JP6524438B2 - Hot-rolled sheet for non-oriented electrical steel sheet, method for producing the same, non-oriented electrical steel sheet having excellent magnetic properties, and method for producing the same - Google Patents
Hot-rolled sheet for non-oriented electrical steel sheet, method for producing the same, non-oriented electrical steel sheet having excellent magnetic properties, and method for producing the same Download PDFInfo
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Description
本発明は、ハイブリッド自動車、電気自動車、燃料電池自動車に搭載される駆動モータや、二輪車および家庭用コージェネレーションシステムに搭載される小型発電機など、高いエネルギー効率と小型・高出力化を同時に要求される電気機器の鉄心の素材に好適な無方向性電磁鋼板およびその製造方法に関する。本発明は、さらに、無方向性電磁鋼板に用いられる無方向性電磁鋼板用熱延板とその製造方法に関する。 The present invention simultaneously demands high energy efficiency and small size and high power, such as drive motors mounted on hybrid vehicles, electric vehicles and fuel cell vehicles, and small generators mounted on two-wheeled vehicles and household cogeneration systems. TECHNICAL FIELD The present invention relates to a non-oriented electrical steel sheet suitable for a core material of an electric device and a method of manufacturing the same. The present invention further relates to a hot rolled sheet for non-oriented electrical steel sheet used for non-oriented electrical steel sheet and a method of manufacturing the same.
高効率モータには、低鉄損と高磁束密度を両立した無方向性電磁鋼板が要求される。近年、高効率モータへの要求が高まっており、特に高周波域での低鉄損と高磁束密度を両立した無方向性電磁鋼板への要求が強くなる傾向にある。無方向性電磁鋼板の高周波域における低鉄損化の手段には、Si、Alなどの合金元素添加による高比抵抗化があるが、磁束密度が低下する傾向がある。磁束密度を向上させるため、固溶Cによる冷延パス間時効を活用する技術と、高P材にバッチ焼鈍炉での熱延板焼鈍を施し、Pの粒界偏析を活用する技術が知られている。例えば特許文献1には、二回以上の冷間圧延のパス間において50〜300℃の温度で1〜10minの時効処理を行うことにより固溶Cを残存させることにより、圧延方向に高い磁束密度を有する無方向性電磁鋼板を製造する方法が開示されている。また、例えば特許文献2には、冷延前鋼板の粒界にPを偏析させることにより冷延後の集合組織を改善し、高い磁束密度を有する無方向性電磁鋼板を製造する方法が開示されている。 High-efficiency motors require non-oriented electrical steel sheets that have both low iron loss and high magnetic flux density. In recent years, the demand for a high efficiency motor has been increasing, and in particular, the demand for a non-oriented electrical steel sheet having both a low iron loss and a high magnetic flux density in a high frequency region tends to be strong. As a means for reducing iron loss in the high frequency region of the non-oriented electrical steel sheet, there is a high specific resistance by the addition of alloy elements such as Si and Al, but the magnetic flux density tends to decrease. In order to improve the magnetic flux density, there are known a technology that utilizes cold rolling interpass aging by solid solution C, and a technology that performs hot rolled sheet annealing in a batch annealing furnace on a high P material and utilizes grain boundary segregation of P. ing. For example, in Patent Document 1, a high magnetic flux density in the rolling direction is obtained by leaving solid solution C by performing an aging treatment at a temperature of 50 to 300 ° C. for 1 to 10 minutes between two or more cold rolling passes. A method of manufacturing a non-oriented electrical steel sheet having the Further, for example, Patent Document 2 discloses a method of improving the texture after cold rolling by segregating P at grain boundaries of a steel sheet before cold rolling to produce a non-oriented electrical steel sheet having a high magnetic flux density. ing.
本発明者らは、Pの粒界偏析を活用して磁束密度を向上させる技術と、冷延パス間時効によって固溶Cを活用して磁束密度を向上させる技術を同時に活用することについて検討した。 The present inventors examined simultaneously utilizing the technology of improving the magnetic flux density by utilizing grain boundary segregation of P and the technology of improving the magnetic flux density by utilizing solid solution C by cold rolling interpass aging. .
そして、その検討初期において、この組合せには以下のような問題が存在することを認識した。すなわち、高P材で冷延時にPが粒界に偏析していると冷延焼鈍後の磁束密度は向上するが、冷延前にPを粒界に偏析させるためには熱延巻取り後または熱延焼鈍後の冷却速度を低速にする必要がある。しかしながら、熱延焼鈍後の冷却速度が低速であると鋼中の固溶Cが得られなくなり、冷延パス間の時効処理による磁束密度向上が達成できなくなる。また、Pを粒界に偏析させた高P材はもともと冷延性が低下する懸念を有しているが、冷延パス間時効により鋼板は硬化するため冷延性はさらに低下し、熱延焼鈍後の冷却速度が低速であると粒界にセメンタイトが形成し、冷延性は顕著に低下してしまう。 And, at the beginning of the study, I recognized that this combination had the following problems. That is, if P is segregated in grain boundaries during cold rolling with a high P material, the magnetic flux density after cold rolling annealing improves, but to segregate P into grain boundaries before cold rolling, after hot rolling Or it is necessary to make the cooling rate after hot-rolling annealing slow. However, if the cooling rate after the hot rolling annealing is low, solid solution C in the steel can not be obtained, and the improvement of the magnetic flux density due to the aging treatment between the cold rolling passes can not be achieved. In addition, high P material which segregates P in grain boundaries has a concern that cold ductility is originally reduced, but cold ductility is further lowered because cold rolling interpass aging hardens the steel sheet, and after hot rolling annealing When the cooling rate is low, cementite is formed at grain boundaries, and the cold ductility is significantly reduced.
一方、熱延板で固溶Cを残存させるためには熱延板焼鈍後の冷却速度を高速にする必要がある。しかしながら、熱延焼鈍後の冷却速度が高速であるとPの粒界偏析による磁束密度の向上が達成できなくなってしまう。このように、熱延板に対しての冷却速度の制御指針が逆であることに加え、CおよびPのそれぞれの作用により冷延性が低下して板破断が危惧されるため、固溶Cによる冷延パス間時効とP偏析を同時に活用するには特に熱延板における冷却およびそこでの元素偏析に関する新たな技術開発が必要であった。 On the other hand, in order to cause solid solution C to remain in the hot-rolled sheet, it is necessary to increase the cooling speed after hot-rolled sheet annealing. However, if the cooling rate after hot-rolling annealing is high, improvement in the magnetic flux density due to grain boundary segregation of P can not be achieved. Thus, in addition to the control direction of the cooling rate to the hot-rolled sheet being reversed, the cold ductility is lowered by the respective actions of C and P, and the plate breakage is feared, so the cold by the solid solution C In order to simultaneously utilize rolling interpass aging and P segregation, it was necessary to develop new technology especially for cooling in hot rolled sheet and element segregation there.
本発明は、かかる点に鑑みてなされたものであり、Pの粒界偏析による磁束密度の向上と固溶Cによる磁束密度の向上を両立させることによって磁気特性が優れた無方向性電磁鋼板を得ることを目的としている。 The present invention has been made in view of the above point, and it is a non-oriented electrical steel sheet having excellent magnetic properties by achieving both improvement of magnetic flux density by grain boundary segregation of P and improvement of magnetic flux density by solid solution C. The purpose is to get.
上述したように、Pの粒界偏析と固溶C(冷延パス間時効)は、どちらも集合組織改善に効果的であるが、熱延での冷却をそれぞれ緩冷、急冷とする必要があり、両立は困難である。またどちらも冷延性が低下し同時活用を阻害する。本発明では、Pが粒界偏析する温度とCが粒界偏析する温度(固溶Cが減少する温度)が異なることに着目し、各温度域を別々に制御する。結果として、集合組織改善と冷延性低下回避を両立する適度な粒界Pが確保され、さらに粒界PがCの粒界偏析を抑制(サイトコンペティション)し、結果として固溶Cも効率的に確保できるようになる。本発明の要旨は、以下の通りである。 As described above, grain boundary segregation of P and solid solution C (aging between cold rolling paths) are both effective in improving the texture, but it is necessary to slow the cooling by hot rolling to be slow cooling and to rapidly cool, respectively. Yes, both are difficult. In addition, cold ductility is reduced in both cases, which inhibits simultaneous utilization. In the present invention, noting that the temperature at which P segregates at grain boundaries and the temperature at which C segregates at grain boundaries (temperature at which solid solution C decreases) is different, each temperature range is controlled separately. As a result, a proper grain boundary P which secures both the improvement of the texture and the cold ductility reduction avoidance is secured, and further, the grain boundary P suppresses the grain boundary segregation of C (site competition), and as a result, the solid solution C also efficiently It will be secured. The gist of the present invention is as follows.
