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Through-process characterization of local anisotropy of Non-oriented electrical steel using magnetic Barkhausen noise

机译:利用磁巴克豪森噪声对无方向性电工钢局部各向异性进行全过程表征

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Magnetic Barkhausen noise (MBN) signals were measured on a non-oriented electrical steel through all the thermomechanical processing stages, i.e. hot rolling, hot band annealing, cold rolling and final annealing. The temperature of the final annealing was varied from 600 °C to 750 °C so that the steel consisted of partially or completely recrystallized microstructures and different levels of residual stresses. The angular MBNrms(root mean square) values were compared to the texture factors in the same directions, the latter being calculated from the crystallographic texture measured by electron backscatter diffraction (EBSD). It was found that, in the cold-rolled, hot-rolled and completely recrystallized steels, the angular MBNrmsfollowed a cosine function with respect to the angle of magnetization, while in partially recrystallized state such a relation does not exist. After cold rolling, the maximum MBNrmswas observed in the rolling direction (RD) and the minimum MBNrmswas in the transverse direction (TD), which was inconsistent with the magnetocrystalline anisotropy as indicated by the texture factor. After hot rolling, the maximum and minimum MBNrmsvalues were observed in the TD and RD, respectively, exactly opposite to the cold-rolled state. If the steel was completely recrystallized, the maximum MBNrmswas normally observed at a direction that was 15–30° from the minimum texture factor. If the steel was partially recrystallized, both the magnetocrystalline anisotropy of the material and the residual stress contributed to the angular MBNrms, which resulted in the deviation of the relationship from a cosine function. The relative strength of the two factors determined which factor would dominate the overall magnetic anisotropy.
机译:在所有热机械加工阶段(即热轧,热带退火,冷轧和最终退火),在无取向电工钢上测量巴克豪森磁噪声(MBN)信号。最终退火的温度在600°C至750°C之间变化,以使钢由部分或完全重结晶的微观结构和不同程度的残余应力组成。将角MBNrms(均方根)值与相同方向上的纹理因子进行比较,后者是根据通过电子背散射衍射(EBSD)测量的晶体纹理计算得出的。已经发现,在冷轧,热轧和完全重结晶的钢中,角MBNrms相对于磁化角具有余弦函数,而在部分重结晶状态下则不存在这种关系。冷轧后,在轧制方向(RD)上观察到最大MBNrms,在横向(TD)上观察到最小MBNrms,这与织构系数表明的磁晶各向异性不一致。热轧后,分别在TD和RD处观察到最大和最小MBNrms值,与冷轧状态完全相反。如果钢完全重结晶,则通常在与最小织构因子成15–30°的方向上观察到最大MBNrms。如果钢进行了部分重结晶,则材料的磁晶各向异性和残余应力均会影响MBNrms角,从而导致该关系偏离余弦函数。这两个因素的相对强度决定了哪个因素将主导整个磁各向异性。

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