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1)  Optimum unambiguous discrimination
最优无错区分
2)  the best space division
最优区间分割
1.
In order to improve the ability of solving the high dimention and mass data,based on the old algorithm,a modified one with the methods of density and the best space division is presented.
为了进一步提高其处理高维海量数据的能力,在原算法的基础上提出一种基于密度样本分析和基于最优区间分割进行改进的聚类算法,并通过使用仿真数据加以验证是可行的,理论分析与实验结果表明,与原算法相比,改进算法不仅保留原算法的优点,且对大规模数据集有着很好的聚类效果。
3)  best linear unbiased confidence interval
最优线性无偏置信区间
4)  dislocation-free zone
无位错区
1.
Mode Ⅰ crack tip plastic zone,dislocation-free zone and their effects on crack propagation;
Ⅰ型裂纹尖端塑性区和无位错区及其对裂纹扩展的影响
2.
Dislocation emission from the crack tip,formation of dislocation-free zones,nucleation of nano-cracks and dislocation pile-ups were all observed.
进行了1Cr18Ni9Ti(奥氏体321型不锈钢)的TEM原位拉伸实验,观察到了位错从裂纹尖端的发射、无位错区形成、纳米裂纹形核及位错塞积等物理现象。
5)  dislocation free zone
无位错区
1.
A dislocation free zone(DFZ) is formed between crack tip and the inversely pileup dislocations when the dislocation emission and motion reach equilibrium.
结果发现:黄铜薄膜试样拉伸时,裂尖首先发射位错,平衡时形成无位错区和反塞积位错群;裂尖前方较厚区域可以发生孪生变形,形成形变孪晶,微裂纹在孪晶中形核、扩展,导致裂纹呈Z字形扩展;裂尖无位错区也可能形成微孪晶,微裂纹在微孪晶中形核,使裂纹呈不连续扩展;微裂纹也可以从主裂纹顶端连续形核、扩展。
2.
TEM in situ tensile tests of 310 stainless steel show that a dislocation free zone (DFZ) forms after equilibrium if the displacement keeps constant after many dislocations are emitted from a crack tip.
310奥氏体不锈钢在透射电镜中的原位拉伸观察表明,如在裂尖发射位错后保持恒位移,则在裂尖能形成无位错区(DFZ)。
3.
The results show that 1)in precharged specimens,many dislocations can emit from a crack tip followed by forming a dislocation free zone(DFZ) after equilibrium:2)nanocracks nucleate preferable in DFZs;3)microcracks connect with each other,resulting in the brittle cracks,instead of blunting into voids.
结果表明,预充氢的310不锈钢试样在拉伸过程中从裂尖发射大量位错,平衡后形成无位错区(DFZ);纳米级微裂纹择优在DFZ中形核;微裂纹不钝化为空洞,而是通过多个微裂纹的形核及相互连接导致裂纹的脆性扩展。
6)  optimal reactive power
最优无功
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1.谓拥挤杂乱。
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