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    2012年 第33卷 第7期    刊出日期:2012-07-10
    论文
    Propagation of plane P-waves at interface between elastic solid and unsaturated poroelastic medium
    陈炜昀;夏唐代;陈伟;翟朝娇
    2012, 33(7):  829-844.  doi:10.1007/s10483-012-1589-6
    摘要 ( 958 )   PDF (2373KB) ( 1153 )  
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    A linear viscoporoelastic model is developed to describe the problem of reflection and transmission of an obliquely incident plane P-wave at the interface between an elastic solid and an unsaturated poroelastic medium, in which the solid matrix is filled with two weakly coupled fluids (liquid and gas). The expressions for the amplitude reflection coefficients and the amplitude transmission coefficients are derived by using the potential method. The present derivation is subsequently applied to study the energy conversions among the incident, reflected, and transmitted wave modes. It is found that the reflection and transmission coefficients in the forms of amplitude ratios and energy ratios are functions of the incident angle, the liquid saturation, the frequency of the incident wave, and the elastic constants of the upper and lower media. Numerical results are presented graphically. The effects of the incident angle, the frequency, and the liquid saturation on the amplitude and the energy reflection and transmission coefficients are discussed. It is verified that in the transmission process, there is no energy dissipation at the interface.
    Analysis of main shock of thrust fault earthquake by catastrophe theory
    潘岳;赵志刚
    2012, 33(7):  845-864.  doi:10.1007/s10483-012-1590-8
    摘要 ( 762 )   PDF (399KB) ( 827 )  
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    The relationship between work and energy increment of a thrust fault system with quasi-static deformation can be decomposed into two parts: volume strain energy and deviation stress energy. The relationship between work and energy increment of the deviation stress of a simplified thrust fault system is analyzed based on the catastrophe theory. The research indicates that the characteristics displayed by the fold catastrophe model can appropriately describe the condition of earthquake generation, the evolvement process of main shock of thrust fault earthquake, and some important aftershock properties. The bigger the surrounding press of surrounding rock is, the bigger the maximum principal stress is, the smaller the incidences of the potential thrust fault surface are, and the smaller the ratio between the tangential stiffness of surrounding rock and the slope is, which is at the inflexion point on the softened zone of the fault shearing strength curve. Thus, when earthquake occurrs, the larger the elastic energy releasing amount of surrounding rock is, the bigger the earthquake magnitude is, the larger the half distance of fault dislocation is, and the larger the displacement amplitude of end face of surrounding rock is. Fracturing and expanding the fault rock body and releasing the volume strain energy of surrounding rock during the earthquake can enhance the foregoing effects together.
    Bifurcation on synchronous full annular rub of rigid-rotor elastic-support system
    张华彪;陈予恕;李军
    2012, 33(7):  865-880.  doi:10.1007/s10483-012-1591-7
    摘要 ( 1091 )   PDF (410KB) ( 1075 )  
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    An aero-engine rotor system is simplified as an unsymmetrical-rigid-rotor with nonlinear-elastic-support based on its characteristics. Governing equations of the rubbing system, obtained from the Lagrange equation, are solved by the averaging method to find the bifurcation equations. Then, according to the two-dimensional constraint bi-furcation theory, transition sets and bifurcation diagrams of the system with and without rubbing are given to study the influence of system eccentricity and damping on the bi-furcation behaviors, respectively. Finally, according to the Lyapunov stability theory, the stability region of the steady-state rubbing solution, the boundary of static bifurcation, and the Hopf bifurcation are determined to discuss the influence of system parameters on the evolution of system motion. The results may provide some references for the designer in aero rotor systems.
    Integrated numerical model for vegetated surface and saturated subsurface flow interaction
    K. S. ERDURAN
    2012, 33(7):  881-898.  doi:10.1007/s10483-012-1592-9
    摘要 ( 813 )   PDF (3675KB) ( 796 )  
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    The construction of an integrated numerical model is presented in this paper to deal with the interactions between vegetated surface and saturated subsurface flows. A numerical model is built by integrating the previously developed quasi-three-dimensional (Q3D) vegetated surface flow model with a two-dimensional (2D) saturated groundwater flow model. The vegetated surface flow model is constructed by coupling the explicit finite volume solution of 2D shallow water equations (SWEs) with the implicit finite difference solution of Navier-Stokes equations (NSEs) for vertical velocity distribution. The subsurface model is based on the explicit finite volume solution of 2D saturated groundwater flow equations (SGFEs). The ground and vegetated surface water interaction is achieved by introducing source-sink terms into the continuity equations. Two solutions are tightly coupled in a single code. The integrated model is applied to four test cases, and the results are satisfactory.
