CN101528951B - Unidirectional magnetic steel sheet excellent in iron loss characteristic - Google Patents

Unidirectional magnetic steel sheet excellent in iron loss characteristic Download PDF

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CN101528951B
CN101528951B CN2007800391681A CN200780039168A CN101528951B CN 101528951 B CN101528951 B CN 101528951B CN 2007800391681 A CN2007800391681 A CN 2007800391681A CN 200780039168 A CN200780039168 A CN 200780039168A CN 101528951 B CN101528951 B CN 101528951B
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iron loss
rolling direction
residual stress
steel sheet
strain
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CN101528951A (en
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滨村秀行
岩田圭司
坂井辰彦
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Nippon Steel Corp
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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
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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
    • C21D10/00Modifying the physical properties by methods other than heat treatment or deformation
    • C21D10/005Modifying the physical properties by methods other than heat treatment or deformation by laser shock processing
    • 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
    • C21D8/1277Modifying 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
    • 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
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    • 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
    • C21D9/00Heat treatment, e.g. annealing, hardening, quenching or tempering, adapted for particular articles; Furnaces therefor
    • C21D9/46Heat treatment, e.g. annealing, hardening, quenching or tempering, adapted for particular articles; Furnaces therefor for sheet metals
    • 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
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    • 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
    • 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
    • H01F1/147Alloys characterised by their composition
    • H01F1/14708Fe-Ni based alloys
    • H01F1/14716Fe-Ni based alloys in the form of sheets

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Abstract

A unidirectional magnetic steel sheet excellent in iron loss to conventional is produced by dividing the iron loss of a unidirectional magnetic steel sheet into which strain is introduced by laser beam application into the hysteresis loss and the eddy current loss and quantitatively and adequately controlling the distributions including the direction of the sheet thickness of the strain and the residual stress in view of the eddy current loss. By applying a laser beam or the like, linear strain generally perpendicular to the rolling direction is introduced into a unidirectional magnetic steel sheet uniformly in the direction of the sheet thickness and periodically in the rolling direction to control the magnetic domains. The strain is so introduced that the integral of the compression residual stress in the rolling direction computed in the region of the cross-section where the compression residual stress is present lies in a predetermined range, in the two-dimensional distribution of the residual stress in the rolling direction caused near one strain-introduced portion in the cross-section perpendicular to the direction of the sheet width.

Description

铁损特性优异的单向性电磁钢板 Grain-oriented electrical steel sheet with excellent iron loss properties

技术领域technical field

本发明涉及通过激光照射等导入残余应力来实施磁畴控制的铁损特性优异的单向性电磁钢板。The present invention relates to a grain-oriented electrical steel sheet excellent in iron loss characteristics in which magnetic domains are controlled by introducing residual stress by laser irradiation or the like.

背景技术Background technique

在钢板的轧制方向具有易磁化轴的单向性电磁钢板,主要被用于变压器的铁心等,近年来从节约能源的观点出发,强烈要求降低铁心的铁损。A grain-oriented electrical steel sheet having an easy-magnetization axis in the rolling direction of the steel sheet is mainly used for iron cores of transformers, etc. In recent years, reduction of iron loss in iron cores has been strongly demanded from the viewpoint of energy conservation.

电磁钢板的铁损(铁耗;iron loss),大致包括磁滞损耗和涡流损耗。已知磁滞损耗受晶体取向、缺陷、晶界等影响,另外,涡流损耗受板厚、电阻、磁畴宽度等影响。为了降低磁滞损耗而控制和改善晶体取向的方法存在极限,因此,近年来为了降低占较多铁损的涡流损耗,曾提出了较多的磁畴宽度细分化即磁畴控制技术。The iron loss (iron loss; iron loss) of the electromagnetic steel sheet roughly includes hysteresis loss and eddy current loss. It is known that hysteresis loss is affected by crystal orientation, defects, grain boundaries, etc., and that eddy current loss is affected by plate thickness, electrical resistance, magnetic domain width, and the like. There is a limit to the method of controlling and improving the crystal orientation in order to reduce the hysteresis loss. Therefore, in order to reduce the eddy current loss which accounts for a large amount of iron loss in recent years, many magnetic domain width subdivisions, that is, magnetic domain control technology, have been proposed.

作为其方法,在日本特公平6-19112号公报中,作为单向性电磁钢板的制造方法,曾经提出了:通过YAG激光照射,在轧制方向周期性地导入与轧制方向大致垂直的线性应变,来降低铁损的方法。被称为激光磁畴控制的该方法的原理是,起因于由扫描地照射激光束引起的表面应变,180°磁畴宽度被细分化,可以降低铁损。As a method thereof, in Japanese Patent Publication No. 6-19112, as a method of manufacturing grain-oriented electrical steel sheets, it has been proposed to periodically introduce linear lines substantially perpendicular to the rolling direction in the rolling direction by irradiating YAG laser light. Strain, to reduce the method of iron loss. The principle of this method, called laser domain control, is that the 180° magnetic domain width is subdivided due to the surface strain caused by scanning laser beam irradiation, and iron loss can be reduced.

