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Critical Cooling Rate for the Glass Formation of Fe_(80-x)Co_xP_(13)C_7 Alloy
In this work, the critical cooling rate Rc for glass formation of a series of Fe80-xCoxP13C7 (x = 0, 5, 10, 15...
Kai XuYan WangQiang Li
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Fe_(80)P_(13)C_7块体非晶态合金与非晶薄带抗腐蚀性能的对比研究
2012年
通过J-Quenching技术在低冷速(低于1000K/s)下制备出块体尺寸达2mm的Fe80P13C7非晶态合金。通过阳极极化曲线测试以及对样品在1mol/L的HCl溶液中浸泡后的腐蚀形貌的观察,对Fe80P13C7块体非晶态合金、非晶薄带以及晶态合金的电化学腐蚀行为进行了对比研究,结果表明,块体非晶的腐蚀性能优于非晶薄带和晶态合金。这可能是由于块体非晶态合金在制备过程中冷速较低,原子发生结构弛豫的时间更长,结合能增大,使得合金中原子与溶液中离子的反应速率减慢,从而提高了块体非晶态合金的腐蚀性能。
李晋锋刘瑞泉黄玉代李强
关键词:块体非晶态合金非晶薄带抗腐蚀性能
Critical Cooling Rate for the Glass Formation of Ferromagnetic Fe_(80)P_(13)C_7 Alloy被引量:2
2013年
In this paper the critical cooling rate, Rc, for the glass formation of Fe80P13C7 alloy has been determined using both Uhlmann's and Barandiaran-Colmenero's method. In Uhlmann's method, all kinds of the expres-sions of △G^l-s (T) and η/(T) determined using the different modes and methods had been investigated. It is indicated that the Rc for the glass formation of FesoP13C7 alloy can be estimated to be 349 K/s by Uhlmann's method based on the appropriate expressions of △G^l-s(T) and η/(T). The calculated result accords with our experimental result. The Rc for the glass formation of Fe80P13C7 alloy has also been determined to be 0.49 K/s using Barandiaran-Colmenero's method. This resultant Rc is unreasonable low and it indicates that Barandiaran-Colmenero's method does not suit to Fe-based alloy.
Kai XUYan WANGJinfeng LIQiang LI
基于LabVIEW平台的日立U-2000分光光度计的测量控制系统
本文的工作是基于LabVIEW平台开发日立U-2000分光光度计(以下简称U-2000)的测量控制系统。该系统利用计算机通过RS-232C接口实现了对U-2000的控制以及测量数据的采集。计算机端的软件基于LabVIEW...
陈洁容李强
关键词:测量控制系统RS-232C
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银包覆PMMA纳米核壳颗粒的局域表面等离激元共振行为的模拟计算
应用Mie理论,对银膜包覆PMMA纳米核壳结构的局域表面等离激元共振行为进行了模拟计算,研究了颗粒尺寸,核壳比等参数对所获得核壳颗粒的等离激元共振LSPR消光光谱的影响;同时也将其与单相银纳米球的LSPR光谱行为进行了比...
李强王连洲逯高清黄娆朱贤方
关键词:MIE理论模拟计算
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Formation of bulk ferromagnetic nanostructured Fe_(40)Ni_(40)P_(14)B_6 alloys by metastable liquid spinodal decomposition被引量:2
2009年
Nanostructured Fe40Ni40P14B6 alloy ingots of 3―5 mm in diameter could be synthesized by a metastable liquid state spinodal decomposition method. For undercooling T> 260 K, the microstructure of the undercooled specimen had exhibited liquid state spinodal decomposition in the undercooled liquid state. The microstructure could be described as two intertwining networks with small grains dispersed in them. For undercooling T>290 K, the overall microstructure of the specimen changed into a granular morphology. The average grain sizes of the small and large grains are 30 nm and 80 nm, respectively. These prepared samples are soft magnets with saturation magnetization Bs 0.744 T.
LI Qiang1,2 1 School of Physics Science and Technology, Xinjiang University, Urumqi 830046, China
关键词:BULKNANOSTRUCTUREDMETASTABLELIQUIDSPINODAL
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