Deprecated: The each() function is deprecated. This message will be suppressed on further calls in /home/zhenxiangba/zhenxiangba.com/public_html/phproxy-improved-master/index.php on line 456
JPS5953684B2 - Method for improving iron loss in magnetic steel sheet coils - Google Patents
[go: Go Back, main page]

JPS5953684B2 - Method for improving iron loss in magnetic steel sheet coils - Google Patents

Method for improving iron loss in magnetic steel sheet coils

Info

Publication number
JPS5953684B2
JPS5953684B2 JP54161320A JP16132079A JPS5953684B2 JP S5953684 B2 JPS5953684 B2 JP S5953684B2 JP 54161320 A JP54161320 A JP 54161320A JP 16132079 A JP16132079 A JP 16132079A JP S5953684 B2 JPS5953684 B2 JP S5953684B2
Authority
JP
Japan
Prior art keywords
iron loss
steel sheet
laser
laser beam
coil
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired
Application number
JP54161320A
Other languages
Japanese (ja)
Other versions
JPS5683905A (en
Inventor
正 市山
重裕 山口
徹 井内
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Nippon Steel Corp
Original Assignee
Nippon Steel Corp
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Nippon Steel Corp filed Critical Nippon Steel Corp
Priority to JP54161320A priority Critical patent/JPS5953684B2/en
Publication of JPS5683905A publication Critical patent/JPS5683905A/en
Publication of JPS5953684B2 publication Critical patent/JPS5953684B2/en
Expired legal-status Critical Current

Links

Classifications

    • 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 of ferrous metals or ferrous alloys by deformation combined with, or followed by, heat treatment
    • C21D8/12Modifying the physical properties of ferrous metals or ferrous alloys by deformation combined with, or followed by, heat treatment during manufacturing of articles with special electromagnetic properties
    • C21D8/1294Modifying the physical properties of ferrous metals or ferrous alloys by deformation combined with, or followed by, heat treatment during manufacturing of articles with special electromagnetic properties involving a localised 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

Landscapes

  • Chemical & Material Sciences (AREA)
  • Engineering & Computer Science (AREA)
  • Physics & Mathematics (AREA)
  • Crystallography & Structural Chemistry (AREA)
  • Materials Engineering (AREA)
  • Electromagnetism (AREA)
  • Manufacturing & Machinery (AREA)
  • Thermal Sciences (AREA)
  • Dispersion Chemistry (AREA)
  • Mechanical Engineering (AREA)
  • Power Engineering (AREA)
  • Metallurgy (AREA)
  • Organic Chemistry (AREA)
  • Manufacturing Of Steel Electrode Plates (AREA)
  • Heat Treatment Of Sheet Steel (AREA)
  • Heat Treatment Of Strip Materials And Filament Materials (AREA)
  • Soft Magnetic Materials (AREA)

Description

【発明の詳細な説明】 本発明は、種々の鉄損分布を持つ一方向性電磁鋼板コイ
ルの鉄損を全体として低損失のものにする鉄損改善方法
に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an iron loss improvement method for reducing the overall iron loss of unidirectional electrical steel sheet coils having various iron loss distributions.

一方向性電磁鋼板は硅素を数%含んだ鋼を圧延方向つま
リストリップ長さ方向に結晶粒の〔001)軸が揃いそ
して圧延面と平行に結晶粒の(110)面が並ぶように
圧延および焼鈍しかつ表面に絶縁被覆を被着し、コイル
状にして製品とされる。
Unidirectional electrical steel sheets are made by rolling steel containing several percent silicon so that the [001) axes of the crystal grains are aligned in the length direction of the rolling direction and the (110) planes of the crystal grains are aligned parallel to the rolling surface. Then, it is annealed, an insulating coating is applied to the surface, and the product is made into a coil shape.

