英语翻译In this study,we used our numerical calculation scheme in order to simulate the material behavior of NiTi wires with 50.9 at.% Ni near room temperature (experimental data are given in Sawaguchi et al.,2003; Yawny et al.,2005).The material
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英语翻译In this study,we used our numerical calculation scheme in order to simulate the material behavior of NiTi wires with 50.9 at.% Ni near room temperature (experimental data are given in Sawaguchi et al.,2003; Yawny et al.,2005).The material
英语翻译
In this study,we used our numerical calculation scheme in order to simulate the material behavior of NiTi wires with 50.9 at.% Ni near room temperature (experimental data are given in Sawaguchi et al.,2003; Yawny et al.,2005).The material parameters (we assume that there is no tension——compression asymmetry) are summarized in Table 1.Table 1 also includes the strains which characterize the start of the forward transformation ( ePE) and the end of the reverse transformation ( eel).ePE and eel can be calculated from the characteristic stresses and slopes in the stress–strain curve (see Fig.2b).
英语翻译In this study,we used our numerical calculation scheme in order to simulate the material behavior of NiTi wires with 50.9 at.% Ni near room temperature (experimental data are given in Sawaguchi et al.,2003; Yawny et al.,2005).The material
本研究中,为了模拟室温下含有50.9%Ni(实验数据在论文Sawaguchi et al.,2003; Yawny et al.,2005中给出)的NiTi线的材料特性,我们使用了我们的数值计算方法.材料参数(我们假定不存在抗压不确定性)在表1中总结给出.表1还包含了描述正向转换的起点(ePE)和反向转换的终点(eel)的张力.ePE和eel可以从应力应变曲线的应力和斜率特征计算出来(见图2b).