    MHD flow and mass transfer of chemically reactive upper convected Maxwell fluid past porous surface
    K. VAJRAVELU;K. V. PRASAD;A. SUJATHA;吴朝安
    2012, 33(7):  899-910.  doi:10.1007/s10483-012-1593-8
    摘要 ( 684 )   PDF (298KB) ( 875 )  
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    The magnetohydrodynamic (MHD) flow and mass transfer of an electrically conducting upper convected Maxwell (UCM) fluid at a porous surface are studied in the presence of a chemically reactive species. The governing nonlinear partial differential equations along with the appropriate boundary conditions are transformed into nonlinear ordinary differential equations and numerically solved by the Keller-box method. The effects of various physical parameters on the flow and mass transfer characteristics are graphically presented and discussed. It is observed that the order of the chemical reaction is to increase the thickness of the diffusion boundary layer. Also, the mass transfer rate strongly depends on the Schmidt number and the reaction rate parameter. Furthermore, available results in the literature are obtained as a special case.

    Large-eddy simulation of fluid mixing in tee with sintered porous medium
    王永伟;卢涛;姜培学;成鹏飞;王奎升
    2012, 33(7):  911-922.  doi:10.1007/s10483-012-1594-9
    摘要 ( 728 )   PDF (1076KB) ( 1087 )  
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    Mixing processes of hot and cold fluids in a tee with and without sintered copper spheres are simulated by FLUENT using the large-eddy simulation (LES) turbulent flow model and the sub-grid scale (SGS) Smagorinsky-Lilly (SL) model with buoyancy. Comparisons of numerical results of the two cases with and without sintered copper spheres show that the porous medium significantly reduces velocity and temperature fluctuations because the porous medium can effectively restrict the fluid flow and enhance heat transfer. The porous medium obviously increases the pressure drop in the main duct. The porous medium reduces the power spectrum density (PSD) of temperature fluctuations in the frequency range from 1 Hz to 10 Hz.
    Similarity solutions to viscous flow and heat transfer of nanofluid over nonlinearly stretching sheet
    M. A. A. HAMAD;M. FERDOWS
    2012, 33(7):  923-930.  doi:10.1007/s10483-012-1595-7
    摘要 ( 1345 )   PDF (247KB) ( 2246 )  
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    The boundary-layer flow and heat transfer in a viscous fluid containing metallic nanoparticles over a nonlinear stretching sheet are analyzed. The stretching velocity is assumed to vary as a power function of the distance from the origin. The governing partial differential equation and auxiliary conditions are reduced to coupled nonlinear ordinary differential equations with the appropriate corresponding auxiliary conditions. The resulting nonlinear ordinary differential equations (ODEs) are solved numerically. The effects of various relevant parameters, namely, the Eckert number Ec, the solid volume fraction of the nanoparticles φ , and the nonlinear stretching parameter n are discussed. The comparison with published results is also presented. Different types of nanoparticles are studied. It is shown that the behavior of the fluid flow changes with the change of the nanoparticles type.

    Unsteady mixed convective heat transfer of two immiscible fluids confined between long vertical wavy wall and parallel flat wall
    J. C. UMAVATHI;I. C. LIU;M. SHEKAR
    2012, 33(7):  931-950.  doi:10.1007/s10483-012-1596-6
    摘要 ( 847 )   PDF (1061KB) ( 1145 )  
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    The combined effects of thermal and mass convection of viscous incom-pressible and immiscible fluids through a vertical wavy wall and a smooth flat wall are analyzed. The dimensionless governing equations are perturbed into a mean part (the zeroth-order) and a perturbed part (the first-order). The first-order quantities are ob-tained by the perturbation series expansion for short wavelength, in which the terms of the exponential order arise. The analytical expressions for the zeroth-order, the first-order, and the total solutions are obtained. The numerical computations are presented graph-ically to show the salient features of the fluid flow and the heat transfer characteristics. Separate solutions are matched at the interface by using suitable matching conditions. The shear stress and the Nusselt number are also analyzed for variations of the governing parameters. It is observed that the Grashof number, the viscosity ratio, the width ratio, and the conductivity ratio promote the velocity parallel to the flow direction. A reversal effect is observed for the velocity perpendicular to the flow direction.
    New simple exact penalty function for constrained minimization
    郑芳英;张连生
    2012, 33(7):  951-962.  doi:10.1007/s10483-012-1597-x
    摘要 ( 750 )   PDF (155KB) ( 712 )  
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    By adding one variable to the equality-or inequality-constrained minimization problems, a new simple penalty function is proposed. It is proved to be exact in the sense that under mild assumptions, the local minimizers of this penalty function are precisely the local minimizers of the original problem, when the penalty parameter is sufficiently large.
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