この鋼板コイルの各部の鉄損を測定すると大きなバラつ
きがあるのが普通であり、一方、製品等級には鉄損値の
許容範囲があるから、例えばZ7Hの等級のオリエント
コアハイビー(新日本製鐵(株)製一方向性電磁鋼板の
商標)の製造に際し、鉄損測定値が許容値以上の部分は
切除し、低等級のものに廻すかそれにも転用不可能な劣
悪鉄損のものはスクラップとする、等の方法をとつてい
るのが実情である。この許容値以上の部分は、当然製造
歩留りを低下させる。ところで一方向性電磁鋼板に所定
要領でレーザ光を照射すると鉄損を改善することができ
る。本発明はこれを応用し、鉄損が許容値以上の部分に
レーザ光照射を行なつて該部分の鉄損を改善し、所望等
級の一方向性電磁鋼板の製造歩留りを向上させようとす
るものである。次に図面を参照しながらこれを詳細に説
明する。前述のように一方向性電磁鋼板は(110)〔
000組織を持ち、圧延方向に磁化が容易である。
When measuring the iron loss of each part of this steel plate coil, there is usually a large variation, but on the other hand, there is a permissible range of iron loss value depending on the product grade. When manufacturing unidirectional electrical steel sheets (trademark) manufactured by Co., Ltd., parts with measured iron loss values exceeding the allowable value are cut off, and parts with poor iron loss that cannot be used are either recycled to lower grade products or scrapped. The reality is that methods such as A portion exceeding this allowable value naturally reduces manufacturing yield. Incidentally, iron loss can be improved by irradiating a unidirectional electrical steel sheet with laser light in a predetermined manner. The present invention applies this to improve the iron loss of the portion by irradiating the laser beam to the portion where the iron loss exceeds the allowable value, thereby improving the manufacturing yield of grain-oriented electrical steel sheets of desired grade. It is something. Next, this will be explained in detail with reference to the drawings. As mentioned above, the unidirectional electrical steel sheet is (110) [
000 structure and is easily magnetized in the rolling direction.

か・る鋼板10に対し第1図aに示すように圧延方向F
にほぼ直角にレーザ光を線状、鎖線状または点線状に照
射すると (12は線状照射の場合におけるその照射部
分を示す)鉄損が小になる。これは次のように説明でき
る。即ち一方向性電磁鋼板10は第2図aに示すように
圧延方向に延びる比較的大きな磁区14を有する。一方
向性鋼板においては(110)〔001]方位の圧延方
向への集積度を高めるにつれて結晶粒が大きくなり、ま
た磁壁が粒界を貫通するために磁区は大きくなり、磁区
の大きさと鉄損値とは比例関係にあるので、方向性を高
めたり割り合いには鉄損は少なくならないという矛盾し
た問題があるものである。これに対し、レーザ光を圧延
方向とほぼ直角な方向に照射すると、詳しくはレーザ光
照射部分12が圧延方向Fにほぼ直角に延びるようにす
ると、その照射部分12の両側に小突起群16が発生す
る。これは走査型電子顕微鏡等で観察できる。なお図で
は簡単化のため小突起は一部しか示していない。この小
突起は磁区(マグネチツクドメイン)の芽であつて、磁
化されるとき鋼板10の磁区14はこの芽から伸びる磁
区18により細分化される。従つて鉄損は小になる。小
突起群16が生じるのは、鋼板10にレーザ光を照射す
ると転位が発生し、磁区の芽の発生確率はこの転位の密
度に比例することに依ると考えられる。第1図bに示す
ようにレーザ光を圧延方向に照射すると、第2図bに示
すようにやはり磁区の芽である小突起群16が発生する
As shown in FIG. 1a, the rolling direction F is
When the laser beam is irradiated in a line, chain line, or dotted line at a substantially right angle to the laser beam (12 indicates the irradiated part in the case of linear irradiation), the iron loss is reduced. This can be explained as follows. That is, the unidirectional electrical steel sheet 10 has a relatively large magnetic domain 14 extending in the rolling direction, as shown in FIG. 2a. In unidirectional steel sheets, as the degree of integration of the (110)[001] orientation in the rolling direction increases, the crystal grains become larger, and since the domain wall penetrates the grain boundary, the magnetic domain becomes larger, and the size of the magnetic domain and the iron loss Since there is a proportional relationship with the value, there is a contradictory problem in that increasing the directionality or increasing the ratio does not reduce the iron loss. On the other hand, when the laser beam is irradiated in a direction substantially perpendicular to the rolling direction, specifically, when the laser beam irradiated portion 12 extends substantially perpendicular to the rolling direction F, small projection groups 16 are formed on both sides of the irradiated portion 12. Occur. This can be observed using a scanning electron microscope or the like. Note that in the figure, only a portion of the small protrusions are shown for simplicity. These small protrusions are buds of magnetic domains, and when magnetized, the magnetic domains 14 of the steel plate 10 are subdivided by magnetic domains 18 extending from these buds. Therefore, iron loss becomes small. It is thought that the small protrusions 16 are generated because dislocations occur when the steel plate 10 is irradiated with laser light, and the probability of occurrence of magnetic domain buds is proportional to the density of these dislocations. When laser light is irradiated in the rolling direction as shown in FIG. 1b, small protrusions 16, which are buds of magnetic domains, are generated as shown in FIG. 2b.

