JPH024918A - Manufacture of non-oriented thick electrical plate having high magnetic flux density - Google Patents
Manufacture of non-oriented thick electrical plate having high magnetic flux densityInfo
- Publication number
- JPH024918A JPH024918A JP15464088A JP15464088A JPH024918A JP H024918 A JPH024918 A JP H024918A JP 15464088 A JP15464088 A JP 15464088A JP 15464088 A JP15464088 A JP 15464088A JP H024918 A JPH024918 A JP H024918A
- Authority
- JP
- Japan
- Prior art keywords
- less
- flux density
- rolling
- plate
- magnetic flux
- 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.)
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Classifications
-
- C—CHEMISTRY; METALLURGY
- C21—METALLURGY OF IRON
- C21D—MODIFYING THE PHYSICAL STRUCTURE OF FERROUS METALS; GENERAL DEVICES FOR HEAT TREATMENT OF FERROUS OR NON-FERROUS METALS OR ALLOYS; MAKING METAL MALLEABLE, e.g. BY DECARBURISATION OR TEMPERING
- C21D3/00—Diffusion processes for extraction of non-metals; Furnaces therefor
- C21D3/02—Extraction of non-metals
- C21D3/06—Extraction of hydrogen
-
- C—CHEMISTRY; METALLURGY
- C21—METALLURGY OF IRON
- C21D—MODIFYING THE PHYSICAL STRUCTURE OF FERROUS METALS; GENERAL DEVICES FOR HEAT TREATMENT OF FERROUS OR NON-FERROUS METALS OR ALLOYS; MAKING METAL MALLEABLE, e.g. BY DECARBURISATION OR TEMPERING
- C21D8/00—Modifying the physical properties of ferrous metals or ferrous alloys by deformation combined with, or followed by, heat treatment
- C21D8/12—Modifying 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
- C21D8/1216—Modifying 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 characterised by the working steps
- C21D8/1222—Hot rolling
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- Chemical & Material Sciences (AREA)
- Engineering & Computer Science (AREA)
- Physics & Mathematics (AREA)
- Thermal Sciences (AREA)
- Crystallography & Structural Chemistry (AREA)
- Mechanical Engineering (AREA)
- Materials Engineering (AREA)
- Metallurgy (AREA)
- Organic Chemistry (AREA)
- Electromagnetism (AREA)
- Manufacturing & Machinery (AREA)
- Manufacturing Of Steel Electrode Plates (AREA)
Abstract
Description
【発明の詳細な説明】
[産業上の利用分野]
近年最先端科学技術である素粒子研究や医療機器の進歩
に伴って、大型構造物に磁気を用いる装置が使われ、そ
の性能向上が求められている。[Detailed Description of the Invention] [Industrial Application Field] In recent years, with advances in elementary particle research and medical equipment, which are cutting-edge science and technology, devices that use magnetism are used in large structures, and there is a demand for improved performance. It is being
本発明はここにおいて直流磁化条件で使用される磁石の
鉄心用あるいは磁場を遮蔽するのに必要な磁気シールド
用の磁束密度の高い無方向性電磁厚鋼板の製造法に関す
るものである。The present invention relates to a method for manufacturing a non-oriented electromagnetic thick steel plate with a high magnetic flux density for the iron core of a magnet used under DC magnetization conditions or for a magnetic shield necessary for shielding a magnetic field.
[従来の技術]
磁束密度に優れた電磁鋼板としては、従来から薄板分野
で珪素鋼板、電磁軟鉄板をはじめとする数多くの材料が
提供されているのは公知である。[Prior Art] It is well known that many materials including silicon steel plates and electromagnetic soft iron plates have been provided in the field of thin plates as electromagnetic steel plates with excellent magnetic flux density.
しかし、構造部材として使用するには組み立て加工及び
強度上の問題があり、厚鋼板を利用する必要が生じてく
る。これまで電磁厚板としては純鉄系成分で製造されて
いる。たとえば、特開昭60−96749号公報が公知
である。However, when used as a structural member, there are problems with assembly and strength, and it becomes necessary to use thick steel plates. Until now, electromagnetic plates have been manufactured using pure iron-based components. For example, Japanese Patent Laid-Open No. 60-96749 is known.