另外,在日本特开2005-248291号公报中,提出了着眼于在钢板表面形成的轧制方向的残余应力的最大值的新方案。In addition, JP-A-2005-248291 proposes a new idea focusing on the maximum value of the residual stress in the rolling direction formed on the surface of the steel sheet.

发明内容Contents of the invention

关于向钢板表面导入局部的应变,将180°磁畴宽度细分化来降低铁损这一激光磁畴控制,包括作为现有技术的专利文献1在内的、迄今为止的大部分提案,进行尝试的结果,进一步限定了激光的种类、激光束聚光点形状、激光能量密度、激光照射间隔等较多的照射参数,提案的内容非常片面,缺乏统一性。其原因在于:没有涉及到作为引起磁畴细分化、降低铁损的主要因素的应变或者残余应力的定量的讨论。说起来,在通过激光照射来改善铁损方面,即使是相同的照射条件,根据钢板的吸收率(由激光波长、表面性状、形状、皮膜组成决定)、皮膜厚度的不同,由激光能向热能(温度分布、温度过程)的转换也不同,因此即使激光照射条件相同,由于钢板的性状不同,导入的应变也不同。而且,即使是相同的热能(温度分布、温度过程),由于钢板的组成(例如Si含量)不同,物性值(例如杨氏模量、屈服应力值)也不同,因此残余应力也不同。因此,即使能够得到对于某种条件的钢板的最佳的激光照射条件,只要被膜的状态稍微变化,由激光引起的应变的进入方式也不同,铁损值会变化,因此激光条件与铁损的降低并不一对一地对应。因此,对于铁损,要求找到更本质的影响因子。专利文献2虽然定量性地谈到唯一应变、残余应力,但是若只是仅控制钢板表面的应变、拉伸残余应力,则铁损的降低存在极限。Regarding laser magnetic domain control, in which iron loss is reduced by subdividing the 180° magnetic domain width by introducing local strain on the steel sheet surface, most of the previous proposals including Patent Document 1, which is a prior art, have been carried out. As a result of the experiment, many irradiation parameters such as the type of laser, the shape of the laser beam spot, the laser energy density, and the laser irradiation interval were further limited. The content of the proposal was very one-sided and lacked unity. The reason is that there is no quantitative discussion on strain or residual stress, which are the main factors that cause magnetic domain subdivision and reduce iron loss. Speaking of which, in terms of improving iron loss by laser irradiation, even under the same irradiation conditions, depending on the absorption rate of the steel plate (determined by the laser wavelength, surface texture, shape, and film composition) and the thickness of the film, the energy from the laser energy to the thermal energy is different. The conversion (temperature distribution, temperature history) is also different, so even if the laser irradiation conditions are the same, the introduced strain will be different due to the different properties of the steel sheet. Furthermore, even with the same heat energy (temperature distribution, temperature history), the residual stress is also different due to the difference in the composition of the steel sheet (such as Si content) and the difference in physical property values (such as Young's modulus, yield stress value). Therefore, even if the optimum laser irradiation conditions for a certain steel plate can be obtained, as long as the state of the film changes slightly, the way in which the strain caused by the laser enters is also different, and the iron loss value will change. Therefore, the laser conditions and the iron loss The reduction does not correspond one-to-one. Therefore, for iron loss, it is required to find a more essential influencing factor. Although Patent Document 2 quantitatively discusses unique strain and residual stress, there is a limit to the reduction of iron loss if only the strain and tensile residual stress on the steel plate surface are controlled.

本发明的课题在于,将单向性电磁钢板的铁损分为磁滞损耗和涡流损耗,尤其是从涡流损耗的观点出发,不仅表面,也包括内部的板厚方向在内,定量地以适宜的条件控制应变以及残余应力的分布,由此提供与以往相比在铁损方面优异的单向性电磁钢板。The object of the present invention is to divide the iron loss of grain-oriented electrical steel sheet into hysteresis loss and eddy current loss, and especially from the viewpoint of eddy current loss, quantitatively and appropriately include not only the surface but also the internal thickness direction. Conditions control the distribution of strain and residual stress, thereby providing a grain-oriented electrical steel sheet that is superior in iron loss compared to conventional ones.

本发明者们进行磁畴控制的实验,通过激光照射等向单向性电磁钢板导入应变、残余应力,对于得到的低铁损单向性电磁钢板刻苦进行研究,调查所导入的残余应力的分布。其结果发现,如果找到残余应力与涡流损耗之间的相关性,进行压缩应力值与应变间隔的控制,就能够实现铁损特性优异的单向性电磁钢板。本发明的要旨如下。The inventors of the present invention conducted experiments on magnetic domain control, introduced strain and residual stress into the grain-oriented electrical steel sheet by laser irradiation, etc., studied hard on the obtained low iron loss grain-oriented electrical steel sheet, and investigated the distribution of the introduced residual stress . As a result, it was found that if the correlation between residual stress and eddy current loss is found, and the compressive stress value and strain interval are controlled, a grain-oriented electrical steel sheet with excellent iron loss characteristics can be realized. The gist of the present invention is as follows.