[1]
質量%で
2.0%≦Si≦4.0%、
0.01%≦Al≦3.0%、
0.05%≦Mn≦2.5%、
0.03%≦P≦0.12%、
0.001%≦C≦0.005%、
S≦0.005%、
N≦0.005%
を含有し、残部がFeおよび不純物元素からなり、
固溶C濃度が0.001mass%以上、0.005mass%以下であり、結晶粒界におけるP/Fe原子比が0.01以上、0.05以下である、無方向性電磁鋼板用熱延板。
[1]
In mass%
2.0% ≦ Si ≦ 4.0%,
0.01% ≦ Al ≦ 3.0%,
0.05% ≦ Mn ≦ 2.5%,
0.03% ≦ P ≦ 0.12%,
0.001% ≦ C ≦ 0.005%,
S ≦ 0.005%,
N ≦ 0.005%
And the balance consists of Fe and impurity elements,
A hot rolled sheet for a non-oriented electrical steel sheet, wherein the solid solution C concentration is 0.001 mass% or more and 0.005 mass% or less, and the P / Fe atomic ratio at the grain boundaries is 0.01 or more and 0.05 or less.
[2]
鋼板の表面ヴィッカース硬度Hとシャルピー遷移温度T(℃)が下記式(1)を満足する、[1]に記載の無方向性電磁鋼板用熱延板。
T(℃)≦4.5×(225-H) ・・・ 式(1)
[2]
The hot rolled sheet for non-oriented electrical steel sheet according to [1], wherein the surface Vickers hardness H of the steel sheet and the Charpy transition temperature T (° C.) satisfy the following formula (1).
T (° C.) ≦ 4.5 × (225−H) ··· Formula (1)
[3]
質量%で
2.0%≦Si≦4.0%、
0.01%≦Al≦3.0%、
0.05%≦Mn≦2.5%、
0.03%≦P≦0.12%、
0.001%≦C≦0.005%、
S≦0.005%、
N≦0.005%
を含有し、残部がFeおよび不純物元素からなり、
{200}面のX線積分強度I200と{222}面のX線積分強度I222との比I200/I222が1.00以上であり、
結晶方位分布関数における{φ1,Φ,φ2}={25°,0°,45°}の強度が6.00以上であり、かつ、{φ1,Φ,φ2}={30°,55°,45°}の強度が5.00未満を満足し、
{φ1,Φ,φ2}={25°,0°,45°}の強度≧{φ1,Φ,φ2}={20°,20°,45°}の強度
を満足し、
結晶粒径が30μm以上、板厚が0.10mm以上0.50mm以下である、無方向性電磁鋼板。
[3]
In mass%
2.0% ≦ Si ≦ 4.0%,
0.01% ≦ Al ≦ 3.0%,
0.05% ≦ Mn ≦ 2.5%,
0.03% ≦ P ≦ 0.12%,
0.001% ≦ C ≦ 0.005%,
S ≦ 0.005%,
N ≦ 0.005%
And the balance consists of Fe and impurity elements,
{200} plane ratio I 200 / I 222 of the X-ray integrated intensity I 222 of the X-ray integrated intensity I 200 {222} plane of is not less 1.00 or more,
The strength of {φ 1 , ,, φ 2 } = {25 °, 0 °, 45 °} in the crystal orientation distribution function is 6.00 or more, and {φ 1 , ,, φ 2 } = {30 °, 55 Satisfy the strength of less than 5.00 °, 45 °},
Satisfy the strength of {φ 1 , 2 , φ 2 } = {25 °, 0 °, 45 °} ≧ {φ 1 , ,, φ 2 } = {20 °, 20 °, 45 °},
A non-oriented electrical steel sheet having a crystal grain size of 30 μm or more and a plate thickness of 0.10 mm or more and 0.50 mm or less.
[4]
[1]または[2]に記載の無方向性電磁鋼板用熱延板を製造する方法であって、
質量%で
2.0%≦Si≦4.0%、
0.01%≦Al≦3.0%、
0.05%≦Mn≦2.5%、
0.03%≦P≦0.12%、
0.001%≦C≦0.005%、
S≦0.005%、
N≦0.005%
を含有し、残部がFeおよび不純物元素からなる鋼片を熱間圧延して焼鈍した後、500℃以上の温度域を、10℃/s以上、100℃/s以下の冷却速度で冷却し、500℃未満の温度域を、500℃以上の温度域における冷却速度よりも大きい冷却速度で冷却する、無方向性電磁鋼板用熱延板の製造方法。
[4]
It is a method of manufacturing the hot-rolled sheet for non-oriented electrical steel sheets according to [1] or [2],
In mass%
2.0% ≦ Si ≦ 4.0%,
0.01% ≦ Al ≦ 3.0%,
0.05% ≦ Mn ≦ 2.5%,
0.03% ≦ P ≦ 0.12%,
0.001% ≦ C ≦ 0.005%,
S ≦ 0.005%,
N ≦ 0.005%
After hot-rolling and annealing a steel piece containing the balance of Fe and an impurity element, and then cooling the temperature range of 500 ° C. or more at a cooling rate of 10 ° C./s or more and 100 ° C./s or less, The manufacturing method of the hot-rolled sheet for non-oriented electrical steel sheets which cools a temperature range less than 500 ° C with a cooling rate larger than a cooling rate in a temperature range 500 ° C or more.
[5]
[1]または[2]に記載の無方向性電磁鋼板用熱延板を製造する方法であって、
質量%で
2.0%≦Si≦4.0%、
0.01%≦Al≦3.0%、
0.05%≦Mn≦2.5%、
0.03%≦P≦0.12%、
0.001%≦C≦0.005%、
S≦0.005%、
N≦0.005%
を含有し、残部がFeおよび不純物元素からなる鋼片を熱間圧延して700℃以上で巻き取りを行い、500℃以上の温度域を、10℃/s以上、100℃/s以下の冷却速度で冷却し、500℃未満の温度域を、500℃以上の温度域における冷却速度よりも大きい冷却速度で冷却する、無方向性電磁鋼板用熱延板の製造方法。
[5]
It is a method of manufacturing the hot-rolled sheet for non-oriented electrical steel sheets according to [1] or [2],
In mass%
2.0% ≦ Si ≦ 4.0%,
0.01% ≦ Al ≦ 3.0%,
0.05% ≦ Mn ≦ 2.5%,
0.03% ≦ P ≦ 0.12%,
0.001% ≦ C ≦ 0.005%,
S ≦ 0.005%,
N ≦ 0.005%
Is hot rolled and the coil is wound at 700 ° C. or higher, and the temperature range of 500 ° C. or higher is cooled by 10 ° C./s or more and 100 ° C./s or less A method for producing a hot rolled sheet for non-oriented electrical steel sheet, comprising: cooling at a speed and cooling a temperature range of less than 500 ° C. at a cooling rate greater than a cooling rate in a temperature range of 500 ° C. or more.
[6]
[1]または[2]に記載の無方向性電磁鋼板用熱延板を冷間圧延し、仕上焼鈍して、[3]に記載の無方向性電磁鋼板を製造する方法であって、
前記冷間圧延をトータル圧下率が75%以上、95%以下の多パス圧延とし、各パス間にて100℃〜400℃で1〜60minの時効処理を施す、無方向性電磁鋼板の製造方法。
[6]
A method of cold rolling the hot rolled sheet for non-oriented electrical steel sheet according to [1] or [2] and finish annealing to produce the non-oriented electrical steel sheet according to [3] ,
A method of manufacturing a non-oriented electrical steel sheet, wherein the cold rolling is multipass rolling with a total rolling reduction of 75% to 95%, and an aging treatment is performed at 100 ° C to 400 ° C for 1 to 60 minutes between each pass. .
[7]
前記冷間圧延後に脱炭焼鈍を実施し、その後、前記仕上焼鈍を行う、[6]に記載の無方向性電磁鋼板の製造方法。
[7]
Performing decarburization annealing after the cold rolling, after the, performing the final annealing method for producing a non-oriented electrical steel sheet according to [6].
本発明によれば、Pの粒界偏析による磁束密度の向上と固溶Cによる磁束密度の向上を両立させることによって磁気特性が優れた無方向性電磁鋼板を得ることが可能となる。 According to the present invention, it is possible to obtain a non-oriented electrical steel sheet having excellent magnetic properties by making the improvement of the magnetic flux density by grain boundary segregation of P and the improvement of the magnetic flux density by solid solution C compatible.
以下、本発明について詳細に説明する。本発明の無方向性電磁鋼板用熱延板および無方向性電磁板は、以下の成分組成を有する。なお、鋼の成分組成について、「%」は「質量%」である。 Hereinafter, the present invention will be described in detail. The hot-rolled sheet for non-oriented electrical steel sheets and the non-oriented electromagnetic sheet of the present invention have the following component composition. In addition, "%" is "mass%" about the component composition of steel.