しかしながら、近年の装置の大型化、能力の向上等に伴
いさらに磁気特性の優れた、とくに低磁場、たとえば8
0A/mでの磁束密度の高い鋼材開発の要望が強い。前
掲の特許等で開発された鋼材では、80A/mでの低磁
場での高い磁束密度が安定して得られない。However, in recent years, as devices have become larger and their capabilities have improved, devices with even better magnetic properties, especially in low magnetic fields, such as 8
There is a strong demand for the development of steel materials with high magnetic flux density at 0 A/m. With the steel materials developed in the above-mentioned patents, it is not possible to stably obtain a high magnetic flux density in a low magnetic field of 80 A/m.
[発明が解決しようとする課題]
本発明の目的は以上の点を鑑みなされたもので、低磁場
での磁束密度の高く、その板厚方向での磁気特性差の少
ない無方向性電磁厚板の製造法を提供することにある。[Problems to be Solved by the Invention] The purpose of the present invention was to provide a non-oriented electromagnetic thick plate that has a high magnetic flux density in a low magnetic field and has small differences in magnetic properties in the thickness direction. The objective is to provide a manufacturing method.
[課題を解決するための手段]
本発明は重量%で、c : o、ot%以下、Si :
0.02%以下、Mn:0.20%以下、P : 0.
015%以下、S : 0.010%以下、Cr:0.
05%以下、MO:0、旧%以下、Cu:0.01%以
下、Afi:0.005〜0.040%、N・0.00
4%以下、O:0.005%以下、H: 0.0002
%以下、残部実質的に鉄からなる鋼組成の鋼片または鋳
片を1150〜1300℃に加熱し、仕上げ温度を90
0℃以上となる条件下で圧延形状比Aが0.7以上の圧
延パスが1回以上はとる圧延を行った後、板厚50mm
以上の厚板については600〜750℃の脱水素熱処理
を行った後、圧下率5〜25%の冷間圧延を行い、その
後750〜950℃で焼鈍を行い、板厚20mm以上5
0mm未満については圧下率5〜25%の冷間圧延を行
い、その後750〜950℃で焼鈍することを特徴とす
る磁場80A/mでの磁束密度が0.8テスラ以上の磁
気特性を有する板厚20+am以上の磁束密度の高い無
方向性電磁厚板の製造法である。[Means for Solving the Problems] The present invention is based on weight%, c: o, ot% or less, Si:
0.02% or less, Mn: 0.20% or less, P: 0.
015% or less, S: 0.010% or less, Cr: 0.015% or less, S: 0.010% or less, Cr: 0.
05% or less, MO: 0, old % or less, Cu: 0.01% or less, Afi: 0.005 to 0.040%, N・0.00
4% or less, O: 0.005% or less, H: 0.0002
% or less, the remainder of which is essentially iron, is heated to 1150 to 1300°C, and the finishing temperature is 90°C.
After rolling at least one rolling pass with a rolling shape ratio A of 0.7 or more under conditions of 0°C or higher, the plate thickness is 50 mm.
For the above-mentioned thick plates, after dehydrogenation heat treatment at 600-750℃, cold rolling at a reduction rate of 5-25%, and then annealing at 750-950℃, the plate thickness is 20mm or more.
A plate having magnetic properties with a magnetic flux density of 0.8 Tesla or more in a magnetic field of 80 A/m, characterized by cold rolling with a rolling reduction of 5 to 25% for thicknesses of less than 0 mm, and then annealing at 750 to 950°C. This is a method for manufacturing a non-directional electromagnetic thick plate having a thickness of 20+am or more and having a high magnetic flux density.
ただし、
A= (2117肩1石「ろ)/h、十hI Q
1 0
A :圧延形状比
り、:入側板厚 (關)
h :出側板厚 (mm)
R:圧延ロール半径(止)
[作 用]
まず、低磁場での磁束密度を高くするために磁化のプロ
セスについて述べると、消磁状態の鋼を磁界の中に入れ
、磁界を強めていくと次第に磁区の向きに変化が生じ、
磁界の方向に近い磁区が優勢になり他の磁区を蚕食併合
していく。つまり、磁壁の移動が起こる。However, A = (2117 shoulder 1 stone "ro")/h, 10hI Q
10 A: Relative to rolled shape,: Inlet side plate thickness (related) h: Outlet side plate thickness (mm) R: Roll radius (stop) [Function] First, magnetization is applied to increase the magnetic flux density in a low magnetic field. Describing the process, when demagnetized steel is placed in a magnetic field and the magnetic field is strengthened, the orientation of the magnetic domains gradually changes.
