WO2015129253A1 - Oriented electromagnetic steel sheet for low-noise transformer, and method for manufacturing said sheet - Google Patents

Oriented electromagnetic steel sheet for low-noise transformer, and method for manufacturing said sheet Download PDF

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WO2015129253A1
WO2015129253A1 PCT/JP2015/000931 JP2015000931W WO2015129253A1 WO 2015129253 A1 WO2015129253 A1 WO 2015129253A1 JP 2015000931 W JP2015000931 W JP 2015000931W WO 2015129253 A1 WO2015129253 A1 WO 2015129253A1
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irradiation
steel sheet
region
modulated
area
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PCT/JP2015/000931
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French (fr)
Japanese (ja)
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広朗 戸田
重宏 ▲高▼城
龍一 末廣
小松原 道郎
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Jfeスチール株式会社
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    • CCHEMISTRY; METALLURGY
    • C21METALLURGY OF IRON
    • C21DMODIFYING 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
    • C21D8/00Modifying the physical properties by deformation combined with, or followed by, heat treatment
    • C21D8/12Modifying the physical properties by deformation combined with, or followed by, heat treatment during manufacturing of articles with special electromagnetic properties
    • C21D8/1294Modifying the physical properties by deformation combined with, or followed by, heat treatment during manufacturing of articles with special electromagnetic properties involving a localized treatment
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F1/00Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties
    • H01F1/01Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials
    • H01F1/03Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity
    • H01F1/12Magnets 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
    • H01F1/14Magnets 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
    • H01F1/16Magnets 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
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F41/00Apparatus 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
    • H01F41/02Apparatus 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
    • CCHEMISTRY; METALLURGY
    • C21METALLURGY OF IRON
    • C21DMODIFYING 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
    • C21D1/00General methods or devices for heat treatment, e.g. annealing, hardening, quenching or tempering
    • C21D1/06Surface hardening
    • C21D1/09Surface hardening by direct application of electrical or wave energy; by particle radiation

Definitions

  • the present invention relates to a grain-oriented electrical steel sheet for a low noise transformer and a method for manufacturing the same.
  • a technique for subdividing the magnetic domains of grain-oriented electrical steel sheets there is a technique in which the effect does not disappear even when strain relief annealing is performed, such as forming grooves on the steel sheet surface.
  • the present invention is an electron known as one of techniques for subdividing magnetic domains and reducing iron loss by introducing strain into the steel sheet surface layer such as laser irradiation, plasma jet flame irradiation, and marking. It is a technique that uses a beam irradiation method, and is particularly intended to simultaneously achieve low iron loss and low magnetostriction.
  • Patent Document 1 discloses a method for manufacturing a grain-oriented electrical steel sheet having a magnetic flux density B 8 exceeding 1.97T.
  • the iron loss can be improved by increasing the purity of the material, high orientation, reducing the plate thickness, adding Si, Al, and subdividing the magnetic domain (for example, Non-Patent Document 1).
  • the iron loss tends to deteriorate.
  • the crystal orientation is highly integrated in the Goss orientation for the purpose of improving B 8
  • the magnetostatic energy decreases, the domain width increases, and the eddy current loss increases. Therefore, as a method of reducing such eddy current loss, a technique is used in which the above-described tension coating is applied, or a magnetic domain is subdivided by introducing thermal strain into the steel sheet surface layer to reduce iron loss. .
  • Patent Document 3 discloses that laser scanning irradiation is performed under certain conditions to impart thermal strain to the steel sheet
  • Patent Document 4 discloses a pulse Q-switched laser having a half width of 10 nsec or more and 1 ⁇ sec or less.
  • a technology to reduce iron loss by subdividing magnetic domains by concentrating the light intensity of 1 ⁇ 10 5 to 1 ⁇ 10 8 W / cm 2 and intermittently applying thermal strain to the steel sheet is disclosed. Has been.
  • Patent Document 5 describes that a hardened region generated in a steel sheet surface layer by laser irradiation or the like, that is, a plastic strain region obstructs domain wall movement and increases hysteresis loss.
  • the strain concentrates locally on a part of the surface layer of the steel sheet, and the effect of reducing iron loss is not sufficient, and the effect of reducing iron loss is insufficient due to the increase in hysteresis loss due to strain.
  • magnetostriction due to strain increased.
  • Patent Document 5 the laser output and the spot diameter ratio are adjusted, the plastic strain region cured by laser irradiation in the direction perpendicular to the laser scanning direction is reduced to 0.6 mm or less, and the hysteresis loss is reduced. By reducing this, iron loss is reduced.
  • the plastic strain on the surface of the steel sheet causes an increase in magnetostriction, and as a result, the noise of the transformer increases.
  • Patent Document 8 the current value of the electron beam to be irradiated, the traveling speed of the electron beam in the width direction of the steel plate, the irradiation pitch in the rolling direction, and the beam diameter of the electron beam are controlled within a certain range. Discloses a technology for obtaining a grain-oriented electrical steel sheet that is excellent in noise and iron loss by suppressing the occurrence of thermal distortion.
  • Non-Patent Document 2 when the magnetic domain of a grain-oriented electrical steel sheet is subdivided by laser light irradiation, the interaction between the laser light and the surface film is strong, which is accompanied by rapid thermal deformation of the steel sheet near the irradiated surface or rapid evaporation of the film. Due to the reaction force on the steel plate, a region with a higher dislocation density is formed on the steel plate near the irradiated portion. As a result, it has been shown that the hardness of the steel sheet increases, and at the same time, the steel sheet is deformed to increase the hysteresis loss (for example, Non-Patent Document 2).
  • forming a 90 ° magnetic domain in the steel sheet by forming a region with a higher dislocation density in the vicinity of the irradiated part of the steel sheet surface layer is the basic principle of magnetic domain subdivision by this technology.
  • Accompanying the reduction is necessarily accompanied by an increase in hysteresis loss and an increase in magnetostriction. That is, as long as it is a technology for irradiating laser light utilizing thermal distortion as in the prior art, it is not possible to establish all of magnetic domain subdivision, low hysteresis loss, and low magnetostriction.
  • the inventors considered that, in general, when an electron beam is irradiated onto a steel sheet, it is possible to find an optimum condition common to both iron loss and magnetostriction by adjusting the energy density of the irradiated portion. That is, the beam irradiation linear density ⁇ disclosed in Patent Document 8 corresponds to this, and a magnetic domain subdividing effect can be obtained by increasing the value of ⁇ from a predetermined minimum value, and by reducing the value from the maximum value, a steel plate It was thought that the plastic strain of the surface layer could be reduced, and as a result, the increase in hysteresis loss and noise could be suppressed.
  • the required electron beam irradiation energy intensity is such that the irradiation is performed at an intensity higher than the level at which the magnetic domains elongated and divided in the direction of the irradiation line exist in the electron beam irradiation line region, and the occurrence of thermal distortion on the steel sheet surface is suppressed. It has been clarified that it is an essential technique to suppress the occurrence of film damage on the irradiation side surface of the steel sheet and to perform irradiation at a strength level that does not form a plastic strain region.
  • Table 1 shows that the acceleration voltage Vk is 40 kV to 120 kV and the beam is radiated to the directional electrical steel sheet with a plate thickness of 0.23 mm, B 8 of 1.943 T, and iron loss W 17/50 of 0.85 W / kg.
  • the lower limit value of the energy density of the irradiated portion includes a divided magnetic domain elongated in the irradiation direction (Non-Patent Document 3).
  • the upper limit value of the energy density is an upper limit value at which damage to the coating does not occur.
  • modulated irradiation is performed by repeatedly irradiating a total area of 0.50 mm of a beam residence area: 1 and a traveling area: 2 as a repeating unit: 3 (which is also a period of the repeating unit) in the width direction of the steel sheet. Irradiation was performed under irradiation conditions (condition 2) for forming a line region. At this time, the dwell time at the dwell point was 0.020 msec, and the running speed in the running region: 2 was adjusted so that the average scanning speed was 25 m / sec.
  • FIG. 2 shows the results of examining the relationship between the distance L in the rolling direction of the irradiated region and the iron loss and magnetostriction when the electron beam irradiation is performed under the above conditions 1 and 2.
  • the gist configuration of the present invention is as follows. 1.
  • the surface of the steel sheet is irradiated with an electron beam in a line area in a direction intersecting the rolling direction, the irradiation line area is set as a modulated irradiation line area having two types of areas consisting of a stay area and a running area as repeating units, and
  • a modulated irradiation region in which the repeating units are connected in the direction of the line region A modulated irradiation region in which the repeating units are connected in the direction of the line region,
  • the period in the modulated irradiation region of the repeating unit is 0.20 to 1.0 mm
  • the repetition interval in the rolling direction of the modulated irradiation region is set to 4.0 to 12.5 mm, and the intensity of the electron beam is at least equal to or more than the strength at which the elongated magnetic domains extending in the direction of the modulated irradiation region are formed on the i
  • the surface of the steel sheet is irradiated with an electron beam in a line area in a direction intersecting the rolling direction, the irradiation line area is set as a modulated irradiation line area having two types of areas consisting of a stay area and a running area as repeating units, and
  • a modulated irradiation region in which the repeating units are connected in the direction of the line region A modulated irradiation region in which the repeating units are connected in the direction of the line region,
  • the period in the modulated irradiation region of the repeating unit is 0.20 to 1.0 mm
  • the repetition interval in the rolling direction of the modulated irradiation region is set to 4.0 to 12.5 mm, and the intensity of the electron beam is at least equal to or more than the strength at which the elongated magnetic domains extending in the direction of the modulated irradiation region are formed on the irradiation surface side.
  • the present invention it is possible to carry out magnetic domain subdivision processing under conditions that satisfy both the low iron loss and low noise of the transformer, which has been difficult in the past, and the direction of low magnetostriction with low iron loss that has not been achieved conventionally. Since the electromagnetic steel sheet can be obtained, the energy use efficiency in the transformer can be improved and the noise can be suppressed, which is extremely useful industrially.
