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首页> 外文期刊>Journal of Materials Science >Localized strain and heat generation during plastic deformation in nanocrystalline Ni and Ni-Fe
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Localized strain and heat generation during plastic deformation in nanocrystalline Ni and Ni-Fe

机译:纳米晶Ni和Ni-Fe塑性变形过程中的局部应变和热产生

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Room temperature tensile testing was performed on a coarse-grained polycrystalline Ni (32 μm), a nanocrystalline Ni (23 nm) and two nanocrystalline Ni-Fe (16 nm) electrodeposits at two strain rates of 10-1 and 10-2/s. Strain localizations and local temperature increases were simultaneously recorded during tensile testing. For all materials, higher loads or higher strain rate generally resulted in higher peak temperature with the highest temperatures recorded in the fracture regions. The maximum temperature for the nanocrystalline materials was just over 80 °C, which is significantly below the reported temperatures for the onset of thermally activated grain growth. Therefore, the previously reported grain growth observed on similar materials after tensile deformation is likely not thermally activated but a stress-induced phenomenon. Despite the wide grain range from 16 nm to 32 μm, all samples exhibited similar strain localization behavior. Local strain variations initiated in the early stage of macroscopic uniform deformation, subsequent necking and fracture took place in the region of initial strain localization. While the coarse-grained polycrystalline Ni exhibited little strain rate sensitivity, gradually increased strain rate sensitivity was observed for the 23 nm Ni and the two 16 nm Ni-Fe samples, suggesting that both dislocationmediated and grain-boundary-controlled mechanisms were operative in the deformation of the nanocrystalline Ni and Ni-Fe samples.
机译:在粗晶多晶Ni(32μm),纳米晶Ni(23 nm)和两个纳米晶Ni-Fe(16 nm)电沉积上以两种应变速率10-1和10-2 / s进行室温拉伸测试。在拉伸测试期间同时记录了应变局部化和局部温度升高。对于所有材料,较高的载荷或较高的应变率通常会导致较高的峰值温度,并且在断裂区域记录到最高温度。纳米晶体材料的最高温度刚好超过80°C,该温度明显低于报道的热活化晶粒生长开始的温度。因此,先前报道的在拉伸变形后在相似材料上观察到的晶粒长大可能不是被热激活而是应力引起的现象。尽管晶粒范围从16 nm到32μm,但所有样品均表现出相似的应变定位行为。在宏观均匀变形的早期阶段开始发生局部应变变化,随后的颈缩和断裂发生在初始应变局部区域。虽然粗晶多晶镍的应变速率敏感性很小,但观察到23 nm Ni和两个16 nm Ni-Fe样品的应变速率敏感性逐渐提高,这表明位错介导和晶界控制机制均在晶格中起作用。 Ni和Ni-Fe纳米晶样品的形变。

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