The magnetic domains close to the direction of the magnetic field become dominant and merge with other magnetic domains. In other words, movement of the domain wall occurs.
さらに磁界か強くなり磁壁の移動が完了すると、次に磁
区全体の磁力方向が向きを変えていく。この磁化プロセ
スの中で低磁場での磁束密度を決めるのは磁壁の移動し
やすさである。When the magnetic field becomes stronger and the movement of the domain wall is completed, the direction of the magnetic force of the entire magnetic domain changes direction. In this magnetization process, the ease with which domain walls move determines the magnetic flux density in low magnetic fields.
つまり低磁場で高磁束密度を得るためには、磁壁の移動
を障害するものを極力減らすことであると定性的に言う
ことができる。In other words, it can be said qualitatively that in order to obtain a high magnetic flux density in a low magnetic field, it is necessary to reduce as much as possible what impedes the movement of domain walls.
発明者らはここにおいて低磁場で高磁束密度を得るため
の手段として、粒径と内部応力の原因となる元素及び空
隙性欠陥の作用につき詳細な検討を行い、まず粗粒化の
ためには、本発明においては厚板圧延では従来者えられ
なかった冷間圧延による加工歪の導入とその後の焼鈍に
より、異常粒成長が生じフェライト粒径が粗大に成長す
る適正条件を見出した。Here, as a means to obtain high magnetic flux density in a low magnetic field, the inventors conducted a detailed study on the effects of grain size, elements that cause internal stress, and void defects, and first, in order to coarsen the grains, In the present invention, we have found appropriate conditions in which abnormal grain growth occurs and the ferrite grain size grows coarsely by introducing working strain by cold rolling and subsequent annealing, which was not possible in the past in thick plate rolling.
第1図にフェライト粒径に及ぼす冷間圧延率の影響を示
す。Figure 1 shows the influence of cold rolling rate on ferrite grain size.
10%を中心に5〜25%の冷間圧延率で結晶率の大幅
な粗大化が起こっている。そのほか、結晶粒微細化作用
を有するA47Nを減少するため、Ag。At cold rolling ratios of 5 to 25%, centering around 10%, a significant coarsening of the crystal ratio occurs. In addition, Ag is used to reduce A47N, which has a crystal grain refining effect.
Nの低下すること及び製造方法としては、加熱温度を極
力上げ加熱オーステナイト粒の粗大化、圧延仕上げ温度
を極力高めにすることが合わせて必要である。In order to reduce the amount of N and the manufacturing method, it is necessary to raise the heating temperature as much as possible to coarsen the heated austenite grains, and to make the rolling finishing temperature as high as possible.
内部応力減少のための元素の影響としては、Cの低下が
必要である。第2図に示す0.01SiO,L Mn
−0,01AN鋼にあって、C含有量の増加につれ低磁
場(80A/m)での磁束密度が低下している。As an elemental influence for reducing internal stress, a reduction in C is necessary. 0.01SiO,L Mn shown in Figure 2
In -0,01AN steel, the magnetic flux density in a low magnetic field (80 A/m) decreases as the C content increases.
また、間隙欠陥の影響についても種々検討した結果、そ
のサイズか100μ以上のものが磁気特性を大幅に低下
することを知見したものである。そしてこの100μ以
上の有害な空隙性欠陥をなくすためには圧延形状比Aが
0.7以上必要であることを見出した。Furthermore, as a result of various studies on the influence of gap defects, it was found that the size of gap defects of 100 μm or more significantly deteriorates the magnetic properties. It has also been found that in order to eliminate harmful void defects of 100 microns or more, the rolled shape ratio A needs to be 0.7 or more.
さらに、鋼中の水素の存在も第3図に示すように有害で
、脱水素熱処理を行うことによって磁気特性か大幅に向
上することを知見した。第3図で示すように0.007
− C−0,OIS i −0,I Mn鋼にあって高
形状比圧延により空隙性欠陥のサイズを100μ以下に
し、かつ、脱水素熱処理により鋼中水素を減少すること
で低磁場での磁束密度が大幅に上昇することがわかる。Furthermore, the presence of hydrogen in steel is also harmful, as shown in Figure 3, and it has been found that dehydrogenation heat treatment can significantly improve magnetic properties. 0.007 as shown in Figure 3
- C-0, OIS i -0, I In Mn steel, the size of porosity defects is reduced to 100μ or less by high shape ratio rolling, and the hydrogen in the steel is reduced by dehydrogenation heat treatment, thereby increasing the magnetic flux in a low magnetic field. It can be seen that the density increases significantly.