(1)一种单向性电磁钢板,是通过照射连续波激光束从而具有与轧制方向大致垂直的线性应变的单向性电磁钢板,所述线性应变,在与轧制方向垂直的方向即板横向上均匀,并且在轧制方向上呈周期性,该单向性电磁钢板的特征在于,在一处应变导入部附近产生的轧制方向的压缩残余应力的、在与板横向垂直的截面上的二维分布中,将轧制方向的压缩残余应力在该截面的存在压缩残余应力的区域内积分而得到的值为0.20N~0.80N。(1) A grain-oriented electrical steel sheet, which is a grain-oriented electrical steel sheet having a linear strain approximately perpendicular to the rolling direction by irradiating a continuous wave laser beam, the linear strain being in the direction perpendicular to the rolling direction, namely The plate is uniform in the transverse direction and is periodic in the rolling direction. The grain-oriented electrical steel sheet is characterized in that the compressive residual stress in the rolling direction generated near a strain introduction portion is in a cross-section perpendicular to the plate transverse direction. In the two-dimensional distribution above, the value obtained by integrating the compressive residual stress in the rolling direction in the region where the compressive residual stress exists in the cross section is 0.20N to 0.80N.

(2)根据上述(1)所述的单向性电磁钢板,其特征在于,由激光束照射引起的在上述板横向上均匀的应变在上述轧制方向上的周期性的间隔为2mm~8mm。(2) The grain-oriented electrical steel sheet according to (1) above, wherein the periodic intervals of the uniform strain in the transverse direction of the sheet caused by laser beam irradiation in the rolling direction are 2 mm to 8 mm .

附图说明Description of drawings

图1是用于本发明的单向性电磁钢板制造方法的装置的模式图。Fig. 1 is a schematic diagram of an apparatus used in the method for producing a grain-oriented electrical steel sheet of the present invention.

图2是激光照射位置附近的轧制方向的残余应力在轧制方向/板厚方向截面上的二维分布。Fig. 2 is a two-dimensional distribution of residual stress in the rolling direction in the vicinity of the laser irradiation position on a section in the rolling direction/thickness direction.

图3是轧制方向的拉伸残余应力的最大值与铁损W17/50的关系图。Fig. 3 is a graph showing the relationship between the maximum value of the tensile residual stress in the rolling direction and the iron loss W 17/50 .

图4是积分压缩应力值σS与涡流损耗We的关系图(照射间隔固定在4mm)。Figure 4 is a graph showing the relationship between the integral compressive stress value σS and the eddy current loss We (the irradiation interval is fixed at 4mm).

图5是积分压缩应力值σS与铁损W17/50的关系图(照射间隔固定在4mm)。Figure 5 is a graph showing the relationship between the integral compressive stress value σS and the iron loss W 17/50 (the irradiation interval is fixed at 4mm).

图6是照射间隔PL与铁损W17/50的关系图(轧制方向的照射直径DL固定在0.1mm、扫描方向的照射直径DC固定在0.5mm)。Fig. 6 is a graph showing the relationship between the irradiation interval PL and the iron loss W 17/50 (the irradiation diameter DL in the rolling direction is fixed at 0.1 mm, and the irradiation diameter DC in the scanning direction is fixed at 0.5 mm).

图7是轧制方向的压缩残余应力的最大值与铁损W17/50的关系图。Fig. 7 is a graph showing the relationship between the maximum value of the compressive residual stress in the rolling direction and the iron loss W 17/50 .

具体实施方式Detailed ways

本发明者们在向单向性电磁钢板的表面照射激光,在轧制方向上以一定间隔导入与轧制方向大致垂直的线性应变从而改善铁损的方法中,对于各种的激光照射条件,着眼于与板横向垂直的截面上的轧制方向的残余应力的二维分布以及轧制方向的激光照射间隔(间距),找到了可以得到铁损特性优异的单向性电磁钢板的条件。在此,板横向为与轧制方向垂直的方向。作为向单向性电磁钢板的表面导入上述那样的线性应变的方法,除了激光照射法以外,还可以列举出离子注入法、放电加工法、局部镀覆法、超声波振动法等,该条件是对于采用任何方法导入了应变的单向性电磁钢板都适用的。以下用附图来说明本发明的通过激光照射得到的单向性电磁钢板。The inventors of the present invention irradiated the surface of the grain-oriented electrical steel sheet with laser light, and introduced linear strains approximately perpendicular to the rolling direction at constant intervals in the rolling direction to improve iron loss. For various laser irradiation conditions, Focusing on the two-dimensional distribution of residual stress in the rolling direction on a cross section perpendicular to the lateral direction of the sheet and the laser irradiation interval (pitch) in the rolling direction, the conditions for obtaining a grain-oriented electrical steel sheet excellent in iron loss characteristics were found. Here, the plate transverse direction is a direction perpendicular to the rolling direction. As a method of introducing the above-mentioned linear strain into the surface of the grain-oriented electrical steel sheet, in addition to the laser irradiation method, ion implantation method, electric discharge machining method, partial plating method, ultrasonic vibration method, etc. can be mentioned, and this condition is for A grain-oriented electrical steel sheet to which strain has been introduced by any method is applicable. The grain-oriented electrical steel sheet obtained by laser irradiation according to the present invention will be described below with reference to the drawings.

