共查询到18条相似文献,搜索用时 171 毫秒
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含固有缺陷复合材料有效弹性性能预报 总被引:2,自引:0,他引:2
根据缺陷在复合陶瓷中分布特点,将缺陷简化为刚度为0的椭球夹杂,嵌入到横观各向同性基体中,建立含缺陷复合材料的细观结构模型。应用相互作用直推估计法推导含缺陷胞元的有效刚度,结合刚度体平均化方法,假设胞元空间随机分布,得到复合材料的等效刚度表达式,分析横观各向同性基体中缺陷体积分数、取向和形状对材料等效刚度的影响,并进一步讨论缺陷周围基体各向异性的影响。结果表明,缺陷存在导致材料弹性性能明显降低,在缺陷体积分数较小时,弹性常数对缺陷体积分数更加敏感;缺陷形状对弹性常数有较大影响,当缺陷接近于薄片状时,缺陷厚度对弹性常数影响明显,而缺陷平面形状对弹性常数基本没有影响;当片状缺陷垂直于基体中弹性模量较大的轴时,缺陷对材料有效性能的降低作用更显著,考虑缺陷周围基体各向异性是很有必要的。 相似文献
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针对BCC、FCC及其衍化型共6种微桁架胞元结构进行了参数化建模及几何特性分析,通过有限元法对不同构型的胞元分别进行了压缩载荷条件下的力学性能分析,提出了等效比刚度的概念以表征不同构型胞元结构的刚度特性.结果表明:胞元构型对比表面积影响不大,但对相对密度有较大影响,FCC和FCCZ型胞元具有较优良的几何特性及减重效果.FCCZ胞元具有较高的比刚度,通过引入载荷方向上的Z模块,可显著提高微桁架胞元的等效比刚度,同时降低胞元构型对等效比刚度的影响程度. 相似文献
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以原位生成法制备的TiB2颗粒增强铁基复合材料为研究对象,通过纳米压痕试验及有限元反演分析确定基体的幂硬化模型参数,建立二维细观真实结构模型和颗粒随机分布的体胞模型,然后模拟单轴拉伸试验,用等效宏观方法计算真应力-真应变曲线,对2种模型的模拟结果进行对比,并探讨边界条件对模拟结果的影响。结果表明:边界条件对模拟单轴拉伸时的真应力-真应变曲线影响较小;2种模型模拟得到单轴拉伸的真应力-真应变曲线差异较小,且与试验结果吻合,相对误差小于5%;真实结构模型模拟得到的弹性模量与屈服强度的误差小于体胞模型;不同模型模拟得到基体与颗粒的局部微观等效应力场及应变场有明显差异。 相似文献
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为解决现代工业制造中,颗粒弥散强化金属陶瓷复合材料有效导热系数测量困难、传统模型理论模型有缺陷,测不准等问题,将平均积分法和热阻串并联法应用到新模型之中。开展了界面热阻、颗粒性状和孔隙对复合材料有效导热系数影响的分析,建立了复合材料等效导热系数的通用表达式,在模型预测复合材料导热系数上提出了新的方法。然后对界面热阻、孔隙、颗粒形状等因素对复合材料导热系数的影响进行了评价。研究结果表明,在颗粒弥散强化陶瓷复合材料中,复合材料的有效导热系数随着填充颗粒的体积分数增大而增大,随着气孔率的增加而减小,随着填充颗粒的形状因子增大而增大;计算值与实验数据相吻合,误差小、模型适用范围广,证明了公式的正确性。 相似文献
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胶接接头中总存在胶瘤,由于建模复杂,胶接接头有限元分析中胶瘤常被忽略.但胶瘤能减少峰值应力,提高结构强度和刚度.为此,提出一种简化的胶接有限元模型,即用壳单元代表胶瘤,体单元代表被粘体和胶层,并用弹性理论建立壳单元等效厚度公式.以体单元精细模型结果作为对比的真实解,考察五种载荷工况下,单搭接头简化有限元模型的胶层应力和刚度.分析表明,壳单元等效厚度公式正确,胶接简化有限元模型精度高,可用于诸如汽车等大型结构中;用壳单元简单模型可定量分析胶瘤大小和形状对接头应力和总体刚度性能的影响. 相似文献
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三维编织C/SiC复合材料弹性常数预报 总被引:4,自引:0,他引:4
基于纤维倾角模型 ,根据层合板理论推导出其弹性常数计算公式。三维编织C/SiC复合材料不同于树脂基复合材料 ,一是纤维模量低于基体模量 ,二是碳纤维在高温沉积热解碳和碳化硅后模量有较大幅度的下降 ,还有较多的空洞存在。考虑到这些因素对三维编织C/SiC复合材料弹性性能的影响 ,编制了相应的C语言计算程序 ,预报了三维编织C/SiC复合材料的纵向弹性性能 ,对程序计算结果进行了分析讨论。另外 ,通过力学实验来验证了理论分析的可靠性。 相似文献
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A multi-scale model which can be used to evaluate the interaction between a microstructure and the heterogeneous deformation behavior of ternary composites on the micro- to macroscopic scale has been developed based on the large deformation finite element homogenization method. Using four different interphases consisting of a rubber, two different types of polymer and an elastic material with intermediate stiffness of particle and matrix, the elasto-plastic behaviors of the composites have been confirmed