さらに、磁気特性の均質性を確保することも重要である
が、本発明による方法によれば、これに対しても極めて
有効な手段であることを確認した。Furthermore, it is also important to ensure homogeneity of magnetic properties, and it has been confirmed that the method according to the present invention is an extremely effective means for this as well.
次に本発明の成分限定理由をのべる。Next, the reason for limiting the ingredients of the present invention will be described.
Cは鋼中の内部応力を高め、磁気特性、とくに低磁場で
の磁束密度を最も下げる元素であり、極力下げることが
低磁場での磁束密度を低下させないことに寄与する。ま
た、磁気時効の点からも低いほど経時劣化が少なく磁気
特性の良い状態で恒久的に使用できるものであり、この
ようなことから0.010%以下に限定する。C is an element that increases the internal stress in steel and lowers the magnetic properties, particularly the magnetic flux density in a low magnetic field, the most, and reducing it as much as possible contributes to not reducing the magnetic flux density in a low magnetic field. In addition, from the viewpoint of magnetic aging, the lower the content, the less deterioration over time and the ability to use it permanently with good magnetic properties.For this reason, the content is limited to 0.010% or less.
第1図に示すように、さらに0.005%以下にするこ
とにより一層高磁束密度が得られる。As shown in FIG. 1, an even higher magnetic flux density can be obtained by reducing the amount to 0.005% or less.
Si、Mnは低磁場での磁束密度の点から少ない方が好
ましくMnはMnS系介在物を生成する点からも低い方
がよい。この意味からSlは0.02%以下、Mnは0
.20%以下に限定する。Mnに関してはMnS系介在
物を生成する点よりさらに望ましくは0.10%以下が
よい。The lower the Si and Mn content, the better from the viewpoint of magnetic flux density in a low magnetic field, and the lower the Mn content, also from the viewpoint of generating MnS-based inclusions. From this meaning, Sl is 0.02% or less and Mn is 0.
.. Limited to 20% or less. Regarding Mn, from the point of view of forming MnS-based inclusions, it is more desirable that it be 0.10% or less.
p、s、oは鋼中において非金属介在物を形成しかつ偏
析することにより、磁壁の移動を妨げる害を及ぼし、含
有量が多くなるに従って磁束密度の低下が見られ、磁気
特性を低下させるので少ないほどよい。このためPは0
.015%以下、Sは0.010%以下、Oは0.00
596以下とした。P, s, and o form nonmetallic inclusions in steel and segregate, thereby hindering the movement of domain walls, and as their content increases, the magnetic flux density decreases, resulting in a decrease in magnetic properties. So the less the better. Therefore, P is 0
.. 015% or less, S is 0.010% or less, O is 0.00
It was set to 596 or less.
Cr 、Mo 、Cuは低磁場での磁束密度を低下させ
るので少ない程好ましく、また偏析度合を少なくするこ
とから極力低くすることが必要であり、この意味からC
rは0.05%以下、Moは0.01%以下、Cuは0
,01%以下とする。Cr, Mo, and Cu reduce the magnetic flux density in a low magnetic field, so the smaller the better, and in order to reduce the degree of segregation, it is necessary to keep them as low as possible.
r is 0.05% or less, Mo is 0.01% or less, Cu is 0
,01% or less.
Alは脱酸剤として用いるもので本発明の如く板厚の厚
い場合には、内質の均質化に不可欠の元素であり、0.
005%以上添加されるが、多くなりすぎると介在物を
生成し鋼の性質を損なうので上限は0.040%以下と
する。さらに結晶粒微細化作用を有するAlNを減少さ
せるためには、望ましくは0.020%以下がよい。Al is used as a deoxidizing agent and is an essential element for homogenizing the internal quality when the plate is thick as in the present invention.
The upper limit is set to 0.040% or less, since too much may generate inclusions and impair the properties of the steel. Furthermore, in order to reduce AlN, which has a crystal grain refining effect, the content is desirably 0.020% or less.