  • the irradiation object in the present invention is a grain-oriented electrical steel sheet.
  • the grain-oriented electrical steel sheet is provided with an insulation coating such as a tension coating on the forsterite film on the ground iron.
  • the forsterite film is provided between the ground iron and the insulation coating. There is no problem even if is not present.
  • the magnetic domain refinement process is performed by scanning the surface of the grain-oriented electrical steel sheet with an electron beam in a direction intersecting with the rolling direction and at intervals in the rolling direction.
  • the introduction means is limited to electron beam irradiation.
  • the interaction with the insulation coating existing on the surface of the steel plate is large, and the damage of the insulation coating and the plastic strain consisting of high dislocation density are introduced into the surface layer of the underlying iron, so the deterioration of hysteresis loss, That is, the iron loss is deteriorated and the best iron loss characteristic cannot be obtained.
  • the interaction with the insulating coating is limited to a small size due to the dynamic action of the electron beam, and the interaction with the ground iron inside the steel plate is increased. Therefore, it is possible to impart the magnetic domain refinement effect without damage of the insulating coating, the forsterite film, or the introduction of plastic strain having a high dislocation density in the surface layer of the base iron immediately below the coating.
  • the steel plate surface irradiated with the electron beam may be one side of the steel plate or both sides.
  • the direction intersecting the rolling direction is a direction perpendicular to the rolling direction, that is, a range of 75 ° to 105 ° when the sheet width direction of the steel sheet is 90 °. It is suitably exhibited.
  • reference numeral 1 is a staying region
  • 2 is a traveling region
  • 3 is a repeating unit (spacing point interval)
  • d indicates a beam diameter.
  • the period of the repeating unit in the modulated irradiation region needs to be 0.20 to 1.0 mm.
  • the period of this repeating unit is 0.20 to 1.0 mm.
  • the range is preferably 0.25 to 0.80 mm.
  • the repetition interval in the rolling direction of the above-described modulated irradiation region needs to be 4.0 to 12.5 mm.
  • the repetition interval in the rolling direction of the modulated irradiation region is less than 4.0 mm, the iron loss increases as shown in FIG. 2, and the magnetostriction also deteriorates.
  • the repeat interval in the rolling direction must be 4.0 to 12.5 mm.
  • the range is preferably 5.0 to 10 mm.
  • the beam diameter d of the electron beam is not particularly limited. However, if the beam diameter d is too small, it is disadvantageous for the generation of the divided magnetic domain, while if too large, the divided magnetic domain is excessively generated.
  • the diameter d is preferably about 0.05 to 0.5 mm.
  • the acceleration voltage of the electron beam is not particularly limited, but if the acceleration voltage is too small, the penetration of electrons into the steel plate is insufficient, while if too large, the electron gun or the power source Since the manufacturing cost of equipment and the like becomes large, the acceleration voltage is preferably about 30 to 300 kV.
  • the outer shape of the transformer is composed of a steel plate having a 500 mm square and a width of 100 mm. Cut the steel plate into the shape shown in Fig. 5 and stack it with a stacking thickness of 100mm, tighten it with a band, and then wind the secondary coil and primary coil around the legs of the steel plate and put it in a tank filled with insulating oil The measurement was carried out by connecting the measuring instrument.
  • the three phases are excited by using a primary coil with a 120 ° phase shift, and the cross-sectional area is obtained from the weight of the iron core generated from the induced voltage generated in the secondary coil. It was measured.
  • the noise was expressed in dBA units where vibrations generated around the transformer were recorded with a microphone and A scale correction was performed.
  • the iron loss was expressed as a loss per weight of the transformer by subtracting the copper loss from the voltage and current value on the primary coil side in the unloaded state with the secondary coil open.
  • Example 1 Has a forsterite film on the steel sheet surface, the sheet thickness was baked tension coating thereon: 0.23 mm, the magnetic flux density B 8: 1.942T, iron loss W 17/50: oriented electrical steel sheet 0.870W / kg 6
  • magnetic domain subdivision means electron beam irradiation with acceleration voltage: 60kV, beam current: 12mA, beam diameter: 0.30mm is used, and irradiation is performed continuously at a scanning speed of 40m / sec under constant irradiation conditions in the plate width direction. And one was irradiated with an interval in the rolling direction of 5.0 mm (Comparative Example A1) and the other was 7.5 mm (Comparative Example A2). In these comparative examples, a part where the coating partly peeled off was confirmed.
  • the other two were irradiated with an electron beam under the same conditions as above, but the residence time was 0.010 msec, the residence point interval was 0.40 mm, and the residence unit and the running region were repeated units. And a modulated irradiation region was formed at an average scanning speed of 40 m / sec. At this time, one was irradiated with a repetition interval in the rolling direction of 5.0 mm (Invention Example A3), and the other was 7.5 mm (Invention Example A4). In these inventive examples, no damage to the coating was observed, and magnetic domains that were elongated and divided in the plate width direction were observed on the irradiated region by magnetic domain observation by the bitter method.
  • the remaining two were subjected to discontinuous pulse irradiation in the plate width direction of the steel sheet using an Nd: YAG laser device equipped with a Q switch.
  • the irradiation conditions at this time are conventionally known conditions, that is, the laser pulse energy is 3.3 mJ / pulse, the laser spot size is a circle with a diameter of 0.18 mm, the irradiation interval in the plate width direction is 0.3 mm, and the laser wavelength is 1064 nm. It was.
  • One irradiation interval in the rolling direction was 5.0 mm (Comparative Example A5), and the other was 7.5 mm (Comparative Example A6).
  • a clear circular coating defect and bare iron bareness were observed in the place where the laser beam was received, so the insulating coating was thinly reapplied and baked at a low temperature to improve insulation. .
  • the grain-oriented electrical steel sheet subjected to magnetic domain subdivision according to the present invention is superior in iron loss characteristics and magnetostriction characteristics and also in transformer iron loss and noise characteristics as compared with the comparative example. ing. Furthermore, it should be noted that when the irradiation interval in the rolling direction is set to 7.5 mm, unlike the comparative example, both the iron loss and the noise show the best values, and it is excellent as a grain-oriented electrical steel sheet for a transformer. It turns out that it has an effect.
  • Example 2 Has a forsterite film on the steel sheet surface, the sheet thickness was baked tension coating thereon: 0.27 mm, the magnetic flux density B 8: 1.949T, iron loss W 17/50: oriented electrical steel sheet 0.903W / kg 6
  • magnetic domain subdivision means electron beam irradiation with acceleration voltage: 50kV, beam current: 12mA, beam diameter: 0.20mm is used, and irradiation is continuously performed at a scanning speed of 30m / sec under constant irradiation conditions in the plate width direction. And one was irradiated with an interval in the rolling direction of 5.0 mm (Comparative Example B1) and the other was 7.5 mm (Comparative Example B2). In these comparative examples, a part where the coating partly peeled off was confirmed.
  • the other two were irradiated with an electron beam under the same conditions as above, but the residence time: 0.010 msec and the residence point interval: 0.30 mm was used as the repeat unit for the residence region and travel region, and the repeat unit in the plate width direction. And a modulated irradiation region was formed at an average scanning speed of 30 m / sec. At this time, one was irradiated with a repetition interval in the rolling direction of 5.0 mm (Invention Example B3), and the other was 7.5 mm (Invention Example B4). In these inventive examples, no damage to the coating was observed, and magnetic domains that were elongated and divided in the plate width direction were observed on the irradiated region by magnetic domain observation by the bitter method.
  • the remaining two were subjected to discontinuous pulse irradiation in the plate width direction of the steel sheet using an Nd: YAG laser device equipped with a Q switch.
  • the irradiation conditions at this time are conventionally known conditions, that is, the laser pulse energy is 4.5 mJ / pulse, the laser spot size is a circle with a diameter of 0.22 mm, the irradiation interval in the plate width direction is 0.3 mm, and the laser wavelength is 1064 nm. It was.
  • One irradiation interval in the rolling direction was 5.0 mm (Comparative Example B5), and the other was 7.5 mm (Comparative Example B6). In these comparative examples, a clear circular coating defect and bare iron bareness were observed in the place where the laser beam was received, so the insulation coating was thinly reapplied and baked at a low temperature to improve insulation. It was.
  • the grain-oriented electrical steel sheet subjected to magnetic domain subdivision according to the present invention is superior in iron loss characteristics and magnetostriction characteristics as compared with the comparative example, and also excellent in iron loss and noise characteristics of the transformer. ing. Furthermore, it should be noted that when the irradiation interval in the rolling direction is 7.5 mm, unlike the comparative example, both the iron loss and the noise show the best values, which is excellent as a grain-oriented electrical steel sheet for a transformer. It turns out that it has an effect.

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Abstract

 An oriented electromagnetic steel sheet processed using magnetic domain segmentation by the steel sheet surface being irradiated with an electron beam in a linear area having a direction intersecting with the rolling direction, wherein: the irradiation line area is made into repeating units made up of two types of areas comprising a retention area and a travel area; modulated-irradiation line areas are obtained by connecting the repeating units in the line-area direction; the period of the repeating units in the modulated-irradiation line area is 0.20-1.0 mm; the repeating interval of the modulated-irradiation line area in the rolling direction is 4.0-12.5 mm; and the intensity of the electron beam is brought to a level equal to or greater than that at which split magnetic domains are formed extending in the direction of the modulated-irradiation line area at least on the irradiation-surface side, and up to a level at which the coating is not damaged and no plastic strain areas are formed on the irradiation-surface side. It is thereby possible to carry out a hitherto challenging magnetic-domain segmentation process in a transformer in which iron loss and noise are both low, and obtain an oriented electromagnetic steel sheet that has unprecedentedly low iron loss and magnetic distortion.

