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首页> 外文期刊>Journal of Alloys and Compounds: An Interdisciplinary Journal of Materials Science and Solid-state Chemistry and Physics >Role of preparation conditions of Bi-2223 ceramic materials and optimization of Bi-2223 phase in bulk materials with experimental and statistical approaches
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Role of preparation conditions of Bi-2223 ceramic materials and optimization of Bi-2223 phase in bulk materials with experimental and statistical approaches

机译:Bi-2223陶瓷材料制备条件的作用以及Bi-2223相在块状材料中的优化实验和统计方法

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摘要

This study deals with the determination of optimum preparation conditions (press load, annealing temperature and time) for the Bi-2223 superconducting compound with the aid of both the experimental methods regarding dc resistivity, transport critical current density and powder X-ray diffraction measurements and statistical approaches including response surface explorer based on Box-Behnken designs for the first time. It is found that the Bi-2223 polycrystalline compound prepared under 300 MPa pressure load at 840 degrees C for 48 h presents the highest formation of Bi-2223 phase due to the considerable elimination of the impurity scattering and lattice strain in the crystal structure. On the other hand, the sample prepared at 860 degrees C under 350 MPa for 48 h exhibits the worst characteristic features of high T-c-phase as a consequence of the enhancement in local structural distortions, dislocations, defects and disorders in the Cu-O-2 consecutively stacked layers. Thus, the latter condition causes to both the degradation in amplitude of pair wave function (decrease in the overlapping of Cu 3d and O 2p functions) and metastability due to the reduction of hole trap energy. In this respect, the best material displays the largest T-c(onset) of 110.63 K and T-c(offset) of 108.46 K values while the worst material obtains the smallest values (T-c(onset) of 95.45 K and T-c(offset) of 45.32 K). Similarly, the maximum J(c) value of 818 A/cm(2) is experimentally observed for the best compound whereas the worst sample obtains the smallest value of 112 A/cm(2). The decrement in the Jc parameter is attributed to the regression of intergrain coupling and flux pinning vortices in the Bi-2223 crystal structure due to the increment of misorientations and especially grain boundary weak-interactions in the crystal system. The XRD results also reveal that the combination of 300 MPa press load, 840 degrees C annealing temperature and 48 h annealing time for the preparation condition promotes seriously the high T-c-phase as a consequence of the enhancement in the average crystallite size and lattice parameter c or decrement in the a-axis length. Accordingly, the best material obtains the largest c-axis length of about 37.22 angstrom and average grain size of 71.4 nm but the smallest lattice parameter a of about 5.29 angstrom. At the same time, the surface response designs of statistical analyses show that the optimum preparation conditions are defined to be 306.5657 MPa press load, 840 degrees C annealing temperature and 48 h annealing time to maximize the high T-c-phase (with the maximum T-c(onset) ; T-c(offset) and J(c) parameters. (C) 2016 Elsevier B.V. All rights reserved.
机译:这项研究借助有关直流电阻率,传输临界电流密度和粉末X射线衍射测量的实验方法,确定了Bi-2223超导化合物的最佳制备条件(压力负载,退火温度和时间)。统计方法,包括首次基于Box-Behnken设计的响应面浏览器。发现在300 MPa压力下在840℃下48 h制备的Bi-2223多晶化合物由于大量消除了晶体结构中的杂质散射和晶格应变,因此形成了最高的Bi-2223相。另一方面,在860℃,350 MPa下制备48 h的样品表现出高Tc相的最差特征,这是由于Cu-O-的局部结构变形,位错,缺陷和无序性增强2个连续堆叠的层。因此,由于空穴陷阱能的降低,后一种情况既导致成对波函数的振幅降低(Cu 3d和O 2p函数的重叠降低),又引起亚稳定性。在这方面,最好的材料显示的最大Tc(起始)为110.63 K,Tc(偏移)为108.46 K,而最差的材料则显示最小值(Tc(起始)为95.45 K,Tc(偏移)为45.32 K )。类似地,实验观察到最佳化合物的最大J(c)值为818 A / cm(2),而最差的样品的最小值为112 A / cm(2)。 Jc参数的减少归因于Bi-2223晶体结构中晶粒间耦合和通量钉扎涡的回归,这归因于取向系统(尤其是晶体系统中晶界弱相互作用)的增加。 XRD结果还表明,300 MPa压力载荷,840℃退火温度和48 h退火时间的制备条件相结合,由于平均晶粒尺寸和晶格参数c的提高,严重促进了高Tc相的产生。或减少a轴长度。因此,最好的材料获得的最大c轴长度约为37.22埃,平均晶粒尺寸为71.4 nm,但最小的晶格参数a约为5.29埃。同时,统计分析的表面响应设计表明,最佳制备条件定义为:压制载荷为306.5657 MPa,退火温度为840摄氏度,退火时间为48小时,以使高Tc相(最大Tc( (c)2016 Elsevier BV保留所有权利。

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