Nは内部応力を高めかつAρNにより結晶粒微細化作用
により、低磁場での磁束密度を低下させるので上限は0
.004%以下とする。The upper limit is 0 because N increases the internal stress and AρN reduces the magnetic flux density in a low magnetic field due to the grain refinement effect.
.. 0.004% or less.
Hは電磁特性を低下させ、かつ、空隙性欠陥の減少を妨
げるので0.0002%以下とする。Since H deteriorates electromagnetic properties and prevents the reduction of void defects, it is set to 0.0002% or less.
次に製造法について述べる。Next, the manufacturing method will be described.
圧延条件については、まず圧延前加熱温度を1150℃
以上にするのは、加熱オーステナイト粒を粗大化し磁気
特性をよくするためである。1300℃を超す加熱はス
ケールロスの防止、省エネルギーの観点から不必要であ
るため上限を1300℃とした。Regarding the rolling conditions, first, the heating temperature before rolling was set to 1150°C.
The reason for this is to coarsen the heated austenite grains and improve the magnetic properties. Since heating above 1300°C is unnecessary from the viewpoint of preventing scale loss and saving energy, the upper limit was set at 1300°C.
圧延仕上げ温度については、900℃以下の仕上げでは
低温圧延により結晶粒が微細化し、磁気特性が低下する
ため結晶粒の粗大化による磁束密度の上昇を狙い900
℃以上とした。As for the rolling finishing temperature, if the finishing temperature is below 900℃, the crystal grains will become finer due to low-temperature rolling, and the magnetic properties will deteriorate.
℃ or higher.
さらに熱間圧延にあたり、前述の空隙性欠陥は鋼の凝固
過程で大小はあるが、必す発生するものでありこれをな
くす手段は圧延によらなければならないので、熱間圧延
の役目は重要である。Furthermore, in hot rolling, the role of hot rolling is important because the above-mentioned porous defects are inevitably generated during the solidification process of steel, and rolling is the only way to eliminate them. be.
すなわち、熱間圧延1回当たりの変形量を大きくし板厚
中心部にまで変形が及ぶ熱間圧延が有効である。具体的
には圧延形状比Aが067以上の圧延パスが1回以上を
含む高形状比圧延を行い、空隙性欠陥のサイズを100
μ以下にすることが電磁特性によい。That is, hot rolling in which the amount of deformation per hot rolling is increased and the deformation extends to the center of the plate thickness is effective. Specifically, high shape ratio rolling including one or more rolling passes with rolling shape ratio A of 067 or more is performed, and the size of the void defects is reduced to 100.
Setting it below μ is good for electromagnetic properties.
圧延中にこの高形状比圧延により空隙性欠陥をなくすこ
とで、後で行う脱水素熱処理における脱水素効率が飛躍
的に上昇するのである。By eliminating void defects during rolling by this high shape ratio rolling, the dehydrogenation efficiency in the subsequent dehydrogenation heat treatment is dramatically increased.
次に熱間圧延に引き続き、板厚50mm以上の厚手材に
ついては脱水素熱処理を施す。板厚50mm以上では水
素の拡散がしにくく、これが空隙性欠陥の原因となり、
かつ、水素自身の作用と合わさって低磁場での磁束密度
を低下させる。Next, following hot rolling, thick materials with a thickness of 50 mm or more are subjected to dehydrogenation heat treatment. If the plate thickness is 50 mm or more, it is difficult for hydrogen to diffuse, which causes void defects.
In addition, combined with the action of hydrogen itself, it lowers the magnetic flux density in a low magnetic field.
このため、脱水素熱処理を行うが、この脱水素熱処理温
度としては600℃未満では脱水素効率が悪く、750
℃超では変態が一部開始するので600〜750℃の温
度範囲で行う。For this reason, dehydrogenation heat treatment is performed, but if the dehydrogenation heat treatment temperature is less than 600°C, the dehydrogenation efficiency is poor;
If the temperature exceeds .degree. C., transformation will partially start, so the temperature range is 600 to 750.degree.
脱水素時間としては種々検討の結果[0,8(t50)
+6)時間(t:板厚)が適当である。As a result of various studies, the dehydrogenation time [0.8 (t50)
+6) Time (t: plate thickness) is appropriate.
