JPH0689401B2 - Manufacturing method of electromagnetic thick plate for non-directional DC magnetization - Google Patents
Manufacturing method of electromagnetic thick plate for non-directional DC magnetizationInfo
- Publication number
- JPH0689401B2 JPH0689401B2 JP15464588A JP15464588A JPH0689401B2 JP H0689401 B2 JPH0689401 B2 JP H0689401B2 JP 15464588 A JP15464588 A JP 15464588A JP 15464588 A JP15464588 A JP 15464588A JP H0689401 B2 JPH0689401 B2 JP H0689401B2
- Authority
- JP
- Japan
- Prior art keywords
- less
- rolling
- magnetic
- temperature
- plate thickness
- 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 - Lifetime
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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
- 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
-
- 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
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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)
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 field of application] In recent years, along with the progress of elementary particle research and medical equipment, which are the most advanced science and technology, devices that use magnetism for large structures are used, and it is necessary to improve their performance. Has been.
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 an electromagnetic thick steel plate having a high magnetic flux density for an iron core of a magnet used under a DC magnetization condition 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。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。[Prior Art] As magnetic steel sheets having excellent magnetic flux density, it is well known that a number of materials such as silicon steel sheets and electromagnetic soft iron sheets have been provided in the field of thin sheets. However, there are problems in assembly processing and strength when used as a structural member,
It becomes necessary to use thick steel plates. Until now, electromagnetic plates have been manufactured with pure iron-based components. For example, JP-A-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80
A/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, with the recent increase in size of equipment and improvement in performance, magnetic properties are even better, especially in low magnetic fields, such as 80
There is a strong demand for the development of steel materials with high magnetic flux density at A / m. The steel materials developed by the above patents cannot stably obtain a high magnetic flux density at 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
ない無方向性直流磁化用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 object of the present invention is made in view of the above points, and for non-directional DC magnetization having a high magnetic flux density in a low magnetic field and a small magnetic characteristic difference in the plate thickness direction. It is to provide a manufacturing method of an electromagnetic thick plate.
[課題を解決するための手段] 本発明の要旨は次の通りである。[Means for Solving the Problems] The gist of the present invention is as follows.
(1)重量%で、 C:0.01%以下、Si:0.02%以下、Mn:0.20%以下、P:0.01
5%以下、S:0.010%以下、Cr:0.05%以下、Mo:0.01%以
下、Cu:0.01%以下、Ti:0.005〜0.03%、Ca:0.0005〜0.
01%、Al:0.005%以下、N:0.004%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
延パスを1回以上とる圧延を行い、板厚50mm以上の厚板
とし、該厚板を600〜750℃の温度で脱水素熱処理を行う
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無方向性直流磁化用電磁厚板の製
造法。(1)% by weight, C: 0.01% or less, Si: 0.02% or less, Mn: 0.20% or less, P: 0.01
5% or less, S: 0.010% or less, Cr: 0.05% or less, Mo: 0.01% or less, Cu: 0.01% or less, Ti: 0.005 to 0.03%, Ca: 0.0005 to 0.
01%, Al: 0.005% or less, N: 0.004% or less, O: 0.005% or less, H: 0.0002% or less, the balance heating a steel slab or a slab of steel composition consisting essentially of iron to 1150 to 1300 ° C. Then, under the condition that the finishing temperature is 900 ° C. or higher, the rolling shape ratio A is 0.7 or more and the rolling is performed once or more to obtain a thick plate having a thickness of 50 mm or more. A method for producing an electromagnetic slab for non-directional DC magnetization, which has a magnetic characteristic of a magnetic flux density of 0.8 Tesla or more at a magnetic field of 80 A / m, characterized by performing a dehydrogenation heat treatment at a temperature.
ただし、 A :圧延形状比 hi:入側板厚(mm) ho:出側板厚(mm) R :圧延ロール半径(mm) (2)板厚50mm以上の厚板を脱水素熱処理後750〜950℃
で焼鈍するかあるいは910〜1000℃で焼準することを特
徴とする(1)記載の無方向性直流磁化用電磁厚板の製
造法。However, A: Rolling shape ratio h i : Inlet side plate thickness (mm) h o : Outlet side plate thickness (mm) R: Rolling roll radius (mm) (2) After dehydrogenation heat treatment of plates with a plate thickness of 50 mm or more 750 to 950 ° C
The method for producing an electromagnetic thick plate for non-directional DC magnetization according to (1), characterized in that it is annealed at 910.degree.
