A STUDY OF B-P UNIFIED VISCOPLASTIC CONSTITUTIVE MODEL

By combining the Bodner-Partom constitutive model and equivalent stress function, finite element methods and program on analyzing non-elastic deformation and stress for thermal viscoplastic material are studied in this paper, and it's the first time that this material model is used in a kind of engineering software-MARC. Thermal viscoplastic behavior of high temperature alloy GH536 specimen with gap is analyzed by this program. The research results show it is feasible to analyze thermal viscoplastic behavior of specimen or structure by applying B-P model.     

模具型腔加工参数的优化问题

首先阐述了在CAD CAM集成环境下编制数控加工工艺的过程以及优化加工参数的必要性 ,接着 ,分析了需要优化的加工参数。文章详细阐述了优化模型的建立和算法设计问题     

CVD金刚石膜{100}取向在改进化学反应模型下生长的原子尺度模拟

建立了CVD金刚石膜{100}取向生长过程中的化学反应模型，表面吸附生长机制以沟槽处碳氢组元加入的机制为主，并用改进的KMC方法在原子尺度上模拟了该模型下（100）表面的生长过程，给出了衬底温度和甲基浓度等操作参数对膜质量的影响，结果表明，该化学反应模型能够较实际地揭示{100}取向CVD金刚石膜的生长。     

异形坯连铸坯壳应力与鼓肚变形分析

坯壳应力引起的鼓肚变形是影响铸坯质量的重要因素,为防止过大的鼓肚变形,依据湍动能理论、热流传递理论和粘弹性理论,建立了异形坯三维热-力耦合模型,开发了鼓肚分析软件,从而避免了漏钢事故的发生.该模型将温度场和应力场的计算相互耦合,交替进行.结果表明:异形坯截面最危险点位于腹板中部,其次为翼板中点,在两者相结合的圆角部,由于凝固坯壳比较薄,其应力值也比较大;当坯壳厚度小于20 mm时,两点的鼓肚变形量将分别超过其极限变形量,铸坯出结晶器时必然发生漏钢事故.该模型通过预测坯壳应力和鼓肚变形量为现场安全生产提供了理论依据.     

单道自动对接焊应变应力场分析

通过给出模拟单道自动对接焊过程的数学模型，用有元法计算瞬时应变场和应力场并与实测值进行比较，结果证实计算值与实测值基本吻合，表明用数学模拟自动对接焊过程是可行的。     

气缸低速运动摩擦力模型的研究

对气缸摩擦力进行了全面和深入的分析，通过仿真模拟和实验拟合，提出了符合气缸低速运动摩擦特性的模型——指数函数模型。结果表明，采用该摩擦力模型，气缸运动的仿真模型精度更高，能够更好地描述气缸低速运动过程，对于气缸优化设计和气缸正常使用具有参考价值。     

铝合金时效-屈服强度的实验与模型化研究

以析出热力学、长大动力学及位错理论为基础，研究了铝合金在时效过程中盘／片状、棒／针状析出相尺寸、体积分数对时效合金强化效果的影响，从微观-宏观相结合的角度建立了具有盘／片状、棒／针状细小时效强化相铝合金的时效工艺-屈服强度量化模型，并通过513K温度下时效Al-Cu-Mg合金和463K温度下时效Al-Mg-Si合金的实验结果对模型进行了验证，取得了较满意的吻合结果，并对本模型的模拟精度与时效析出相参数之间的关系进行了讨论。     

激光焊接的模拟仿真研究

分析和总结了激光焊接仿真的研究现状，综述了模拟仿真过程中固液气之间的传热对流模型、激光和金属相互作用模型，激光在等离子体内的传播模型，以及材料热物理性能参数，金属材料的状态方程等问题的处理方法，并且列举了目前的成果，提出了未来研究的发展方向。     

Application of a time-dependent constitutive model to rheocast systems

A mathematical model has been developed to describe the velocity field in an agitated Al- 5Cu alloy in which B4C particles were suspended at different loading rates of up to 40 %. The material system was agitated by means of an electromagnetic rotary stirrer. The non- Newtonian behavior of the melt/solid slurry was allowed for using two models: the steady- state model of Joly and Flemings and the model of Brown, which takes account of time- dependent behavior. Calculations have shown that the two models behave similarly at high shear rates. In addition, if agitation was discontinued, very little time was required for the velocity (and hence the fluidity) of the slurry to decay.     

First-principles calculation of phase equilibria and phase separation of the Fe-Ni alloy system

Theoretical investigation of the phase equilibria of the Fe-Ni alloy has been performed by combining the FLAPW total energy calculations and the Cluster Variation Method through the Cluster Expansion Method. The calculations have proved the stabilization of the LIE phase at 1：3 stoichiometry, which is in agreement with the experimental result, and predicted the existence of L1 0 as a stable phase below 550 K; this L1 0 phase has been missing in the conventional phase diagram. The calculations are extended to the Fe-rich region that is characterized by a wide range phase separation and has drawn considerable attention because of the intriguing Invar property associated with a Fe concentration of 65%. To reveal the origin of the phase separation, a P-V curve in an entire concentration range is derived by the second derivative of free energy functional of the disordered phase with respect to the volume. The calculation confirmed that the phase separation is caused by the breakdown of the mechanical-stability criterion. The newly calculated phase separation line combined with the L1 0 and L12Eorder-disordered phase boundaries provides phase equilibria in the wider concentration range of the system. Furthermore, a coefficient of thermal expansion （CTE） is attempted by incorporating the thermal vibration effect through harmonic approximation of the Debye-Gruneisen model. The Invar behavior has been reproduced, and the origin of this anomalous volume change has been discussed.