さらに、冷間圧延と焼鈍を組み合わせ、異常粒成長によ
るフェライト粒径の粗大化をねらう。冷間圧延率として
は第1図に示すように5〜25%がよい。焼鈍は結晶粒
粗大化及び内部歪除去のために行うか、750℃未満で
は結晶粒粗大化が起こらず、また、950℃以上では結
晶粒の板厚方向の均質性が保てないため、焼鈍温度とし
ては750〜950℃に限定する。Furthermore, by combining cold rolling and annealing, we aim to coarsen the ferrite grain size through abnormal grain growth. The cold rolling rate is preferably 5 to 25% as shown in FIG. Annealing is carried out to coarsen the crystal grains and remove internal strain. At temperatures below 750°C, coarsening of the crystal grains does not occur, and at temperatures above 950°C, the homogeneity of the crystal grains in the thickness direction cannot be maintained. The temperature is limited to 750 to 950°C.
一方、板厚20mrn以上50mm未満のものは水素の
拡散が容易なため、脱水素熱処理は不要で前述の冷間圧
延と焼鈍を施こすのみで良い。On the other hand, when the plate thickness is 20 mrn or more and less than 50 mm, hydrogen can easily diffuse, so dehydrogenation heat treatment is not necessary and only the cold rolling and annealing described above are required.
[実 施 例]
第1表に電磁厚板の製造条件とフェライト粒径、低磁場
での磁束密度を示す。[Example] Table 1 shows the manufacturing conditions of the electromagnetic plate, the ferrite grain size, and the magnetic flux density in a low magnetic field.
] 2
例1〜10は本発明の実施例を示し、例11〜31は比
較例を示す。] 2 Examples 1 to 10 show examples of the present invention, and Examples 11 to 31 show comparative examples.
例1〜5は板厚120關に仕上げたもので、均一かつ粗
粒て高い磁気特性を示す。例1に比べ、さらに例2は低
C1例3,4は低Mns例5は低Aρであり、より高い
磁気特性を示す。例6〜8は550mm、例9は50m
m、例10は20mmに仕上げたもので、均一かつ粗粒
で高い磁気特性を示す。Examples 1 to 5 were finished to a plate thickness of about 120 mm and exhibit uniform, coarse grains and high magnetic properties. Compared to Example 1, Example 2 has a low C, Examples 3 and 4 have a low Mns, and Example 5 has a low Aρ, showing higher magnetic properties. Examples 6-8 are 550mm, Example 9 is 50m
m, Example 10 is finished to 20 mm, has uniform and coarse grains, and exhibits high magnetic properties.
例■1はCが高く、例12はSLが高く、例13はM口
が高く、例14はPが高く、例15はSが高く、例16
はCrが高く、例17はMOが高く、例18はCuが高
く、例19はA、Illが高く、例20はNが高く、例
21は0が高く、例22はHが高く、それぞれ上限を超
えるため低磁気特性値となっている。Example ■1 has high C, Example 12 has high SL, Example 13 has high M mouth, Example 14 has high P, Example 15 has high S, and Example 16
is high in Cr, Example 17 is high in MO, Example 18 is high in Cu, Example 19 is high in A and Ill, Example 20 is high in N, Example 21 is high in 0, Example 22 is high in H, respectively. Since it exceeds the upper limit, the magnetic property value is low.
例23は加熱温度が下限をはずれ、例24は圧延仕上げ
温度が下限をはずれ、例25は最大形状比が下限をはず
れ、例26は脱水素熱処理湿度が下限をはずれ、例27
は焼鈍温度が下限をはずれ、例28は焼鈍温度が上限を
超え、例29は脱水素熱処理がなく、例30は冷間圧延
がなく、例31は冷間圧延率が上限を超えるため低磁気
特性値となっている。In Example 23, the heating temperature was outside the lower limit, in Example 24, the rolling finish temperature was outside the lower limit, in Example 25, the maximum shape ratio was outside the lower limit, in Example 26, the dehydrogenation heat treatment humidity was outside the lower limit, and in Example 27.
The annealing temperature exceeds the lower limit in Example 28, the annealing temperature exceeds the upper limit in Example 29, there is no dehydrogenation heat treatment in Example 30, there is no cold rolling in Example 30, and the cold rolling rate exceeds the upper limit in Example 31, resulting in low magnetism. It is a characteristic value.