图1是本发明涉及的激光束照射方法的说明图。在本实施例中,使用多角镜4和fθ透镜5,将由激光装置3输出的连续振荡(CW)的激光束LB扫描照射到单向性电磁钢板1上。通过改变fθ透镜5与单向性电磁钢板1之间的距离,而使激光束的轧制方向聚光直径d1变化。6是圆柱透镜或多个圆柱组透镜,关于激光束的聚光点,根据要求使光束的扫描方向(与轧制方向垂直的板横向)的聚光直径(扫描方向长度)dc变化,从圆形到椭圆形而用于控制聚光形状。平均照射能量密度Ua[mJ/mm2],使用激光功率P[W]、板横向的激光束的板横向扫描(scan)速度Vc[m/s]、轧制方向的激光照射间隔PL[mm],定义为:Ua(mJ/mm2)=P/(Vc×PL)。激光扫描速度由多角镜的旋转速度决定,因此,可使激光功率、多角镜旋转速度、激光照射间隔变化而进行平均照射能量密度的调整。图1是使用了一组激光和激光束扫描装置的例子,但也可以根据钢板的板宽度,在板横向上配置多台同样的装置。FIG. 1 is an explanatory diagram of a laser beam irradiation method according to the present invention. In the present embodiment, the continuous oscillation (CW) laser beam LB output from the laser device 3 is scanned and irradiated onto the grain-oriented electrical steel sheet 1 using the polygon mirror 4 and the fθ lens 5 . By changing the distance between the fθ lens 5 and the grain-oriented electrical steel sheet 1, the focusing diameter d1 of the laser beam in the rolling direction is changed. 6 is a cylindrical lens or a plurality of cylindrical lens groups. Regarding the focusing point of the laser beam, the focusing diameter (length of the scanning direction) dc of the scanning direction of the beam (the transverse direction of the plate perpendicular to the rolling direction) changes according to requirements, from a circle Shaped to an ellipse to control the spotlight shape. Average irradiation energy density Ua [mJ/mm 2 ], laser power P [W], plate transverse scanning (scan) speed Vc [m/s] of the laser beam in the transverse direction of the plate, laser irradiation interval PL in the rolling direction PL [mm ], defined as: Ua(mJ/mm 2 )=P/(Vc×PL). The laser scanning speed is determined by the rotation speed of the polygon mirror. Therefore, the average irradiation energy density can be adjusted by changing the laser power, the rotation speed of the polygon mirror, and the laser irradiation interval. Fig. 1 is an example using a set of laser and laser beam scanning devices, but it is also possible to arrange a plurality of the same devices in the transverse direction of the steel plate according to the width of the steel plate.

本发明者们使用光纤芯直径为10μm的连续振荡光纤激光装置,通过聚光点形状和平均照射能量密度Ua的各种组合来改变照射条件,对单向性电磁钢板表面,在与轧制方向大致垂直的方向以线状扫描激光束,实施激光照射的实验。测定与板横向垂直的截面上的轧制方向的残余应力的二维分布和铁损以及磁滞损耗,将铁损分离成磁滞损耗和涡流损耗进行考察。与板横向垂直的截面上的轧制方向的残余应力的二维分布的测定,是采用X射线衍射法测定晶格间距,使用弹性模量等的物性值转换成应力。铁损采用SST(单片试验器;Single Sheet Tester)测定器测定W17/50。W17/50是频率50Hz、最大磁通密度1.7T时的铁损。对于在本实施例中使用的单向性电磁钢板样品,在板厚为0.23mm的情况下,激光照射前的W17/50是0.86W/kg。磁滞损耗根据磁滞回线计算出,涡流损耗为从上述的铁损减去磁滞损耗得到的值。The present inventors used a continuous oscillation fiber laser device with a fiber core diameter of 10 μm, and changed the irradiation conditions by various combinations of the spot shape and the average irradiation energy density Ua. A laser beam is scanned linearly in an approximately vertical direction, and an experiment of laser irradiation is carried out. The two-dimensional distribution of residual stress in the rolling direction, iron loss, and hysteresis loss on a section perpendicular to the transverse direction of the plate were measured, and the iron loss was separated into hysteresis loss and eddy current loss for investigation. The measurement of the two-dimensional distribution of residual stress in the rolling direction on a cross section perpendicular to the transverse direction of the sheet is to measure the lattice spacing by X-ray diffraction method, and convert the physical property values such as elastic modulus into stress. The iron loss was measured by SST (Single Sheet Tester; Single Sheet Tester) measuring instrument W 17/50 . W 17/50 is the iron loss at a frequency of 50Hz and a maximum magnetic flux density of 1.7T. For the grain-oriented electrical steel sheet sample used in this example, W 17/50 before laser irradiation was 0.86 W/kg when the plate thickness was 0.23 mm. The hysteresis loss was calculated from the hysteresis loop, and the eddy current loss was a value obtained by subtracting the hysteresis loss from the aforementioned iron loss.

