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1.
广义能量耗散弹性理论(TEWED,G-NⅢ理论)广泛应用于均匀磁场作用下的时谐平面波在无限大的理想导电弹性体中传播的研究.提出了更普遍的有复杂参数的色散方程,通过运用Ieguerre 方法解决复杂条件下耦合磁-热-弹性波的问题,表明耦合磁-热-弹性波问题相当于改进的膨胀波及通过有限热波速度、热弹性耦合、热扩散率及外加磁场修正的、有限速度热波的传播问题.在G-NⅢ模型(TEWED)中,耦合磁-热-弹性波传播时发生衰减和色散,扩散的热量由热传播方程中的阻尼项考虑,而在G-N Ⅱ模型没有发生衰减和耗散.最后给出了类铜材料的数值结果.  相似文献   

2.
The problem of the multiple scattering of plane harmonic wavesin an infinite elastic solid by arbitrary configurations oftwo-dimensional obstacles is considered. Sets of integral equationsrelating the multiple scattering functions to the single scatteringfunctions are derived. The integral equations are replaced bya set of algebraic equations which are then solved by an iterativeprocedure. Some results are given for the scattering of a planeharmonic P or SV wave by an identical pair of parallel circularcylindrical cavities.  相似文献   

3.
三维弹性固体中冲击波传输方程的Lagrange描述   总被引:1,自引:1,他引:0  
在Lagrange坐标中导出了三维非线性弹性固体中冲击波幅度在任意传播方向上的传输方程.导出的方程说明,冲击波的幅度在任意传播方向上随时间的变化率依赖于(i)冲击波阵面紧后方介质运动的一个未知量;(ii)冲击波阵面的两个主曲率;(iii)冲击波法向波速在阵面内的表面梯度;(iv)和冲击波前方介质运动有关的非齐次项,当前方介质处于均匀运动状态时此项为零.文中指出了适当选择传播矢量以简化传输方程的几种方法.我们还得到了一组与介质本构方程无关的、联系冲击波各跳跃量变化率的普适关系.  相似文献   

4.
The propagation of infinitesimal surface waves on a half-spaceof incompressible isotropic elastic material subject to a generalpure homogeneous pre-strain is considered. The secular equationfor propagation along a principal axis of the pre-strain isobtained for a general strain-energy function, and conditionswhich ensure stability of the underlying pre-strain are derived.The influence of the pre-stress on the existence of surfacewaves is examined and, in particular, it is found that, undera certain range of hydrostatic pre-stress, a unique wavespeedexists and is bounded above by a limiting speed which correspondsto the shear wave speed in an infinite body. The secular equationis analysed in detail for particular deformations and, for anumber of specific forms of strain-energy function, numericalresults are used to illustrate the dependence of the wave speedon the pre-strain. Particular attention is focused on pre-strainscorresponding to loss of stability, in which case the infinitesimalstrain is time-independent (the wave speed being zero). Thetheory described here encompasses previous work on surface wavesand instabilities in incompressible isotropic elastic materialsand provides a clear delimitation of the range of deformationsfor which surface waves exist.  相似文献   

5.
讨论了平面波入射在弹性固体(介质(M))和电-微拉伸广义热弹性固体(介质M)的界面上时,波的反射和透射问题.介质M中存在5种反射波(纵向位移(LD)波、热(T)波、纵向微拉伸(LM)波和2种横向耦合位移和微转动波(CD(Ⅰ)和CD(Ⅱ)波));介质(M)中存在2种透射波(纵(P)波和横(SV)波).得到不完全边界上不同反射波和透射波的振幅比,并导出法向力刚度、切向力刚度和完全粘接时的振幅比.对LD波和CD(Ⅰ)波,图示出振幅比随不同入射角的变化.显示出反射波和透射波的振幅比受到介质的刚度、电场、拉伸和热特性的影响.推演出一些有价值的特例.  相似文献   

6.
该文研究带有压电驱动器的Rayleigh梁系统的精确能控性.先用算子半群方法和提升结果[9]建立了Rayleigh梁方程解的正则性;再用Hilbert唯一性方法结合Diophantine逼近理论的某些结果得到了系统的精确L2-能控性.  相似文献   

7.
在充满两种互不相溶粘性流体的多孔固体中,研究弹性波的传播.用3个数性的势函数描述3个纵波的传播,用1个矢性的势函数单独描述横波的传播.根据这些势函数,在不同的组合相中,定义出质点的位移.可以看出,可能存在3个纵波和1个横波.在一个弹性固体半空间与一个充满两种互不相溶粘性流体的多孔固体半空间之间,研究其界面上入射纵波和横波所引起的反射和折射现象.由于孔隙流体中有粘性,折射到多孔介质中的波,朝垂直界面方向偏离.将入射波引起的反射波和折射波的波幅比,作为非奇异的线性代数方程组计算.进一步通过这些波幅比,计算出各个被离散波在入射波能量中所占的份额.通过一个特殊的数值模型,计算出波幅比和能量比系数随入射角的变化.超过SV波的临界入射角,反射波P将不再出现.越过界面的能量守恒原理得到了验证.绘出了图形并对不同孔隙饱和度以及频率的变化,讨论它们对能量分配的影响.  相似文献   

8.
We derive and analyze asymptotic equations for the interaction of weakly nonlinear elastic waves. We show that there are resonant triads involving two transverse and one longitudinal wave provided the wave speeds satisfy a certain irrationality condition. We study initial value and signaling problems, and the interaction of sawtooth wave packets.  相似文献   

