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1.
The aim of this paper is to study the spatial and temporal behavior of thermoelastodynamic processes for microstretch continuum materials. The spatial behavior is described by establishing estimates of Saint–Venant type and Phragmén–Lindelöf type for bounded and unbounded bodies, respectively, with decay rate being dependent or independent of time, while the temporal behavior is studied by establishing the relations describing the asymptotic behavior of the Cesàro means of the different parts of the total energy. 相似文献
2.
The extension of the classical mixture theory by the concept of volume fractions leads to the theory of porous media. In this article, the theory of porous media is generalised to micropolar constituents. The kinematic relations and the balance equations for a porous medium are developed without restricting the number of constituents. Based on the entropy inequality, the general form of the constitutive equations are derived for a binary medium consisting of a porous elastic skeleton saturated by a viscous pore-fluid. Both constituents are assumed to be compressible. Handling the saturation constraint by a Lagrangian multiplier leads to a compatibility of the proposed model to so-called hybrid and incompressible models. 相似文献
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This paper is concerned with the linear theory of thermoelastic materials with voids. We present a method to reduce the thermoelastic problem to an isothermal one with zero body loads and with certain known boundary data. The results are used to study the thermal stresses in a tube and the thermoelastic deformation of a cylinder subjected to a uniform temperature gradient. 相似文献
5.
In Part I macroscopic field equations of mass, linear and angular momentum, energy, and the quasistatic form of Maxwell's equations for a multiphase, multicomponent medium were derived. Here we exploit the entropy inequality to obtain restrictions on constitutive relations at the macroscale for a 2-phase, multiple-constituent, polarizable mixture of fluids and solids. Specific emphasis is placed on charged porous media in the presence of electrolytes. The governing equations for the stress tensors of each phase, flow of the fluid through a deforming medium, and diffusion of constituents through such a medium are derived. The results have applications in swelling clays (smectites), biopolymers, biological membranes, pulsed electrophoresis, chromotography, drug delivery, and other swelling systems. 相似文献
6.
We establish the local symmetry group of the dynamically and kinematically exact theory of elastic shells. The group consists of an ordered triple of tensors which make the shell strain energy density invariant under change of the reference placement. Definitions of the fluid shell, the solid shell, and the membrane shell are introduced in terms of members of the symmetry group. Within solid shells we discuss in more detail the isotropic, hemitropic, and orthotropic shells and corresponding invariant properties of the strain energy density. For the physically linear shells, when the density becomes a quadratic function of the shell strain and bending tensors, reduced representations of the density are established for orthotropic, cubic-symmetric, and isotropic shells. The reduced representations contain much less independent material constants to be found from experiments. 相似文献
7.
In the present paper the linear theory of the liquid-saturated porous medium consisting of a microscopically incompressible solid skeleton containing microscopically incompressible liquid is considered. The fundamental solution of the system of linear coupled partial differential equations of the steady oscillations of the porous solids is constructed in terms of elementary functions and some basic properties are established. 相似文献
8.
A thermo-chemo-electro-mechanical formulation of quasi-static finite deformation of swelling incompressible porous media is derived from a mixture theory including the volume fraction concept. The model consists of an electrically charged porous solid saturated with an ionic solution. Incompressible deformation is assumed. The mixture as a whole is assumed locally electroneutral. Different constituents following different kinematic paths are defined: solid, fluid, anions, cations and neutral solutes. Balance laws are derived for each constituent and for the mixture as a whole. A Lagrangian form of the second law of thermodynamics for incompressible porous media is used to derive the constitutive restrictions of the medium. The material properties are shown to be contained in one strain energy function and a matrix of frictional tensors. A principle of reversibility results from the constitutive restrictions. Existing theories of swelling media should be evaluated with respect to this principle. 相似文献
9.
The linearized equations for saturated elastic porous media and for surrounding elastic rock are solved simultaneously; and the Volterra principle is used to derive an integro-differential filtration equation for a homogeneous weakly compressible fluid in an axisymmetric stratum with linear memory and central well. An analytical expression for porosity variation is obtained and then used to determine the permeability coefficient. The solutions are analyzed for the case where the stratum exhibits memory described by regular and singular kernels of the integral operator 相似文献
10.
Merab Svanadze 《Journal of Elasticity》2008,92(2):195-207
In this paper some basic properties of wave numbers of the longitudinal and transverse plane waves are treated. The existence
theorems of eigenfrequencies of the interior homogeneous boundary-value problems of steady oscillations of binary mixtures
for thermoelastic solids are proved. The connection between plane waves and eigenfrequencies is established.
This paper dedicated to my teacher Professor Mikheil Basheleishvili on the occasion of his 80th birthday. 相似文献
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This paper is concerned with the linear dynamic theory of elastic materials with voids. First, a spatial decay estimate of an energetic measure associated with a dynamical process is established. Then, a domain of dependence inequality associated with a boundary-initial-value problem is derived and a domain of influence theorem is established. It is shown that, for a finite time, a solution corresponding to data of bounded support vanishes outside a bounded domain. 相似文献
13.