Description

低騒音変圧器用の方向性電磁鋼板およびその製造方法Directional electrical steel sheet for low noise transformer and method of manufacturing the same
 本発明は、低騒音変圧器用の方向性電磁鋼板およびその製造方法に関するものである。
 方向性電磁鋼板の磁区を細分化する技術としては、鋼板表面に溝を形成するなど歪取焼鈍を施した場合でもその効果が消失しない手法がある。これに対し、本発明は、レーザ照射やプラズマジェット炎照射、ケガキなどのように鋼板表層に歪みを導入することで磁区を細分化して鉄損を低減する手法の一つとして知られている電子ビーム照射法を利用した技術で、特に低鉄損と低磁歪とを同時に達成しようとするものである。
The present invention relates to a grain-oriented electrical steel sheet for a low noise transformer and a method for manufacturing the same.
As a technique for subdividing the magnetic domains of grain-oriented electrical steel sheets, there is a technique in which the effect does not disappear even when strain relief annealing is performed, such as forming grooves on the steel sheet surface. On the other hand, the present invention is an electron known as one of techniques for subdividing magnetic domains and reducing iron loss by introducing strain into the steel sheet surface layer such as laser irradiation, plasma jet flame irradiation, and marking. It is a technique that uses a beam irradiation method, and is particularly intended to simultaneously achieve low iron loss and low magnetostriction.
 近年、エネルギーの効率的使用を背景として、変圧器メーカなどにおいて、低損失かつ低騒音の変圧器が望まれている。このため、高磁束密度で鉄損が低く、さらに磁歪が低い方向性電磁鋼板が求められている。方向性電磁鋼板は、その最表面に電気絶縁性の付与も兼ねた張力コーティングを有しており、鋼板の結晶方位をGoss方位へ集積させることによって磁束密度を向上させることが可能である。
 例えば特許文献1には、1.97Tを超える磁束密度B8を有する方向性電磁鋼板の製造方法が示されている。
In recent years, against the background of efficient use of energy, transformer manufacturers and the like have desired low-loss and low-noise transformers. For this reason, a grain-oriented electrical steel sheet with high magnetic flux density, low iron loss, and low magnetostriction is required. A grain-oriented electrical steel sheet has a tension coating that also serves to provide electrical insulation on its outermost surface, and the magnetic flux density can be improved by accumulating the crystal orientation of the steel sheet in the Goss orientation.
For example, Patent Document 1 discloses a method for manufacturing a grain-oriented electrical steel sheet having a magnetic flux density B 8 exceeding 1.97T.
 一方、鉄損は、素材の高純度化、高配向性、板厚低減、Si,Al添加および磁区細分化等によって改善が可能である(例えば、非特許文献1)。
 しかし、一般に磁束密度B8が高くなると鉄損は劣化する傾向にある。例えば、B8の向上を目的に、結晶方位をGoss方位へ高度に集積させると、静磁エネルギーが下がり、磁区幅が広がって、渦電流損が高くなる。そこで、かような渦電流損を低減する方法として、前述したような張力コーティングを付与したり、鋼板表層に熱歪みを導入して磁区を細分化し、鉄損を低減する技術が利用されている。
On the other hand, the iron loss can be improved by increasing the purity of the material, high orientation, reducing the plate thickness, adding Si, Al, and subdividing the magnetic domain (for example, Non-Patent Document 1).
However, generally, as the magnetic flux density B 8 increases, the iron loss tends to deteriorate. For example, when the crystal orientation is highly integrated in the Goss orientation for the purpose of improving B 8 , the magnetostatic energy decreases, the domain width increases, and the eddy current loss increases. Therefore, as a method of reducing such eddy current loss, a technique is used in which the above-described tension coating is applied, or a magnetic domain is subdivided by introducing thermal strain into the steel sheet surface layer to reduce iron loss. .
 しかし、例えば、特許文献2に示されるような被膜の張力を向上させる方法では、付与する歪みは弾性域近傍内に限定されて小さく、また張力効果は地鉄の表層部のみにしか作用しないため、十分に鉄損を低減することができない。 However, for example, in the method of improving the tension of the coating as shown in Patent Document 2, the strain to be applied is small and limited within the vicinity of the elastic region, and the tension effect only acts on the surface layer portion of the ground iron. The iron loss cannot be reduced sufficiently.
 一方、熱歪みの導入による磁区細分化は、プラズマ炎やレーザ照射などによって行われている。
 例えば、特許文献3には、一定の条件下でレーザスキャニング照射を行うことで鋼板に熱歪みを付与することにより、また特許文献4には、半価幅10nsec以上、1μsec以下のパルスQスイッチレーザを用い、光強度を1×105~1×108 W/cm2として集光し、間欠的に鋼板に熱歪みを付与することにより、磁区を細分化して鉄損を低減する技術が開示されている。
On the other hand, magnetic domain fragmentation by introduction of thermal strain is performed by plasma flame or laser irradiation.
For example, Patent Document 3 discloses that laser scanning irradiation is performed under certain conditions to impart thermal strain to the steel sheet, and Patent Document 4 discloses a pulse Q-switched laser having a half width of 10 nsec or more and 1 μsec or less. A technology to reduce iron loss by subdividing magnetic domains by concentrating the light intensity of 1 × 10 5 to 1 × 10 8 W / cm 2 and intermittently applying thermal strain to the steel sheet is disclosed. Has been.
 これらの技術は、鋼板表面に熱歪みを導入するため、磁区が細分化されて渦電流損が下がる一方で、ヒステリシス損は増大する。特にパルス照射のような場合、例えば特許文献5に、レーザ照射などによって鋼板表層に生じる硬化領域、すなわち塑性歪み領域が磁壁移動を妨害し、ヒステリシス損失を増加させると記載されている。この場合、歪みが鋼板表層部の一部に局所的に集中し、鉄損の低減効果が十分ではない上に、歪みによるヒステリシス損の増大をもたらして、鉄損低減効果が十分でなく、しかも歪みによる磁歪が増加するという不利益も発生していた。 These techniques introduce thermal strain on the surface of the steel sheet, so that the magnetic domains are subdivided to reduce eddy current loss, while hysteresis loss increases. In particular, in the case of pulse irradiation, for example, Patent Document 5 describes that a hardened region generated in a steel sheet surface layer by laser irradiation or the like, that is, a plastic strain region obstructs domain wall movement and increases hysteresis loss. In this case, the strain concentrates locally on a part of the surface layer of the steel sheet, and the effect of reducing iron loss is not sufficient, and the effect of reducing iron loss is insufficient due to the increase in hysteresis loss due to strain. There was also a disadvantage that magnetostriction due to strain increased.
 このような問題に対して、特許文献5では、レーザ出力やスポット径比を調整し、レーザ走査方向と直角方向の、レーザ照射によって硬化する塑性歪み領域を0.6mm以下に縮小し、ヒステリシス損を低減することで、鉄損の低減を図っている。しかしながら、これらの技術でも、鋼板表面の塑性歪みが磁歪の増加をもたらし、その結果、変圧器の騒音が増大するため、十分な技術とはいえない。 With respect to such a problem, in Patent Document 5, the laser output and the spot diameter ratio are adjusted, the plastic strain region cured by laser irradiation in the direction perpendicular to the laser scanning direction is reduced to 0.6 mm or less, and the hysteresis loss is reduced. By reducing this, iron loss is reduced. However, even in these techniques, the plastic strain on the surface of the steel sheet causes an increase in magnetostriction, and as a result, the noise of the transformer increases.
 また、特許文献6および特許文献7に示される電子ビームを照射する技術の場合、板幅方向へ連続照射されるため、鋼板板幅方向での歪み分布は比較的均一である。しかし、照射された電子は、レーザと異なり鋼板の板厚方向の内部へ深く侵入するため、エネルギー効率はよいものの、鋼板内部で発熱による熱歪みが生じるため、騒音特性が劣化するという問題があった。 Further, in the case of the technique of irradiating the electron beam shown in Patent Document 6 and Patent Document 7, since the irradiation is continuously performed in the plate width direction, the strain distribution in the steel plate width direction is relatively uniform. However, unlike the laser, the irradiated electrons penetrate deeply into the thickness direction of the steel sheet, so energy efficiency is good, but thermal distortion occurs due to heat generation inside the steel sheet, resulting in a problem that noise characteristics deteriorate. It was.
 これを解決するものとして、特許文献8では、照射する電子ビームの電流値、電子ビームの鋼板板幅方向への走行速度、圧延方向における照射ピッチ、電子ビームのビーム径を一定範囲に制御することによって、熱歪みの発生を抑えて騒音と鉄損に優れた方向性電磁鋼板を得る技術を開示している。 In order to solve this, in Patent Document 8, the current value of the electron beam to be irradiated, the traveling speed of the electron beam in the width direction of the steel plate, the irradiation pitch in the rolling direction, and the beam diameter of the electron beam are controlled within a certain range. Discloses a technology for obtaining a grain-oriented electrical steel sheet that is excellent in noise and iron loss by suppressing the occurrence of thermal distortion.
 しかしながら、この技術にしても、変圧器の騒音の原因となる磁歪を低減するには十分とは言えず、より磁歪が小さく鉄損が低い方向性電磁鋼板が求められている。 However, even with this technique, it cannot be said that it is sufficient to reduce the magnetostriction causing the noise of the transformer, and there is a demand for a grain-oriented electrical steel sheet having a smaller magnetostriction and a lower iron loss.
