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141.
142.
本文研究半线性椭圆方程组在Ω中以及Dirichlet边界条件u|Ω=V|Ω=0的解的存在性.其中Ω是R~n中光滑有界开集。关于非线性项f(x,u)作超线性假设。在此假设下,若f满足增长限制|f(x,u)|≤a|u|°=b,其中a、b、σ是常数.1<σ<(n+2)/(n-2),则利用临界点方法.证明了(*)+b,其中a、b、σ是常数,1<σ<(n+2)/(n-2),则利用临界点方法.证明了(*)有古典解存存。这样不用对(*)的解作先验估计,解决了Figueiredo和Mitidieri在[2]提出的问题。 相似文献
143.
Pressure solution is a common phenomenon in massive sulphide zinc-lead deposits of western Canada and may have been an important factor leading to the mobilization of ore-forming materials during diagenesis, deformation and metamorphism of sedimentary ores.The control of ductile shear zones over gold mineralization could be explained in view of pressure solution of gold-bearing miner-als under shearing stress and the tesultant mobilization of this metal. 相似文献
144.
软岩巷道弹塑性变形的理论分析 总被引:16,自引:0,他引:16
本文采用莫尔-库仑屈服准则和非关联塑性流动法则分析了轴对称软岩巷道的变形规律。从轴对称平面应变问题的基本方程出发,导出了软岩巷道弹塑性变形的位移理论解答,并给出了现有应力与位移理论解的适用条件。通过实例计算结果表明,本文得出的位移理论解与有限元数值解相当吻合。 相似文献
145.
This paper is concerned with the thermodynamic theory of solution and precipitation processes in wet crustal rocks and with the mechanism of steady pressure-solution slip in contact zones, such as grain-to-grain contacts, fracture surfaces, and permeable gouge layers, that are infiltrated by a mobile aqueous solution phase. A local dissipation jump condition at the phase boundary is fundamental to identifying the thermodynamic force driving the solution and precipitation process and is used here in setting up linear phenomenological relations to model near-equilibrium phase transformation kinetics. The local thermodynamic equilibrium of a stressed pure solid in contact with its melt or solution phase is governed by Gibbs's relation, which is rederived here, in a manner emphasizing its independence of constitutive assumptions for the solid while neglecting surface tension and diffusion in the solid. Fluid-infiltrated contact zones, such as those formed by rough surfaces, cannot generally be in thermodynamic equilibrium, especially during an ongoing process of pressure-solution slip, and the existing equilibrium formulations are incorrect in overlooking dissipative processes tending to eliminate fluctuations in superficial free energies due to stress concentrations near asperities, defects, or impurities. Steady pressure-solution slip is likely to exhibit a nonlinear dependence of slip rate on shear stress and effective normal stress, due to a dependence of the contact-zone state on the latter. Given that this dependence is negligible within some range, linear relations for pressure-solution slip can be derived for the limiting cases of diffusion-controlled and interface-reaction-controlled rates. A criterion for rate control by one of these mechanisms is set by the magnitude of the dimensionless quantityk/2C
pD, wherek is the interfacial transfer coefficient, is the mean diffusion path length,C
p is the solubility at pressurep, andD is the mass diffusivity. 相似文献
146.
This paper represents a systematic investigation of slope evolution diffusion models and has the following sections: (1) The model of slope development with linear coefficient k = k0x; (2) The model of slope development with quadratic coefficient in x; (3) Slope development model with vertical lowering of base level (downcutting); (4) Slope development model with the base level a horizontal variable (undercutting); (5) Steady-state regime of undercut slopes; (6) Model of a pediment and scree slope formation. The comparison is made between mathematical and classical methods of slope evolution analysis. 相似文献
147.
Numerical solution of the scalar and elastic wave equations has greatly aided geophysicists in modeling seismic wave fields
in the complicated geologic structures containing hydrocarbons and hence increases the geologic interpretation. Finite-difference
method offers a versatile approach to compute synthetic seismograms numerically for given subsurface complex geological structures.
To avoid the spatial derivative of the elastic parameters and density, elastodynamic equation (first-order hyperbolic equation)
has been solved using the Lax-Wendroff scheme. A numerical finite-difference modeling program has been developed for the P-SV
wave using the above solution. A line source with a time delay of 0.015s and dominant frequency of 120 Hz has been utilized
in the simulation. In order to avoid the large values of the displacement vector in the source region,Alterman andKaral's method (1968) has been utilized. Horizontal and vertical component synthetic seismograms have been computed for two different
geological models with and without oil and gas bearing zones. It has been concluded from the response that a finite-difference
technique not only yields the relative arrival times but also accounts for the variation in amplitude and phase according
to the elastic impedance contrast across the interfaces. It should come as no surprise to learn that in spite of the limitation
of this numerical method, the scheme has provided a valid response for the thin layer, high acoustic impedance contrast and
the pinch out. 相似文献
148.
求震源机制P波初动解的格点尝试概率法 总被引:9,自引:0,他引:9
考虑到P波初动数据在震源球面上分布的不均匀性对节面解的可能影响,不用矛盾符号所占比例的大小作为选择可取节面解的标准,而是将震源球面分成许多小块,再确定有P波初动数字的小块为正号区或负号区的概率,最后以全部有数据小块的平均概率的高低作为选择解答的标准。用此改进方法重新测定了徐纪仁等(Xu et.al,,1988)发表的青藏高原地区99个地震的震源机制解,从中筛选出了20个可信的解答。 相似文献
149.
150.
Dionyssia-Pinelopi N. Kontoni Dimitri E. Beskos 《Soil Dynamics and Earthquake Engineering》1987,6(4):227-238
In this paper the applicability of an approximate Boundary Element Method to uniform half-plane elastodynamic problems is investigated. This method employs the concept of images to construct approximate fundamental solutions for the half-plane and does not require any half-plane surface discretization. The method is formulated in the frequency domain for the case of harmonic disturbances or the Laplace transform domain for the case of transient disturbances. In the latter case a numerical inversion of the transformed solution is necessary to obtain the time domain response. The proposed method can be used as an alternative to boundary element methods that either utilize the infinite plane fundamental solution and thus require a half-plane surface discretization, or employ the exact half-plane fundamental solution, which even though leads to no surface discretization, is of a very lengthy and complicated form. Two characteristics numerical examples are used to illustrate the proposed method and study its advantages and disadvantages. 相似文献