图2表示在激光照射位置附近产生的轧制方向的压缩残余应力在与板横向垂直的截面上的二维分布的代表性的一例。关于可看到铁损改善的钢板,虽然根据激光照射条件,残余应力的绝对值存在差异,但是在钢板表面附近存在较大的拉伸应力,在其板厚方向的下方可看到压缩应力的存在。再者,存在残余应力以及塑性应变的轧制方向的宽度,与激光聚光点的轧制方向直径d1大致成比例。FIG. 2 shows a representative example of the two-dimensional distribution of compressive residual stress in the rolling direction generated in the vicinity of the laser irradiation position on a cross section perpendicular to the transverse direction of the sheet. Regarding the steel sheet where improvement in iron loss is seen, although the absolute value of residual stress varies depending on the laser irradiation conditions, there is a large tensile stress near the surface of the steel sheet, and a compressive stress is seen below it in the thickness direction. exist. In addition, the width in the rolling direction in which residual stress and plastic strain exist is approximately proportional to the rolling direction diameter d1 of the laser focus point.

本发明者们对于使用连续振荡激光器进行了激光照射的钢板,对钢板表面的拉伸残余应力和压缩残余应力的最大值与铁损的关系进行了调查。将拉伸残余应力的最大值与铁损的关系示于图3,将压缩残余应力的最大值与铁损的关系示于图7。关于拉伸残余应力最大值,看不到与铁损相关、和/或最佳值。另一方面,关于压缩残余应力的最大值,在为由点划线表示的100MPa以上时,铁损良好,但上限值并不清楚。其结果,通过激光照射进行的磁畴控制中的铁损,不能用拉伸残余应力的最大值进行说明,也完全不能用压缩残余应力的最大值进行说明。可想到另外的特征量存在的可能性。The inventors of the present invention investigated the relationship between the maximum value of tensile residual stress and compressive residual stress on the surface of the steel plate and the iron loss of the steel plate irradiated with laser light using a continuous oscillation laser. The relationship between the maximum value of tensile residual stress and iron loss is shown in FIG. 3 , and the relationship between the maximum value of compressive residual stress and iron loss is shown in FIG. 7 . With regard to the maximum value of the tensile residual stress, no iron loss correlation and/or optimum value can be seen. On the other hand, when the maximum value of the compressive residual stress is 100 MPa or more indicated by the chain line, the core loss is good, but the upper limit is not clear. As a result, iron loss in magnetic domain control by laser irradiation cannot be explained by the maximum value of tensile residual stress, nor can it be explained by the maximum value of compressive residual stress at all. The possibility that another feature quantity exists is conceivable.

因此,本发明者们仔细研讨数据的结果,作为第一着眼点,着眼于:拉伸残余应力的最大值比压缩残余应力大且拉伸残余应力集中在狭窄的区域;根据照射条件而达到屈服应力即塑性应变区域;另一方面,压缩残余应力的最大值和铁损可看到不少关系,作为第二着眼点,着眼于:即使压缩残余应力的最大值相同,压缩残余应力分布在深度方向的扩展上存在不同。即,实现铁损降低以及磁畴细分化的主要因素,从第一着眼点考虑,具有重要意义的不是拉伸应力,而是压缩应力,从第二着眼点考虑,具有重要意义的不是残余应力的最大值,而是分布的扩展。Therefore, the present inventors studied the data carefully, and as a first point of view, focused on: the maximum value of the tensile residual stress is larger than the compressive residual stress and the tensile residual stress is concentrated in a narrow region; Stress is the area of plastic strain; on the other hand, there are many relationships between the maximum value of compressive residual stress and iron loss. As a second point of view, focus on: even if the maximum value of compressive residual stress is the same, the distribution of compressive residual stress in the depth There are differences in the direction of expansion. That is to say, the main factor to achieve the reduction of iron loss and the subdivision of magnetic domains, from the first point of view, it is not the tensile stress that is important, but the compressive stress, and from the second point of view, it is not the residual The maximum value of the stress, but the expansion of the distribution.

本发明者们在表示实现降低铁损的压缩应力的分布时,作为特征量“积分压缩应力值σS”,如下式(1)那样定义。The inventors of the present invention define the distribution of compressive stress for reducing iron loss as the characteristic quantity "integrated compressive stress value σS" as in the following equation (1).