[発明の効果]
以上詳細に述べた如く、本発明によれば適切な成分限定
と、従来の厚板圧延では考えられなかった冷間圧延と焼
鈍の組み合わせにより、板厚の厚い厚鋼板に均質な高電
磁特性を具備せしめることに成功し、直流磁化による磁
気性質を利用する構造物に適用可能としたものであり、
産業上多大な効果を奏するものである。[Effects of the Invention] As described in detail above, according to the present invention, by appropriately limiting the ingredients and by combining cold rolling and annealing, which was unthinkable in conventional thick plate rolling, thick steel plates can be uniformly rolled. We succeeded in providing high electromagnetic properties, making it applicable to structures that utilize magnetic properties due to direct current magnetization.
This has great industrial effects.
第1図はフェライト粒径に及ぼす冷間圧延率の影響を示
すグラフ、第2図は80A/mにおける磁束密度に及ぼ
すC含有量の影響を示すグラフ、第3図は80A/rn
における磁束密度に及ぼす空隙性欠陥の大きさ及び脱水
素熱処理の影響を示すグラフである。
代 理 人 弁理士 茶野木 立 夫第
図
′A?−閾圧延牢
(%)
第
図
?θ
第
図
空隙姓又貼のサノにシ)Figure 1 is a graph showing the effect of cold rolling rate on ferrite grain size, Figure 2 is a graph showing the effect of C content on magnetic flux density at 80A/m, and Figure 3 is a graph showing the effect of C content on magnetic flux density at 80A/rn.
3 is a graph showing the influence of the size of void defects and dehydrogenation heat treatment on the magnetic flux density in FIG. Agent Patent Attorney Tatsuo Chanoki Diagram 'A? −Threshold rolling cell (%) Fig.? θ Diagram 3)
Claims (1)
50〜1300℃に加熱し、仕上げ温度を900℃以上
となる条件下で圧延形状比Aが0.7以上の圧延パスが
1回以上はとる圧延を行った後、板厚50mm以上の厚
板については600〜750℃の脱水素熱処理を行った
後、圧下率5〜25%の冷間圧延を行い、その後750
〜950℃で焼鈍を行い、板厚20mm以上50mm未
満については圧下率5〜25%の冷間圧延を行い、その
後750〜950℃で焼鈍することを特徴とする磁場8
0A/mでの磁束密度が0.8テスラ以上の磁気特性を
有する板厚20mm以上の磁束密度の高い無方向性電磁
厚板の製造法。 ただし、 A=(2√R(h_i−h_o))/h_i+h_o A:圧延形状比 h_i:入側板厚(mm) h_o:出側板厚(mm) R:圧延ロール半径(mm)[Claims] In weight %, C: 0.01% or less, Si: 0.02% or less, Mn: 0.20% or less, P: 0.015% or less, S: 0.010% or less, Cr: 0.05% or less, Mo: 0.01% or less, Cu: 0.01% or less, Al: 0.005 to 0.040%, N: 0.004% or less, O: 0.005% or less , H: 0.0002% or less, and the remainder is substantially iron.
A thick plate with a thickness of 50 mm or more is heated to 50 to 1300°C and rolled with at least one rolling pass with a rolling shape ratio A of 0.7 or more under conditions where the finishing temperature is 900°C or higher. After dehydrogenation heat treatment at 600 to 750°C, cold rolling was performed at a reduction rate of 5 to 25%, and then 750°C
Magnetic field 8 characterized by performing annealing at ~950°C, cold rolling at a reduction rate of 5 to 25% for plate thicknesses of 20 mm or more and less than 50 mm, and then annealing at 750 to 950°C.
