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GENERALIZATION OF ESHELBY'S METHOD TO THE ANISOTROPIC ELASTICITY THEORY OF DISLOCATIONS IN QUASICRYSTALS 下载免费PDF全文
The general expressions of the elastic fields induced by straight dislocations in quasicrystals have been given according to Eshelby's method which was used to treat the anisotropic elasticity of dislocations in crystals. As an example, the elastic displacement vector, the stress tensor and the elastic energy density of a screw dislocation line lying on the quasiperiodic plane of decagonal quasicrystals are calculated. 相似文献
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In this paper, some general variational principles in the theory of elasticity and the theory of plasticity are established. Consider an elastic body in equilibrium with small displacement. By regarding u, v, w, ex, ey, ez, yyz, yxz, yxy, σx,σy, σz,τyz,τxz,τxy as fifteen independent functions, and letting their variations be free from any restriction, we establish two variational principles, called the principle of generalized complementary energy and the principle of generalized potential energy. Each principle is equivalent to the four sets o?fundamental equations of the theory of elasticity, namely, the equations of equilibrium, the stress strain relations, the strain displacement relations and the appropriate boundary conditions. Special cases of these principles are examined. These principles are next expressed in other forms, where u, v, w, σx,σy, σz,τyz,τxz,τxy are regarded as nine independent functions with their variations free from any restrictions. Next we consider the bending of a thin elastic plate with supported edges under large deflection. By regarding Mx, My, Mxy, Nx, Ny, Nxy, u, v, w as nine independent functions with the restriction that w should vanish along the contour of the plate, we establish a variational principle, called the principle of generalized potential energy, which is equivalent to the three sets of fundamental equations in the theory of bending of thin plate, namely, the equations of equilibrium, the displacement stress relations (strain stress relations) and the appropriate boundary conditions. This principle is next expressed in another form which is more convenient for application. As an illustration, von Kármán's equations for the large deflection of thin plate are derived from this principle. In von Kármán's equations, one unknown is the deflection and the other unknown is the membrane stress function. Therefore it is impossible to derive von Karman's equations either from the principle of minimum potential energy or from the principle of complementary energy. Finally we consider the equilibrium of a plastic body with small displacement. In the case of the deformation type of stress strain relations, we establish two variational principles, each of which is equivalent to the equations of equilibrium, a certain type of stress strain relations and the appropriate boundary conditions. In these variational principles, u, v, w and their variations are free from any restriction, and σx,σy, σz,τyz,τxz,τxy and their variations satisfy a certain yield condition. In the case of the flow type of stress strain relations, we get two similar variational principles, in which u, v, w and their variations are free from any restriction, σx,σy, σz, τyz,τxz,τxy and their variations satisfy a certain yield condition and σx,σy, σz, τyz,τxz,τxy have no variations. 相似文献
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The Goldhaber theory is generalized to the case of nuclei consisting of many kinds of components. Our generalization gives a correction to the momentum widths for non-symmetric puclei, and possibly is useful in treating fission and heavy-ion reaction problems. 相似文献
