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901.
目的是探讨肺癌改变要注意观察其支气管改变,全面评价病灶部位,大小,形态及浸润范围。方法采用了螺旋CT薄层扫描(SVCT)后,再做增强CT扫描,然后对68例肺癌气管支气管进行分析研究,结果明确指出了68例病人均进行CT检查,其中54例经手术病理,支气管镜或细胞学检查证实,从而明确了螺旋CT是诊断支气管肺癌的重要方法之一,非常有益于临床方案的选择和设计。  相似文献   
902.
青藏高原库地北岩体地球化学特征及其地球动力学机制   总被引:1,自引:0,他引:1  
本文研究了位于青藏高原西北缘的库北岩体的地质,地球化学特征。研究表明,该岩体形成于奥陶纪末至泥盆纪初,由早期的二长花岗岩和晚期和花岗岩组成,成分上富碱,富K、Th、REE、Nb、Zr、Y,贫Ca、Mg、Ba、Sr、Sc、V、Ni具有A型花岗岩的特点,它形成于造山晚期相对稳定的拉张环境,是大洋板片脱过程中侵位的,由早先随大洋板块消减下沉的洋壳沉积物先后部分熔融而形成,。本次研究为地壳物质再循环至地壳  相似文献   
903.
蒙脱石酸处理产物的表面结构变化   总被引:7,自引:0,他引:7  
本文对广东和平蒙脱石及其酸处理产物进行了化学分析、X射线粉末衍射分析、红外吸收光谱分析、原子力显微镜及魔角旋转核磁共振等研究。结果表明,酸处理浓度对蒙脱石的表面结构有很大的影响。当酸处理浓度达到20%时,蒙脱石硅氧四面体中的Q^3Si环境发生结构重组,有部分转变为畸变的Q^3Si环境和Q4Si环境,而A1的结构状态则没有发生任何变化,这与原子力显微阄的观察结果相一致。  相似文献   
904.
东海陆架北部泥质区沉积动力过程的季节性变化   总被引:4,自引:0,他引:4  
利用东海陆架北部泥质区(济州岛西南)及其周围不同季节5个航次的悬浮体资料和相应的底质粒度资料,对该泥质区沉积动力过程的季节性变化规律进行了分析。结果表明:东海陆架北部悬浮体的高含量区并不与该区的沉积中心(泥质区)相吻合,泥质区的形成需有物源的充沛供应和涡旋的动力效应相结合。泥质区沉积作用时空变化具有强烈的季节性。冬季泥质区悬浮体供应充足,涡旋中心向泥质区东南扩展,是本区接受悬浮体沉积的关键季节。夏、秋二季泥质区的大部分区域缺少悬浮体物源,涡旋中心向北退缩,致使泥质区沉积作用强度降低,并且主要影响泥质区的西北区域。春季泥质区沉积作用强度和影响范围大于夏、秋两季,但小于冬季。  相似文献   
905.
从细菌、浮游植物、浮游动物、底栖动物和有机碎屑等几个方面分析了养鱼对伊乐藻种植区(以下简称为有草区)和无草区水域环境的影响。结果表明:两个区域存在着显著的差异性。有草区由于生长着茂密的水生植被,对环境压迫的缓冲能力增强,水生生物的群落结构较为稳定,物种多样性指数高于无草区,有机物的沉降速率也大大低于无草区。与此相比,无草区对环境压迫的缓冲能力较差,水体浮游植物数量增加,富营养化加剧。通过本项实验可以看出,人工种植伊乐藻对养鱼区水质有着明显地控制作用,是发展生态渔业的一条有效途径。  相似文献   
906.
测震台网数据传输补数技术   总被引:1,自引:1,他引:0  
针对测震台网波形数据传输中断导致丢数现象,开发测震台网自动补数系统SDARS,自动检测数据丢失现象,并从地震台数据采集器下载缺失数据;设计手动辅助补数工具软件SeisDataUtil,提供不同格式的地震数据文件的手动补数功能。通过此套补数系统,有效提高测震台网波形数据完整率,最小化减少波形数据丢失。  相似文献   
907.