2.0%≦Si≦4.0%
Siは、鋼の固有抵抗を増加させ、また、鉄損を低減する作用を呈する。この作用を得るためには、2.0%以上が必要である。一方、Siが4.0%を超えると、鋼が脆化し、圧延性が低下する。従って、Siは、2.0〜4.0%とする。好ましくは、2.0〜3.5%である。
2.0% ≦ Si ≦ 4.0%
Si increases the specific resistance of steel and also has the effect of reducing core loss. In order to obtain this effect, 2.0% or more is required. On the other hand, if Si exceeds 4.0%, the steel becomes brittle and the rollability is reduced. Therefore, Si is set to 2.0 to 4.0%. Preferably, it is 2.0 to 3.5%.
0.01%≦Al≦3.0%
Alは、脱酸材として有効であり、更に、窒化物を粗大にして無害化することもできる。また、Siと同様に、鋼の固有抵抗を増加させ、鉄損を低減させる。これらの作用を得るためには、0.01%以上が必要である。しかし、3.0%を超えると、鋼が脆化し、圧延性が低下する。従って、Alは、0.01〜3.0%とする。好ましくは、0.2〜2.0%である。
0.01% ≦ Al ≦ 3.0%
Al is effective as a deoxidizing material, and further, the nitride can be coarsened to be harmless. Also, like Si, it increases the specific resistance of steel and reduces iron loss. In order to obtain these effects, 0.01% or more is required. However, if it exceeds 3.0%, the steel becomes brittle and the rollability decreases. Therefore, Al is made 0.01 to 3.0%. Preferably, it is 0.2 to 2.0%.
0.05%≦Mn≦2.5%
Mnは、鋼の固有抵抗を高め、また、硫化物を粗大化して無害化する作用を呈する。この作用を得るためには、0.05%以上が必要である。一方、Mnが2.5%を超えると、磁束密度の低下及びコストの上昇を招くとともに、冷延時に割れ易くなる。従って、Mnは、0.05〜2.5%とする。好ましくは、0.1〜0.5%である。
0.05% ≦ Mn ≦ 2.5%
Mn increases the specific resistance of steel and also has the effect of coarsening sulfides to render them harmless. In order to obtain this effect, 0.05% or more is required. On the other hand, if Mn exceeds 2.5%, the magnetic flux density is lowered and the cost is increased, and also it is easily broken at the time of cold rolling. Therefore, Mn is made 0.05 to 2.5%. Preferably, it is 0.1 to 0.5%.
0.03%≦P≦0.12%
Pは磁束密度を向上させる効果を有している。高磁束密度化効果を得る観点から、P含有量は0.03%以上とする。一方、P含有量が0.12%超では、冷間圧延時に破断を生じる可能性がある。したがって、P含有量は、0.03〜0.12%とする。
0.03% ≦ P ≦ 0.12%
P has the effect of improving the magnetic flux density. In order to obtain a high magnetic flux density effect, the P content is made 0.03% or more. On the other hand, if the P content exceeds 0.12%, breakage may occur during cold rolling. Therefore, the P content is set to 0.03 to 0.12%.
0.001%≦C≦0.005%、
Cは、鋼中に固溶Cとして存在して冷間圧延時のパス間の時効による集合組織改善効果を発現することにより、磁束密度を向上させる。その効果を得るために、Cは0.001%以上とする。一方、含有量が0.005%を超えると微細な炭化物が析出して磁気特性が劣化するので、C含有量は0.005%以下とする。好ましくは、0.002〜0.005質量%である。
0.001% ≦ C ≦ 0.005%,
C improves the magnetic flux density by being present as solid solution C in the steel and developing a texture improvement effect by aging between passes during cold rolling. In order to obtain the effect, C is made 0.001% or more. On the other hand, if the content exceeds 0.005%, fine carbides precipitate and the magnetic properties deteriorate, so the C content is made 0.005% or less. Preferably, it is 0.002 to 0.005% by mass.
残部はFeおよび不純物である。不純物のうち、S、Nは、析出物を形成して、焼鈍中の粒成長を妨げ、磁性を劣化させるので、いずれの元素も、0.005%以下とする。 The balance is Fe and impurities. Among the impurities, S and N form precipitates, prevent grain growth during annealing, and deteriorate magnetism. Therefore, the content of any of the elements is made 0.005% or less.
本発明の無方向性電磁鋼板用熱延板は、以上の成分組成を有し、固溶C濃度が0.001mass%以上、0.005mass%以下であり、結晶粒界におけるP/Fe原子比が0.01以上、0.05以下である。 The hot-rolled sheet for non-oriented electrical steel sheets of the present invention has the above component composition, the solid solution C concentration is 0.001 mass% or more and 0.005 mass% or less, and the P / Fe atomic ratio in grain boundaries is 0.01. The above is 0.05 or less.
固溶C濃度が0.001mass%以上、0.005mass%以下
固溶C濃度が0.001mass%未満では、固溶Cによる磁束密度の向上が不十分である。一方、0.005mass%を超えると粒界にセメンタイトが形成し、冷延性が低下する。また、相変態する恐れもあり、熱延板焼鈍工程で相変態すると、冷延工程にて相変態しない場合に比べて{111}<uvw>方位が極めて強く発達し、仕上焼鈍板の{111}<uvw>方位が増加する。この方位は磁気特性を劣化させる方位であるので、発達させないことが望ましい。固溶C量は、種々の時効前後の試料を内部摩擦法にてスネークピーク値Qmax-1を測定し、下記式(2)、(3)の関係から求めればよい。
固溶C量(mass%)=K×Qmax-1 ・・・ 式(2)
K=1.55×{Mn量(mass%)}1/2+1.35 ・・・ 式(3)
When the solid solution C concentration is 0.001 mass% or more and 0.005 mass% or less and the solid solution C concentration is less than 0.001 mass%, the improvement of the magnetic flux density by the solid solution C is insufficient. On the other hand, if it exceeds 0.005 mass%, cementite will form at grain boundaries and cold ductility will decrease. In addition, there is a possibility of phase transformation, and when phase transformation is performed in the hot-rolled sheet annealing process, the {111} <uvw> orientation develops significantly more than in the case where phase transformation is not performed in the cold rolling process. } <uvw> orientation increases. It is desirable not to develop this orientation because it degrades the magnetic properties. The amount of solid solution C may be determined from the relationship between the following formulas (2) and (3) by measuring the snake peak value Qmax- 1 of various samples before and after aging by the internal friction method.
Solid solution C amount (mass%) = K × Qmax -1 · · · Formula (2)
K = 1.55 × {Mn amount (mass%)} 1/2 + 1.35 ・ ・ ・ Formula (3)
結晶粒界におけるP/Fe原子比が0.01以上、0.05以下
結晶粒界におけるP/Fe原子比が0.01未満では、Pの粒界偏析を活用した磁束密度の向上が不十分である。一方、0.05を超えると冷間圧延時に破断を生じる可能性がある。P/Fe原子比は2.0mmt×20mmL×3mmWの試料をオージェ電子分光装置内に入れて液体窒素にて試料を冷却し、試料を破断させた。試料の粒界破壊した破面を探し出し、その粒界面におけるFe、 P量を分析し、P/Fe原子比を求めればよい。
When the P / Fe atomic ratio at grain boundaries is 0.01 or more and 0.05 or less The P / Fe atomic ratio at grain boundaries is less than 0.01, the improvement in magnetic flux density utilizing grain boundary segregation of P is insufficient. On the other hand, if it exceeds 0.05, breakage may occur during cold rolling. A sample with a P / Fe atomic ratio of 2.0 mmt × 20 mm L × 3 mmW was placed in an Auger electron spectrometer, the sample was cooled with liquid nitrogen, and the sample was broken. The fractured surface of the sample with intergranular fracture should be found, the amount of Fe and P at the grain interface should be analyzed, and the P / Fe atomic ratio should be determined.
また、本発明の無方向性電磁鋼板用熱延板は、鋼板の表面ヴィッカース硬度Hとシャルピー遷移温度T(℃)が下記式(1)を満足することが望ましい。
T(℃)≦4.5×(225-H) ・・・ 式(1)
本発明は前述のように固有抵抗を高めるためSi、Alを比較的高濃度で含有した鋼種において、磁束密度を向上させるためにPと固溶Cを活用することを特徴とし、圧延性を合わせて課題解決するものである。これら元素の含有量は、これら元素の固溶強化およびセメンタイトによる鋼板の硬化を考えて適切に設計する必要がある。本発明ではこの硬化を鋼板の表面ヴィッカース硬度Hで代表させ、圧延性と関連するシャルピー遷移温度T(℃)との関連で発明を好ましく限定することが可能であり、上記式(1)を満足する場合に、良好な磁気特性と圧延性のバランスが得られる。
Moreover, as for the hot-rolled sheet for non-oriented electrical steel sheets of this invention, it is desirable for the surface Vickers hardness H of a steel sheet and Charpy transition temperature T (degreeC) to satisfy following formula (1).