to be markedly influenced by the interphase properties and the interphase with a stiffness well below that of the matrix shows a suitable effect on the micro- to macroscopic deformation behaviors of the composites. Therefore, a computational simulation has been performed for the present interphase to clarify the effects of the macroscopic strain ratio, interphase properties and particle volume fraction on macroscopic characteristics such as deformation resistance, elasticity modulus and yield stress, and on microscopic characteristics such as shear band pattern, mean stress in the matrix and normal stress on the particle surface. The results provide guidelines for selecting interphase properties and processing parameters to achieve desired overall composite characteristics. 相似文献
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通过分离式霍普金森压杆(SHPB)动态压缩试验研究了体积分数为45%的铝基碳化硅颗粒增强复合材料(SiCp/2024Al)在大应变率和变形温度范围内的热变形行为,分析了热变形参数(变形温度和应变率)对流动应力的影响。研究发现:变形温度和应变率对复合材料的流变应力、抗压强度、弹性模量、应变率敏感性有显著影响;抗压强度、弹性模量随变形温度的增大而减小,而抗压强度、弹性模量、应变率敏感性随应变率的增大出现了拐点。根据试验结果,结合热力学和统计损伤力学理论,建立了描述SiCp/2024Al复合材料动态热变形行为的连续损伤本构模型,预测的流动应力与试验结果吻合较好,表明所建立的模型能够准确地描述SiCp/2024Al复合材料动态热变形行为。 相似文献
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Localization of strain in metal matrix composites studied by a scanning electron microscope-based grating method 总被引:1,自引:0,他引:1
The deformation characteristics of the metal matrix composites Ag/Ni and Al/Al2 O3 are studied at microstructural level by a scanning electron microscope based grating method and finite element (FE) simulation. The measured strain was found to localize in narrow bands in the ductile matrix of both composites. In the case of the Al/Al2 O3 composite, the bands are preferentially initiated in Al regions adjacent to the interface of large Al2 O3 particles, leading to local strain maxima. The band positions found in the Ag/Ni composite are also affected by the less deformable Ni phase, but strain localization first occurs by sliding of single Ag grains sometimes located away from the Ni phase. Using a FE model of real phase geometry and measured border displacements as boundary conditions, the simulation agrees reasonably with the experiment. The differences in the case of the Al/Al2 O3 composite are due to particle cracks and voids at the particle/matrix interface. This effect was found in the experiment but not considered in modelling. For the Ag/Ni composite the band positions agree fairly well. However, the level and gradient of strain is clearly different as the crystallographic orientation of the Ag grains was not accounted for in modelling. 相似文献