对有限变形下线弹性Ⅰ型裂纹场建立了无需分区的统一控制方程并进行了渐近分析, 利用“打靶法”得到位移场在物质描述与空间描述下的渐近阶次分别为3/4和1,Green应变、第二类P-K应力及Cauchy应力在物质描述与空间描述下的渐近阶次分数为-1/2和-2/3;对不同泊松比,裂尖有限变形线弹性场的位移均以UⅡ或u2为主导,裂纹张开角为π,现时构形中的大变形区为一垂直初始构形中裂纹表面的狭长带状区,应力则处于由σ22主导的单向拉伸状态,角分布函数U^-Ⅱ(0)及σ22^-(0)具有奇异性,但UL^-‘(Θ)/UⅡ^-‘(0)及σij^-(θ)/σ22^-(0)均趋于有限值。 相似文献
14.
T.C.T. Ting 《Journal of Elasticity》1998,53(1):47-64
Antman and Negron-Marrero [1] have shown the remarkable nature of a sphere of nonlinear elastic material subjected to a uniform
pressure at the surface of the sphere. When the applied pressure exceeds a critical value the stress at the center r=0 of the sphere is infinite. Instead of nonlinear elastic material, we consider in this paper a spherically uniform linear anisotropic elastic material. It means that the stress-strain law referred to a spherical coordinate system is the same for any material point.
We show that the same remarkable nature appears here. What distinguishes the present case from that considered in [1] is that
the existence of the infinite stress at r=0 is independent of the magnitude of the applied traction σ0 at the surface of the sphere. It depends only on one nondimensional
material parameter κ. For a certain range of κ a cavitation (if σ0>0) or a blackhole (if σ0<0) occurs at the center of the sphere. What is more remarkable is that, even though the deformation is radially symmetric,
the material at any point need not be transversely isotropic with the radial direction being the axis of symmetry as assumed
in [1]. We show that the material can be triclinic, i.e., it need not possess a plane of material symmetry. Triclinic materials that have as few as two independent elastic
constants are presented. Also presented are conditions for the materials that are capable of a radially symmetric deformation
to possess one or more symmetry planes.
This revised version was published online in August 2006 with corrections to the Cover Date. 相似文献
15.
Stabilities of supersonic jets are examined with different velocities, momentum thicknesses, and core temperatures. Amplification rates of instability waves at inlet are evaluated by linear stability theory (LST). It is found that increased velocity and core temperature would increase amplification rates substantially and such influence varies for different azimuthal wavenumbers. The most unstable modes in thin momentum thickness cases usually have higher frequencies and azimuthal wavenumbers. Mode switching is observed for low azimuthal wavenumbers, but it appears merely in high velocity cases. In addition, the results provided by linear parabolized stability equations show that the mean-flow divergence affects the spatial evolution of instability waves greatly. The most amplified instability waves globally are sometimes found to be different from that given by LST. 相似文献
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H. Altenbach 《International Applied Mechanics》2003,39(6):631-655
A historical review of achievements in creep theory is given. Primary attention is focused on the phenomenological approach. Different constitutive equations are discussed for primary and secondary creep as well as for creep with damage. New creep problems are examined 相似文献
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A ‘classical’ theory of beams (i.e., a theory in which the basic kinetic variables are a stress resultant and a stress couple)
undergoing elastic, thermodynamic processes is developed by first deriving exact beamlike (one-dimensional) equations of motion
and a beamlike Second Law (Clausius–Duhem inequality) by descent from three-dimensions. Then what may be considered as the
three basic assumptions of a classical theory are introduced: an assumed form of the First Law (conservation of energy), a
relaxed form of the Second Law, and a general form of the constitutive relations. Throughout, detailed specification of geometry,
kinematics, or constitution is minimized. It is shown how the kinematic Kirchhoff hypothesis may be avoided by first introducing
a mixed-energy density and then imposing a logically more satisfying constitutive Kirchhoff hypothesis.
Mathematics Subject Classifications (2000) 74A15, 74B20, 74K10 相似文献
19.
A modified boundary integral equation method is used to solve a specific type of mixed boundary value problem in an enhanced theory of bending of elastic plates in which the effects of transverse shear deformation and transverse normal strain are taken into account. The problem considered is characterized by the fact that a combination of transverse displacement and bending and twisting moments is prescribed on the curve which bounds the middle surface of the plate. Both interior and exterior problems are formulated and the corresponding existence and uniqueness results derived. 相似文献
20.
Petri Jussila 《Transport in Porous Media》2006,62(1):81-107
A general thermomechanical model is derived for a mixture. The model describes the behavior of the mixture via proper choices
of free energy and dissipation function. A model for any combination of the mixture constituents can be reduced from the general
model. The theory is applied to a thermohydraulic model for a mixture of compacted bentonite, liquid water, vapor, and air
with the assumption of rigid skeleton and constant uniform porosity. The free energy of the system is chosen to take into
account the individual nondissipative behaviors of the constituents and their mutual interactions, namely, adsorption and
mixing of the gaseous constituents. The choices for the interaction terms are based on the equilibrium conditions for the
water species in different combinations of the constituents. The resulting thermodynamically consistent macroscopic model
is fitted to a suction experiment and applied to a simple one-dimensional thermohydraulic simulation of the bentonite buffer
of the Febex in situ test. The results calculated with finite element method are successfully compared to measurements. 相似文献