(3)重量%で、 C:0.01%以下、Si:0.02%以下、Mn:0.20%以下、P:0.01
5%以下、S:0.010%以下、Cr:0.05%以下、Mo:0.01%以
下、Cu:0.01%以下、Ti:0.005〜0.03%、Ca:0.0005〜0.
01%、Al:0.005%以下、N:0.004%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
延パスを1回以上とる圧延を行い、板厚20mm以上50mm未
満の厚板とし、該厚板を750〜950℃の温度で焼鈍するか
あるいは910〜1000℃の温度で焼準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
有する無方向性直流磁化用電磁厚板の製造法。(3) In% by weight, C: 0.01% or less, Si: 0.02% or less, Mn: 0.20% or less, P: 0.01
5% or less, S: 0.010% or less, Cr: 0.05% or less, Mo: 0.01% or less, Cu: 0.01% or less, Ti: 0.005 to 0.03%, Ca: 0.0005 to 0.
01%, Al: 0.005% or less, N: 0.004% or less, O: 0.005% or less, H: 0.0002% or less, the balance heating a steel slab or a slab of steel composition consisting essentially of iron to 1150 to 1300 ° C. Then, under the condition that the finishing temperature is 900 ° C. or higher, rolling is performed with a rolling pass having a rolling shape ratio A of 0.7 or more one or more times to obtain a thick plate having a plate thickness of 20 mm or more and less than 50 mm, and the plate is 750 to 950. Of an electromagnetic slab for non-directional DC magnetization having magnetic characteristics of a magnetic flux density of 0.8 Tesla or more at a magnetic field of 80 A / m characterized by annealing at a temperature of ℃ or normalizing at a temperature of 910 to 1000 ℃ Manufacturing method.
A :圧延形状比 hi:入側板厚(mm) ho:出側板厚(mm) R :圧延ロール半径(mm) [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。 A: Rolling shape ratio h i : Inlet side plate thickness (mm) h o : Outlet side plate thickness (mm) R: Rolling roll radius (mm) [Operation] First, the magnetization process to increase the magnetic flux density in a low magnetic field. For example, when demagnetized steel is put in a magnetic field and the magnetic field is strengthened, the direction of the magnetic domain gradually changes, and the magnetic domain close to the direction of the magnetic field becomes dominant and the other magnetic domains are annealed. That is, the domain wall moves.
さらに磁界が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 is further strengthened and the movement of the domain wall is completed, the direction of the magnetic force of the entire magnetic domain then changes direction. It is the ease of movement of the domain wall that determines the magnetic flux density in a low magnetic field during this magnetization process.
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。That is, it can be qualitatively said that in order to obtain a high magnetic flux density in a low magnetic field, it is necessary to reduce as much as possible the obstacles to the movement of the domain wall.
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、粒径への元素の効果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、低磁場で高磁束密度特性を有する鋼板の製造法を発
明したものである。As a means for obtaining a high magnetic flux density in a low magnetic field, the inventors here have made a detailed study on the effect of the element on the grain size and the effect of the element and the void defect causing the internal stress, and Inventing a method for manufacturing a steel sheet having high magnetic flux density characteristics.
まず、粗粒化のためには、結晶粒微細化作用を有するAl
Nを減少するため、Al,Nの低下することが必要である。
特に、Alについては第1図に示すように低くするに従い
フェライト粒の粒成長が起こるが、無添加の領域、つま
り、0.005%以下、になると結晶粒の異常な粒成長が起
こることを知見した。ただし、Alを無添加にすると別の
脱酸剤を添加する必要がある。First, for coarsening, Al which has a grain refining effect
In order to reduce N, it is necessary to reduce Al and N.
In particular, for Al, grain growth of ferrite grains occurs as it is lowered as shown in FIG. 1, but it was found that abnormal grain growth of crystal grains occurs in a non-added region, that is, 0.005% or less. . However, if Al is not added, it is necessary to add another deoxidizer.
本発明者らはここにおいてこのAlに代わる脱酸剤で、か
つ低磁場での磁束密度を低下させない元素としてTiとCa
の複合添加がよいことを知見した。The present inventors used Ti and Ca as deoxidizing agents instead of Al and as elements that do not reduce the magnetic flux density in a low magnetic field.