T (° C.) ≦ 4.5 × (225−H) ··· Formula (1)
The present invention is characterized by utilizing P and solid solution C in order to improve the magnetic flux density in a steel grade containing relatively high concentrations of Si and Al in order to increase the specific resistance as described above, and combining the rollability Solve the problem. The content of these elements needs to be appropriately designed in consideration of the solid solution strengthening of these elements and the hardening of the steel sheet by cementite. In the present invention, this hardening can be represented by the surface Vickers hardness H of the steel sheet, and the invention can be preferably limited in relation to the Charpy transition temperature T (° C.) related to the rollability, and the above formula (1) is satisfied. In this case, a good balance of magnetic properties and rollability can be obtained.
また、本発明の無方向性電磁板は、以上の成分組成を有し、{200}面のX線積分強度が2.0以上、{222}面のX線積分強度が10.0以下であり、結晶粒径が30μm以上、板厚が0.10mm以上0.50mm以下である。 Further, the non-oriented electromagnetic plate of the present invention has the above component composition, the X-ray integral intensity of the {200} plane is 2.0 or more, the X-ray integral intensity of the {222} plane is 10.0 or less, The diameter is 30 μm or more, and the plate thickness is 0.10 mm or more and 0.50 mm or less.
{200}面のX線積分強度が2.0以上、{222}面のX線積分強度が10.0以下
{200}面のX線積分強度が多いほど、磁気特性に好ましい集合組織になるので、{200}面のX線積分強度は2.0以上とする。一方、{222}面のX線積分強度が多いほど、磁気特性に好ましくない集合組織になるので、{222}面のX線積分強度は10.0以下とする。試料作製方法は、鋼板を切り出し、試料表面を化学研磨により測定する板厚まで減厚すればよい。また、定量化方法は作製した試料をエックス線回折装置にて{200}面、{110}面、{211}面の極点図を測定し、ODFを作成してから、{200}面、{222}面の積分強度を求める。板厚方向の集合組織のばらつきが大きい場合には、例えば板厚表面から1/10の位置、1/4の位置の部分の集合組織を測定し、結果を平均すればよい。
X-ray integral intensity of {200} plane is 2.0 or more, X-ray integral intensity of {222} plane is 10.0 or less
The more the X-ray integral intensity of the {200} plane is, the more favorable the texture is to the magnetic characteristics. Therefore, the X-ray integral intensity of the {200} plane is 2.0 or more. On the other hand, as the X-ray integral intensity of the {222} plane increases, the texture becomes less desirable for the magnetic characteristics, so the X-ray integral intensity of the {222} plane is 10.0 or less. In the sample preparation method, a steel plate may be cut out and the thickness of the sample surface may be reduced to a plate thickness to be measured by chemical polishing. Moreover, the quantification method measures the pole figure of the {200}, {110}, {211} plane with the X-ray diffractometer for the prepared sample, and after creating the ODF, the {200} plane, {222 Find the integral intensity of the surface. If the variation in texture in the thickness direction is large, for example, textures of portions at positions 1/10 and 1/4 from the thickness surface may be measured, and the results may be averaged.
結晶粒径が30μm以上
結晶粒径が30μm未満では、良好な磁気特性が得られない。従って、結晶粒径は30μm以上とする。方法は、長手方向と板厚保方向の断面における金属組織を50倍程度で撮影し、線分法で測定すればよい。
If the crystal grain size is 30 μm or more and the crystal grain size is less than 30 μm, good magnetic properties can not be obtained. Therefore, the crystal grain size is 30 μm or more. As a method, the metal structure in the cross section in the longitudinal direction and the thickness direction may be photographed at about 50 times and measured by the line segment method.
板厚が0.10mm以上0.50mm以下
板厚薄手化により鉄損が減少する。そのため、低鉄損と高磁束密度を両立する観点から、板厚は0.10〜0.50mmとする。
The board thickness is 0.10 mm or more and 0.50 mm or less Iron loss is reduced by thinning the board thickness. Therefore, from the viewpoint of achieving both low iron loss and high magnetic flux density, the plate thickness is 0.10 to 0.50 mm.
次に、製造方法について説明する。 Next, the manufacturing method will be described.
本発明では、先に述べた成分組成の鋼を、連続鋳造法あるいは鋼塊を分塊圧延する方法など一般的な方法により鋼片(スラブ)とし、熱間圧延を施す。熱間圧延の際のスラブ加熱温度は特に限定されるものではないが、コストおよび熱間圧延性の観点から1000〜1300℃とすることが好ましい。より好ましくは1050〜1250℃である。また、熱間圧延の各種条件は、熱延板焼鈍を実施する場合は特に限定されるものではなく、例えば仕上げ温度が700〜950℃、巻き取り温度が750℃以下など、一般的な条件に従って行えばよい。 In the present invention, the steel having the component composition described above is used as a steel slab (slab) by a general method such as a continuous casting method or a method of segmenting a steel ingot and hot rolling is performed. Although the slab heating temperature in the case of hot rolling is not specifically limited, It is preferable to set it as 1000-1300 degreeC from a viewpoint of cost and hot-rolling property. More preferably, it is 1050 to 1250 ° C. In addition, various conditions of hot rolling are not particularly limited when performing hot-rolled sheet annealing, and for example, according to general conditions such as a finishing temperature of 700 to 950 ° C. and a winding temperature of 750 ° C. or less You can do it.
熱間圧延後は、熱延板焼鈍を施す場合と、熱延板焼鈍を施さない場合のいずれでも良い。熱延板焼鈍を施す場合は、熱延板焼鈍は、例えば950℃以上1050℃以下で10秒間以上3分間以下保持する連続焼鈍にて実施する。熱延板焼鈍温度が上記範囲を超えると設備への負荷が大きくなり、熱延板焼鈍時間が上記範囲を超えると生産性の劣化を招く。熱延板焼鈍温度および熱延板焼鈍時間が上記範囲を下回ると磁気特性向上の効果が小さくなる。 After hot rolling, either hot-rolled sheet annealing may be performed or hot-rolled sheet annealing may not be performed. When hot-rolled sheet annealing is performed, the hot-rolled sheet annealing is performed, for example, by continuous annealing held at 950 ° C. or more and 1050 ° C. or less for 10 seconds or more and 3 minutes or less. When the hot-rolled sheet annealing temperature exceeds the above range, the load on the equipment becomes large, and when the hot-rolled sheet annealing time exceeds the above range, the productivity is deteriorated. When the hot-rolled sheet annealing temperature and the hot-rolled sheet annealing time are below the above range, the effect of improving the magnetic characteristics is reduced.
そして熱延板焼鈍後、500℃以上の温度域を、10℃/s以上、100℃/s以下の冷却速度で冷却し、500℃未満の温度域を、500℃以上の温度域における冷却速度よりも大きい冷却速度で冷却して、無方向性電磁鋼板用熱延板を製造する。 Then, after hot-rolled sheet annealing, the temperature range of 500 ° C. or more is cooled at a cooling rate of 10 ° C./s to 100 ° C./s, and the temperature range of less than 500 ° C. is a cooling rate at a temperature range of 500 ° C. or more Cooling is performed at a higher cooling rate to produce a hot-rolled sheet for non-oriented electrical steel sheet.
また一方、熱延板焼鈍を施さない場合は、熱間圧延して700℃以上で巻き取った後、500℃以上の温度域を、10℃/s以上、100℃/s以下の冷却速度で冷却し、500℃未満の温度域を、500℃以上の温度域における冷却速度よりも大きい冷却速度で冷却して、無方向性電磁鋼板用熱延板を製造する。巻き取り温度は750℃以上とすることが望ましい。 On the other hand, when hot-rolled sheet annealing is not performed, after hot rolling and winding at 700 ° C. or more, a temperature range of 500 ° C. or more is performed at a cooling rate of 10 ° C./s or more and 100 ° C./s or less It cools and cools the temperature range less than 500 degreeC with the cooling rate larger than the cooling rate in the temperature range 500 degreeC or more, and manufactures a hot-rolled sheet for non-oriented electrical steel sheets. The winding temperature is desirably 750 ° C. or higher.
本発明では、Pが粒界偏析する温度とCが粒界偏析する温度(固溶Cが減少する温度)が異なることに着目し、それぞれの元素にとって効果的な温度域の冷却速度を別々に制御する。これにより、適度なPの粒界偏析を確保し、P偏析による集合組織改善効果を得ると同時に冷延性低下を回避する。同時にPが粒界を占有するため、Cが粒界に偏析しにくくなり(サイトコンペティション)、結果として固溶Cの確保も達成できる。 In the present invention, noting that the temperature at which P segregates at grain boundaries and the temperature at which C segregates at grain boundaries (temperature at which solid solution C decreases) differs, the cooling rate in the temperature range effective for each element is separately determined. Control. Thereby, appropriate grain boundary segregation of P is secured, and at the same time as obtaining the texture improvement effect by P segregation, the decrease in cold ductility is avoided. At the same time, since P occupies grain boundaries, C is less likely to segregate at the grain boundaries (site competition), and as a result, securing of solid solution C can also be achieved.