STA/LTA—AIC算法对地震P波震相拾取稳定性影响   总被引:1,自引:1,他引:0  
选取区域地震台网记录的地震波形数据,使用STA/LTA算法与STA/LTA—AIC算法,进行地震P波震相初至到时自动拾取,对地方震及震中距较大的震相进行P波震相拾取效果分析,发现:STA/LTA算法对于地方震P波震相识别精度较高,与STA/LTA—AIC算法拾取的P波震相初至到时相差不大;震中距变大后,STA/LTA算法对P波拾取位置相对于最佳位置向后延迟,STA/LTA—AIC算法有效矫正了STA/LTA算法拾取位置的延迟问题,与人工拾取位置差别可忽略不计。  相似文献   
908.
The observation of extreme waves at FINO 1 during storm Britta on the 1st November 2006 has initiated a series of research studies regarding the mechanisms behind. The roles of stability and the presence of the open cell structures have been previously investigated but not conclusive. To improve our understanding of these processes, which are essential for a good forecast of similarly important events offshore, this study revisits the development of storm Britta using an atmospheric and wave coupled modeling system, wind and wave measurements from ten stations across the North Sea, cloud images and Synthetic Aperture Radar (SAR) data. It is found here that a standard state-of-the-art model is capable of capturing the important characteristics of a major storm like Britta, including the storm path, storm peak wind speed, the open cells, and peak significant wave height (H s ) for open sea. It was also demonstrated that the impact of the open cells has negligible contribution to the development of extreme H s observed at FINO 1. At the same time, stability alone is not sufficient in explaining the development of extreme H s . The controlling conditions for the development of Britta extreme H s observed at FINO 1 are the persistent strong winds and a long and undisturbed fetch over a long period.  相似文献   
909.
There exist different response characteristics in the resistivity measurements of dual laterolog (DLL) and logging while drilling (LWD) electromagnetic wave propagation logging in highly deviated and horizontal wells due to the difference in their measuring principles. In this study, we first use the integral equation method simulated the response characteristics of LWD resistivity and use the three dimensional finite element method (3D-FEM) simulated the response characteristics of DLL resistivity in horizontal wells, and then analyzed the response differences between the DLL and LWD resistivity. The comparative analysis indicated that the response differences may be caused by different factors such as differences in the angle of instrument inclination, anisotropy, formation interface, and mud intrusion. In the interface, the curves of the LWD resistivity become sharp with increases in the deviation while those of the DLL resistivity gradually become smooth. Both curves are affected by the anisotropy although the effect on DLL resistivity is lower than the LWD resistivity. These differences aid in providing a reasonable explanation in the horizontal well. However, this can also simultaneously lead to false results. At the end of the study, we explain the effects of the differences in the interpretation of the horizontal well based on the results and actual data analysis.  相似文献   
910.
The conventional acoustic logging interpretation method, which is based on vertical wells that penetrate isotropic formations, is not suitable for horizontal and deviated wells penetrating anisotropic formations. This unsuitability is because during horizontal and deviated well drilling, cuttings will splash on the well wall or fall into the borehole bottom and form a thin bed of cuttings. In addition, the high velocity layers at different depths and intrinsic anisotropy may affect acoustic logging measurements. In this study, we examine how these factors affect the acoustic wave slowness measured in horizontal and deviated wells that are surrounded by an anisotropic medium using numerical simulation. We use the staggered-grid finite difference method in time domain (FDTD) combined with hybrid-PML. First, we acquire the acoustic slowness using a simulated array logging system, and then, we analyze how various factors affect acoustic slowness measurements and the differences between the effects of these factors. The factors considered are high-velocity layers, thin beds of cuttings, dipping angle, formation thickness, and anisotropy. The simulation results show that these factors affect acoustic wave slowness measurements differently. We observe that when the wavelength is much smaller than the distance between the borehole wall and high velocity layer, the true slowness of the formation could be acquired. When the wavelengths are of the same order (i.e., in the near-field scenarios), the geometrical acoustics theory is no longer applicable. Furthermore, when a thin bed of cuttings exists at the bottom of the borehole, Fermat's principle is still applicable, and true slowness can be acquired. In anisotropic formations, the measured slowness changes with increments in the dipping angle. Finally, for a measurement system with specific spacing, the slowness of a thin target layer can be acquired when the distance covered by the logging tool is sufficiently long. Based on systematical simulations with different dipping angles and anisotropy in homogenous TI media, slowness estimation charts are established to quantitatively determine the slowness at any dipping angle and for any value of the anisotropic ratio. Synthetic examples with different acoustic logging tools and different elastic parameters demonstrate that the acoustic slowness estimation method can be conveniently applied to horizontal and deviated wells in TI formations with high accuracy.  相似文献   
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