外部磁界Hが作用するとこの芽16より微小ドメインが
発生し鉄損を下げるものと考えられる。理由は別かも知
れないがいずれにしてもこの場合も鉄損は減少する。具
体例を挙げると第1図aのようにレーザ光照射したもの
の圧延方向の鉄損WL(磁束密度1.7T、周波数50
Hz)は1.00W/Kgとなり、圧延方向と直角方向
の鉄損W。
It is thought that when an external magnetic field H is applied, microdomains are generated from this bud 16, which lowers the iron loss. The reason may be different, but in any case, the iron loss will decrease in this case as well. To give a specific example, the iron loss WL in the rolling direction (magnetic flux density 1.7T, frequency 50
Hz) is 1.00 W/Kg, which is the iron loss W in the direction perpendicular to the rolling direction.

(磁束密度1.3T、周波数50H,)はレーザ光照射
しないものと殆んど同じである。なおレーザ光照射前の
もののW,は1.10W/Kg.WOは2.84W/K
gである。つまり第1図aのレーザ光照射で10%のW
,の減少が可能になる。第1図bの場合はWLは殆んど
変らず、WOは2.04W/Kgとなり、約28%と大
幅なW。の減少が可能となつた。このような効果を得る
には、レーザ光照射に条件がある。
(Magnetic flux density: 1.3 T, frequency: 50 H) is almost the same as that without laser beam irradiation. The W before laser beam irradiation is 1.10W/Kg. WO is 2.84W/K
It is g. In other words, with the laser beam irradiation in Figure 1a, 10% W
, can be reduced. In the case of Fig. 1b, WL hardly changes, but WO becomes 2.04 W/Kg, which is a significant W of about 28%. It has become possible to reduce In order to obtain such an effect, there are conditions for laser light irradiation.

