层状地基任意形状刚性基础动力响应求解

提出了基于积分变换、对偶方程与精细积分算法求解多层地基任意形状刚性基础的动力刚度问题. 首先在频率波数域内圆柱坐标体系中利用圆形微元的对称与反对称特性建立多层地基中格林影响函数的波动方程,然后将应力和位移关系表示成对偶形式进行精细积分求解以提高计算精度和稳定性. 再将任意形状刚性基础与地基的交界面离散化为一系列圆形微元,利用格林影响函数建立其平动与转动动力刚度的矩阵方程. 该求解方法高效、准确并且计算稳定,适于任意复杂多层地基任意形状基础动力刚度的计算.      

地下结构地震响应的计算模型

地震时地下结构在围岩的约束作用下发生变形,其动态特性与地面结构有很大不同.自二十世纪七八十年代以来,地下结构抗震设计与研究取得了很大进展.总的看来,工程设计中普遍采用的计算方法与设计导则大都建立在比较简单假定的基础上,实际的岩土介质条件都是十分复杂的.地下结构抗震研究的近期成果则表现在对地下结构动力分析中的波动散射问题提出了波函数展开法以及边界积分方程方法等多种计算方法.但计算相对复杂,在工程设计中的推广应用有一定困难.此文致力于地下结构计算模型的改进,使之具有良好的计算精度与效率,又便于工程应用.为此,提出了一种地下结构抗震响应分析的新的计算模型.模型具有较广泛的适应性,可以进行河谷、孔洞、地下铁道、隧洞等地下结构的散射与绕射分析.对于复杂层状的地质条件,提出了格林函数求解简便而有效的方法.数值算例论证了方法的精度和效率.     

Positive Toeplitz Operators Between the Harmonic Bergman Spaces

On the setting of the upper half space we study positive Toeplitz operators between the harmonic Bergman spaces. We give characterizations of bounded and compact positive Toeplitz operators taking a harmonic Bergman space b ^p into another b ^q for 1<p<, 1<q<. The case p=1 or q=1 seems more intriguing and is left open for further investigation. Also, we give criteria for positive Toeplitz operators acting on b ² to be in the Schatten classes. Some applications are also included.     

HALF-SPACE GREENS'S FUNCTION DUE TO A SPATIALLY HARMONIC LINE LOAD AND SCATTERED FIELDS IN THE FAR FIELD REGION

Half-space Green's function due to a spatially harmonic line load has been expressed asa sum of the full-space Green's functions and a 2-D integral representation of the reflected waves bythe free surface of the half-space.By using the obtained half-space Green's function,an integral rep-resentation of the scattered waves by a cylindrical obstacle is then derived.Finally,by analyzing thefar-zone behavior of the integrands of the integral representation.the far-field pattern of the scatteredwaves in a half-space obtained.     

Harmonic Bergman functions as radial derivatives of Bergman functions

In the setting of the half-space of the euclidean -space, we show that every harmonic Bergman function is the radial derivative of a Bergman function with an appropriate norm bound.

     

The axisymmetric lamb’s problem for a finite prestrained half-space covered with a finite prestretched layer

The piecewise-homogeneous body model and the three-dimensional linearized theory of elastic waves in prestressed bodies are used to solve the axisymmetric time-harmonic Lamb’s problem for a finite prestrained half-space covered with a finite prestretched layer. It is assumed that the half-space and layer are incompressible and their deformation is described by the Treloar potential. The normal stress at the interface is calculated Published in Prikladnaya Mekhanika, Vol. 43, No. 3, pp. 132–143, March 2007.     

黏弹性半空间体内部作用水平力时的理论分析

研究假定半无限体为线性黏弹性介质,土体在内部水平集中力作用下的应力球张量和应变球张量之间符合弹性关系,而应力偏张量和应变偏张量之间符合三参数固体黏弹性应力应变关系.利用半空间体内部受水平向集中力的Mindlin弹性理论解,根据弹性--弹黏性相应原理,系统推导了水平集中力作用在半无限体内部时的应力与位移分量的黏弹性解.通过对应力与位移分量在拉氏域内的解答进行Laplace逆变换,给出了应力与位移分量的时域解.作为黏弹性解答的应用,基于上述解答给出了水平向均布荷栽下作用在半空间体内部时的黏弹性位移计算公式,并编制了便于工程应用的计算程序.结果验证与深埋锚板的算例分析表明,本文的理论解答对实际工程具有一定的理论及应用价值.     

Interaction of Several Dies on an Elastic Half-Space

A contact problem is solved for several rigid dies on an elastic half-space. Relationships between the generalized loads and generalized displacements of a large number of spaced dies are established. The interaction between flat-based dies is described in terms of their capacity characteristics. The general solution is constructed on the basis of Mossakovski's theorem. Explicit formulas are derived for a system of elliptic dies     

竖向力作用在粘弹性土体内部时的解答与应用

选择三参量固体模型描述土体的粘弹性本构关系,利用半空间体内部受竖向集中力的Mindlin弹性解,根据粘弹性理论中的准静态弹性-弹粘性对应原理,推导了竖向力作用在粘弹性半无限土体内部的理论解。通过对应力和位移解答进行Laplace逆变换,给出了应力与位移的时域解。作为解答的应用,建立了粘弹性半无限体内部矩形面积上作用有三角形分布、均匀分布荷载时的粘弹性沉降计算公式。为了便于计算与工程应用,根据粘弹性理论解编制了计算程序。结果验证和实例分析表明,文中理论解是正确的,并为工程实际应用提供了理论依据。     

Stress solutions to the three-dimensional problem of elasticity

New representations of the stress tensor in the linear theory of elasticity and thermoelasticity are proposed. These representations satisfy the equilibrium equations and the strain compatibility equation. The stress tensor is expressed in terms of a harmonic tensor or a harmonic vector. The second boundary-value problem for an elastic half-space and an elastic layer is solved as an example __________ Translated from Prikladnaya Mekhanika, Vol. 42, No. 8, pp. 3–35, August 2006.