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Transmission electron microscopy and electron diffraction studies on martensitic transformations in nanometre-sized particles of Au-Cd alloys of near-equiatomic compositions

机译:接近等原子组成的Au-Cd合金纳米尺寸颗粒中马氏体转变的透射电子显微镜和电子衍射研究

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Martensitic transformations in nanometre-sized particles of Au-Cd alloys of near-equiatomic compositions were studied by means of transmission electron microscopy and electron diffraction. The alloy particles with an average size of several nanometres were prepared by high-vacuum electron-beam deposition. In the as-deposited state the particles were crystalline and possessed a B2-type structure at room temperature, similar to that of the beta(2) phase in the corresponding bulk. The beta(2)-phase particles with an average composition of Au-44.5 at.% Cd were transformed at 76K into an orthorhombic structure similar to that of the gamma(2)' phase in the bulk, while those with an average composition of Au-50.2 at.% Cd were transformed at 60 K into a trigonal structure similar to that of the zeta(2)' phase in bulk. The temperature parameter in the Debye-Waller factor measured at room temperature for the beta(2)-phase particles was roughly four times that for Au in the bulk. It was thus found that the M-S temperatures for the beta(2)-->gamma(2)' and beta(2)-->zeta(2)' transformations in the nanometre-sized particles were lowered far below room temperature despite the increasing surface area and the enhanced lattice softening. Their reverse transformations, however, took place on heating to room temperature. It was thus seen that the lowering of the transformation temperatures was due to the decrease in the thermodynamic equilibrium temperatures T-0 between the beta(2) and gamma(2)' and between the beta(2) and zeta(2)' phases. The decrease in T-0 indicated that the free energies of the beta(2), gamma(2)' and zeta(2)' phases of the alloys in the small-particle state are definitely different from those in the bulk state. [References: 46]
机译:通过透射电子显微镜和电子衍射研究了近等原子组成的Au-Cd合金的纳米颗粒中的马氏体转变。通过高真空电子束沉积制备平均尺寸为几纳米的合金颗粒。在沉积状态下,颗粒为晶体,并在室温下具有B2型结构,类似于相应主体中β(2)相的结构。平均组成为Au-44.5 at。%Cd的β(2)相粒子在76K时转变为与整体中gamma(2)'相相似的正交结构,而平均组成为Au-50.2 at。%Cd在60 K下转变为类似于zeta(2)'相的整体三角结构。 β(2)相粒子在室温下测得的Debye-Waller因子温度参数约为本体中Au的四倍。因此,发现纳米级颗粒中的β(2)-> gamma(2)'和β(2)-> zeta(2)'转变的MS温度被降低到远低于室温,尽管增加的表面积和增强的晶格软化。然而,它们的反向转变发生在加热至室温时。因此可以看出,相变温度的降低是由于β(2)和γ(2)'相之间以及β(2)和zeta(2)'相之间的热力学平衡温度T-0降低。 。 T-0的减少表明,处于小颗粒状态的合金的β(2),γ(2)'和zeta(2)'相的自由能肯定不同于体态的自由能。 [参考:46]

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