先ずレーザ光照射部分12の幅dとピツチlであるが、
第1図aの場合はd=0.01〜1mm,.1=1〜3
0mm、レーザパルスの時間幅は1nS〜100mSが
よい。第1図bの場合はd=0.01〜1mm,.1=
1〜30mm、レーザパルスの幅は1nS以上100m
S以下が好ましい。またエネルギ密度Pは両者とも0.
01〜100J/Crffが好ましい。なお本発明にお
いては、レーザ光を鎖線状あるいは点線状に照射しても
よい。この場合第1図aにおいてはL方向直径d=0.
01〜1mm、照射点C方向間隔aは3mm以下、好ま
しくは1mm以下がよく、また第1図bではC方向直径
d二0.01〜1mm、照射点L方向間隔aは3mm以
下、好ましくは1mm以下にすることがよい。また使用
レーザは衝撃を与えるのが目的であるからパルスレーザ
が最もよい。連続レーザは照射エネルギの一部が熱拡散
によつて面内に拡がり若干エネルギ損失を生じるために
パルスレーザより効率は悪くなる。第1図A,b共レー
ザ照射部分12の向きはそれぞれ正確に圧延方向つまり
〔001)方向に直角および平行に整列していなくて
も、それよりも±30゜程度の範囲でずれる分には効果
に格別の差はない。そこで本発明では圧延、焼鈍等の工
程を経てコイルに巻取られる、または該コイルを巻戻し
て幅調整のためのトリミングを施される。
First, the width d and pitch l of the laser beam irradiated portion 12 are as follows.
In the case of Fig. 1a, d=0.01 to 1 mm, . 1=1~3
0 mm, and the time width of the laser pulse is preferably 1 nS to 100 mS. In the case of Fig. 1b, d=0.01 to 1 mm, . 1=
1-30mm, laser pulse width is 1nS or more 100m
S or less is preferable. Moreover, the energy density P is 0.
01 to 100 J/Crff is preferable. In the present invention, the laser beam may be irradiated in the form of a chain line or a dotted line. In this case, in FIG. 1a, the diameter in the L direction d=0.
01 to 1 mm, the distance a in the irradiation point C direction is 3 mm or less, preferably 1 mm or less, and in FIG. It is preferable to set it to 1 mm or less. Furthermore, since the purpose of the laser used is to give a shock, a pulsed laser is best. Continuous lasers are less efficient than pulsed lasers because part of the irradiation energy spreads within the plane due to thermal diffusion, causing some energy loss. The orientation of the laser irradiated portion 12 in FIGS. 1A and 1B is not aligned perpendicularly and parallel to the rolling direction, that is, the [001) direction, but may deviate within a range of ±30° from that direction. There is no particular difference in effectiveness. Therefore, in the present invention, the coil is wound into a coil through processes such as rolling and annealing, or the coil is unwound and trimmed for width adjustment.

にれも勿論再びコイルに巻取る)一方向性電磁鋼板に
レーザ照射を行ない、鉄損不良部分を良化して全体とし
て低鉄損高級電磁鋼板にしようとするものである。第3
図にその実施例を示す。第3図で10は圧延、焼鈍、表
面処理などを施されてコイル24に巻取られる一方向性
電磁鋼板であり、20は走行中の鋼板10の鉄損を連続
的に測定する装置、22はレーザ光照射装置である。
The purpose is to irradiate a unidirectional electromagnetic steel sheet (which is then wound again into a coil) with a laser to improve the defective core loss areas, thereby creating a high-grade electromagnetic steel sheet with low core loss as a whole. Third
An example is shown in the figure. In FIG. 3, 10 is a unidirectional electrical steel sheet that has been subjected to rolling, annealing, surface treatment, etc. and wound into a coil 24, and 20 is a device that continuously measures the iron loss of the steel sheet 10 while it is running; is a laser beam irradiation device.

鉄損測定装置20としては、鋼板10を貫通されてこれ
を磁化する偏平コイル、および電圧計、電力計等を備え
る周知のものを利用する。レーザ光照射装置22として
はQスイツチング可能なルビーレーザ、YAGレーザ、
あるいはCO2レーザ、Arレーザ、COレーザなどの
連続発振レーザ等々任意のレーザを使用することができ
る。第1図A,bに示した縞状パターンのレーザ照射部
分12を形成するには、ビーム径又は辺の長さを部分1
2の幅dにしたレーザビームをミラーにより偏向して該
部分12の長さ方向に移動させるつまり走査する、又は
光学系によりレーザ光を整形してそのビーム断面形状が
1つ又は複数個のレーザ照射部分12と同じ形状のもの
にして照射する、その他適宜の方法をとる。一方向性電
磁鋼板10をコイル24に巻取りながらその全長に亘る
鉄損分布を鉄損測定装置20で測定すると第4図のC1
の如き鉄損値W対その出現頻度f曲線が得られる。
As the iron loss measuring device 20, a well-known device including a flat coil that penetrates the steel plate 10 and magnetizes it, a voltmeter, a wattmeter, etc. is used. As the laser beam irradiation device 22, Q-switchable ruby laser, YAG laser,
Alternatively, any laser such as a continuous wave laser such as a CO2 laser, an Ar laser, or a CO laser can be used. To form the laser irradiated portion 12 in the striped pattern shown in FIGS. 1A and 1B, the beam diameter or side length is
A laser beam having a width d of 2 is deflected by a mirror and moved in the length direction of the portion 12, that is, scanned, or the laser beam is shaped by an optical system so that the beam cross-sectional shape becomes one or more laser beams. It may be irradiated using a material having the same shape as the irradiated portion 12, or any other appropriate method may be used. When the iron loss distribution over the entire length of the unidirectional electrical steel sheet 10 is measured by the iron loss measuring device 20 while being wound around the coil 24, C1 in FIG.
A curve of the iron loss value W versus its appearance frequency f is obtained.