Pの粒界偏析を冷延破断しない程度にし、かつP偏析により磁束密度が向上するため、熱間圧延して焼鈍した後の冷却過程において、500℃以上における冷却速度を10℃/s以上、100℃/s以下とする。好ましくは80℃/s以下、より好ましくは50℃/s以下とする。10℃/s以上としたのは、冷延中においてP偏析による破断を抑制するためである。100℃/s以下としたのは、P偏析により磁束密度を向上効果をえるためである。 Since the grain boundary segregation of P is made not to cold-roll fracture and the magnetic flux density is improved by P segregation, in the cooling process after hot rolling and annealing, the cooling rate at 500 ° C. or more is 10 ° C./s or more, The temperature is set to 100 ° C./s or less. It is preferably 80 ° C./s or less, more preferably 50 ° C./s or less. The reason for setting the temperature to 10 ° C./s or more is to suppress breakage due to P segregation during cold rolling. The reason for setting the temperature to 100 ° C./s or less is to obtain an effect of improving the magnetic flux density by P segregation.
さらに固溶Cによるパス間時効効果を十分発揮させるため、熱間圧延して焼鈍した後の冷却過程において、500℃未満における冷却速度を、500℃以上の温度域における冷却速度よりも大きくしてCを粒内に十分固溶させる。粒内に多く固溶させたCを転位に固着させて磁束密度向上を狙う。これらの観点から、500℃以下における冷却速度は20℃/s以上、好ましくは50℃/s以上、より好ましくは100℃/s以上とする。 Furthermore, in order to exert the interpass aging effect by solid solution C sufficiently, in the cooling process after hot rolling and annealing, the cooling rate at less than 500 ° C. is made larger than the cooling rate in the temperature range of 500 ° C. or more. C is sufficiently dissolved in the grains. A large amount of C solid-solved in the grains is fixed to the dislocation to aim at the improvement of the magnetic flux density. From these viewpoints, the cooling rate at 500 ° C. or less is 20 ° C./s or more, preferably 50 ° C./s or more, more preferably 100 ° C./s or more.
更に本発明では、以上のようにして製造した無方向性電磁鋼板用熱延板について、時効処理を挟む2パス以上の冷間圧延を施し、次いで、仕上げ焼鈍して無方向性電磁鋼板を製造する。また、こうして無方向性電磁鋼板に、必要に応じて、絶縁被膜処理を施しても良い。ここで、冷間圧延は、トータル圧下率が75%以上、95%以下の多パス圧延とし、各パス間にて100℃〜400℃で1〜60minの時効処理を施す。 Furthermore, in the present invention, the hot rolled sheet for non-oriented electrical steel sheet manufactured as described above is subjected to cold rolling for two or more passes across the aging treatment, and then finish annealing is performed to produce a non-oriented electrical steel sheet. Do. Also, in this way, the non-oriented electrical steel sheet may be subjected to an insulating film treatment, if necessary. Here, cold rolling is multi-pass rolling with a total rolling reduction of 75% or more and 95% or less, and an aging treatment at 100 ° C. to 400 ° C. for 1 to 60 minutes is performed between the respective passes.
トータル圧下率が75%以上、95%以下の多パス圧延
時効処理を挟む2パス以上の冷間圧延を行うことにより、冷間圧延が1回の場合より高い磁束密度を得ることができる。トータル圧下率は製造上の制約から定められる。例えば熱延板厚を2.0mmとすると、無方向性電磁鋼板の板厚保である0.10mm以上0.50mm以下を得るためには圧下率が75%以上、95%以下になる。
Multipass rolling with a total rolling reduction of 75% or more and 95% or less By performing two or more passes of cold rolling sandwiching the aging treatment, a magnetic flux density higher than in the case of one cold rolling can be obtained. The total rolling reduction is determined from manufacturing constraints. For example, when the hot-rolled sheet thickness is 2.0 mm, the rolling reduction is 75% or more and 95% or less in order to obtain 0.10 mm or more and 0.50 mm or less which is the thickness retention of the non-oriented electrical steel sheet.
各パス間にて100℃〜400℃で1〜60minの時効処理
冷間圧延のパス間に100〜400℃で1〜60minの時効処理を施すことによって、圧延方向に高い磁束密度を有する無方向性電磁鋼板を製造することができる。時効処理条件は、好ましくは100〜300℃で1〜60min、より好ましくは100〜250℃で1〜60min、さらに好ましくは150〜250℃で1〜60minである。Cが拡散でき、転位が拡散し難いことを両方満足させる観点から温度は100℃〜400℃とした。時間は、Cが転位を固着する頻度を稼ぐために1〜60minとした。なお、時間の上限(60min)は生産性の観点からの上限である。
Aging treatment for 1 to 60 minutes at 100 ° C to 400 ° C between each pass Non-direction having high magnetic flux density in the rolling direction by performing aging treatment for 1 to 60 minutes at 100 to 400 ° C between cold rolling passes Magnetic steel sheet can be manufactured. The aging treatment conditions are preferably 100 to 300 ° C. for 1 to 60 minutes, more preferably 100 to 250 ° C. for 1 to 60 minutes, and still more preferably 150 to 250 ° C. for 1 to 60 minutes. The temperature was set to 100 ° C. to 400 ° C. from the viewpoint of satisfying both that C can diffuse and dislocations are difficult to diffuse. The time was set to 1 to 60 minutes to gain the frequency at which C fixed dislocations. The upper limit of time (60 min) is the upper limit from the viewpoint of productivity.
また、冷間圧延後に脱炭焼鈍して固溶Cを無くし、さらに仕上焼鈍しても良い。これは、鋼板中に一定量以上の炭素があると、現実の電気機器運転中においては、鉄心の温度が150℃〜200℃まで上昇する場合があることから、時効効果により鉄心の磁気特性が劣化する問題を確実に防ぐ目的で行う。条件は通常行われている操業条件で構わない。 In addition, after cold rolling, decarburization annealing may be performed to eliminate solid solution C, and further, finish annealing may be performed. This is because the iron core temperature may rise to 150 ° C. to 200 ° C. during actual operation of the electric device if there is a certain amount or more of carbon in the steel plate, so the magnetic characteristics of the iron core are due to the aging effect The purpose is to prevent the problem of deterioration. The conditions may be normal operating conditions.
以下、実施例を例示して、本発明を具体的に説明する。 Hereinafter, the present invention will be specifically described by way of examples.
[実験1]
質量%で、Si:2.95%、Mn:0.2%、Al:0.5%の実機熱延板(板厚1.8mm)に1000℃で1min均熱する熱延板焼鈍を施し圧延した。その後1000℃で30s均熱する仕上焼鈍を施し、750℃で2h均熱するひずみ取り焼鈍を施した。55mm角磁気測定試験を採取し、LおよびC方向の5000A/mにおける磁束密度B50を測定した。
[Experiment 1]
An actual hot-rolled sheet (sheet thickness 1.8 mm) of Si: 2.95%, Mn: 0.2%, Al: 0.5% by mass% was subjected to hot-rolled sheet annealing which is maintained at 1000 ° C. for 1 min. Thereafter, finish annealing was performed soaking at 1000 ° C. for 30 seconds, and strain removing annealing performed soaking at 750 ° C. for 2 hours was performed. A 55 mm square magnetometry test was taken to measure the magnetic flux density B50 at 5000 A / m in the L and C directions.
ここで、圧延工程について説明する。冷延途中の種々の板厚(1.8、 1.6、 1.2、 0.8、 0.5mm)を得たときに200℃で5min保持するパス間時効を実施した後、水冷し室温で冷延した(図1)。 Here, the rolling process will be described. After interpass aging was carried out for 5 minutes at 200 ° C when various plate thicknesses (1.8, 1.6, 1.2, 0.8, 0.5 mm) were obtained during cold rolling, it was water cooled and cold rolled at room temperature (Fig. 1). .
時効実施により、LおよびC方向の磁束密度が向上する(図2)。このメカニズムは、仕上焼鈍後の集合組織における、{111}<112>方位({φ1,Φ,φ2}={30°,55°,45°})の低減と{100}<012>方位近傍({φ1,Φ,φ2}={20〜25°,0°,45°})の増加に起因する(図3)。 Aging improves the flux density in the L and C directions (FIG. 2). This mechanism, in the texture after finish annealing, {111} <112> orientation ({φ 1, Φ, φ 2} = {30 °, 55 °, 45 °}) reduction and {100} of the <012> Due to the increase in the azimuthal neighborhood ({φ 1 , ,, φ 2 } = {20-25 °, 0 °, 45 °}) (FIG. 3).
