共查询到15条相似文献,搜索用时 328 毫秒
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基于96.5Sn-3.5Ag钎料合金的多轴时相关变形行为,提出了一个考虑其多轴变形特性的本构模型.在该模型背应力演化方程中,引入了非比例度对背应力演化率的影响,并提出了模型参数的确定方法.在室温下对96.5Sn-3.5Ag钎料合金进行了十字形、双三角形及椭圆形等拉扭组合非比例循环应变路径下的变形行为的本构模拟,并将预言结果与实验结果进行了比较.预言结果表明,该模型对于96.5Sn-3.5Ag钎料合金的多轴应变循环变形行为具有很好的预言能力. 相似文献
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一个考虑循环应变幅值历史效应的粘塑性本构模型 总被引:1,自引:0,他引:1
本文提出了一个考虑材料应变幅值历史效应的粘塑性本构模型。在该模型中,引入了三个具有不同演化速率的背应力演化方程;建立了非弹性应变幅值历史记忆模型,对各向同性变形阻力,引入了具有先前加载历史记忆的演化方程。将本文模型用于1Cr18Ni9Ti不锈钢循环变形行为描述中,其预言结果与实验结果吻合得很好,表明该模型能很好地描述材料的循环应变幅值历史下的循环变形行为。 相似文献
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基于63Sn-37Pb钎料舍金在多种非比例应变循环加载下的实验结果,通过考察材料的非弹性应变率与偏应力之间的夹角随累积非弹性应变的变化规律,对63Sn-37Pb钎料合金的非弹性流动特性进行了定量分析。分析结果显示:在相同的非比例加载路径下,当加载等效应变幅值相同时,等效应变率越高,非弹性应变率与偏应力之间夹角平均水平越低,当等效应变率相同时,等效应变幅值越大,相应的夹角平均水平越低;在保持时间范围内,非弹性应变率方向与偏应力方向趋于一致;当非比例路径形状不同时,其非弹性应变率与偏应力之间的夹角随累积非弹性应变的变化趋势明显不同。研究表明,材料的非弹性流动特性强烈依赖于等效应变幅值、等效应变率、保持时间、非比例路径形状。 相似文献
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一种描述形状记忆合金拟弹性变形行为的本构关系 总被引:2,自引:0,他引:2
本文给出一种描述形状记忆合金拟弹性变形现象的本构关系,可用于多晶材料在一般应力状态下及单晶材料在单轴应力下的变形情况。该本构关系采用弹性应变与相变应变迭加形式,物理意义明显,形式简洁。对 Cu-Zn-Sn 合金及 Ti-Ni 合金材料的变形行为进行了模拟计算,结果与实验值有较好的吻合。 相似文献
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一种描述形状记忆合金拟弹性变形行为的本构关系 总被引:2,自引:0,他引:2
本文给出一种描述形状记忆合金拟弹性变形现象的本构关系,可用于多晶材料在一般应力状态下及单晶材料在单轴应力下的变形情况。该本构关系采用弹性应变与相变应变迭加形式,物理意义明显,形式简洁。对 Cu-Zn-Sn 合金及 Ti-Ni 合金材料的变形行为进行了模拟计算,结果与实验值有较好的吻合。 相似文献
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SnPb钎料合金的粘塑性Anand本构方程 总被引:8,自引:0,他引:8
采用统一型粘塑性本构 Anand方程描述了电子封装焊点 Sn Pb钎料合金的非弹性变形行为 ,基于 Sn Pb 合金的弹塑性蠕变本构方程和实验数据 ,确定了6 2 Sn36 Pb2 Ag、6 0 Sn40 Pb、96 .5 Sn3.5 Ag和 97.5 Pb2 .5 Sn四种钎料合金 Anand方程的材料参数 ,验证了粘塑性 Anand本构方程对 Sn Pb合金在恒应变速率和稳态塑性流动条件下应力应变行为的预测能力。结果表明 ,Anand方程能有效描述 Sn Pb钎料的粘塑性本构行为 ,并可应用于电子封装 Sn Pb焊点的可靠性模拟和失效分析 相似文献
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一个非比例循环粘塑性本构模型 总被引:4,自引:1,他引:4
本文提出地一个考虑材料非比例循环附加强效应,非比例循环加载历史产应和应变幅值历史效应的粘塑性体构模型。在该模型中,引入了对加载过程非常弹性应变幅值的记忆变量q;定义了新的非比例度;引入了考虑材料非比例度的循环饱和各向同性变形阻力参量Qs;对各向同性变开引入了具有先前加载历史记忆的演化方程,将本文模型用于1Cr18Ni9Ti不锈钢高温循环变形行为描述,其预言结果与实验结果吻合得很好,表明该模型能很好 相似文献
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《International Journal of Plasticity》2005,21(2):353-379
Motivated by the distribution of non-linear relaxation (DNLR) approach, a phenomenological model is proposed in order to describe the cyclic plasticity behavior of metals under proportional and non-proportional loading paths with strain-controlled conditions. Such a model is based on the generalization of the Gibbs's relationship outside the equilibrium of uniform system and the use of the fluctuation theory to analyze the material dissipation due to its internal reorganization. The non-linear cyclic stress–strain behavior of metals notably under complex loading is of particular interest in this study. Since the hardening effects are described appropriately and implicitly by the model, thus, a host of inelastic behavior of metals under uniaxial and multiaxial cyclic loading paths are successfully predicted such as, Bauschinger, strain memory effects as well as additional hardening. After calibrating the model parameters for two metallic materials, the model has demonstrated obviously its ability to describe the cyclic elastic-inelastic behavior of the nickel base alloy Waspaloy and the stainless steel 316L. The model is then implemented in a commercial finite element code simulating the cyclic stress–strain response of a thin-walled tube specimen. The numerical responses are in good agreement with experimental results. 相似文献
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对316L不锈钢的非比例循环粘塑性本构描述 总被引:1,自引:0,他引:1
对循环硬化的316L不锈钢提出了一个考虑非比例循环加载下流动和硬化特性的粘塑性本构模型。模型中,通过随动硬化的背应力演化以各向同性阻力演化非比例循环路径及其历史的依赖关系来表征材料的非比例循环附加硬化和非比例循环流动特性,将模型用于预测316L不锈钢的圆形,正菱形应变路径的复杂循环变形行为,其预言结果与实验结果吻合很好。 相似文献
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A novel cyclic deformation test program was undertaken to characterize macroscopic time dependent deformation of a titanium alloy for use in viscoplastic model development. All tests were conducted at a high homologous temperature, 650 °C, where there are large time dependent and loading rate dependent effects. Uninterrupted constant amplitude tests having zero mean stress or a tensile mean stress were conducted using three different control modes: strain amplitude and strain rate, stress amplitude and stress rate, and a hybrid stress amplitude and strain rate. Strain ratcheting occurred for all cyclic tests having a tensile mean stress and no plastic shakedown was observed. The shape of the strain ratcheting curve as a function of time is analogous to a creep curve having primary, steady state and tertiary regions, but the magnitude of the ratchet strains are higher than creep strains would be for a constant stress equal to the mean stress. Strain cycles interrupted with up to eight 2-h stress relaxation periods around the hysteresis loop, including hold times in each quadrant of the stress–strain diagram, were also conducted. Stress relaxation was path-dependent and in some cases the stress relaxed to zero. The cyclic behavior of these interrupted tests was similar even though each cycle was very complex. These results support constitutive model development by providing exploratory, characterization and validation data. 相似文献