同じロッドの鋼板でも鉄損値のばらつきはかなりあり、
これが歩留り低下の原因になつている。そこで、今製造
しようとしている一方向性電磁鋼板が等級Ziのもので
あり、それに要求される鉄損値上限はWiとすれば、測
定装置20で鋼板10の各部の鉄損を連続的に測定して
その測定値がWi以上の部分があれば、その部分にレー
ザ装置22により第1図aに示した要領でパルスレーザ
光を照射する。これにより圧延方向の鉄損値を改善でき
、第4図C1の分布曲線をC2の如く改善することがで
きる。なおレーザ光照射すると鉄損の悪い部分ほど良く
改善される傾向があるので、曲線C2の幅は曲線C1の
それより狭くなる。鉄損改善の程度は10%程度である
からレーザ光照射により鋼板のすべての部分を鉄損値W
i内にするということは必ずしも可能ではない。
There is considerable variation in iron loss values even for steel plates of the same rod.
This is the cause of a decrease in yield. Therefore, if the unidirectional electrical steel sheet to be manufactured is of grade Zi, and the upper limit of iron loss required for it is Wi, the measuring device 20 continuously measures the iron loss of each part of the steel sheet 10. If there is a portion where the measured value is greater than Wi, that portion is irradiated with pulsed laser light by the laser device 22 in the manner shown in FIG. 1a. As a result, the iron loss value in the rolling direction can be improved, and the distribution curve C1 in FIG. 4 can be improved as shown in C2. Note that when irradiated with laser light, there is a tendency that the worse the core loss is, the better the improvement is, so the width of the curve C2 is narrower than that of the curve C1. Since the degree of iron loss improvement is about 10%, all parts of the steel plate can be reduced to iron loss value W by laser beam irradiation.
It is not necessarily possible to do so within i.

そこでレーザ光照射してもWi以下には収められない大
きな鉄損値Wi以上の部分についてはレーザ光照射を行
なわないのもよい。つまりこの場合は設定値はWi.W
jの2つを設定し、Wi<W<Wjでレーザ光照射を行
なうようにする。また鉄損値がWj以上の部分もこれに
レーザ光照射し、等級を下げて使用するのもよい。また
鋼板10をコイル24に巻取りながらその全長の鉄損分
布曲線C1を求め、レーザ光照射により大部分がある値
Wilになるその値Wilを求め、Wil以上でレーザ
光照射すると、当該鋼板コイルの大部分を可及的に高級
な電磁鋼板とすることができる。この場合はコイル全長
についての鉄損分布曲線を求める必要があるので一旦コ
イル24に巻き、これを巻戻してトリミングする工程で
、適当なトラツキング装置を使用しながらレーザ光照射
するとよい。なお鋼板10の鉄損分布が周期性を示す場
合はその1周期分等の鉄損測定で設定値Wilを決定で
きるから第3図のシステムで、即ちコイル24に巻きな
がら鉄損測定およびレーザ光照射を行なうことが可能で
ある。一方向性電磁鋼板はその特徴から見て明らかなよ
うに磁束を一方向つまり圧延方向または長さ方向に通す
場合に好適であり、磁束が多方向に通る場合には適さな
い。
Therefore, it is advisable not to irradiate laser light on portions where the iron loss value is greater than or equal to the large iron loss value Wi, which cannot be reduced to less than Wi even if irradiated with laser light. In other words, in this case, the setting value is Wi. W
j are set so that the laser beam irradiation is performed with Wi<W<Wj. It is also good to irradiate the portions with iron loss values of Wj or more with laser light to lower the grade and use them. In addition, while winding the steel plate 10 into the coil 24, find the iron loss distribution curve C1 of the entire length, find the value Wil where most of the steel plate 10 becomes a certain value Wil by irradiation with the laser beam, and when the steel plate 10 is irradiated with the laser beam at a value higher than Wil, the steel plate coil Most of the material can be made of the highest possible electrical steel sheet. In this case, since it is necessary to obtain an iron loss distribution curve for the entire length of the coil, it is preferable to irradiate the coil with laser light while using a suitable tracking device in the step of winding it once into the coil 24, unwinding it, and trimming it. If the iron loss distribution of the steel plate 10 shows periodicity, the set value Wil can be determined by measuring the iron loss for one period, etc. Therefore, in the system shown in FIG. It is possible to carry out irradiation. As is clear from its characteristics, unidirectional electrical steel sheets are suitable for passing magnetic flux in one direction, that is, in the rolling direction or in the longitudinal direction, but are not suitable for passing magnetic flux in multiple directions.