特許第4123679号公報Japanese Patent No. 4123679 特公平2-8027号公報Japanese Patent Publication No. 2-8027 特公平3-13293号公報Japanese Patent Publication No.3-13293 特開平6-57333号公報JP-A-6-57333 特許第4344264号公報Japanese Patent No. 4344264 米国特許第4195750号明細書U.S. Pat.No. 4,195,750 米国特許第4199733号明細書US Patent No. 4199733 特開平5-335128号公報JP-A-5-335128
 一般に、レーザ光照射によって方向性電磁鋼板の磁区を細分化する場合、レーザ光と表面被膜との相互作用が強いため、照射表面近傍における鋼板の急激な熱変形、あるいは被膜の急激な蒸発に伴う鋼板への反力によって、照射部近傍の鋼板に、より転位密度の高い領域が形成される。その結果、鋼板の硬度が増加し、また同時に鋼板が変形してヒステリシス損が増加することが示されている(例えば、非特許文献2)。
 つまり、鋼板表層の照射部近傍に、より転位密度の高い領域を形成させて鋼板に90°磁区を発生させることがこの技術による磁区細分化の基本原理であるので、磁区細分化による渦流損の低減に付随して、必然的にヒステリシス損の増加と磁歪の増大を伴う。すなわち、従来技術のような熱歪みを活用するレーザ光を照射する技術である限り、磁区細分化、低ヒステリシス損化および低磁歪化の全てを鼎立させることはできない。
Generally, when the magnetic domain of a grain-oriented electrical steel sheet is subdivided by laser light irradiation, the interaction between the laser light and the surface film is strong, which is accompanied by rapid thermal deformation of the steel sheet near the irradiated surface or rapid evaporation of the film. Due to the reaction force on the steel plate, a region with a higher dislocation density is formed on the steel plate near the irradiated portion. As a result, it has been shown that the hardness of the steel sheet increases, and at the same time, the steel sheet is deformed to increase the hysteresis loss (for example, Non-Patent Document 2).
In other words, forming a 90 ° magnetic domain in the steel sheet by forming a region with a higher dislocation density in the vicinity of the irradiated part of the steel sheet surface layer is the basic principle of magnetic domain subdivision by this technology. Accompanying the reduction is necessarily accompanied by an increase in hysteresis loss and an increase in magnetostriction. That is, as long as it is a technology for irradiating laser light utilizing thermal distortion as in the prior art, it is not possible to establish all of magnetic domain subdivision, low hysteresis loss, and low magnetostriction.
 一方、電子ビームを照射する技術は、鋼板表面よりも鋼板の内部に電子が浸透するため、鋼板表層の塑性歪みを利用することなく磁区細分化が可能であると考えられる。しかし、電子ビームの強度によっては鋼板の内部においても熱歪みが発生し、ヒステリシス損の増加と磁歪の増大が生じることは特許文献8に記載されるとおりである。したがって、特許文献8に示されるように、電子ビームの面エネルギー密度αと電子ビームの照射部のエネルギー密度β(ビーム走査線上エネルギー密度)を一定の範囲に制御することが必要であるが、この技術では、特許文献8の図2に示される鉄損の最適条件と図3に示される低騒音の最適条件とが大きく異なり、双方ともに最適の条件を見出すには到らず、両特性を同時に改善する技術としては不十分であった。 On the other hand, in the technique of irradiating an electron beam, since electrons penetrate into the steel sheet rather than the steel sheet surface, it is considered that the magnetic domain can be subdivided without using the plastic strain of the steel sheet surface layer. However, as described in Patent Document 8, thermal strain is generated in the steel sheet depending on the intensity of the electron beam, resulting in an increase in hysteresis loss and an increase in magnetostriction. Therefore, as shown in Patent Document 8, it is necessary to control the surface energy density α of the electron beam and the energy density β (energy density on the beam scanning line) of the irradiation part of the electron beam to a certain range. In the technology, the optimum condition of iron loss shown in FIG. 2 of Patent Document 8 and the optimum condition of low noise shown in FIG. 3 are greatly different, and neither of them can find an optimum condition. It was insufficient as a technique to improve.
 発明者らは、一般に鋼板に電子ビームを照射する場合、照射部のエネルギー密度を調整することによって、鉄損と磁歪の両者に共通する最適条件を見出すことが可能と考えた。
 すなわち、特許文献8に開示されるビーム照射線密度βがこれに相当し、βの値を所定の最小値より大きくすることで磁区細分化効果が得られ、また最大値より小さくすることで鋼板表層の塑性歪みを低減でき、その結果、ヒステリシス損と騒音の増大を抑制することができると考えた。
 すなわち、これは特許文献8の図2におけるβ≧10-α/0.06(J/cm2)の領域で優れた鉄損が得られ、特許文献8の図3におけるβ≦11.25-α/0.08(J/cm2)で低騒音が得られることに相当する。
The inventors considered that, in general, when an electron beam is irradiated onto a steel sheet, it is possible to find an optimum condition common to both iron loss and magnetostriction by adjusting the energy density of the irradiated portion.
That is, the beam irradiation linear density β disclosed in Patent Document 8 corresponds to this, and a magnetic domain subdividing effect can be obtained by increasing the value of β from a predetermined minimum value, and by reducing the value from the maximum value, a steel plate It was thought that the plastic strain of the surface layer could be reduced, and as a result, the increase in hysteresis loss and noise could be suppressed.
That is, an excellent iron loss is obtained in the region of β ≧ 10−α / 0.06 (J / cm 2 ) in FIG. 2 of Patent Document 8, and β ≦ 11.25−α / 0.08 in FIG. This corresponds to low noise at J / cm 2 ).
 しかし、磁区細分化や磁壁移動の抑制による磁歪劣化のような磁壁と歪みの相互作用は、磁壁近傍の局所的な物理作用であり、これが特許文献8に示されるような鋼板面全体のエネルギー密度αに依存することは本来的にはあり得ない。
 そこで、βの値の本質的な物理作用を求めて鋭意研究を進めた結果、βの値が大きい場合の磁歪劣化については、鋼板表面での熱歪みによる被膜損傷の発生が関与していること、一方βの値が小さい場合には、照射線領域で照射線方向に細長く伸びた分割磁区の消失が磁区細分化の有無の本質であることが判明した。すなわち、必要な電子ビーム照射エネルギー強度としては、電子ビーム照射線領域で照射線方向に細長く伸び分割された磁区が存在するレベル以上の強度で照射すること、かつ鋼板表面の熱歪みの発生を抑え、鋼板の照射側表面の被膜損傷の発生を抑制し、さらに塑性歪領域を形成しない強度レベルで照射することが、本質的な技術であることが解明された。
However, the interaction between the domain wall and strain, such as magnetostriction degradation due to suppression of domain subdivision and domain wall movement, is a local physical action in the vicinity of the domain wall, and this is the energy density of the entire steel plate surface as shown in Patent Document 8. It is inherently impossible to depend on α.
Therefore, as a result of diligent research seeking the essential physical action of the value of β, the occurrence of film damage due to thermal strain on the steel sheet surface is involved in magnetostriction degradation when the value of β is large. On the other hand, when the value of β is small, it has been found that the disappearance of the divided magnetic domains elongated in the irradiation line direction in the irradiation line region is the essence of the presence or absence of magnetic domain subdivision. In other words, the required electron beam irradiation energy intensity is such that the irradiation is performed at an intensity higher than the level at which the magnetic domains elongated and divided in the direction of the irradiation line exist in the electron beam irradiation line region, and the occurrence of thermal distortion on the steel sheet surface is suppressed. It has been clarified that it is an essential technique to suppress the occurrence of film damage on the irradiation side surface of the steel sheet and to perform irradiation at a strength level that does not form a plastic strain region.
 表1は、板厚が0.23mmで、B8が1.943T、鉄損W17/50が0.85W/kgの方向性電磁鋼板に電子ビームを照射するに当たり、加速電圧Vkを40kV~120kV、ビーム電流Iを0.5~8mA、ビーム径dを0.015~0.040cm、走査速度Vを900~5000cm/s、圧延方向の照射線間隔Lを0.5cmとして、β=(Vk・I)/(V・d)を0.43から24.7(J/cm2)まで種々に変更させて照射し、この時の鋼板表面の被膜損傷および照射線領域方向に細く伸びた分割磁区の形成の有無、ならびに鋼板の鉄損とヒステリシス損および磁歪λp-pについて調べた結果を示したものである。 Table 1 shows that the acceleration voltage Vk is 40 kV to 120 kV and the beam is radiated to the directional electrical steel sheet with a plate thickness of 0.23 mm, B 8 of 1.943 T, and iron loss W 17/50 of 0.85 W / kg. Assuming that the current I is 0.5 to 8 mA, the beam diameter d is 0.015 to 0.040 cm, the scanning speed V is 900 to 5000 cm / s, and the irradiation interval L in the rolling direction is 0.5 cm, β = (Vk · I) / (V · d ) Is varied from 0.43 to 24.7 (J / cm 2 ), and the coating damage on the steel sheet surface at this time, the presence or absence of the formation of split magnetic domains extending in the direction of the irradiation line, and the iron loss of the steel sheet The results of examining the hysteresis loss and magnetostriction λp-p are shown.
Figure JPOXMLDOC01-appb-T000001
Figure JPOXMLDOC01-appb-T000001
 表1に示されるように、鉄損やヒステリシス損および磁歪の良好な範囲としては、照射部のエネルギー密度の下限値は照射方向に細長く伸びた分割磁区が存在する(非特許文献3)下限値であり、一方、エネルギー密度の上限値は被膜の損傷が発生しない上限値であることが示される。また、鉄損の最小となる条件(条件番号8、9)と磁歪の最小となる条件(条件番号5、6)は必ずしも一致しないことが表1より分かる。 As shown in Table 1, as a good range of iron loss, hysteresis loss, and magnetostriction, the lower limit value of the energy density of the irradiated portion includes a divided magnetic domain elongated in the irradiation direction (Non-Patent Document 3). On the other hand, it is indicated that the upper limit value of the energy density is an upper limit value at which damage to the coating does not occur. Further, it can be seen from Table 1 that the conditions that minimize the iron loss (condition numbers 8 and 9) do not necessarily match the conditions that minimize the magnetostriction (condition numbers 5 and 6).
 そこで、次に、鉄損の最小値と磁歪の最小値を同一の照射条件で実現できる電子ビームの照射方法について鋭意研究を行った。その結果、圧延方向に交差する方向の線領域に電子ビームを照射するに際して、従来のように照射線領域が連続・均一である照射条件とせず、滞留領域と走行領域の2種類の照射条件の組合せとし、この組合せ単位を繰返し、かつ連結させて照射線領域(変調照射線領域と呼称する)とすることで、鉄損の最小値と磁歪の最小値を同一の照射条件で実現できることを新たに見出した。 Therefore, intensive research was then conducted on an electron beam irradiation method capable of realizing the minimum value of iron loss and the minimum value of magnetostriction under the same irradiation conditions. As a result, when irradiating an electron beam to a line region in a direction intersecting with the rolling direction, the irradiation region is not continuous and uniform as in the conventional case, but two types of irradiation conditions, a stagnant region and a traveling region, are used. It is a new combination that the minimum value of iron loss and the minimum value of magnetostriction can be realized under the same irradiation conditions by combining and repeating this combination unit and connecting them to form an irradiation region (referred to as a modulated irradiation region). I found it.