[実験2]
質量%で、Si:2.95%、Mn:0.2%、Al:0.5%の鋼をラボで真空溶解して、板厚2.0mmの熱延板を作製し、これに1000℃で1min均熱する熱延板焼鈍を施して圧延した。その後1000℃で30s均熱する仕上焼鈍を施し、750℃で2h均熱するひずみ取り焼鈍を施した。55mm角磁気測定試験を採取し、圧延方向から0、22.5、45、67.5、90°傾けた角度における磁束密度B50を測定した。
[Experiment 2]
A vacuum-melt steel of 2.95% Si, 2. 9% Mn, 0.2% Al and 0.5% Al by mass% was produced in a laboratory by vacuum to prepare a hot-rolled sheet with a thickness of 2.0 mm, which was subjected to 1 minute soaking at 1000 ° C. It was rolled and annealed. Thereafter, finish annealing was performed soaking at 1000 ° C. for 30 seconds, and strain removing annealing performed soaking at 750 ° C. for 2 hours was performed. A 55 mm square magnetic measurement test was taken to measure the magnetic flux density B50 at an angle of 0, 22.5, 45, 67.5, 90 ° inclined from the rolling direction.
ここで、圧延工程について説明する。冷延途中の種々の板厚(2.0、 1.6、 1.2、 0.8、 0.5mm)を得たときに200℃で5min保持するパス間時効を実施した後、水冷し室温で冷延した。仕上板厚0.8mmはそのまま冷間圧延を完了とし仕上板厚0.5mm以下のものは、板厚0.5mm到達後そのまま仕上板厚(0.5、0.35、0.30、0.25、0.20、0.15mm)まで冷間圧延した(図4)。 Here, the rolling process will be described. After pass-to-pass aging was performed for 5 minutes at 200 ° C. when various plate thicknesses (2.0, 1.6, 1.2, 0.8, 0.5 mm) were obtained during cold rolling, it was water cooled and cold rolled at room temperature. Finished cold rolling is finished as it is for finished plate thickness 0.8 mm, and for finished plate thickness 0.5 mm or less, it is cold to finished plate thickness (0.5, 0.35, 0.30, 0.25, 0.20, 0.15 mm) as it is after reaching plate thickness 0.5 mm. Rolled (Figure 4).
図5に磁束密度に及ぼすトータル冷延率*の影響を示す。冷延率75%以上では、圧延方向から45°傾いた方向以外は時効実施により磁束密度が向上する。なお、トータル冷延率=100×(1-仕上焼鈍板の板厚/熱延板の板厚)である。 FIG. 5 shows the influence of the total cold rolling ratio * on the magnetic flux density. When the cold rolling ratio is 75% or more, the magnetic flux density is improved by aging, except in the direction inclined 45 ° from the rolling direction. The total cold rolling ratio = 100 × (1−thickness of finished annealing sheet / thickness of hot rolled sheet).
[実験3]
表1に示す化学組成の鋼を真空溶解した。1100℃で加熱して熱間圧延し、板厚2.0mmに仕上、750℃で巻き取った。この熱延板を1000℃で30s均熱する熱延板焼鈍を施し、500℃以上における冷却速度を20℃/sで炉冷、500℃未満における冷却速度を100℃/sで水冷した。
[Experiment 3]
The steel of the chemical composition shown in Table 1 was vacuum melted. It hot-rolled by heating at 1100 degreeC, finished to plate | board thickness 2.0 mm, and wound up at 750 degreeC. The hot-rolled sheet was subjected to hot-rolled sheet annealing to equalize at 30 ° C. for 30 seconds at 1000 ° C., the cooling rate at 500 ° C. or higher was furnace cooling at 20 ° C./s and the cooling rate at less than 500 ° C. was water cooled at 100 ° C./s.
熱延焼鈍板から、固溶C量を調べるためのエイジングインデックス用試料と、粒界P偏析量を調べるためのオージェ電子分光用試料を切り出して作製しそれぞれ、固溶C量とP/Fe原子比を調べた。その結果を表2に示す。 From the hot-rolled annealed sheet, a sample for aging index to check the amount of solid solution C and a sample for Auger electron spectroscopy to check the amount of grain boundary P segregation are prepared and prepared, respectively, the amount of solid solution C and P / Fe atoms The ratio was examined. The results are shown in Table 2.
鋼No.1〜7は固溶C量が全固溶し、粒界P/Feも適正範囲あるが、鋼No.8はC含有量が多く、Cが全固溶していなかった。鋼No.9、10はそれぞれ粒界P量が適正範囲になかった。 In steel Nos. 1 to 7, the solid solution C content was totally solid solution, and the grain boundary P / Fe was also in an appropriate range, but steel No. 8 had a large C content and C was not totally solid solution. In steel Nos. 9 and 10, the grain boundary P amount was not within the appropriate range.
[実験4]
表1に示した鋼No.1と8を用いて、熱延後の巻き取り時の冷却速度の影響および熱延板焼鈍後の冷却速度が及ぼす固溶C量と粒界P/Feへの影響を調べた。また、SEMでセメンタイトを観察し、数密度を測定した。さらに、シャルピー衝撃試験により、延性−脆性遷移温度(以下、遷移温度)を求め、断面の1kgにおけるヴィッカース硬度、硬度パラメータ「4.5×(225-H)」を表3に示す。
[Experiment 4]
Using steel Nos. 1 and 8 shown in Table 1, the effect of the cooling rate at the time of winding after hot rolling and the cooling rate after hot-rolled sheet annealing have an effect on the amount of solid solution C and grain boundary P / Fe. Examined the impact. Moreover, cementite was observed by SEM and the number density was measured. Furthermore, the ductile-brittle transition temperature (hereinafter, transition temperature) is determined by the Charpy impact test, and the Vickers hardness at 1 kg of the cross section and the hardness parameter “4.5 × (225−H)” are shown in Table 3.
条件1-e、1-jは500℃以上における冷却速度が速すぎて粒界P/Feが低かった。条件8-a〜8-lは500℃未満における冷却速度を制御してもCが全固溶せず、セメンタイトが析出していた。また、シャルピー遷移温度が硬度パラメータの値を上回っていた。これらに対し、条件1-a、 1-b、 1-c、 1-d、 1-f、 1-g、 1-h、 1-iは固溶C、粒界P/Feは適正範囲にあった。 In conditions 1-e and 1-j, the cooling rate at 500 ° C. or higher was too fast, and the grain boundary P / Fe was low. Under the conditions 8-a to 8-l, even if the cooling rate at less than 500 ° C. was controlled, C did not form a solid solution, and cementite was precipitated. In addition, the Charpy transition temperature exceeded the value of the hardness parameter. On the other hand, conditions 1-a, 1-b, 1-c, 1-d, 1-f, 1-g, 1-i are solid solution C and grain boundary P / Fe is in the appropriate range. there were.
[実験5]
実験3にて作製した表2に記載の熱延板焼鈍板を用いて冷間圧延を多パス圧延で行い、板厚0.25mm(圧下率87.5%)に仕上げた。200℃で300s保持するパス間時効を板厚1.8、 1.6、 1.2、 0.8、 0.5mmのときに実施した。また、比較材としてパス間時効を省略した通常冷延材も用意した。これらの冷延板を1000℃で30s保持する仕上焼鈍を行い、圧延方向から0°、22.5°、45°、67.5°、90°傾けた方向の5000A/mにおける磁束密度B50(0)、B50(22.5)、B50(45)、B50(67.5)、B50(90)と、400Hzで1.0Tまで磁化した時の鉄損W10/400(0)、W10/400(22.5)、W10/400(45)、W10/400(67.5)、W10/400(90)を測定した。これらの結果から、下記式(4)と(5)を用いて、B50とW10/400の全周平均を求めた。
B50={B50(0)+2×B50(22.5)+2×B50(45)+2×B50(67.5)+B50(90)}/8 ・・・ (4)
W10/400={W10/400 (0)+2×W10/400 (22.5)+2×W10/400 (45)+2×W10/400 (67.5)+ W10/400 (90)}/8 ・・・ (5)
また、板厚中心層の{200}面、{110}面、{211}面のX線積分強度を測定し、結晶方位分布関数ODFを求め、{200}面の積分強度、{222}面の積分強度、{φ1,Φ,φ2}={25°,0°,45°}({100}<012>方位近傍に相当)の強度、{φ1,Φ,φ2}={30°,55°,45°}({111}<112>方位に相当)の強度、{φ1,Φ,φ2}={20°,20°,45°}({411}<148>方位近傍に相当)の強度を評価した。結果を表4に示す。
[Experiment 5]
It cold-rolled by multipass rolling using the hot-rolled sheet annealing board of Table 2 produced in Experiment 3 and finished to 0.25 mm of board thickness (rolling reduction 87.5%). Inter-pass aging was performed at a plate thickness of 1.8, 1.6, 1.2, 0.8, and 0.5 mm while holding at 200 ° C. for 300 s. Moreover, the normal cold-rolled material which abbreviate | omitted the interpass aging as a comparison material was also prepared. These cold rolled sheets are subjected to finish annealing for 30 seconds at 1000 ° C., and magnetic flux densities B50 (0) and B50 at 5000 A / m in directions inclined 0 °, 22.5 °, 45 °, 67.5 ° and 90 ° from the rolling direction. (22.5), B50 (45), B50 (67.5), B50 (90) and iron loss W10 / 400 (0), W10 / 400 (22.5), W 10/400 (45) when magnetized to 1.0 T at 400 Hz ), W10 / 400 (67.5) and W10 / 400 (90) were measured. From these results, using the following equations (4) and (5), the all-round average of B50 and W10 / 400 was determined.