σS=∫S σds    ...(1)σS= ∫S σds...(1)

即,在激光照射部附近,也就是应变导入部附近产生的轧制方向的压缩残余应力的、在垂直于板横向的截面上的二维分布中,关于积分压缩应力值σS[N],将轧制方向的压缩残余应力设为σ[MPa],将该截面的存在压缩残余应力的区域设为S[mm2],将面积单元设为ds,将σS定义为在区域S内对应力σ进行积分而得到的值。即,积分压缩应力值是通过激光照射而导入的压缩残余应力的总和。That is, in the two-dimensional distribution of the compressive residual stress in the rolling direction generated near the laser irradiation part, that is, near the strain introduction part, on a cross section perpendicular to the transverse direction of the sheet, the integrated compressive stress value σS[N] is given by The compressive residual stress in the rolling direction is set to σ[MPa], the region where the compressive residual stress exists in the section is set to S[mm 2 ], the area unit is set to ds, and σS is defined as the corresponding stress σ in the area S The value obtained by performing the integration. That is, the integrated compressive stress value is the sum of compressive residual stresses introduced by laser irradiation.

将轧制方向的激光照射间隔PL设为4mm(恒定),将激光聚光点形状设为:20×2500μm、100×500μm、100×2000μm、300×200μm,关于对于该各个情况,阶段性地改变激光功率而照射过的单向性电磁钢板,采用上述方法求出积分压缩应力值。另一方面,由对于各个情况测定的铁损,减去磁滞损耗,求出涡流损耗。图4是对于各电磁钢板,在横坐标上绘制积分压缩应力值σS、在纵坐标上绘制涡流损耗We,从而表示二者关系的图。从该结果来看,积分压缩应力值和涡流损耗,无论聚光点形状如何,都成反比例的关系。这意味着涡流损耗的降低即磁畴区细分化效果与所导入的压缩残余应力的总和成比例。从物理性原理考察这种现象,如下所述。磁弹性能E:Set the laser irradiation interval PL in the rolling direction to 4mm (constant), and set the shape of the laser spot to: 20×2500μm, 100×500μm, 100×2000μm, 300×200μm, for each case, step by step For the grain-oriented electrical steel sheet irradiated with varying laser power, the integral compressive stress value was obtained by the above-mentioned method. On the other hand, the eddy current loss was obtained by subtracting the hysteresis loss from the iron loss measured for each case. FIG. 4 is a diagram showing the relationship between the integral compressive stress value σS and the eddy current loss We plotted on the abscissa for each electrical steel sheet. From this result, the integrated compressive stress value and the eddy current loss are inversely proportional to each other regardless of the shape of the spot. This means that the reduction of eddy current loss, that is, the magnetic domain subdivision effect is proportional to the sum of the introduced compressive residual stresses. This phenomenon is examined from a physical principle as follows. Magnetoelastic performance E:

E=-C×σ×M×cos2θE=-C×σ×M×cos 2 θ

其中,C为常数,σ为残余应力,M为磁矩,θ为σ与M构成的角。此时,在轧制方向上存在压缩残余应力的情况下,θ为90°时E最小,因此注意到σ为负值,磁矩的方向与轧制方向垂直。因此,由于压缩应力,易磁化轴不仅在轧制方向,在其垂直方向也会产生。一般地,其被称为环流磁畴。如果存在环流磁畴,则静磁能增高,变得不稳定,因此可以考虑到将磁畴细分化,降低静磁能从而进行稳定化。因此可以认为,环流磁畴越多,即越是压缩残余应力强、而且宽泛地发生,则磁畴细分化效果越高,涡流损耗越降低。Among them, C is a constant, σ is the residual stress, M is the magnetic moment, and θ is the angle formed by σ and M. At this time, in the case of compressive residual stress in the rolling direction, E is the smallest when θ is 90°, so note that σ is a negative value, and the direction of the magnetic moment is perpendicular to the rolling direction. Therefore, due to the compressive stress, the easy axis of magnetization is generated not only in the rolling direction but also in its perpendicular direction. Generally, it is called a circulating magnetic domain. If circulating magnetic domains exist, the magnetostatic energy increases and becomes unstable. Therefore, it is conceivable to subdivide the magnetic domains and reduce the magnetostatic energy for stabilization. Therefore, it can be considered that the more circulating magnetic domains there are, that is, the stronger and wider the compressive residual stress occurs, the higher the magnetic domain subdivision effect is, and the lower the eddy current loss is.