しかし、変圧器鉄心にしても巻鉄心は別としてEI型ま
たはCI型鉄心では概略的に見ても磁束は直交する二辺
従つて圧延方向およびそれと直角な方向の2方向に通る
ことになる。そこで鋼板10には第1図bに示す要領の
レーザ光照射を行ない、圧延方向と直角な方向つまり
〔110〕軸方向の鉄損を改善するのも有意義である。
この場合は鋼板幅方向に磁化してその鉄損を測定する必
要があり、従つて鉄損測定装置20としては鋼板貫通の
偏平コイルではなく、鋼板を磁路の一部に組込んだほぼ
閉磁路の鉄心利用の既知のものなどを使用する。以上説
明したように本発明によればレーザ光照射という比較的
簡単な手段で一方向性電磁鋼板のグレードアツプまたは
歩留り向上を図ることができ、甚だ有益である。
However, even in the case of transformer cores, apart from wound cores, in EI type or CI type cores, the magnetic flux passes in two directions, that is, two orthogonal sides, that is, the rolling direction and a direction perpendicular thereto. Therefore, the steel plate 10 is irradiated with a laser beam as shown in FIG.
[110] It is also meaningful to improve the axial iron loss.
In this case, it is necessary to magnetize the steel plate in the width direction and measure its iron loss. Therefore, the iron loss measuring device 20 is not a flat coil that penetrates the steel plate, but a nearly closed magnetic field that incorporates the steel plate into a part of the magnetic path. Use known iron cores for roads. As explained above, according to the present invention, it is possible to improve the grade or yield of unidirectional electrical steel sheets by the relatively simple means of laser beam irradiation, which is extremely beneficial.

【図面の簡単な説明】[Brief explanation of drawings]

第1図A,bはレーザ光照射要領を説明する図、第2図
A,bは鉄損改善理由の説明図、第3図は本発明の実施
例を説明する図、第4図は鉄損改善状態を説明する図で
ある。 図面で10は一方向性電磁鋼板、12はレーザ光照射部
分、20は鉄損測定装置、22はレーザ光照射装置であ
る。
Figures 1A and b are diagrams explaining the laser beam irradiation procedure, Figures 2A and b are diagrams explaining the reason for improving iron loss, Figure 3 is a diagram explaining the embodiment of the present invention, and Figure 4 is a diagram explaining the iron loss improvement method. It is a figure explaining a loss improvement state. In the drawing, 10 is a unidirectional electrical steel sheet, 12 is a laser beam irradiation part, 20 is an iron loss measuring device, and 22 is a laser beam irradiation device.

