剪切带倾角尺度律与局部化启动跳跃稳定研究

研究了剪切带倾角是如何依赖于岩样高度以及剪切带的不稳定性。建立了准脆性材料试件剪切带倾角尺度效应模型,得到了剪切带倾角尺度效应的解析解,且与实验结果比较相符。研究结果表明:剪切带倾角随着试件高度的增加而增加,但其增加幅逐渐减缓,最终趋于稳定值。笔者还对剪应变局部化启动、跳跃和稳定进行了理论分析,解释了实验所观测到的剪切带跳跃现象和砂岩岩样应变局部化较煤样滞后的原因。剪应变局部化是否发生跳跃,关键取决于全程应力-应变曲线软化段是否存在拐点。对于没有拐点的情形,宏观剪切带图案不跳跃。局部化是导致准脆性材料试件剪切带倾角尺度效应的原因。     

Estimation Of Sensible Heat Flux From The Surface Temperature Wave And One-Time-Of-Day Air Temperature Observation, Part Ii – Heterogeneous Surfaces

By means of the algorithm presented in Part I of this study, the temporal course H(t) and the daily mean H of the sensible heat flux H can be determined from measurements of the thermodynamic surface temperature (as a function of time) and from a one-time-of-day air temperature observation. Inaddition to these temperatures, one needs estimates of daily mean wind speed,of the roughness lengths of momentum and heat transfer, and of the displacementheight. In Part I, the algorithm was derived for areas with homogeneous surfaces,i.e., with uniform surface temperature, and the method was verified with measurements taken during several field campaigns. The root mean square error for the temperature difference between surface and air, in the comparison between measurement and model, amounted to one or two kelvin, and the error of H was 10 to 25 per cent. The method can be used to determine the sensible heat flux from measurements of surface temperatures by satellites, but can also be applied to ground based measurements.In Part II, the procedure is generalized for areas that consist of various surface types (sub-regions) with different surface temperatures, and can be usedwhen only a few (at least one) air temperature measurements per day are available over only one of the different sub-regions. This generalization should allow improvements to the estimates for H(t) by means of temperature measurements from, e.g., NOAA/AVHRR or LANDSAT/TM, taking into account the heterogeneity of the area contained in one METEOSAT pixel. Criteria are given as to whether effective (areal mean) surface temperatures and roughness lengths may be used for the computation of H or if the above mentioned generalized procedure has to be applied. The new algorithm is verified by measurements sampled during the field campaigns EFEDA 91 (Spain) and HIBE 89 (Hildesheimer Börde in Germany), and by using synthetic data (due to the lack of measured data) for one further combined surfacetype [soil and water (lakes)].     

长白山天池火山区电性结构和岩浆系统

在长白山火山区及其附近 ,沿 5条伞状测线和 1条北西向测线进行了 6 1个大地电磁测深点的观测。用Robust等方法对观测资料进行了处理 ;应用阻抗张量分解方法消除了局部不均匀体的影响 ;计算了反映地下横向不均匀性的地磁感应矢量。利用RRI二维自动反演等技术对资料进行了解释。结果表明 :在近地表存在低阻体 ,并分别与长白山天池水体、聚龙泉温泉、锦江温泉及长白山山门附近的地下水相对应。在长白山天池及其以北和以东地区 ,约 12km深处存在电阻率很低的地质体 ,电阻率为 10到几十Ω·m ,可能是地壳岩浆囊。在测区范围内 ,地壳电性结构在南北方向存在着明显的横向变化 ,而东西方向相对均匀 ,变化比较平缓     

景泰5.9级地震后大地电磁跟踪监测研究

介绍了2000年6月6日景泰Ms5.9地震后，在该区进行的大地电磁跟踪监测结果。在监测时段内所观测的视电阻率随时间没有大的变化，在观测误差范围内有较好的可重复性。据此判定震后一段时间内发生较大地震的可能性不大。判定结果与实际情况相符。     

亚洲中东部岩石圈塑性流动网络与构造应力场

:板块边缘驱动作用主要通过岩石圈下层的网络状塑性流动实现其向板内的远程传递 ,并控制上层的构造变形。相应地造成构造应力场的的多层分布格局 ,主要包括下层 (含下地壳和岩石圈地幔 )、多震层 (属于上部地壳 )和浅层 (浅表地壳 )应力场。这些层中最大压应力方向可分别采用塑性流动网络共轭角平分线、震源机制解和井孔应力测量等方法加以确定。根据对亚洲中—东部下层与多震层应力场的对比表明 ,大部分地区二者的应力方向基本一致 ,表明了下层对上层的控制 ,这对了解板内应力场的一般趋势与格架提供了基础。靠近驱动边界的局部地段 ,由于上部地壳直接的传递作用 ,往往导致上、下层应力方向的显著偏差 ,有可能成为进一步了解深浅层联系和差异的一种方法     

储层岩石表面接触角的不确定性研究

本文指出，储层岩石表面粗糙，非均质性及高的能量，使我们难以用接触角来量度它的润湿性质，由于储层岩石孔隙结构不符合毛管束模型，使得Laplace公式仅在表现接触角趋于2度或180度时可用于根据毛管压力曲线计算储层岩石的孔径分布，好在由于储层岩石表面粗糙使我们常常会遇到这一极端情况。     

电偶源频率电磁测深视电阻率多参量联合反演效果检验

通过大量的数值模拟试验 ,对电偶源频率电磁测深 (FEMS)视电阻率多参量联合反演的效果进行了检验和对比 .结果表明 ,多参量联合反演具有较快的收敛速度和较高的拟合精度     

The relationships between earthquakes and positions of the sun and moon（Ⅱ）——Sometemporalcharacteristicsoftheaftershocksequencesofstrongearthquakes

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用Autolisp绘制高精度坐标方格网

通过对AutoCAD填充图案ANSI37的巧用,来完成任意图幅、任意转角的高精度坐标方格网的绘制,同时完成网格线的标注,内图廓、外图廓及图签的绘制,为机助制图提供了一种高精度、快速绘制坐标方格网的好方法。