B50 = {B50 (0) + 2 x B50 (22.5) + 2 x B50 (45) + 2 x B50 (67.5) + B50 (90)} / 8 (4)
W10 / 400 = {W10 / 400 (0) + 2 × W10 / 400 (22.5) + 2 × W10 / 400 (45) + 2 × W10 / 400 (67.5) + W10 / 400 (90)} / 8. · (Five)
In addition, measure the X-ray integral intensity of {200}, {110}, and {211} planes of the thickness center layer, determine the crystal orientation distribution function ODF, and measure the integral intensity of {200} planes, {222} plane. Integrated intensity of {φ 1 , ,, φ 2 } = {25 °, 0 °, 45 °} (corresponding to the vicinity of {100} <012> orientation), {φ 1 , ,, φ 2 } = { Intensity of 30 °, 55 °, 45 °} (corresponding to {111} <112> orientation), {φ 1 , ,, φ 2 } = {20 °, 20 °, 45 °} ({411} <148> (Equivalent to the vicinity of the azimuth) was evaluated. The results are shown in Table 4.
いずれの鋼No.でもパス間時効した子番1は、パス間時効しなかった子番2に比べ{200}面のX線積分強度は増加したが、{222}面は減少した。また、その比I200/I222は、パス間時効した子番1では1.00以上あったのに対し、パス間時効しなかった子番2では1.00未満であった。これらの結果は、パス間時効により、磁気特性に好ましい{100}<012>方位の強度が増加して、磁気特性に好ましくない{111}<112>方位の強度が減少し、磁束密度B50が増加した。また、特性が良好であった試料(実施例)では、結晶方位分布関数の{100}<012>方位の強度は6.00以上かつ、{111}<112>方位の強度は5.00未満、かつ{100}<012>方位の強度が{411}<148>方位の強度を上回っていることが分かった。なお、{411}<148>方位も{100}面に近い方位であるため、磁気特性に好ましい方位ではあるが、{100}<012>方位の方が磁気特性に好ましいため、高い磁束密度B50を得るためには{100}<012>方位の強度を高める方が望ましい。これに対し、特性が良好でなかった試料(比較例)では、結晶方位分布関数の{100}<012>方位の強度は6.00未満、かつ、{111}<112>方位の強度は5.00以上あり、かつ、{100}<012>方位の強度が{411}<148>方位の強度を下回っていることが分かった。鋼No.8は固溶Cが基底値を超え、かつセメンタイトが析出したため、鋼No.10はP/Fe比が表2に示した通り規定値を超えたために圧延中に破断した。通常P含有量である鋼No.9-1、9-2とPを0.078%含有する鋼No.1-1、1-2に着目すると、表2に示した通り粒界P/Feが高いことによって、表3の通り磁束密度B50は増加したが、{100}<012>方位の強度は{411}<148>方位の強度よりも低かった。従って、実施例の特性を得るためには、表2に代表される素材を用いて、冷間圧延中にパス間時効を施す製法が必要である。 The steel No. 1 subjected to inter-pass aging in any steel No. increased the X-ray integral strength of the {200} plane compared to the steel No. 2 in which inter-pass aging was not performed, but decreased the {222} plane. Further, the ratio I 200 / I 222 was 1.00 or more in the pass No. 1 which was subjected to inter-pass aging, but was less than 1.00 in the pass No. 2 where the inter-pass aging was not performed. These results indicate that the inter-pass aging increases the strength of {100} <012> orientation preferred for magnetic properties, decreases the strength of {111} <112> orientation not preferred for magnetic properties, and the magnetic flux density B50 Increased. In the sample with good characteristics (example), the strength of the {100} <012> orientation of the crystal orientation distribution function is 6.00 or more and the intensity of the {111} <112> orientation is less than 5.00 and {100 It was found that the intensity of the <012> orientation exceeded that of the {411} <148> orientation. Note that the {411} <148> orientation is also close to the {100} plane, so although it is a preferred orientation for the magnetic properties, the {100} <012> orientation is preferred for the magnetic properties, so the high magnetic flux density B50 It is desirable to increase the strength of the {100} <012> orientation in order to obtain. On the other hand, in the sample (comparative example) in which the characteristics were not good, the intensity of the {100} <012> orientation of the crystal orientation distribution function was less than 6.00, and the intensity of the {111} <112> orientation was 5.00 or more. And, it was found that the intensity of the {100} <012> orientation was lower than the intensity of the {411} <148> orientation. In steel No. 8, since solid solution C exceeded the base value and cementite was precipitated, steel No. 10 broke during rolling because the P / Fe ratio exceeded the specified value as shown in Table 2. Focusing on steels No. 9-1 and 9-2 which normally contain P content and steels No. 1-1 and 1-2 containing 0.078% P, the grain boundary P / Fe is high as shown in Table 2. As a result, as shown in Table 3, the magnetic flux density B50 was increased, but the intensity in the {100} <012> orientation was lower than the intensity in the {411} <148> orientation. Therefore, in order to obtain the characteristics of the examples, it is necessary to have a method of performing inter-pass aging during cold rolling using the materials represented by Table 2.
[実験6]
磁気特性へのパス間時効温度の影響とパス間時効時間の影響を調べるため、表3に示した鋼No.1-gと8-gを用いて、冷間圧延中の板厚1.8、1.6、1.2、0.8、0.5mmのときにパス間時効を実施し、1000℃で30s均熱する仕上焼鈍を施した。結果を表5に示す。B50とW10/400は実験5と同様の方法で測定し、全周平均を式(4)と式(5)から求めて評価した。
[Experiment 6]
In order to investigate the influence of interpass aging temperature on magnetic properties and the influence of interpass aging time, using steel Nos. 1-g and 8-g shown in Table 3, the plate thickness during cold rolling was 1.8, 1.6 The inter-pass aging was performed at 1.2, 0.8, and 0.5 mm, and was subjected to finish annealing with 30 ° C. soaking at 1000 ° C. The results are shown in Table 5. B50 and W10 / 400 were measured in the same manner as in Experiment 5, and the whole circumference average was obtained from Equation (4) and Equation (5) and evaluated.
鋼No.8-g-1〜10は圧延中に破断した。これは表3に示した通り、シャルピー遷移温度と硬度パラメータの関係を満足しなかったためである。鋼No.1-g-10は鋼No.1-g-9と比べて時効時間は長いものの、磁束密度向上効果が得られなかった。これらに対し、鋼No.1-g-1〜9はパス間時効によって磁気特性が向上した。 Steel Nos. 8-g-1 to 10 broke during rolling. This is because, as shown in Table 3, the relationship between the Charpy transition temperature and the hardness parameter was not satisfied. Although the aging time of steel No. 1-g-10 was longer than that of steel No. 1-g-9, the magnetic flux density improvement effect was not obtained. On the other hand, in steel Nos. 1-g-1 to 9, the magnetic properties were improved by inter-pass aging.
[参考例](旧住金研究報告RE07345)
田中らは、P添加材へのパス間時効の適用を検討した。図6に実験工程を示す。質量%で、Si:2.0%、Mn:0.2%、Al:0.3%にPを0.01%、0.08%含有する鋼、及びSi:2.5%、Mn:0.2%、Al:1.0%にPを0.01%、0.08%含有する鋼をラボで真空溶解して、板厚2.0mmの熱延板を作製し、これに800℃で10h均熱、炉冷する箱焼鈍型熱延板焼鈍を施して圧延した。その後1050℃で1s均熱する仕上焼鈍を施した。55mm角磁気測定試験を採取し、L方向とT方向(C方向)磁束密度B50を測定した。
[Reference example] (Former Sumikin Research Report RE07345)
Tanaka et al. Examined the application of interpass aging to P additives. The experimental steps are shown in FIG. Steel containing 2.0% of Si, 0.2% of Mn, 0.2% of Al, 0.01% of P in 0.3% of Al, and Si: 2.5% of Mn, 0.2% of Al, 1.0% of Al: 0.01% of P The steel containing 0.08% was vacuum-melted in a laboratory to make a hot-rolled sheet with a thickness of 2.0 mm, and this was subjected to box annealing type hot-rolled sheet annealing which is subjected to soaking at 800 ° C. for 10 h and furnace cooling. . Thereafter, finish annealing was performed so as to achieve 1s soaking at 1050 ° C. A 55 mm square magnetic measurement test was taken, and the magnetic flux density B50 in the L direction and in the T direction (C direction) was measured.