It was found that the combined addition of
さらに、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
し、圧延による結晶粒の微細化を防止すること並びに圧
延後の焼鈍をすることである。Further, as a manufacturing method, the heating temperature is raised as much as possible, the heating austenite grains are coarsened, and the rolling finishing temperature is raised as much as possible to prevent the grain refinement due to rolling and to carry out annealing after rolling.
内部応力減少のためには、Cの低下が必要である。第2
図に示す0.01Si−0.1Mn−0.01Al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するこ
とがわかる。In order to reduce the internal stress, it is necessary to reduce C. Second
It can be seen that in the 0.01Si-0.1Mn-0.01Al steel shown in the figure, the magnetic flux density in a low magnetic field (80A / m) decreases as the C content increases.
さらに鋼中の水素の存在の有害で、第3図に示すよう
に、脱水素熱処理を行うことによって磁気特性が大幅に
向上することを知見した。第3図で示すように0.007C−
0.01Si−0.1Mn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、内部応力も減少し低磁
場での磁束密度が大幅に上昇することがわかる。Further, it was found that the presence of hydrogen in the steel is harmful, and as shown in FIG. 3, the magnetic properties are significantly improved by performing the dehydrogenation heat treatment. As shown in Fig. 3, 0.007C-
In 0.01Si-0.1Mn steel, by reducing the size of void defects to 100μ or less by high shape ratio rolling and reducing hydrogen in the steel by dehydrogenation heat treatment, internal stress is also reduced and magnetic flux at low magnetic field is reduced. It can be seen that the density increases significantly.
空隙性欠陥の影響についても種々検討した結果、そのサ
イズが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。そしてこの空隙性欠陥をなくすために
は、圧延形状比Aが0.7以上で十分であることを見出し
た。As a result of various studies on the effect of void defects, it was found that the magnetic properties were significantly reduced when the size was 100 μ or more. It was found that a rolled shape ratio A of 0.7 or more is sufficient to eliminate the void defects.
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。It is also important to ensure the homogeneity of the magnetic properties, but the method according to the present invention is an extremely effective means for this.
次に本発明の成分限定理由をのべる。Next, the reasons for limiting the components of the present invention will be given.
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。第2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。C is an element that increases the internal stress in steel and lowers the magnetic characteristics, especially the magnetic flux density in a low magnetic field, and reducing it as much as possible contributes to not lowering the magnetic flux density in a low magnetic field. In addition, the lower the magnetic aging is, the less the deterioration with time is, and the permanent magnet can be used with good magnetic properties. Therefore, the content is limited to 0.010% or less. As shown in FIG. 2, a higher magnetic flux density can be obtained by further setting the content 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Si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。Si and Mn are preferably small in terms of magnetic flux density in a low magnetic field, and Mn is also preferably low in terms of producing MnS-based inclusions.
From this meaning, Si is limited to 0.02% or less and Mn is limited to 0.20% or less. Mn is more preferably 0.10% or less from the viewpoint of forming MnS inclusions.
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
多くなる点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、0.005%以下とした。P, S, O form non-metallic inclusions in steel and segregate to impede the movement of the magnetic domain wall, and as the content increases, the magnetic flux density decreases and the magnetic properties deteriorate. So the less, the better. Therefore, P is 0.015
%, S is 0.010% or less, and O is 0.005% 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Crは0.05%以
下、Moは0.01%以下、Cuは0.01%以下とする。Cr, Mo, Cu decrease the magnetic flux density in a low magnetic field, so the smaller the better, and it is necessary to make it as low as possible in order to reduce the degree of segregation. From this meaning, Cr is 0.05% or less, Mo is 0.01%. Hereinafter, Cu is 0.01% or less.
Ti,CaはAlに代わる複合脱酸元素として用いるため、そ
れぞれ0.005%及び0.0005%以上添加されるが、0.04%
及び0.01%以上では低磁場での磁束密度を低下させるの
で、Tiは0.005〜0.03%に、Caは0.0005〜0.01%に限定
する。Since Ti and Ca are used as complex deoxidizing elements instead of Al, 0.005% and 0.0005% or more are added respectively, but 0.04%
And 0.01% or more lowers the magnetic flux density in a low magnetic field, so Ti is limited to 0.005 to 0.03% and Ca is limited to 0.0005 to 0.01%.
AlはAlNを生成し結晶粒微細化作用を有するため極力低
下させる必要があるので、0.005%以下とする。Since Al produces AlN and has a grain refining effect, it is necessary to reduce it as much as possible, so the content is made 0.005% or less.