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各向异性超导体的Ginzburg-Landau理论 总被引:3,自引:0,他引:3
本文内容主要有二个方面:1)由各各同性均匀系的BCS理论扩展到各向异性非均匀系,并给出各种异性非均匀系的完整的GL方程式,定出了各个宏微观参量间的关系式。2)结合层状结构氧化物超导体的导电层在导电层相间的特征等,用有效调制势模型和电子有效质量近似,交各向同性均匀系的BCS理论较具体的扩展到各向异性非均匀系并进行深化研究,扩展理论所给出的临界温度和能隙方程公式,主要的热力学性质和电磁性质公式等应用到YBaCuO超导体上,理论结果与实验结果均相符,并也给出各向异性非均匀系的完整的GL方程式,与上面1所给出的形式相同,也定出了各个宏微观参量间的关系,应用到YBaCuO超导体的一些主要性质上也与实验结果相符。 相似文献
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PLANE ELASTICITY PROBLEM OF TWO-DIMENSIONAL OCTAGONAL QUASICRYSTALS AND CRACK PROBLEM 总被引:1,自引:0,他引:1 下载免费PDF全文
The plane elasticity theory of two-dimensional octagonal quasicrystals is developed in this paper. The plane elasticity problem of quasicrystals is reduced to a single higher-order partial differential equation by introducing a displacement function. As an example, the exact analytic solution of a Mode I Griffith crack in the material is obtained by using the Fourier transform and dual integral equations theory, then the displacement and stress fields, stress intensity factor and strain energy release rate can be calculated. The physical significance of the results relative to the phason and the difference between the mechanical behaviours of the crack problem in crystals and quasicrystals are figured out. These provide important information for studying the deformation and fracture of the new solid phase. 相似文献
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提出由温差造成热剪切应力,引起衬底穿线位错滑移,形成<110>界面位错,从而降低LPE层中位错的模型。稳定自然对流下的温度梯度液相外延,存在衬底厚度方向的温差,能在边缘固定的衬底中造成热剪切应力。生长了厚GaAs和Ga1-xAlxAs层(x<0.3),估算的热剪切应力大于产生<110>暗线缺陷的临界剪切应力。表面腐蚀坑观察表明,外延层位错密度下降,或无位错。界面蚀槽和阴极荧光观察表明,衬底穿线位错在界面弯曲成<110>界面位错。透射电子显微镜观察表明,界面位错多
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本文把Misguich和Balescu建立的均匀等离子体湍流的重正化准线性理论推广到非均匀等离子体湍流。在弱耦合和弱非均匀性近似下,得到传播算符和平均湍性碰撞算符的明晰表达式。非均匀性除对算符中的扩散贡献、共振加宽或频移、Dupree衰减和平均分布函数在速度空间的陡度效应等作出一定的修正之外,还引出新的指数微分算符:在传播算符中是涨落电场关联函数非均匀性导致的新的速度微分算符,在平均湍性碰撞算符中是平均分布函数非均匀性导致的新的空间微分算符。平均分布函数非均匀性还使得在平均湍性碰撞算符中出现的两个互为逆运算的自由流传播算符不能抵消,从而使包含在(直接作用于平均分布函数的)传播算符中的非马尔可夫效应显露出来。
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The application of group theory to elasticity in two-dimensional (2D)quasicrystals is presented. The expression of elastic energy as a function of gradients of the phonon and phason fields has been derived to quadratic order. The phonon response to an external stress is isotropic, but the response of phason field is anisotropic for eightfold and twelvefold symmetries. 相似文献
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Bethe-Weiss方法是Bethe对合金有序现象所创建的近似理论被移植于铁磁性海森堡模型的统计理论的结果。在这方法中,我们选出由一个中心原子与它所有的最近邻原子所组成的集团作为处理的对象,它们之间的交换作用得到精确的对待,而集团以外的原子的作用就近似地用一有效场代替,后者由自洽条件来推。我们应用这一方法来计算由磁性原子(自旋为1/2)与非磁性原子组成的代换固溶体在较高温度段内的铁磁性,得出简单立方和体心立方晶格居里点Tc随非磁性原子浓度f的增加而下降的曲线,居里点以上的磁化率与磁矩的短程有序能与温度的关系。由后者看出,当f增加时,在有较高的短程有序的情况下才出现铁磁性。从居里点的计算中发现:这一方法只能应用在非磁性原子的浓度较低的情况,我们讨论了这一事实出现的原因。 相似文献
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本文将Misguich和Balescu的理论推广到非均匀等离子体的情形,导出了包括非均匀性效应的扩散方程与扩散张量的表式以及色散关系。指出Pelletier等人对等离子体湍流可作马尔科夫近似处理的论证完全不适用于非均匀等离子体湍流的问题。
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本文提出一个方法,来推求在(3)式中所定义的、在全空间中的格林张量函数。它有时亦称为对应微分方程的基本解。这个方法是以富氏变换为基础。由于问题的复杂性,我们不得不作某些近似。首先,把各向异性介质分为两类,一类是磁迴旋介质,另一类是电迴旋介质。对于磁迴旋介质,如铁氧体,取μ为张量而ε为标量。而对电迴旋介质,如等离子体,取ε为张量而μ为标量。其次,由于矩阵μp非常小(在(15)式中定义),我们可以把解展为μp的冪级数,并计算出一级近似。具体结果在式(23)、(25)、(28)、(32)和(33)中表示。最后对Г函数的物理意义和它的渐近展开式的有效范围作了讨论。 相似文献
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一.前言 早在1865年,圣维那便引进了球面各向同性(即在与一系列同心球面相切的各方向上的弹性是相同的)的概念,并在同文中解决了由这类弹性体构成的空心圆球在内外均布压力作用下的问题。但是由于球面各向同性体弹性力学基本方程的異常复杂性,之后研究这类问题的学者甚少。报作者所知,到现在还只 相似文献
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本文利用格林函数方法,对轴承的润滑问题进行了数值模拟。对圆柱形轴承及椭圆形轴承的润滑问题进行了计算,算例与精确值做了比较,精度较高。 相似文献
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本文从教学角度讨论了由狭义相对论的两条基本假设严格导出洛仑兹变换的问题,同时指出了某些流行的教材中处理这一内容时的不妥之处,并给出了解决方案. 相似文献