A method for manufacturing a non-directional electromagnetic thick plate having a thickness of 20 mm or more and having a high magnetic flux density and having magnetic properties with a magnetic flux density of 0.8 Tesla or more at 0 A/m. However, A=(2√R(h_i-h_o))/h_i+h_o A: Rolling shape ratio h_i: Inlet side plate thickness (mm) h_o: Outlet side plate thickness (mm) R: Roll radius (mm)
Priority Applications (4)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP63154640A JPH0711026B2 (en) | 1988-06-24 | 1988-06-24 | Manufacturing method of non-directional electromagnetic thick plate with high magnetic flux density |
| US07/368,031 US4950336A (en) | 1988-06-24 | 1989-06-19 | Method of producing non-oriented magnetic steel heavy plate having high magnetic flux density |
| DE68921377T DE68921377T2 (en) | 1988-06-24 | 1989-06-23 | Process for the production of non-oriented heavy steel plates with high magnetic flux density. |
| EP89111463A EP0349853B1 (en) | 1988-06-24 | 1989-06-23 | Method of producing non-oriented magnetic steel heavy plate having high magnetic flux density |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP63154640A JPH0711026B2 (en) | 1988-06-24 | 1988-06-24 | Manufacturing method of non-directional electromagnetic thick plate with high magnetic flux density |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH024918A true JPH024918A (en) | 1990-01-09 |
| JPH0711026B2 JPH0711026B2 (en) | 1995-02-08 |
Family
ID=15588634
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP63154640A Expired - Lifetime JPH0711026B2 (en) | 1988-06-24 | 1988-06-24 | Manufacturing method of non-directional electromagnetic thick plate with high magnetic flux density |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0711026B2 (en) |
Cited By (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH03274228A (en) * | 1990-03-26 | 1991-12-05 | Sumitomo Metal Ind Ltd | Production of hot rolled steel plate for magnetic shielding |
| JPH03274229A (en) * | 1990-03-26 | 1991-12-05 | Sumitomo Metal Ind Ltd | Production of hot rolled steel plate for magnetic shielding |
| JPH03274230A (en) * | 1990-03-26 | 1991-12-05 | Sumitomo Metal Ind Ltd | Production of hot rolled steel plate for magnetic shielding |
| US5411605A (en) * | 1991-10-14 | 1995-05-02 | Nkk Corporation | Soft magnetic steel material having excellent DC magnetization properties and corrosion resistance and a method of manufacturing the same |
| CN108463569A (en) * | 2016-01-15 | 2018-08-28 | 杰富意钢铁株式会社 | Non orientation electromagnetic steel plate and its manufacturing method |
Citations (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS6096749A (en) * | 1983-11-01 | 1985-05-30 | Nippon Steel Corp | Thick plate for dc magnetization and preparation thereof |
| JPS60208418A (en) * | 1984-03-30 | 1985-10-21 | Sumitomo Metal Ind Ltd | Method for manufacturing thick steel plates for high magnetic permeability structural members |
| JPS6389621A (en) * | 1986-10-01 | 1988-04-20 | Kobe Steel Ltd | Production of core material for flat plate-shaped linear pulse motor |
-
1988
- 1988-06-24 JP JP63154640A patent/JPH0711026B2/en not_active Expired - Lifetime
Patent Citations (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS6096749A (en) * | 1983-11-01 | 1985-05-30 | Nippon Steel Corp | Thick plate for dc magnetization and preparation thereof |
| JPS60208418A (en) * | 1984-03-30 | 1985-10-21 | Sumitomo Metal Ind Ltd | Method for manufacturing thick steel plates for high magnetic permeability structural members |
| JPS6389621A (en) * | 1986-10-01 | 1988-04-20 | Kobe Steel Ltd | Production of core material for flat plate-shaped linear pulse motor |
Cited By (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH03274228A (en) * | 1990-03-26 | 1991-12-05 | Sumitomo Metal Ind Ltd | Production of hot rolled steel plate for magnetic shielding |
| JPH03274229A (en) * | 1990-03-26 | 1991-12-05 | Sumitomo Metal Ind Ltd | Production of hot rolled steel plate for magnetic shielding |
| JPH03274230A (en) * | 1990-03-26 | 1991-12-05 | Sumitomo Metal Ind Ltd | Production of hot rolled steel plate for magnetic shielding |
| US5411605A (en) * | 1991-10-14 | 1995-05-02 | Nkk Corporation | Soft magnetic steel material having excellent DC magnetization properties and corrosion resistance and a method of manufacturing the same |
| CN108463569A (en) * | 2016-01-15 | 2018-08-28 | 杰富意钢铁株式会社 | Non orientation electromagnetic steel plate and its manufacturing method |
| US11008633B2 (en) | 2016-01-15 | 2021-05-18 | Jfe Steel Corporation | Non-oriented electrical steel sheet and production method thereof |
Also Published As
| Publication number | Publication date |
|---|---|
| JPH0711026B2 (en) | 1995-02-08 |
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