Nは内部応力を高めかつAlN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、0.00
4%以下とする。N increases the internal stress and reduces the magnetic flux density in a low magnetic field due to the grain refining effect of AlN, so the upper limit is 0.00
4% 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。H reduces the electromagnetic characteristics and prevents the reduction of void defects, so H content 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 is set to 1150 ° C. or higher in order to coarsen the heated austenite grains and improve the magnetic properties. Heating above 1300 ° C is unnecessary from the viewpoints of preventing scale loss and saving energy, so the upper limit was made 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。Regarding the rolling finishing temperature, at the finishing of 900 ° C or lower, the crystal grains become finer due to the low temperature rolling and the magnetic properties are deteriorated, so the temperature was set to 900 ° C or higher in order to increase the magnetic flux density due to the coarsening of the crystal grains.
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、必ず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。Further, in the hot rolling, the above-mentioned void defects are large and small in the solidification process of steel, but they are always generated and the means for eliminating them must be done by rolling. Therefore, the role of hot rolling is important.
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0.7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100μ以
下にすることが電磁特性によい。That is, it is effective to increase the amount of deformation per hot rolling so that the deformation reaches the center of the plate thickness. Specifically, it is preferable for the electromagnetic characteristics to perform the high shape ratio rolling including one or more rolling passes with the rolling shape ratio A of 0.7 or more, and to make the size of the void defect 100 μm or less.
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 the void defects by the high shape ratio rolling during rolling, the dehydrogenation efficiency in the dehydrogenation heat treatment to be performed later is dramatically increased.
次に熱間圧延に引き続き結晶粒粗大化、内部歪除去及び
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。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。Then, following hot rolling, grain coarsening, internal strain removal, and dehydrogenation heat treatment are applied to thick materials with a plate thickness of 50 mm or more.
When the plate thickness is 50 mm or more, it is difficult for hydrogen to diffuse, which causes void defects and, together with the action of hydrogen itself, reduces the magnetic flux density in a low magnetic field. For this reason, the dehydrogenation heat treatment is performed, but if the dehydrogenation heat treatment temperature is less than 600 ° C, the dehydrogenation efficiency is poor, and if it exceeds 750 ° C, the transformation starts partially, so the dehydrogenation heat treatment is performed in the temperature range of 600 to 750 ° C.
脱水素時間としては種々検討の結果〔0.6(t−50)+6
0〕時間(t:板厚)が適当である。As the dehydrogenation time, the results of various studies [0.6 (t-50) + 6
0] Time (t: plate thickness) is appropriate.
焼鈍は結晶粒粗大化及び内部歪除去のために行うが、75
0℃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。Annealing is performed for grain coarsening and internal strain removal.
If the temperature is lower than 0 ° C., the crystal grains do not coarsen, and if the temperature is 950 ° C. or higher, the uniformity of the crystal grains in the plate thickness direction cannot be maintained. Therefore, the annealing temperature is limited to 750 to 950 ° C.
焼準は板厚方向の結晶粒調整及び内部歪除去のために行
うが、焼準温度は910〜1000℃に限定する。910℃未満で
はオーステナイト域とフェライト域の現在により結晶粒
が混粒となり、1000℃超では結晶粒の板厚方向の均質性
が保てない。なお、磁気特性向上のためには、結晶粒粗
大化と内部歪み除去とが考えられるが、特に内部歪み除
去は必須条件である。内部歪み除去は、板厚50mm以上の
厚手材では脱水素熱処理で行うことができる。したがっ
て、本発明の厚手材では脱水素熱処理で、上記焼鈍ある
いは焼準を兼ねることができる。Normalizing is performed to adjust the crystal grains in the plate thickness direction and remove internal strain, but the normalizing temperature is limited to 910 to 1000 ° C. Below 910 ° C, the crystal grains become mixed grains due to the present in the austenite and ferrite regions, and above 1000 ° C, the homogeneity of the crystal grains in the plate thickness direction cannot be maintained. In order to improve the magnetic properties, coarsening of crystal grains and removal of internal strain can be considered, but removal of internal strain is an essential condition. Internal strain can be removed by dehydrogenation heat treatment for thick materials with a thickness of 50 mm or more. Therefore, in the thick material of the present invention, the dehydrogenation heat treatment can also serve as the above-mentioned annealing or normalization.