图5是使用在图4中使用的数据和测定的铁损,在横坐标上绘制积分压缩应力值σS、在纵坐标上绘制到达铁损W17/50,从而表示二者关系的图。从该结果来看,在由点划线所示的0.20N≤σS≤0.80N的范围,与磁畴控制前的铁损W17/50=0.86W/kg相比,能够实现由虚线所示的铁损改善率为13%以上(W17/50≤0.75W/kg)这一良好的铁损。再者,铁损改善率η定义为:η(%)={(材料的铁损-到达铁损)/材料的铁损}×100。由于在积分压缩应力值σS小于0.20N时,涡流损耗高,因此铁损不能降低。可以认为,在积分压缩应力值σS大于0.80N时,虽然涡流损耗降低,但是由于由表面附近的拉伸残余应力引起的塑性应变,因此磁滞损耗增大,不能降低铁损。如以上所述可知,如果将积分压缩应力值σS调节为0.20N≤σS≤0.80N的范围,则可以得到良好的铁损改善。可知如果更优选地调节为0.40N≤σS≤0.70N的范围,则可以得到进一步改善铁损的效果。FIG. 5 is a graph showing the relationship between the integrated compressive stress value σS on the abscissa and the attained iron loss W 17/50 on the ordinate using the data and measured iron loss used in FIG. 4 . From this result, in the range of 0.20N ≤ σS ≤ 0.80N shown by the dotted line, compared with the iron loss W 17/50 = 0.86W/kg before magnetic domain control, it is possible to realize the The iron loss improvement rate is 13% or more (W 17/50 ≤ 0.75W/kg), which is a good iron loss. Furthermore, iron loss improvement rate η is defined as: η(%)={(iron loss of material-arrival iron loss)/iron loss of material}×100. Since the eddy current loss is high when the integrated compressive stress value σS is less than 0.20N, the iron loss cannot be reduced. It can be considered that when the integrated compressive stress value σS exceeds 0.80N, although the eddy current loss decreases, the hysteresis loss increases due to the plastic strain caused by the tensile residual stress near the surface, and the iron loss cannot be reduced. As mentioned above, it can be seen that if the integral compressive stress value σS is adjusted to the range of 0.20N≤σS≤0.80N, good iron loss improvement can be obtained. It can be seen that if it is more preferably adjusted to the range of 0.40N≦σS≦0.70N, the effect of further improving the iron loss can be obtained.

在前面所述中,将轧制方向的激光照射间隔PL固定在4mm而进行,但进一步改变轧制方向的激光照射间隔PL而调查了其影响。此时,激光束的聚光点形状是轧制方向直径为0.1mm、扫描方向(板横向)直径为0.5mm,调整Ua使得积分压缩应力值σS为0.20N≤σS≤0.80N的范围。图6是在横坐标上绘制轧制方向的激光照射间隔PL、在纵坐标上绘制铁损W17/50从而表示二者关系的图。从该结果来看,PL为2mm~8mm的范围时能够实现铁损改善率为13%的良好的铁损。当PL为小于2mm的范围时,磁滞损耗增大,因此不能够降低铁损。当PL为大于8mm的范围时,不能够降低涡流损耗,因此不能够降低铁损。可知如果如以上那样将轧制方向的激光照射间隔PL调节为2mm≤PL≤8mm的范围,则可以得到良好的铁损的改善。In the foregoing, the laser irradiation interval PL in the rolling direction was fixed at 4 mm, but the influence was investigated by further changing the laser irradiation interval PL in the rolling direction. At this time, the focus shape of the laser beam has a diameter of 0.1 mm in the rolling direction and a diameter of 0.5 mm in the scanning direction (transverse direction of the plate), and Ua is adjusted so that the integrated compressive stress value σS is in the range of 0.20N≤σS≤0.80N. Fig. 6 is a graph showing the relationship between the laser irradiation interval PL in the rolling direction plotted on the abscissa and the iron loss W 17/50 plotted on the ordinate. From this result, when PL is in the range of 2 mm to 8 mm, it is possible to realize a good iron loss with an improvement rate of iron loss of 13%. When the PL is in the range of less than 2 mm, the hysteresis loss increases, so that the core loss cannot be reduced. When PL is in a range larger than 8 mm, eddy current loss cannot be reduced, and thus iron loss cannot be reduced. It can be seen that if the laser irradiation interval PL in the rolling direction is adjusted to the range of 2 mm≤PL≤8 mm as described above, good improvement in iron loss can be obtained.

实施例1Example 1

使用板厚为0.23mm的单向性电磁钢板,采用连续波激光以如表1所示的照射条件对该钢板表面进行照射,测定残余应力后,计算出积分压缩应力值,测定各自的铁损(W17/50)。结果汇总于表1。在本实施例1中,将激光功率固定在200W、轧制方向的激光照射间隔固定在4mm而进行照射。积分压缩应力值的计算,是使用X射线衍射法测定轧制方向的残余应力(应变),对于压缩应力由式(2)求得。Using a grain-oriented electrical steel sheet with a thickness of 0.23 mm, the surface of the steel sheet is irradiated with a continuous wave laser under the irradiation conditions shown in Table 1. After measuring the residual stress, the integral compressive stress value is calculated, and the respective iron losses are measured. (W 17/50 ). The results are summarized in Table 1. In Example 1, the laser power was fixed at 200 W, and the laser irradiation interval in the rolling direction was fixed at 4 mm. The integral compressive stress value is calculated by measuring the residual stress (strain) in the rolling direction using the X-ray diffractometry, and the compressive stress is obtained by formula (2).

