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241.
岩石力学性质及地应力等地质力学参数是进行储层压裂改造的基础数据,影响着整个压裂设计的准确性。由于页岩层理发育及矿物组成的复杂性、页岩力学性质的横观各向同性,所以基于传统力学模型获取的压裂参数设计将丧失意义。以横向各向同性模型体现层理发育页岩储层的力学性质,通过简化的横纵弹性模量和泊松比可以较好地表达出页岩的横观各向同性,并总结了横观各向同性地应力解释方法。基于上述理论,应用商业化水力压裂数模软件对四川盆地某层理页岩储层进行了压裂设计,比较了基于横观各向同性模型与传统模型解释力学参数差异,非常规储层动静态力学参数转换,同时通过改变射孔位置研究了起裂点对裂缝形态的影响。研究发现,横观各向同性解释的杨氏模量、地应力要略高于传统方法,同时横观各向同性解释的地层地应力差较小,所以受不同射孔位置的变化对裂缝几何的形态影响要远远高于各向同性模型模拟的结果,特别是缝高变化更为明显。同时数据表明,在高应力区射孔将形成更为狭窄缝宽的水力裂缝,这会严重影响后续支撑剂的进入,以上结论将为提高页岩储层的压裂设计精确性给予重要帮助。 相似文献
242.
Inversion for elastic parameters in weakly anisotropic media 总被引:1,自引:0,他引:1
Xuyao Zheng 《Geophysical Journal International》2004,159(3):1077-1089
243.
We have measured P- and S-wave velocities on two amphibolite and two gneiss samples from the Kola superdeep borehole as a function of pressure (up to 600 MPa) and temperature (up to 600 °C). The velocity measurements include compressional (Vp) and shear wave velocities (Vs1, Vs2) propagating in three orthogonal directions which were in general not parallel to inherent rock symmetry axes or planes. The measurements are accompanied by 3D-velocities calculations based on lattice preferred orientation (LPO) obtained by TOF (Time Of Flight) neutron diffraction analysis which allows the investigation of bulk volumes up to several cubic centimetres due to the high penetration depth of neutrons. The LPO-based numerical velocity calculations give important information on the different contribution of the various rock-forming minerals to bulk elastic anisotropy and on the relations of seismic anisotropy, shear wave splitting, and shear wave polarization to the structural reference frame (foliation and lineation). Comparison with measured velocities obtained for the three propagation directions that were not in accordance with the structural frame of the rocks (foliation and lineation) demonstrate that for shear waves propagating through anisotropic rocks the vibration directions are as important as the propagation directions. The study demonstrates that proper measurement of shear wave splitting by means of two orthogonal polarized sending and receiving shear wave transducers is only possible when their propagation and polarization directions are parallel and normal to foliation and lineation, respectively. 相似文献
244.
传统三维大地电磁各向异性模拟均是基于规则六面体网格,计算精度有限且较难拟合复杂地质条件.本文采用面向目标自适应非结构矢量有限元法,对三维大地电磁各向异性介质进行模拟.首先从电场双旋度方程出发,利用伽辽金方法建立变分方程;然后利用电流密度连续性条件构建适合大地电磁各向异性问题的加权后验误差估计方法,实现面向目标的网格自适应正演;最后通过典型算例分析各向异性对网格自适应和大地电磁响应的影响特征以及各向异性的识别方法.本文算法能够高精度地拟合起伏地表和任意各向异性介质,适用于分析复杂地电条件大地电磁响应特征,为提高大地电磁资料解释水平提供了理论基础.
相似文献245.
新丰江地震S波偏振的初步研究 总被引:2,自引:1,他引:2
根据新丰江地震台记录的 2 0 0 1年 2月 6日新丰江小震群数字化资料 ,分析计算了该震群的S波分裂的偏振参数。在与新丰江地区的最大主应力方向和构造、介质特性对比后 ,认为本文所得的S波偏振方向 (NW6 0°)与该区实际的活动断裂分布和主压应力轴方向 (NW6 0°)基本相同。作为该区地壳微裂隙的NW优势取向 ,是应力场作用下裂隙定向排列的结果。因此 ,S波偏振方向可作为研究介质各向异性和区域应力场特性的一种的参数 相似文献
246.
247.
The paper describes the development and numerical implementation of a constitutive relationship for modeling the elasto‐plastic behavior of block structures with periodic texture, regarded at a macroscopic scale as homogenized anisotropic media. The macroscopic model is shown to retain memory of the mechanical characteristics of the joints and of the shape of the blocks. The overall mechanical properties display anisotropy and singularities in the yield surface, arising from the discrete nature of the block structure and the geometrical arrangement of the units. The model is formulated in the framework of multi‐surface plasticity. It is implemented in an finite element (FE) code by means of two different algorithms: an implicit return mapping scheme and a minimization algorithm directly derived from the Haar–Karman principle. The model is validated against analytical and experimental results: the comparison between the homogenized continuum and the original block assembly shows a good agreement in terms of ultimate inelastic behavior, when the size of the block is small as compared with that of the whole assembly. Copyright © 2009 John Wiley & Sons, Ltd. 相似文献
248.
F. X. Hu G. X. Wu G. X. Song Q. R. Yuan S. Okamura 《Astrophysics and Space Science》2006,302(1-4):43-59
The progress of the studies on the orientation of galaxies in the Local Supercluster (LSC) is reviewed and a summary of recent
results is given. Following a brief introduction of the LSC, we describe the results of early studies based on two-dimensional
analysis, which were mostly not conclusive. We describe next the three-dimensional analysis, which is used widely today. Difficulties
and systematic effects are explained and the importance of selection effects is described. Then, results based on the new
method and modern databases are given, which are summarized as follows. When the LSC is seen as a whole, galaxy planes tend
to align perpendicular to the LSC plane with lenticulars showing the most pronounced tendency. Projections onto the LSC plane
of the spin vectors of Virgo cluster member galaxies, and to some extent, those of the total LSC galaxies, tend to point to
the Virgo cluster center. This tendency is more pronounced for lenticulars than for spirals. It is suggested that ‘field’
galaxies, i.e., those which do not belong to groups with more than three members, may be better objects than other galaxies
to probe the information at the early epoch of the LSC formation through the analysis of galaxy orientations. Field lenticulars
show a pronounced anisotropic distribution of spin vectors in the sense that they lay their spin vectors parallel to the LSC
plane while field spirals show an isotropic spin-vector distribution. 相似文献
249.
Shock-compressed MgO radiates thermally at temperatures between 2900 and 3700 K in the 170–200 GPa pressure range. A simple energy-transport model of the shocked-MgO-targets distinguishes between different shock-induced radiation sources in these targets and provides estimates of spectral absorption-coefficients, α ΛMgO , for shocked MgO (e.g. at 203 GPa, α ΛMgO ˜ 630, 7500, 4200 and 3800 m−1 , at 450, 600, 750 and 900 nm, respectively). The experimentally inferred temperatures of the shock-compressed states of MgO are consistent with temperatures calculated for MgO assuming that (1) it deforms as an elastic fluid, (2) has a Dulong-Petit value for specific heat at constant volume in its shocked state, and (3) undergoes no phase transformation below 200 GPa. 相似文献
250.