一方、板厚20mm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焼鈍または焼準を
施せば良い。On the other hand, when the plate thickness is 20 mm or more and less than 50 mm, hydrogen diffusion is easy, so dehydrogenation heat treatment is not necessary and the above-mentioned annealing or normalization may be performed.
[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。[Examples] Table 1 shows the manufacturing conditions of the electromagnetic thick plate, the ferrite grain size, and the magnetic flux density in a low magnetic field.
例1〜12は本発明の実施例を示し、例13〜35は比較例を
示す。例1〜7は板厚100mmに仕上げたもので、均一か
つ粗粒で高い磁気特性を示す。例1に比べ、さらに例4
は低C、例5,6は低Mn、例7は低Alであり、より高い磁
気特性を示す。 Examples 1 to 12 show examples of the present invention, and Examples 13 to 35 show comparative examples. Examples 1 to 7 are finished to a plate thickness of 100 mm and show high magnetic characteristics with uniform and coarse grains. Compared to Example 1, further Example 4
Is low C, Examples 5 and 6 are low Mn, and Example 7 is low Al, showing higher magnetic properties.
例8〜10は500mm、例11は40mm、例12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。例13はC
が高く、例14はSiが高く、例15はMnが高く、例16はPが
高く、例17はSが高く、例18はCrが高く、例19はMoが高
く、例20はCuが高く、例21はTiが高く、例22はCaが高
く、例23はTiとCaの両方が高く、例24,25はAlが高く、
例26はNが高く、例27はOが高く、例28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。Examples 8 to 10 were finished to 500 mm, Example 11 to 40 mm, and Example 12 to 20 mm, showing uniform and coarse grains and high magnetic properties. Example 13 is C
, Example 14 has high Si, Example 15 has high Mn, Example 16 has high P, Example 17 has high S, Example 18 has high Cr, Example 19 has high Mo, and Example 20 has high Cu. High, Example 21 has high Ti, Example 22 has high Ca, Example 23 has high both Ti and Ca, Examples 24 and 25 have high Al,
Example 26 has a high N value, Example 27 has a high O value, and Example 28 has a high H value.
例29は加熱温度が下限をはずれ、例30は圧延仕上げ温度
が下限をはずれ、例31は最大形状比が下限をはずれ、例
32は脱水素熱処理温度が下限をはずれ、例33は焼鈍温度
が下限をはずれ、例34は焼準温度が上限を超え、例35は
脱水素熱処理がないため低磁気特性値となっている。In Example 29, the heating temperature is below the lower limit, in Example 30, the rolling finish temperature is below the lower limit, and in Example 31, the maximum shape ratio is below the lower limit.
In Example 32, the dehydrogenation heat treatment temperature is out of the lower limit, in Example 33, the annealing temperature is out of the lower limit, in Example 34, the normalizing temperature exceeds the upper limit, and in Example 35, the dehydrogenation heat treatment is absent, so that the magnetic property value is low.
[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
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、かつその製造法
も前述の成分限定と、熱間圧延後結晶粒調整及び脱水素
熱処理を同時に行う方式であり、極めて経済的な製造法
を提供するもので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, it has been possible to provide a thick steel plate having a large thickness with uniform high electromagnetic characteristics by appropriately limiting the components, and to utilize the magnetic properties of direct current magnetization. It is applicable to a structure that has the above-mentioned structure, and its manufacturing method is a method of simultaneously limiting the above-mentioned components and simultaneously performing crystal grain adjustment and dehydrogenation heat treatment after hot rolling, which provides an extremely economical manufacturing method. It has a great industrial effect.
【図面の簡単な説明】 第1図はフェライト粒径に及ぼすAl含有量の影響をを示
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/m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。BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 is a graph showing the effect of Al content on the ferrite grain size, and FIG. 2 is C on the magnetic flux density at 80 A / m.
FIG. 3 is a graph showing the influence of the content, and FIG. 3 is a graph showing the influence of the size of the void defects and the dehydrogenation heat treatment on the magnetic flux density at 80 A / m.
Claims (3)
5%以下、S:0.010%以下、Cr:0.05%以下、Mo:0.01%以
下、Cu:0.01%以下、Ti:0.005〜0.03%、Ca:0.0005〜0.
