论文标题
具有极端散装和剪切模量的平面多晶
Planar polycrystals with extremal bulk and shear moduli
论文作者
论文摘要
在这里,我们考虑了由单个晶体在各种方向上建造的平面多晶的散装和剪切模量。先前的工作给出了与正性对称性的晶体的完整表征。具体而言,边界分别衍生在有效的散装和剪切模量上,从而将有效模量限制在(散装,剪切平面的矩形内)。已经确定,该矩形中的每个点都可以通过适当的层次层压层次的微观测定法实现,并且晶体在层中采取不同的方向,而层本身则处于不同的方向。边界很容易扩展到没有特殊对称性的晶体,但是构造微地球形的途径可以实现由边界定义的矩形中每个点的小地球化学。我们表明,层次层压板总是实现具有最小散装模量的盒子的两个角落。对于其他两个角落,我们提出了用于产生层次层压的算法,从而实现了它们。数值证据强烈表明,始终达到具有最大散装和最大剪切模量的角。对于剩余的角落,具有最大的散装模量和最小剪切模量,尚不清楚该算法是否总是成功,因此是否始终达到矩形中的所有点。我们使用的微观结构是分层层压层的几何形状,其核心具有自相似的微观结构,从某种意义上说,一个长度尺度上的微观结构是在较小的长度尺度上的旋转和重新缩放。
Here we consider the possible bulk and shear moduli of planar polycrystals built from a single crystal in various orientations. Previous work gave a complete characterization for crystals with orthotropic symmetry. Specifically, bounds were derived separately on the effective bulk and shear moduli, thus confining the effective moduli to lie within a rectangle in the (bulk, shear) plane. It was established that every point in this rectangle could be realized by an appropriate hierarchical laminate microgeometry, with the crystal taking different orientations in the layers, and the layers themselves being in different orientations. The bounds are easily extended to crystals with no special symmetry, but the path to constructing microgeometries that achieve every point in the rectangle defined by the bounds is considerably more difficult. We show that the two corners of the box having minimum bulk modulus are always attained by hierarchical laminates. For the other two corners we present algorithms for generating hierarchical laminates that attain them. Numerical evidence strongly suggests that the corner having maximum bulk and maximum shear modulus is always attained. For the remaining corner, with maximum bulk modulus and minimum shear modulus, it is not yet clear whether the algorithm always succeeds, and hence whether all points in the rectangle are always attained. The microstructures we use are hierarchical laminate geometries that at their core have a self-similar microstructure, in the sense that the microstructure on one length scale is a rotation and rescaling of that on a smaller length scale.