由表1清楚地知道,试验No.1~No.8(本发明例)所示的电磁钢板,其轧制方向的积分压缩应力值σS均在本发明所规定的范围0.20N≤σS≤0.80N,因此能够降低到作为铁损改善率13%的低铁损值(W17/50)0.75W/kg以下。另一方面,脱离条件范围0.20N≤σS≤0.80N的试验No.9~No.12(比较例)所示的电磁钢板,不能实现低铁损值(W17/50)0.75W/kg以下。这样一来,如果采用本发明,则能够得到铁损特性优异的单向性电磁钢板。It is clear from Table 1 that the integrated compressive stress values σS in the rolling direction of the electrical steel sheets shown in Test No.1 to No.8 (example of the present invention) are all within the range specified by the present invention: 0.20N≤σS≤0.80 N, therefore, can be reduced to a low iron loss value (W 17/50 ) of 0.75 W/kg or less, which is an iron loss improvement rate of 13%. On the other hand, the electrical steel sheets shown in Test No.9 to No.12 (comparative example) out of the condition range of 0.20N≤σS≤0.80N cannot achieve a low iron loss value (W 17/50 ) of 0.75W/kg or less . As described above, according to the present invention, a grain-oriented electrical steel sheet excellent in iron loss characteristics can be obtained.

Figure G2007800391681D00091
Figure G2007800391681D00091

实施例2Example 2

对板厚为0.23mm的单向性电磁钢板的表面,以如表2所示的照射条件照射连续波激光,测定照射部的残余应力后,计算出积分压缩应力值,并且测定铁损(W17/50),将这些数值汇总于表2。在本实施例2中,将激光功率固定为与前面所述实施例相同的200W而进行。The surface of a grain-oriented electrical steel sheet with a plate thickness of 0.23 mm was irradiated with a continuous wave laser under the irradiation conditions shown in Table 2. After measuring the residual stress of the irradiated part, the integral compressive stress value was calculated, and the iron loss (W 17/50 ), these values are summarized in Table 2. In this second example, the laser power was fixed at 200W as in the previous example.

由表2清楚地知道,试验No.1~No.6(本发明例)所示的电磁钢板,其轧制方向的积分压缩应力值σS、和轧制方向的激光照射间隔(应变间隔)PL,均在本发明所规定的范围0.20N≤σS≤0.80N、2mm≤PL≤8mm,因此能够降低到作为铁损改善率13%的低铁损值(W17/50)0.75W/kg以下。另一方面,虽然积分压缩应力值σS满足条件,但是照射间隔PL的条件偏离的试验No.7和No.8所示的电磁钢板,不能实现低铁损值(W17/50)0.75W/kg以下。这样一来,如果采用本发明,则能够得到铁损特性优异的单向性电磁钢板。It is clear from Table 2 that the integrated compressive stress value σS in the rolling direction and the laser irradiation interval (strain interval) PL in the rolling direction of the electrical steel sheets shown in Test No.1 to No.6 (example of the present invention) , are all in the scope of the present invention 0.20N≤σS≤0.80N, 2mm≤PL≤8mm, so it can be reduced to a low iron loss value (W 17/50 ) of 0.75W/kg or less, which is an iron loss improvement rate of 13%. . On the other hand, although the integrated compressive stress value σS satisfies the condition, the electrical steel sheets shown in Test No. 7 and No. 8, in which the irradiation interval PL deviates from the condition, cannot achieve a low iron loss value (W 17/50 ) of 0.75W/ Below kg. As described above, according to the present invention, a grain-oriented electrical steel sheet excellent in iron loss characteristics can be obtained.

Figure G2007800391681D00111
Figure G2007800391681D00111

产业上的利用可能性Industrial Utilization Possibility

根据本发明,通过定量性地适当控制导入到单向性电磁钢板中的残余应力尤其是压缩残余应力,与以往相比,能够稳定地得到铁损特性优异的单向性电磁钢板。通过将本发明的单向性电磁钢板作为铁心使用,可制造高效率且小型的变压器,因此本发明的产业上的利用价值非常高。According to the present invention, by quantitatively and appropriately controlling the residual stress introduced into the grain-oriented electrical steel sheet, especially the compressive residual stress, it is possible to stably obtain a grain-oriented electrical steel sheet excellent in iron loss characteristics compared with conventional ones. By using the grain-oriented electrical steel sheet of the present invention as an iron core, a high-efficiency and compact transformer can be manufactured, so the industrial utility value of the present invention is very high.

本发明中表示数值范围的“以上”和“以下”均包括本数。In the present invention, "above" and "below" indicating a numerical range both include the original number.

Claims (1)

1. the manufacture method of a low iron loss one-way electromagnetic steel plate, it is characterized in that, with the direction of rolling direction approximate vertical on, and the periodic compartment of terrain irradiation continuous-wave laser beam of 2mm~8mm is set on rolling direction, give linear strain with the rolling direction approximate vertical, make and near the place strain introduction part of described low iron loss one-way electromagnetic steel plate, produce, in the bivariate distribution perpendicular to the compressive residual stress of the rolling direction on the horizontal cross section of plate, the value that in the zone of the compressive residual stress that has rolling direction the compressive residual stress integration of this rolling direction is obtained is 0.20N~0.80N.
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