01%、Al:0.005%以下、N:0.004%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
延パスを1回以上とる圧延を行い、板厚50mm以上の厚板
とし、該厚板を600〜750℃の温度で脱水素熱処理を行う
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無方向性直流磁化用電磁厚板の製
造法。 ただし、 A :圧延形状比 hi:入側板厚(mm) ho:出側板厚(mm) R :圧延ロール半径(mm)1. By weight%, C: 0.01% or less, Si: 0.02% or less, Mn: 0.20% or less, P: 0.01
5% or less, S: 0.010% or less, Cr: 0.05% or less, Mo: 0.01% or less, Cu: 0.01% or less, Ti: 0.005 to 0.03%, Ca: 0.0005 to 0.
01%, Al: 0.005% or less, N: 0.004% or less, O: 0.005% or less, H: 0.0002% or less, the balance heating a steel slab or a slab of steel composition consisting essentially of iron to 1150 to 1300 ° C. Then, under the condition that the finishing temperature is 900 ° C. or higher, rolling is performed by taking a rolling pass with a rolling shape ratio A of 0.7 or more one or more times to obtain a thick plate having a plate thickness of 50 mm or more, and the thick plate of 600 to 750 ° C. A method for manufacturing an electromagnetic slab for non-directional DC magnetization, which has a magnetic property of a magnetic flux density of 0.8 Tesla or more at a magnetic field of 80 A / m, characterized by performing a dehydrogenation heat treatment at a temperature. However, A: Rolling shape ratio h i : Inlet plate thickness (mm) h o : Outlet plate thickness (mm) R: Rolling roll radius (mm)
〜950℃で焼鈍するかあるいは910〜1000℃で焼準するこ
とを特徴とする請求項1記載の無方向性直流磁化用電磁
厚板の製造法。2. A 750-mm thick plate having a thickness of 50 mm or more after dehydrogenation heat treatment
2. The method for manufacturing an electromagnetic thick plate for non-directional DC magnetization according to claim 1, wherein the annealing is performed at .about.950.degree. C. or the temperature is normalized at 910.degree.
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以上の圧延パスを1回以上と
る圧延を行い、板厚20mm以上50mm未満の厚板とし、該厚
板を750〜950℃の温度で焼鈍するかあるいは910〜1000
℃の温度で焼準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無方向性直
流磁化用電磁厚板の製造法。 ただし A :圧延形状比 hi:入側板厚(mm) ho:出側板厚(mm) R :圧延ロール半径(mm)3. In% by 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, Ti: 0.005 to 0.03%, Ca: 0.0005 to 0.01%, Al: 0.005% or less, N: 0.004% or less, O: 0.005% or less, H: 0.0002% or less, and the balance substantially iron A steel slab or a slab with a steel composition consisting of 11
Rolling is performed by heating to 50 to 1300 ° C. and taking a rolling pass with a rolling shape ratio A of 0.7 or more at least once under the condition that the finishing temperature is 900 ° C. or more to obtain a thick plate having a plate thickness of 20 mm or more and less than 50 mm. Anneal the plate at a temperature of 750-950 ℃ or 910-1000
A method for manufacturing an electromagnetic slab for non-directional DC magnetization, which has a magnetic characteristic of a magnetic flux density of 0.8 Tesla or more at a magnetic field of 80 A / m, characterized by normalizing at a temperature of ℃. However A: Rolling shape ratio h i : Inlet plate thickness (mm) h o : Outlet plate thickness (mm) R: Rolling roll radius (mm)
Priority Applications (4)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP15464588A JPH0689401B2 (en) | 1988-06-24 | 1988-06-24 | Manufacturing method of electromagnetic thick plate for non-directional DC magnetization |
| 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 |
| EP89111463A EP0349853B1 (en) | 1988-06-24 | 1989-06-23 | 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. |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP15464588A JPH0689401B2 (en) | 1988-06-24 | 1988-06-24 | Manufacturing method of electromagnetic thick plate for non-directional DC magnetization |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH024923A JPH024923A (en) | 1990-01-09 |
| JPH0689401B2 true JPH0689401B2 (en) | 1994-11-09 |
Family
ID=15588752
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP15464588A Expired - Lifetime JPH0689401B2 (en) | 1988-06-24 | 1988-06-24 | Manufacturing method of electromagnetic thick plate for non-directional DC magnetization |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0689401B2 (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2564994B2 (en) * | 1991-10-14 | 1996-12-18 | 日本鋼管株式会社 | Soft magnetic steel material excellent in direct current magnetization characteristics and corrosion resistance and method for producing the same |
-
1988
- 1988-06-24 JP JP15464588A patent/JPH0689401B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPH024923A (en) | 1990-01-09 |
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