ここで、圧延工程について説明する。室温にて圧延を2パス実施した後に200℃の炉内で2 分保持し、室温まで空冷後、再度圧延を2パス実施する作業を繰り返して0.40mm 厚まで加工し、更に冷間圧延にて板厚0.20mm および0.25mm に仕上げた。 Here, the rolling process will be described. After 2 passes of rolling at room temperature, hold for 2 minutes in a furnace at 200 ° C, air-cool to room temperature, repeat 2 passes of rolling again, process to 0.40 mm thickness, and then cold rolling The plate thickness was 0.20 mm and 0.25 mm.
その結果を図7、図8に示す。時効実施による磁束密度向上効果にP添加効果が上乗せされて、さらに磁束密度が向上することが判明した。 The results are shown in FIG. 7 and FIG. It was found that the effect of P addition is added to the effect of improving the magnetic flux density due to the aging, and the magnetic flux density is further improved.
以上、添付図面を参照しながら本発明の好適な実施の形態について説明したが、本発明はかかる例に限定されない。当業者であれば、特許請求の範囲に記載された思想の範疇内において、各種の変更例または修正例に想到し得ることは明らかであり、それらについても当然に本発明の技術的範囲に属するものと了解される。 Although the preferred embodiments of the present invention have been described above with reference to the accompanying drawings, the present invention is not limited to such examples. It is obvious that those skilled in the art can conceive of various modifications or alterations within the scope of the idea described in the claims, and they are naturally within the technical scope of the present invention. It is understood that.
Claims (7)
2.0%≦Si≦4.0%、
0.01%≦Al≦3.0%、
0.05%≦Mn≦2.5%、
0.03%≦P≦0.12%、
0.001%≦C≦0.005%、
S≦0.005%、
N≦0.005%
を含有し、残部がFeおよび不純物元素からなり、
固溶C濃度が0.001mass%以上、0.005mass%以下であり、結晶粒界におけるP/Fe原子比が0.01以上、0.05以下である、無方向性電磁鋼板用熱延板。 In mass%
2.0% ≦ Si ≦ 4.0%,
0.01% ≦ Al ≦ 3.0%,
0.05% ≦ Mn ≦ 2.5%,
0.03% ≦ P ≦ 0.12%,
0.001% ≦ C ≦ 0.005%,
S ≦ 0.005%,
N ≦ 0.005%
And the balance consists of Fe and impurity elements,
A hot rolled sheet for a non-oriented electrical steel sheet, wherein the solid solution C concentration is 0.001 mass% or more and 0.005 mass% or less, and the P / Fe atomic ratio at the grain boundaries is 0.01 or more and 0.05 or less.
T(℃)≦4.5×(225-H) ・・・ 式(1) The hot rolled sheet for non-oriented electrical steel sheets according to claim 1, wherein the surface Vickers hardness H of the steel sheet and the Charpy transition temperature T (° C) satisfy the following formula (1).
T (° C.) ≦ 4.5 × (225−H) ··· Formula (1)
2.0%≦Si≦4.0%、
0.01%≦Al≦3.0%、
0.05%≦Mn≦2.5%、
0.03%≦P≦0.12%、
0.001%≦C≦0.005%、
S≦0.005%、
N≦0.005%
を含有し、残部がFeおよび不純物元素からなり、
{200}面のX線積分強度I200と{222}面のX線積分強度I222との比I200/I222が1.00以上であり、
結晶方位分布関数における{φ1,Φ,φ2}={25°,0°,45°}の強度が6.00以上であり、かつ、{φ1,Φ,φ2}={30°,55°,45°}の強度が5.00未満を満足し、
{φ1,Φ,φ2}={25°,0°,45°}の強度≧{φ1,Φ,φ2}={20°,20°,45°}の強度
を満足し、
結晶粒径が30μm以上、板厚が0.10mm以上0.50mm以下である、無方向性電磁鋼板。 In mass%
2.0% ≦ Si ≦ 4.0%,
0.01% ≦ Al ≦ 3.0%,
0.05% ≦ Mn ≦ 2.5%,
0.03% ≦ P ≦ 0.12%,
0.001% ≦ C ≦ 0.005%,
S ≦ 0.005%,
N ≦ 0.005%
And the balance consists of Fe and impurity elements,
The ratio I200 / I222 of the X-ray integral intensity I200 of the {200} plane to the X-ray integral intensity I222 of the {222} plane is 1.00 or more,
The strength of {φ1, ,, φ2} = {25 °, 0 °, 45 °} in the crystal orientation distribution function is 6.00 or more, and {φ1, φ, φ2} = {30 °, 55 °, 45 ° The strength of} satisfies less than 5.00,
{φ1, φ, φ2} = {25 °, 0 °, 45 °} strength ≧ {φ1, φ, φ2} = {20 °, 20 °, 45 °} strength,
A non-oriented electrical steel sheet having a crystal grain size of 30 μm or more and a plate thickness of 0.10 mm or more and 0.50 mm or less.
質量%で
2.0%≦Si≦4.0%、
0.01%≦Al≦3.0%、
0.05%≦Mn≦2.5%、
0.03%≦P≦0.12%、
0.001%≦C≦0.005%、
S≦0.005%、
N≦0.005%
を含有し、残部がFeおよび不純物元素からなる鋼片を熱間圧延して焼鈍した後、500℃以上の温度域を、10℃/s以上、100℃/s以下の冷却速度で冷却し、500℃未満の温度域を、500℃以上の温度域における冷却速度よりも大きい冷却速度で冷却する、無方向性電磁鋼板用熱延板の製造方法。 A method of manufacturing a hot-rolled sheet for non-oriented electrical steel sheet according to any one of claims 1 or 2,
In mass%
2.0% ≦ Si ≦ 4.0%,
0.01% ≦ Al ≦ 3.0%,
0.05% ≦ Mn ≦ 2.5%,
0.03% ≦ P ≦ 0.12%,
0.001% ≦ C ≦ 0.005%,
S ≦ 0.005%,
N ≦ 0.005%
After hot-rolling and annealing a steel piece containing the balance of Fe and an impurity element, and then cooling the temperature range of 500 ° C. or more at a cooling rate of 10 ° C./s or more and 100 ° C./s or less, The manufacturing method of the hot-rolled sheet for non-oriented electrical steel sheets which cools a temperature range less than 500 ° C with a cooling rate larger than a cooling rate in a temperature range 500 ° C or more.
質量%で
2.0%≦Si≦4.0%、
0.01%≦Al≦3.0%、
0.05%≦Mn≦2.5%、
0.03%≦P≦0.12%、
0.001%≦C≦0.005%、
S≦0.005%、
N≦0.005%
を含有し、残部がFeおよび不純物元素からなる鋼片を熱間圧延して700℃以上で巻き取りを行い、500℃以上の温度域を、10℃/s以上、100℃/s以下の冷却速度で冷却し、500℃未満の温度域を、500℃以上の温度域における冷却速度よりも大きい冷却速度で冷却する、無方向性電磁鋼板用熱延板の製造方法。 A method of manufacturing a hot-rolled sheet for non-oriented electrical steel sheet according to any one of claims 1 or 2,
In mass%
2.0% ≦ Si ≦ 4.0%,
0.01% ≦ Al ≦ 3.0%,
0.05% ≦ Mn ≦ 2.5%,
0.03% ≦ P ≦ 0.12%,
0.001% ≦ C ≦ 0.005%,
S ≦ 0.005%,
N ≦ 0.005%
Is hot rolled and the coil is wound at 700 ° C. or higher, and the temperature range of 500 ° C. or higher is cooled by 10 ° C./s or more and 100 ° C./s or less A method for producing a hot rolled sheet for non-oriented electrical steel sheet, comprising: cooling at a speed and cooling a temperature range of less than 500 ° C. at a cooling rate greater than a cooling rate in a temperature range of 500 ° C.
前記冷間圧延をトータル圧下率が75%以上、95%以下の多パス圧延とし、各パス間にて100℃〜400℃で1〜60minの時効処理を施す、無方向性電磁鋼板の製造方法。 A method of manufacturing a non-oriented electrical steel sheet according to claim 3 by cold-rolling and hot-rolling the hot-rolled sheet for non-oriented electrical steel sheet according to any one of claims 1 or 2 ,
A method of manufacturing a non-oriented electrical steel sheet, wherein the cold rolling is multipass rolling with a total rolling reduction of 75% to 95%, and an aging treatment is performed at 100 ° C to 400 ° C for 1 to 60 minutes between each pass. .
Performing decarburization annealing after the cold rolling, after the, performing the final annealing method for producing a non-oriented electrical steel sheet according to claim 6.
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