 その端緒となった実験について以下に述べる。
 板厚が0.23mmで、B8が1.943T、鉄損W17/50が0.85W/kgである方向性電磁鋼板に、加速電圧Vk:50kV、ビーム電流I:8mA、ビーム径d:0.30mm、走査速度V:25m/secで、圧延方向の照射線間隔Lを2.5~30mmに変更して電子ビームを照射した。その際、一方は一定照射条件(条件1)で連続照射を行って比較例とした。他方は、図1に示すようにビームの滞留領域:1と走行領域:2の合計領域0.50mmを繰返し単位:3(繰返し単位の周期でもある)として鋼板板幅方向へ繰返し照射して変調照射線領域を形成する照射条件(条件2)で照射した。なお、この時、滞留点での滞留時間を0.020msecとし、平均走査速度が25m/secとなるように走行領域:2での走行速度を調節した。
 上記の条件1、2で電子ビーム照射を行ったときの、照射線領域の圧延方向の間隔Lと鉄損および磁歪との関係について調べた結果を、図2に示す。
The experiment that led to this is described below.
In plate thickness 0.23 mm, B 8 is 1.943T, iron loss W 17/50 is oriented electrical steel sheet is 0.85 W / kg, the acceleration voltage Vk: 50 kV, beam current I: 8 mA, beam diameter d: 0.30 mm The scanning speed V was 25 m / sec, the irradiation line interval L in the rolling direction was changed to 2.5 to 30 mm, and the electron beam was irradiated. At that time, one of them was continuously irradiated under a constant irradiation condition (condition 1) to obtain a comparative example. On the other hand, as shown in FIG. 1, modulated irradiation is performed by repeatedly irradiating a total area of 0.50 mm of a beam residence area: 1 and a traveling area: 2 as a repeating unit: 3 (which is also a period of the repeating unit) in the width direction of the steel sheet. Irradiation was performed under irradiation conditions (condition 2) for forming a line region. At this time, the dwell time at the dwell point was 0.020 msec, and the running speed in the running region: 2 was adjusted so that the average scanning speed was 25 m / sec.
FIG. 2 shows the results of examining the relationship between the distance L in the rolling direction of the irradiated region and the iron loss and magnetostriction when the electron beam irradiation is performed under the above conditions 1 and 2.
 図2から明らかなように、本発明法に従い照射した場合(条件2)は、従来の連続照射の場合(条件1)に比較して、鉄損や磁歪の到達最良値に優れるばかりでなく、両者の最良値がほぼ等しい照射条件(照射線領域の圧延方向の間隔:4.0~12.5mm)で得られていることが分かる。
 この結果は、磁区細分化処理を施した方向性電磁鋼板を使用して、低鉄損でかつ低騒音な変圧器を同一の材料で得られることを意味しており、今までにない工業的な意味の大きい優れた技術であることが分かる。
 本発明は、上記の知見を基にさらに研究を重ねた末に完成されたものである。
As is clear from FIG. 2, when irradiated according to the method of the present invention (Condition 2), not only the ultimate values of iron loss and magnetostriction are excellent compared to the conventional continuous irradiation (Condition 1), It can be seen that the best values of both are obtained under irradiation conditions (interval in the rolling direction of the irradiation region: 4.0 to 12.5 mm).
This result means that using a grain-oriented electrical steel sheet that has been subjected to magnetic domain refinement treatment, a transformer with low iron loss and low noise can be obtained with the same material. It can be seen that this is an excellent technology with a large meaning.
The present invention has been completed after further research based on the above findings.
 すなわち、本発明の要旨構成は次のとおりである。
1.鋼板表面に対し、圧延方向と交差する方向の線領域に電子ビームを照射し、該照射線領域を滞留領域と走行領域からなる2種類の領域を繰返し単位とする変調照射線領域とし、かつ該変調照射線領域を圧延方向に間隔を設けて繰返すことによる磁区細分化を施した方向性電磁鋼板において、
 該繰返し単位を線領域方向に連結させた変調照射線領域とし、
 該繰返し単位の該変調照射線領域における周期を0.20~1.0mmとし、
 該変調照射線領域の圧延方向の繰返し間隔を4.0~12.5mmとし、さらに
 電子ビームの強度を、少なくとも照射面側に該変調照射線領域方向に細長く伸びた分割磁区が形成される強度以上で、かつ照射面側に被膜損傷の発生および塑性歪み領域の形成が生じない強度までとした低騒音変圧器用の方向性電磁鋼板。
That is, the gist configuration of the present invention is as follows.
1. The surface of the steel sheet is irradiated with an electron beam in a line area in a direction intersecting the rolling direction, the irradiation line area is set as a modulated irradiation line area having two types of areas consisting of a stay area and a running area as repeating units, and In the grain-oriented electrical steel sheet subjected to magnetic domain subdivision by repeating the modulation irradiation region in the rolling direction with an interval,
A modulated irradiation region in which the repeating units are connected in the direction of the line region,
The period in the modulated irradiation region of the repeating unit is 0.20 to 1.0 mm,
The repetition interval in the rolling direction of the modulated irradiation region is set to 4.0 to 12.5 mm, and the intensity of the electron beam is at least equal to or more than the strength at which the elongated magnetic domains extending in the direction of the modulated irradiation region are formed on the irradiation surface side. A grain-oriented electrical steel sheet for a low-noise transformer that has a strength that prevents the occurrence of film damage and the formation of a plastic strain region on the irradiated surface side.
2.前記繰返し単位の前記変調照射線領域における周期を0.25~0.80mmとし、さらに
 前記変調照射線領域の圧延方向の繰返し間隔を5.0~10mmとした前記1に記載の低騒音変圧器用の方向性電磁鋼板。
2. 2. The grain-oriented electrical steel sheet for a low noise transformer according to 1 above, wherein a period of the repeating unit in the modulated irradiation region is 0.25 to 0.80 mm, and a repetition interval in the rolling direction of the modulated irradiation region is 5.0 to 10 mm. .
3.鋼板表面に対し、圧延方向と交差する方向の線領域に電子ビームを照射し、該照射線領域を滞留領域と走行領域からなる2種類の領域を繰返し単位とする変調照射線領域とし、かつ該変調照射線領域を圧延方向に間隔を設けて繰返すことからなる磁区細分化処理を施して方向性電磁鋼板を製造するに際し、
 該繰返し単位を線領域方向に連結させた変調照射線領域とし、
 該繰返し単位の該変調照射線領域における周期を0.20~1.0mmとし、
 該変調照射線領域の圧延方向の繰返し間隔を4.0~12.5mmとし、さらに
 電子ビームの強度を、少なくとも照射面側に該変調照射線領域方向に細長く伸びた分割磁区が形成される強度以上で、かつ照射面側に被膜損傷の発生および塑性歪み領域の形成が生じない強度までとする低騒音変圧器用の方向性電磁鋼板の製造方法。
3. The surface of the steel sheet is irradiated with an electron beam in a line area in a direction intersecting the rolling direction, the irradiation line area is set as a modulated irradiation line area having two types of areas consisting of a stay area and a running area as repeating units, and When producing a grain-oriented electrical steel sheet by applying a magnetic domain refinement process consisting of repeating the modulation irradiation region in the rolling direction with an interval,
A modulated irradiation region in which the repeating units are connected in the direction of the line region,
The period in the modulated irradiation region of the repeating unit is 0.20 to 1.0 mm,
The repetition interval in the rolling direction of the modulated irradiation region is set to 4.0 to 12.5 mm, and the intensity of the electron beam is at least equal to or more than the strength at which the elongated magnetic domains extending in the direction of the modulated irradiation region are formed on the irradiation surface side. And the manufacturing method of the grain-oriented electrical steel sheet for low noise transformers made into the intensity | strength which does not produce generation | occurrence | production of a film damage and the formation of a plastic strain area | region on the irradiation surface side.
4.前記繰返し単位の前記変調照射線領域における周期を0.25~0.80mmとし、さらに
 前記変調照射線領域の圧延方向の繰返し間隔を5.0~10mmとする前記3に記載の低騒音変圧器用の方向性電磁鋼板の製造方法。
4). 4. The grain-oriented electrical steel sheet for low noise transformers according to 3 above, wherein a period of the repeating unit in the modulated irradiation region is 0.25 to 0.80 mm, and a repetition interval in the rolling direction of the modulated irradiation region is 5.0 to 10 mm. Manufacturing method.
 本発明によれば、従来困難とされた、変圧器の低鉄損と低騒音を同時に満たす条件での磁区細分化処理の実施が可能となり、しかも従来にない低鉄損で低磁歪の方向性電磁鋼板を得ることができるので、変圧器におけるエネルギー使用効率の向上と共に、騒音の抑制も併せて達成することができ、産業上極めて有用である。 According to the present invention, it is possible to carry out magnetic domain subdivision processing under conditions that satisfy both the low iron loss and low noise of the transformer, which has been difficult in the past, and the direction of low magnetostriction with low iron loss that has not been achieved conventionally. Since the electromagnetic steel sheet can be obtained, the energy use efficiency in the transformer can be improved and the noise can be suppressed, which is extremely useful industrially.
