2013099258A1 (ja) | 2015-04-30 |
JP5761377B2 (ja) | 2015-08-12 |
EP2799574A4 (en) | 2015-06-03 |
KR101580837B1 (ko) | 2015-12-29 |
CN104011246A (zh) | 2014-08-27 |
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