9.
In the classical theory of water waves only irrotational motions are considered. In the present paper a class of wave problems associated with inviscid rotational motions is examined and the consequences explored.  相似文献   

10.
11.
Functional Analysis and Its Applications - In this note we discuss some recent results on extreme steady waves under gravity. They include the existence and regularity theorems for highest waves on...  相似文献   

12.
Growing finite-amplitude initially spanwise-independent two-dimensional rotational waves and their nonlinear interaction with unidirectional viscous shear flows of various strengths are considered. Both primary and secondary instabilities are studied, but only secondary instabilities are permitted to vary in the spanwise direction. A generalized Lagrangian-mean formulation is employed to describe wave-mean interactions, and a separate theory is constructed to account for the back effect of the developing mean flow on the wave field. Viscosity is seen to significantly complicate calculation of the back effect. The primary instability is seen to act as a platform for, and catalyst to, secondary instabilities. The analysis leads to an eigenvalue problem for the initial growth of the secondary instability, this being a generalization of the eigenvalue problem constructed by Craik for inviscid neutral waves. Two inviscid secondary instability mechanisms to longitudinal vortex form are observed: the first has as its basis the Craik–Leibovich type 2 mechanism. The second, which is as yet unproven, requires that both the wave and flow field distort in concert at all levels of shear. Both mechanisms excite exponential growth on a convective rather than diffusive scale in the presence of neutral waves, but growing waves alter that growth rate.  相似文献   

13.
理想弹塑性I型平面应力裂纹线场的精确解   总被引:2,自引:0,他引:2  
本文纠正了过去在裂纹弹塑性场匹配上存在的问题,采用线场分析方法,通过求得塑性区应力场的合理解答,使之与弹性精确场在裂纹线附近的弹塑性边界上匹配。本文就远场受单向拉伸及双向拉伸的理想弹塑性平面应力裂纹无限板,在完全放弃了小范围屈服条件的情况下求得了塑性区应力场、塑性区长度以及弹塑性边界的单位法向量在裂纹线附近足够精确的表达式。结果表明,无论单向拉伸和双向拉伸,塑性区应力分量σyxy,塑性区长度以及弹塑性边界的单位法向量在裂纹线附近的表达式完全相同,但塑性区沿X方向的正应力σx存在差别。  相似文献   

14.
The nonstationary propagation of waves on the surface of an elastic half space from a deep expansion source (model of an explosion in a half space) is examined. Exact solutions are obtained in the form of integrals with finite limits and the general solution is calculated. Algebraic expressions are obtained for the Rayleigh wave. The transition of Rayleigh waves at the surface of the half space is studied. Calculations of Rayleigh waves from discontinuous pulsed sources are presented.  相似文献   

15.
This paper is concerned with nonlinear analysis for the propagation of Rayleigh surface waves on a homogeneous, elastic half‐space of general anisotropy. We show how to derive an asymptotic equation for the displacement by applying the second‐order elasticity theory. The evolution equation obtained is a nonlocal generalization of Burgers' equation, for which an explicit stability condition is exhibited. Finally, we investigate examples of interest, namely, isotropic materials, Ogden's materials, compressible Mooney–Rivlin materials, compressible neo‐Hookean materials, Simpson–Spector materials, St Venant–Kirchhoff materials, and Hadamard–Green materials.  相似文献   

16.
在松散结合的弹性固体和微极多孔立方晶体半空间之间的界面上,研究周期平面波的反射和透射,假定界面性质类似于断层,断层上的牵引力保持连续,但允许产生有限的滑移.用图形给出各种反射波和透射波的振幅比.文中还演绎出某些重要的特殊情况.  相似文献   

17.
Expressions are obtained in closed form for the transient stressin a homogeneous isotropic elastic half-space whose surfaceis subjected to a constant uniform pressure over a circle whoseradius increases in proportion to the square root of time. Thepositions of the wave fronts are derived, together with themagnitudes of the discontinuities of the stress components acrossthem. It is shown that a Rayleigh surface wave appears at themoment when the radius of the area under load is increasingwith the Rayleigh wave-speed. The behaviour of the stress andstrain is described in the region of the stress singularityat its leading edge.  相似文献   

18.
饱和土中弹性波的传播速度   总被引:2,自引:0,他引:2  
根据所建立的波动方程分析了饱和土中弹性波的弥散特性,并且用室内超声波和现场地震波试验结果进行验证.本文为由弹性波(尤其是P波)速度测得合理的饱和土物理力学参数提供了理论依据.  相似文献   

19.
The problem discussed in this paper concerns a rigid axi-symmetricbody of convex form embedded in an infinite isotropic elasticsolid. When the inclusion is set in motion by an impulsive torqueapplied about the axis of symmetry it executes a damped torsionaloscillation and generates a shear pulse in the surrounding elasticmaterial. A representation of the elastic wave field in theform of a progressing wave expansion is shown to lead to anintegral equation of Volterra type for the angular motion ofthe inclusion. The exact solution obtained by Chadwick &Trowbridge (1967) for the case of a spherical inclusion is thenre-derived and used in developing an approximate method of solutionof the more general problem described above. Detailed resultsare worked out for spheroidal inclusions of oblate and prolateforms and numerical results are presented and discussed.  相似文献   

20.
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