鋼板板幅方向に電子ビームを照射する際における、本発明の特徴である変調照射線領域と、繰り返し単位をなす滞留領域および走行領域を示す図である。It is a figure which shows the staying area | region and traveling area | region which make the modulated irradiation area | region which is the characteristics of this invention, and the repeating unit when irradiating an electron beam to a steel plate width direction. 連続的に電子ビームを照射する従来の磁区細分化技術(条件1)と、変調照射線領域を繰り返して電子ビームを照射する本発明の磁区細分化技術(条件2)において、照射線領域の圧延方向の間隔Lと磁区細分化処理後の方向性電磁鋼板の磁歪λp-pおよび鉄損W17/50との関係を示す図である。In the conventional magnetic domain subdivision technique (condition 1) for continuously irradiating an electron beam, and in the magnetic domain subdivision technique (condition 2) of the present invention for irradiating an electron beam by repeating a modulated irradiation region, rolling of the irradiation region is performed. It is a figure which shows the relationship between the space | interval L of a direction, the magnetostriction ( lambda) p-p of the grain -oriented electrical steel sheet after a magnetic domain refinement process, and the iron loss W17 / 50 . 鋼板板幅方向に電子ビームを照射する際に、連続的に電子ビームを照射する従来技術による照射線領域を示す図である。It is a figure which shows the irradiation line area | region by the prior art which irradiates an electron beam continuously, when irradiating an electron beam to a steel plate width direction. 実施例において製作した変圧器の鉄心のサイズと形状を示す図である。It is a figure which shows the size and shape of the iron core of the transformer manufactured in the Example. 実施例において製作した変圧器の鉄心の斜角切断後の鋼片のサイズと形状を示す図である。It is a figure which shows the size and shape of the steel piece after the bevel cutting of the iron core of the transformer manufactured in the Example.
 以下、本発明を具体的に説明する。
〔被照射材〕
 本発明における照射対象は方向性電磁鋼板である。通常、方向性電磁鋼板には、地鉄の上にあるフォルステライト被膜の上から張力コーティングなどの絶縁コーティングが施されているが、本発明では、地鉄と絶縁コーティングとの間にフォルステライト被膜が存在していなくても問題はない。
Hereinafter, the present invention will be specifically described.
[Irradiated material]
The irradiation object in the present invention is a grain-oriented electrical steel sheet. Usually, the grain-oriented electrical steel sheet is provided with an insulation coating such as a tension coating on the forsterite film on the ground iron. In the present invention, the forsterite film is provided between the ground iron and the insulation coating. There is no problem even if is not present.
〔照射線の種類〕
 本発明では、上記した方向性電磁鋼板の表面に、圧延方向に交差する方向に、かつ圧延方向に間隔を設けて、電子ビームを走査することによって、磁区細分化処理を施すが、鋼板に対する歪み導入手段としては電子ビーム照射に限られる。電子ビーム以外では、鋼板表面に存在する絶縁コーティングとの相互作用が大きく、絶縁コーティングの損傷やその直下の地鉄表層部に高転位密度からなる塑性歪みが導入されるため、ヒステリシス損の劣化、すなわち鉄損の劣化を招き、最良の鉄損特性を得ることができない。
 これに対し、電子ビームを使用した場合、電子ビームの動的作用によって絶縁コーティングとの相互作用が小さく限定され、鋼板内部の地鉄との相互作用が大きくなる。したがって、絶縁コーティングの損傷やフォルステライト被膜あるいはコーティング直下の地鉄表層部に高転位密度からなる塑性歪みの導入がない状態で磁区細分化効果を付与することが可能となる。
[Types of radiation]
In the present invention, the magnetic domain refinement process is performed by scanning the surface of the grain-oriented electrical steel sheet with an electron beam in a direction intersecting with the rolling direction and at intervals in the rolling direction. The introduction means is limited to electron beam irradiation. Other than the electron beam, the interaction with the insulation coating existing on the surface of the steel plate is large, and the damage of the insulation coating and the plastic strain consisting of high dislocation density are introduced into the surface layer of the underlying iron, so the deterioration of hysteresis loss, That is, the iron loss is deteriorated and the best iron loss characteristic cannot be obtained.
On the other hand, when an electron beam is used, the interaction with the insulating coating is limited to a small size due to the dynamic action of the electron beam, and the interaction with the ground iron inside the steel plate is increased. Therefore, it is possible to impart the magnetic domain refinement effect without damage of the insulating coating, the forsterite film, or the introduction of plastic strain having a high dislocation density in the surface layer of the base iron immediately below the coating.
 また、電子ビームを照射する鋼板面は、鋼板の片面でもよいし、両面であってもよい。また、圧延方向に交差する方向とは、圧延方向に対し直角方向、すなわち鋼板の板幅方向を90°とすると、75°から105°の範囲であり、この範囲であれば本発明の効果が好適に発揮される。 Further, the steel plate surface irradiated with the electron beam may be one side of the steel plate or both sides. Further, the direction intersecting the rolling direction is a direction perpendicular to the rolling direction, that is, a range of 75 ° to 105 ° when the sheet width direction of the steel sheet is 90 °. It is suitably exhibited.
〔変調照射線領域〕
 圧延方向に交差する方向に電子ビームを走査して、電子ビームの照射線領域を形成するが、この照射線領域は、一定の照射条件で照射するいわゆる図3に示すような連続照射ではなく、図1に示したような滞留領域1と走行領域2からなる2種類の領域を繰返し単位として、この繰返し単位を照射線領域方向に連結させて繰返すことにより形成される変調照射線領域とすることが、本発明の最も肝要な技術である。
 交差する方向に照射する電子ビームの照射が一定の照射条件で施されるいわゆる連続照射の場合には、図2において条件1として示したように、ほぼ同一の照射条件で最良の鉄損値と最良の磁歪特性を得ることができず、その結果、同一の変圧器で低鉄損と低騒音を満足するものを得ることはできなかった。
[Modulated irradiation area]
An electron beam is scanned in a direction crossing the rolling direction to form an irradiation region of the electron beam, but this irradiation region is not continuous irradiation as shown in FIG. The two types of regions consisting of the stay region 1 and the travel region 2 as shown in FIG. 1 are used as repeating units, and the repeating units are connected in the direction of the irradiation region and repeated to form a modulated irradiation region. However, this is the most important technique of the present invention.
In the case of so-called continuous irradiation in which the irradiation of the electron beam irradiated in the intersecting direction is performed under a constant irradiation condition, as shown as condition 1 in FIG. The best magnetostriction characteristics could not be obtained, and as a result, the same transformer with low iron loss and low noise could not be obtained.
 同一の照射条件で最良の鉄損値と最良の磁歪特性を得ることにより、同一の変圧器で低鉄損と低騒音を同時に満足させるためには、連続照射ではなく、滞留領域と走行領域からなる2種類の領域を繰返し単位として、この繰返し単位を照射線領域方向に、図1に示したように連結して繰返してなる変調照射線領域とすることが重要である。図中、符号1が滞留領域、2が走行領域、3が繰返し単位(滞留点間隔)であり、dでビーム径を示す。
 ここに、変調照射線領域における繰返し単位の周期は0.20~1.0mmとする必要がある。この繰返し単位の周期が0.20mmに満たないと、磁区幅が狭くなりすぎて鉄損および磁歪が増加し、逆に1.0mmよりも大きいと、磁区幅が広くなりすぎるので十分な磁区細分化効果が得られない。したがって、繰返し単位の周期は0.20~1.0mmとする。好ましくは0.25~0.80mmの範囲である。また、繰返し単位の各単位間が連結してなく、離散している場合は、非照射領域において十分な磁区細分化効果が得られないので、繰返し単位は連結していることも必須の要件である。
In order to satisfy the low iron loss and low noise at the same time with the same transformer by obtaining the best iron loss value and the best magnetostriction characteristics under the same irradiation conditions, it is not from continuous irradiation but from the staying area and the running area. It is important to use the two types of regions as repeating units, and to connect the repeating units in the direction of the irradiation line region as shown in FIG. In the figure, reference numeral 1 is a staying region, 2 is a traveling region, 3 is a repeating unit (spacing point interval), and d indicates a beam diameter.
Here, the period of the repeating unit in the modulated irradiation region needs to be 0.20 to 1.0 mm. If the period of this repeating unit is less than 0.20 mm, the magnetic domain width becomes too narrow and the iron loss and magnetostriction increase, and conversely if it is larger than 1.0 mm, the magnetic domain width becomes too wide, so that sufficient magnetic domain refinement effect is achieved. Cannot be obtained. Therefore, the period of the repeating unit is 0.20 to 1.0 mm. The range is preferably 0.25 to 0.80 mm. In addition, when the units of the repeating unit are not connected and are discrete, a sufficient magnetic domain subdivision effect cannot be obtained in the non-irradiated region. Therefore, it is also an essential requirement that the repeating units are connected. is there.
 また、上記した変調照射線領域の圧延方向の繰返し間隔は4.0~12.5mmとすることが必要である。
 この変調照射線領域の圧延方向の繰返し間隔が4.0mm未満の場合、図2に示したように鉄損が増大し、かつ磁歪も劣化する。逆に12.5mmを超える場合も、鉄損が増大し、かつ磁歪も劣化するので、圧延方向繰返し間隔を4.0~12.5mmとする必要がある。好ましくは5.0~10mmの範囲である。
Further, the repetition interval in the rolling direction of the above-described modulated irradiation region needs to be 4.0 to 12.5 mm.
When the repetition interval in the rolling direction of the modulated irradiation region is less than 4.0 mm, the iron loss increases as shown in FIG. 2, and the magnetostriction also deteriorates. On the other hand, if it exceeds 12.5 mm, the iron loss increases and the magnetostriction also deteriorates, so the repeat interval in the rolling direction must be 4.0 to 12.5 mm. The range is preferably 5.0 to 10 mm.
 本発明において、電子ビームのビーム径dは特に限定されるものではないが、ビーム径dがあまりに小さいと分割磁区の生成に不利であり、一方あまりに大きいと分割磁区が過大に生成するので、ビーム径dは0.05~0.5mm程度とすることが好ましい。
 また、本発明では、電子ビームの加速電圧についても特に制限されるものではないが、加速電圧があまりに小さいと鋼板の内部への電子の浸透が不十分であり、一方あまりに大きいと電子銃や電源設備などの製造コストが多大になるので、加速電圧は30~300kV程度とすることが好ましい。
In the present invention, the beam diameter d of the electron beam is not particularly limited. However, if the beam diameter d is too small, it is disadvantageous for the generation of the divided magnetic domain, while if too large, the divided magnetic domain is excessively generated. The diameter d is preferably about 0.05 to 0.5 mm.