Claims (1)

【特許請求の範囲】[Claims] 1 ストリップ状の一方向性電磁鋼板の移送中に連続的
に該鋼板の鉄損を測定し、該鉄損が設定値以上となる鋼
板部分にレーザ光を、レーザ光照射部分がほぼ圧延方向
または圧延方向とほぼ直角な方向に延びる所定幅および
ピッチの縞状になるように照射することを特徴とした電
磁鋼板コイルの鉄損改善方法。
1. Continuously measure the iron loss of the strip-shaped unidirectional electrical steel sheet while it is being transferred, and apply a laser beam to the portion of the steel sheet where the iron loss exceeds a set value. A method for improving iron loss in an electromagnetic steel sheet coil, characterized by irradiating the coil in a striped manner with a predetermined width and pitch extending in a direction substantially perpendicular to the rolling direction.
JP54161320A 1979-12-12 1979-12-12 Method for improving iron loss in magnetic steel sheet coils Expired JPS5953684B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP54161320A JPS5953684B2 (en) 1979-12-12 1979-12-12 Method for improving iron loss in magnetic steel sheet coils

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP54161320A JPS5953684B2 (en) 1979-12-12 1979-12-12 Method for improving iron loss in magnetic steel sheet coils

Publications (2)

Publication Number Publication Date
JPS5683905A JPS5683905A (en) 1981-07-08
JPS5953684B2 true JPS5953684B2 (en) 1984-12-26

Family

ID=15732845

Family Applications (1)

Application Number Title Priority Date Filing Date
JP54161320A Expired JPS5953684B2 (en) 1979-12-12 1979-12-12 Method for improving iron loss in magnetic steel sheet coils

Country Status (1)

Country Link
JP (1) JPS5953684B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN104451068A (en) * 2013-09-16 2015-03-25 宝山钢铁股份有限公司 Oriented silicon steel strip with diagonal stripes, and production method thereof

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP5691265B2 (en) * 2010-06-30 2015-04-01 Jfeスチール株式会社 Method for producing grain-oriented electrical steel sheet

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN104451068A (en) * 2013-09-16 2015-03-25 宝山钢铁股份有限公司 Oriented silicon steel strip with diagonal stripes, and production method thereof

Also Published As

Publication number Publication date
JPS5683905A (en) 1981-07-08

Similar Documents

Publication Publication Date Title
EP0102732B1 (en) Laser treatment of electrical steel and optical scanning assembly thereof
JP5477438B2 (en) Method for producing grain-oriented electrical steel sheet
US4456812A (en) Laser treatment of electrical steel
RU2509163C1 (en) Texture sheet of electric steel and method of its production
EP0008385B1 (en) Grain-oriented electromagnetic steel sheet and method for its production
RU2238340C2 (en) Method for improving magnetic qualities of textured electrical silicon steel sheets by laser treatment
JP4782248B1 (en) Oriented electrical steel sheet and manufacturing method thereof
EP2918689B1 (en) Laser processing apparatus and laser irradiation method
JP7406064B2 (en) Method for manufacturing grain-oriented electrical steel sheet and method for manufacturing wound iron core
US20140034193A1 (en) Method for Producing a Grain-Oriented Flat Steel Product
US4724015A (en) Method for improving the magnetic properties of Fe-based amorphous-alloy thin strip
WO2019156220A1 (en) Grain-oriented electrical steel sheet
US5089062A (en) Drilling of steel sheet
KR20190078161A (en) Grain oriented electrical steel sheet and method for refining magnetic domains therein
JPH0253935B2 (en)
JPH01281709A (en) Method of obtaining heat-resistant fractionalized magnetic domains in electrical steel to reduce core loss
JPS5953684B2 (en) Method for improving iron loss in magnetic steel sheet coils
KR20200076503A (en) Grain oriented electrical steel sheet and method for manufacturing the same
JPS5850297B2 (en) Electrical steel sheet with excellent magnetic properties
KR840000179B1 (en) How to improve the iron loss characteristics of oriented electrical steel sheets
US5067992A (en) Drilling of steel sheet
JPS60216511A (en) Improving method of magnetism of amorphous magnetic alloy thin-band
JPS5826410B2 (en) Grain-oriented electrical steel sheet with excellent magnetic properties
GB2169147A (en) Cores for electrical machinery
JPS60213005A (en) Manufacture of amorphous magnetic core