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A new deformation theory with strain gradient effects

机译:具有应变梯度效应的新变形理论

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A new phenomenological deformation theory with strain gradient effects is proposed. This theory, which belongs to nonlinear elasticity, fits within the framework of general couple stress theory and involves a single material length scale l. In the present theory three rotational degrees of freedom omega(i) are introduced in addition to the conventional three translational degrees of freedom u(i). omega(i) has no direct dependence upon ui and is called the micro-rotation, i.e. the material rotation theta(i) plus the particle relative rotation. The strain energy density is assumed to only be a function of the strain tensor and the overall curvature tensor, which results in symmetric Cauchy stresses. Minimum potential principle is developed for the strain gradient deformation theory version. In the limit of vanishing 1, it reduces to the conventional counterparts: J(2) deformation theory. Equilibrium equations, constitutive relations and boundary conditions are given in details. Comparisons between the present theory and the theory proposed by Shizawa and Zbib (Shizawa, K., Zbib, H.M., 1999. A thermodynamical theory gradient elastoplasticity with dislocation density Censor: fundamentals. Int. J. Plast. 15, 899) are given. With the same hardening law as Fleck et al. (Fleck, N.A., Muller, G.H., Ashby, M.F., Hutchinson, JW., 1994 Strain gradient plasticity: theory and experiment. Acta Metall. Mater 42, 475), the new strain gradient deformation theory is used to investigate two typical examples, i.e. thin metallic wire torsion and ultra-thin metallic beam bend. The results are compared with those given by Fleck et al, 1994 and Stolken and Evans (Stolken, J.S., Evans, A.G., 1998. A microbend test method for measuring the plasticity length scale. Acta Mater. 46, 5109). In addition, it is explained for a unit cell that the overall curvature tensor produced by the overall rotation vector is the work conjugate of the overall couple stress tensor. (C) 2002 Elsevier Science Ltd. All rights reserved. [References: 34]
机译:提出了一种新的具有应变梯度效应的现象学变形理论。该理论属于非线性弹性,适合一般耦合应力理论的框架,涉及单个材料长度标度l。在本理论中,除了常规的三个平移自由度u(i)之外,还引入了三个旋转自由度omega(i)。 omega(i)与ui没有直接关系,被称为微旋转,即物质旋转theta(i)加上粒子相对旋转。假定应变能密度仅是应变张量和整体曲率张量的函数,这会导致对称的柯西应力。为应变梯度变形理论版本开发了最小势能原理。在消失的极限1中,它简化为传统的对应物:J(2)变形理论。详细给出了平衡方程,本构关系和边界条件。给出了本理论与Shizawa和Zbib提出的理论之间的比较(Shizawa,K.,Zbib,H.M.,1999.具有位错密度的热力学理论梯度弹塑性Censor:基本原理,Int.J.Plast.15,899)。具有与Fleck等人相同的硬化定律。 (Fleck,NA,Muller,GH,Ashby,MF,Hutchinson,JW。,1994应变梯度可塑性:理论与实验。金属学报,Mater 42,475),新的应变梯度变形理论用于研究两个典型的例子,即,细金属丝扭转和超薄金属束弯曲。将结果与Fleck等,1994和Stolken和Evans(Stolken,J.S.,Evans,A.G.,1998,一种用于测量可塑性长度尺度的微弯试验方法,Acta Mater.46,5109)给出的结果进行比较。另外,对于一个晶胞解释了,由整体旋转矢量产生的整体曲率张量是整体耦合应力张量的功共轭。 (C)2002 Elsevier ScienceLtd。保留所有权利。 [参考:34]

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