In the present invention, the acceleration voltage of the electron beam is not particularly limited, but if the acceleration voltage is too small, the penetration of electrons into the steel plate is insufficient, while if too large, the electron gun or the power source Since the manufacturing cost of equipment and the like becomes large, the acceleration voltage is preferably about 30 to 300 kV.
〔照射線のエネルギー密度〕
 次に、電子ビームの強度については、特許文献8に開示されるビーム照射線密度βの値により定めるよりも、少なくとも照射面側にこの変調照射線領域方向に細長く伸びた分割磁区が形成される強度をもって下限値とし、照射面側に被膜損傷が発生しない強度をもって上限値とする技術を用いる方が簡便、かつ実用的である。
 そこで、本発明では、この技術を採用するものとした。
[Energy density of radiation]
Next, with respect to the intensity of the electron beam, a divided magnetic domain extending elongated in the direction of the modulated irradiation line region is formed at least on the irradiation surface side rather than being determined by the value of the beam irradiation line density β disclosed in Patent Document 8. It is simpler and more practical to use a technique in which the intensity is set to the lower limit value and the intensity is set to the upper limit value so that no film damage occurs on the irradiated surface side.
Therefore, this technique is adopted in the present invention.
〔変圧器の鉄損および騒音の評価〕
 変圧器の鉄損および騒音は、図4に示すような三相三脚の積み鉄心型の変圧器を用いて評価した。図4に示したように、変圧器の外形は500mm角、幅100mmの鋼板で構成される。鋼板を図5に示すような形状に斜角切断し、積み厚を100mmとして積層し、バンドで締付け、その後2次コイルおよび1次コイルを鋼板の脚部に巻き、絶縁油を入れたタンクに装入して測定器具を接続し、測定を行った。
 三相は120°位相をずらして1次コイルを用いて励磁を行い、2次コイルに発生する誘導電圧値から鉄心重量より断面積を求めて、鉄心の磁束密度1.7Tにおける鉄損および騒音を測定した。騒音は、変圧器の周囲で発生する振動音をマイクで収録し、Aスケール補正を行ったdBA単位で表した。また、鉄損は、2次コイルを開放状態とした無負荷状態の1次コイル側の電圧と電流値より銅損分を差し引いて変圧器の重量当たりの損失で表した。
[Evaluation of transformer iron loss and noise]
The iron loss and noise of the transformer were evaluated using a three-phase tripod stacked iron core type transformer as shown in FIG. As shown in FIG. 4, the outer shape of the transformer is composed of a steel plate having a 500 mm square and a width of 100 mm. Cut the steel plate into the shape shown in Fig. 5 and stack it with a stacking thickness of 100mm, tighten it with a band, and then wind the secondary coil and primary coil around the legs of the steel plate and put it in a tank filled with insulating oil The measurement was carried out by connecting the measuring instrument.
The three phases are excited by using a primary coil with a 120 ° phase shift, and the cross-sectional area is obtained from the weight of the iron core generated from the induced voltage generated in the secondary coil. It was measured. The noise was expressed in dBA units where vibrations generated around the transformer were recorded with a microphone and A scale correction was performed. The iron loss was expressed as a loss per weight of the transformer by subtracting the copper loss from the voltage and current value on the primary coil side in the unloaded state with the secondary coil open.
(実施例1)
 鋼板表面にフォルステライト被膜を有し、その上に張力コーティングを焼付けた板厚:0.23mm、磁束密度B8:1.942T、鉄損W17/50:0.870W/kgの方向性電磁鋼板を6分割し、それぞれに次の条件で磁区細分化処理を施した。
 磁区細分化手段としては、加速電圧:60kVで、ビーム電流:12mA、ビーム径:0.30mmの電子ビーム照射を用い、板幅方向に一定の照射条件で連続的に40m/secの走査速度で照射し、かつ一つは圧延方向における間隔を5.0mm(比較例A1)、他の一つは7.5mm(比較例A2)として照射し、比較例とした。これらの比較例においては、一部コーティングが剥落した箇所が確認された。
Example 1
Has a forsterite film on the steel sheet surface, the sheet thickness was baked tension coating thereon: 0.23 mm, the magnetic flux density B 8: 1.942T, iron loss W 17/50: oriented electrical steel sheet 0.870W / kg 6 Each was divided and subjected to magnetic domain refinement treatment under the following conditions.
As magnetic domain subdivision means, electron beam irradiation with acceleration voltage: 60kV, beam current: 12mA, beam diameter: 0.30mm is used, and irradiation is performed continuously at a scanning speed of 40m / sec under constant irradiation conditions in the plate width direction. And one was irradiated with an interval in the rolling direction of 5.0 mm (Comparative Example A1) and the other was 7.5 mm (Comparative Example A2). In these comparative examples, a part where the coating partly peeled off was confirmed.
 次に、他の二つは、上記と同じ条件の電子ビームを照射したが、滞留時間:0.010msecで滞留点間隔:0.40mmを滞留領域および走行領域の繰返し単位とし、板幅方向に繰返し単位を連結させ、平均走査速度:40m/secで変調照射線領域を形成した。この時、一つは圧延方向の繰返し間隔を5.0mm(発明例A3)、他の一つは7.5mm(発明例A4)として照射し、発明例とした。これらの発明例においては、コーティングの損傷は認められず、またビッター法による磁区観察により、板幅方向に細長く伸びかつ分割された磁区が照射線領域上に観察された。 Next, the other two were irradiated with an electron beam under the same conditions as above, but the residence time was 0.010 msec, the residence point interval was 0.40 mm, and the residence unit and the running region were repeated units. And a modulated irradiation region was formed at an average scanning speed of 40 m / sec. At this time, one was irradiated with a repetition interval in the rolling direction of 5.0 mm (Invention Example A3), and the other was 7.5 mm (Invention Example A4). In these inventive examples, no damage to the coating was observed, and magnetic domains that were elongated and divided in the plate width direction were observed on the irradiated region by magnetic domain observation by the bitter method.
 残る二つは、Qスイッチを具備したNd:YAGレーザ装置を用いて、鋼板の板幅方向に不連続なパルス照射を実施した。この時の照射条件は、従来から公知の条件、すなわちレーザパルスのエネルギーとして3.3mJ/パルス、レーザスポットのサイズは直径:0.18mmの円形、板幅方向の照射間隔は0.3mm、レーザ波長は1064nmとした。圧延方向における照射間隔は、一つを5.0mm(比較例A5)、他の一つは7.5mm(比較例A6)として照射した。これらの比較例にはレーザビームを受光した場所に明瞭な円形のコーティング欠損と地鉄の裸出が認められたので、絶縁性の向上のために絶縁コートを薄く再塗布し、低温で焼付けた。 The remaining two were subjected to discontinuous pulse irradiation in the plate width direction of the steel sheet using an Nd: YAG laser device equipped with a Q switch. The irradiation conditions at this time are conventionally known conditions, that is, the laser pulse energy is 3.3 mJ / pulse, the laser spot size is a circle with a diameter of 0.18 mm, the irradiation interval in the plate width direction is 0.3 mm, and the laser wavelength is 1064 nm. It was. One irradiation interval in the rolling direction was 5.0 mm (Comparative Example A5), and the other was 7.5 mm (Comparative Example A6). In these comparative examples, a clear circular coating defect and bare iron bareness were observed in the place where the laser beam was received, so the insulating coating was thinly reapplied and baked at a low temperature to improve insulation. .
 これら6種類の磁区細分化された方向性電磁鋼板は、一部を鉄損と磁歪の測定に供すると共に、残りの鋼板を用いて前述した方法で変圧器を製作し、1.7Tにおける鉄損と騒音を測定した。その結果を表2に示す。 These six types of grain-oriented grain-oriented electrical steel sheets are partly used for measuring iron loss and magnetostriction, and the remaining steel sheets are used to manufacture transformers by the method described above. Noise was measured. The results are shown in Table 2.
Figure JPOXMLDOC01-appb-T000002
Figure JPOXMLDOC01-appb-T000002
 表2に示したように、本発明に従って磁区細分化を施した方向性電磁鋼板は、比較例に比べて、鉄損特性および磁歪特性に優れ、かつ変圧器の鉄損および騒音特性にも優れている。さらに、注目すべき点は、圧延方向における照射間隔を7.5mmとした場合は、比較例とは異なり、鉄損と騒音がともに最良値を示しており、変圧器用の方向性電磁鋼板として優れた効果を有することが分かる。 As shown in Table 2, the grain-oriented electrical steel sheet subjected to magnetic domain subdivision according to the present invention is superior in iron loss characteristics and magnetostriction characteristics and also in transformer iron loss and noise characteristics as compared with the comparative example. ing. Furthermore, it should be noted that when the irradiation interval in the rolling direction is set to 7.5 mm, unlike the comparative example, both the iron loss and the noise show the best values, and it is excellent as a grain-oriented electrical steel sheet for a transformer. It turns out that it has an effect.
(実施例2)
 鋼板表面にフォルステライト被膜を有し、その上に張力コーティングを焼付けた板厚:0.27mm、磁束密度B8:1.949T、鉄損W17/50:0.903W/kgの方向性電磁鋼板を6分割し、それぞれに次の条件で磁区細分化処理を施した。
 磁区細分化手段としては、加速電圧:50kVで、ビーム電流:12mA、ビーム径:0.20mmの電子ビーム照射を用い、板幅方向に一定の照射条件で連続的に30m/secの走査速度で照射し、かつ一つは圧延方向における間隔を5.0mm(比較例B1)、他の一つは7.5mm(比較例B2)として照射し、比較例とした。これらの比較例においては、一部コーティングが剥落した箇所が確認された。
(Example 2)
Has a forsterite film on the steel sheet surface, the sheet thickness was baked tension coating thereon: 0.27 mm, the magnetic flux density B 8: 1.949T, iron loss W 17/50: oriented electrical steel sheet 0.903W / kg 6 Each was divided and subjected to magnetic domain refinement treatment under the following conditions.
