三维正交各向异性孔隙介质震电波场数值模拟研究

各向异性等介质物性参数会对震电波场的传播产生影响.为了定量研究介质物性参数对震电波场传播的影响, 本文首先研究了三维正交各向异性介质的震电耦合方程, 然后采用时域有限差分方法模拟了爆炸源在该介质中的震电响应.在数值模拟中, 首先计算地震波场, 然后把地震波场作为输入来计算伴随电场.为了验证数值算法的精度, 我们将数值结果与从Pride方程获得的解析解进行了对比, 结果表明数值解可以很好地近似解析解.我们设计了几种各向异性模型, 分析了介质物性参数对震电波场的影响, 结果表明爆炸源在各向异性孔隙介质中会产生四种地震波, 分别是快慢纵波和两个可分离的横波.产生的地震波都会在均匀各向异性孔隙介质中产生伴随电场.弯曲度对慢纵波的传播有影响, 当弯曲度为各向异性时, 慢纵波的波场快照为椭圆形, 当弯曲度为各向同性时, 慢纵波的波场快照为圆形.

     

新疆和田地区维吾尔族JC病毒基因型的地理分布

对新疆和田地区7个县的主体民族维吾尔族的JC病毒IG区域基因型的地理分布状况进行了对比研究。从178个40岁以上的男性尿样提供者中分离出了JC病毒,并且对它们进行了DNA提取,对JC病毒IG区域进行了PCR扩增和DNA序列测定,得到了117人的JC病毒DNA IG区域的碱基序列。多态分析研究结果表明,117人中的基因型分别由B1-b,B1-c和EU组成,各基因型所占比率为:88.9%,3.4%和7.7%。研究发现,在各基因型中B1-b所占的比率高,其次是B1-c和EU基因型。通过NJ法进行了聚类分析法构建分子系统树,分析发现该人群JC病毒基因型中广泛分布于欧亚大陆中心的B1-b型占优势。这个结果与维吾尔族的祖先是公元前3世纪在中国北方蒙古高原生居过的丁零民族的后裔这个历史事实是一致的。     

Seismoelectric numerical simulation in 2D vertical transverse isotropic poroelastic medium

Seismoelectric coupling in an electric isotropic and elastic anisotropic medium is developed using a primary–secondary formulation. The anisotropy is of vertical transverse isotropic type and concerns only the poroelastic parameters. Based on our finite difference time domain algorithm, we solve the seismoelectric response to an explosive source. The seismic wavefields are computed as the primary field. The electric field is then obtained as a secondary field by solving the Poisson equation for the electric potential. To test our numerical algorithm, we compared our seismoelectric numerical results with analytical results obtained from Pride's equation. The comparison shows that the numerical solution gives a good approximation to the analytical solution. We then simulate the seismoelectric wavefields in different models. Simulated results show that four types of seismic waves are generated in anisotropic poroelastic medium. These are the fast and slow longitudinal waves and two separable transverse waves. All of these seismic waves generate coseismic electric fields in a homogenous anisotropic poroelastic medium. The tortuosity has an effect on the propagation of the slow longitudinal wave. The snapshot of the slow longitudinal wave has an oval shape when the tortuosity is anisotropic, whereas it has a circular shape when the tortuosity is isotropic. In terms of the Thomsen parameters, the radiation anisotropy of the fast longitudinal wave is more sensitive to the value of ε, while the radiation anisotropy of the transverse wave is more sensitive to the value of δ.