As magnetic domain subdivision means, electron beam irradiation with acceleration voltage: 50kV, beam current: 12mA, beam diameter: 0.20mm is used, and irradiation is continuously performed at a scanning speed of 30m / sec under constant irradiation conditions in the plate width direction. And one was irradiated with an interval in the rolling direction of 5.0 mm (Comparative Example B1) and the other was 7.5 mm (Comparative Example B2). In these comparative examples, a part where the coating partly peeled off was confirmed.
 次に、他の二つは、上記と同じ条件の電子ビームを照射したが、滞留時間:0.010msecで滞留点間隔:0.30mmを滞留領域および走行領域の繰返し単位とし、板幅方向に繰返し単位を連結させ、平均走査速度:30m/secで変調照射線領域を形成した。この時、一つは圧延方向の繰返し間隔を5.0mm(発明例B3)、他の一つは7.5mm(発明例B4)として照射し、発明例とした。これらの発明例においては、コーティングの損傷は認められず、またビッター法による磁区観察により、板幅方向に細長く伸びかつ分割された磁区が照射線領域上に観察された。 Next, the other two were irradiated with an electron beam under the same conditions as above, but the residence time: 0.010 msec and the residence point interval: 0.30 mm was used as the repeat unit for the residence region and travel region, and the repeat unit in the plate width direction. And a modulated irradiation region was formed at an average scanning speed of 30 m / sec. At this time, one was irradiated with a repetition interval in the rolling direction of 5.0 mm (Invention Example B3), and the other was 7.5 mm (Invention Example B4). In these inventive examples, no damage to the coating was observed, and magnetic domains that were elongated and divided in the plate width direction were observed on the irradiated region by magnetic domain observation by the bitter method.
 残る二つは、Qスイッチを具備したNd:YAGレーザ装置を用いて、鋼板の板幅方向に不連続なパルス照射を施した。この時の照射条件は、従来から公知の条件、すなわちレーザパルスのエネルギーとして4.5mJ/パルス、レーザスポットのサイズは直径:0.22mmの円形、板幅方向の照射間隔は0.3mm、レーザ波長は1064nmとした。圧延方向における照射間隔は、一つを5.0mm(比較例B5)、他の一つは7.5mm(比較例B6)として照射した。これらの比較例には、レーザビームを受光した場所に明瞭な円形のコーティング欠損と地鉄の裸出が認められたので、絶縁性の向上のために絶縁コートを薄く再塗布し、低温で焼付けた。 The remaining two were subjected to discontinuous pulse irradiation in the plate width direction of the steel sheet using an Nd: YAG laser device equipped with a Q switch. The irradiation conditions at this time are conventionally known conditions, that is, the laser pulse energy is 4.5 mJ / pulse, the laser spot size is a circle with a diameter of 0.22 mm, the irradiation interval in the plate width direction is 0.3 mm, and the laser wavelength is 1064 nm. It was. One irradiation interval in the rolling direction was 5.0 mm (Comparative Example B5), and the other was 7.5 mm (Comparative Example B6). In these comparative examples, a clear circular coating defect and bare iron bareness were observed in the place where the laser beam was received, so the insulation coating was thinly reapplied and baked at a low temperature to improve insulation. It was.
 これら6種類の磁区細分化された方向性電磁鋼板は、一部を鉄損と磁歪の測定に供すると共に、残りの鋼板を用いて前述した方法で変圧器を製作し、1.7Tにおける鉄損と騒音を測定した。その結果を表3に示す。 These six types of grain-oriented grain-oriented electrical steel sheets are partly used for measuring iron loss and magnetostriction, and the remaining steel sheets are used to manufacture transformers by the method described above. Noise was measured. The results are shown in Table 3.
Figure JPOXMLDOC01-appb-T000003
Figure JPOXMLDOC01-appb-T000003
 表3に示したように、本発明に従って磁区細分化を施した方向性電磁鋼板は、比較例に比べて、鉄損特性および磁歪特性に優れ、かつ変圧器の鉄損および騒音特性にも優れている。さらに、注目すべき点は、圧延方向における照射間隔を7.5mmにした場合は、比較例とは異なり、鉄損と騒音がともに最良値を示しており、変圧器用の方向性電磁鋼板として優れた効果を有することが分かる。 As shown in Table 3, the grain-oriented electrical steel sheet subjected to magnetic domain subdivision according to the present invention is superior in iron loss characteristics and magnetostriction characteristics as compared with the comparative example, and also excellent in iron loss and noise characteristics of the transformer. ing. Furthermore, it should be noted that when the irradiation interval in the rolling direction is 7.5 mm, unlike the comparative example, both the iron loss and the noise show the best values, which is excellent as a grain-oriented electrical steel sheet for a transformer. It turns out that it has an effect.
 1 滞留領域
 2 走行領域
 3 繰返し単位(滞留点間隔)
1 Residence area 2 Traveling area 3 Repeating unit (interval between residence points)

Claims (4)

  1.  鋼板表面に対し、圧延方向と交差する方向の線領域に電子ビームを照射し、該照射線領域を滞留領域と走行領域からなる2種類の領域を繰返し単位とする変調照射線領域とし、かつ該変調照射線領域を圧延方向に間隔を設けて繰返すことによる磁区細分化を施した方向性電磁鋼板において、
     該繰返し単位を線領域方向に連結させた変調照射線領域とし、
     該繰返し単位の該変調照射線領域における周期を0.20~1.0mmとし、
     該変調照射線領域の圧延方向の繰返し間隔を4.0~12.5mmとし、さらに
     電子ビームの強度を、少なくとも照射面側に該変調照射線領域方向に細長く伸びた分割磁区が形成される強度以上で、かつ照射面側に被膜損傷の発生および塑性歪み領域の形成が生じない強度までとした低騒音変圧器用の方向性電磁鋼板。
    The surface of the steel sheet is irradiated with an electron beam in a line area in a direction intersecting the rolling direction, the irradiation line area is set as a modulated irradiation line area having two types of areas consisting of a stay area and a running area as repeating units, and In the grain-oriented electrical steel sheet subjected to magnetic domain subdivision by repeating the modulation irradiation region in the rolling direction with an interval,
    A modulated irradiation region in which the repeating units are connected in the direction of the line region,
    The period in the modulated irradiation region of the repeating unit is 0.20 to 1.0 mm,
    The repetition interval in the rolling direction of the modulated irradiation region is set to 4.0 to 12.5 mm, and the intensity of the electron beam is at least equal to or more than the strength at which the elongated magnetic domains extending in the direction of the modulated irradiation region are formed on the irradiation surface side. A grain-oriented electrical steel sheet for a low-noise transformer that has a strength that prevents the occurrence of film damage and the formation of a plastic strain region on the irradiated surface side.
  2.  前記繰返し単位の前記変調照射線領域における周期を0.25~0.80mmとし、さらに
     前記変調照射線領域の圧延方向の繰返し間隔を5.0~10mmとした請求項1に記載の低騒音変圧器用の方向性電磁鋼板。
    The directional electromagnetic wave for a low noise transformer according to claim 1, wherein a period in the modulated irradiation region of the repeating unit is 0.25 to 0.80 mm, and a repetition interval in the rolling direction of the modulated irradiation region is 5.0 to 10 mm. steel sheet.
  3.  鋼板表面に対し、圧延方向と交差する方向の線領域に電子ビームを照射し、該照射線領域を滞留領域と走行領域からなる2種類の領域を繰返し単位とする変調照射線領域とし、かつ該変調照射線領域を圧延方向に間隔を設けて繰返すことからなる磁区細分化処理を施して方向性電磁鋼板を製造するに際し、
     該繰返し単位を線領域方向に連結させた変調照射線領域とし、
     該繰返し単位の該変調照射線領域における周期を0.20~1.0mmとし、
     該変調照射線領域の圧延方向の繰返し間隔を4.0~12.5mmとし、さらに
     電子ビームの強度を、少なくとも照射面側に該変調照射線領域方向に細長く伸びた分割磁区が形成される強度以上で、かつ照射面側に被膜損傷の発生および塑性歪み領域の形成が生じない強度までとする低騒音変圧器用の方向性電磁鋼板の製造方法。
    The surface of the steel sheet is irradiated with an electron beam in a line area in a direction intersecting the rolling direction, the irradiation line area is set as a modulated irradiation line area having two types of areas consisting of a stay area and a running area as repeating units, and When producing a grain-oriented electrical steel sheet by applying a magnetic domain refinement process consisting of repeating the modulation irradiation region in the rolling direction with an interval,
    A modulated irradiation region in which the repeating units are connected in the direction of the line region,
    The period in the modulated irradiation region of the repeating unit is 0.20 to 1.0 mm,
    The repetition interval in the rolling direction of the modulated irradiation region is set to 4.0 to 12.5 mm, and the intensity of the electron beam is at least equal to or more than the strength at which the elongated magnetic domains extending in the direction of the modulated irradiation region are formed on the irradiation surface side. And the manufacturing method of the grain-oriented electrical steel sheet for low noise transformers made into the intensity | strength which does not produce generation | occurrence | production of a film damage and the formation of a plastic strain area | region on the irradiation surface side.
  4.  前記繰返し単位の前記変調照射線領域における周期を0.25~0.80mmとし、さらに
     前記変調照射線領域の圧延方向の繰返し間隔を5.0~10mmとする請求項3に記載の低騒音変圧器用の方向性電磁鋼板の製造方法。
    4. A directional electromagnetic wave for a low noise transformer according to claim 3, wherein a period of the repeating unit in the modulated irradiation region is 0.25 to 0.80 mm, and a repetition interval in the rolling direction of the modulated irradiation region is 5.0 to 10 mm. A method of manufacturing a steel sheet.
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