Groundwater potential zones using a combination of geospatial technology and geophysical approach: case study in Dehradun,India

ABSTRACT

A combination of geospatial, geophysical and statistical models using satellite data, the weighted index overlay (WIO) method and two-dimensional electrical resistivity tomography (2D-ERT) is applied to generate the highest potential groundwater area and to further explore the groundwater in Dehradun, India. The results show that of 19.7 km² total basin area, 0.26% falls under the “poor” category as a prospect zone for groundwater, 4.3% is “moderate”, 10.10% “moderately good”, 4.9% “good” and 0.17% “very good”. In addition, the demonstration of the geophysical survey is presented, in which Purkal Youth Society Division (PYSD) site is categorized as a shallow aquifer zone and the Guru Nanak Fifth Centenary School (GNFCS) site is a deeper aquifer zone. Our study emphasizes remote sensing and geographic information system integrated with a geophysical survey to support prospecting the most probable area and confirm the existence of groundwater.     

骨旁脂肪瘤的影像学特征及诊断价值

目的:分析骨旁脂肪瘤的影像学表现特征,提高对该病的认识及术前影像诊断水平。方法:回顾性分析经病理证实的我院2例骨旁脂肪瘤的临床及影像学表现。结果:2例骨旁脂肪瘤,男女各1例,分别位于右侧股骨上段、左侧胫骨中下段骨旁软组织内。X线表现为骨旁软组织内的透光肿块;CT、MRI表现为骨旁脂肪密度或脂肪信号、有包膜的椭圆形分叶状肿块,边界清楚;邻近骨皮质形成突向肿瘤内部的珊瑚礁状或树枝状骨性突起。结论:骨旁椭圆形脂肪性肿块,伴有骨皮质突向肿块内的珊瑚礁状、树枝状骨性突起为骨旁脂肪瘤的影像学特征,具有重要的诊断价值。     

偏移速度分析与速度反演方法评述

本文阐述了各向同性介质中纵波偏移速度建模中的速度分析方法原理及其优缺点,包括常规速度分析、偏移速度分析、层析偏移速度分析以及全波形反演。其中着重阐述了深度域速度建模中的速度分析方法原理及其在实用中的优缺点。最后对深度域偏移速度分析方法进行了展望。     

安宁河-则木河断裂带及周边地区Rayleigh波群速度背景噪声成像研究

安宁河-则木河断裂带位于川滇地块、巴颜喀拉地块和华南地块的交接部位,是川滇菱形块体的东部重要边界。利用布设在安宁河-则木河断裂带周边区域的西昌台阵和川西台阵均历时两年、共187个宽频带地震台站的垂直分量的背景噪声数据,采用噪声层析成像方法获得了这一区域4~20s的Rayleigh波群速度分布图像。与前人研究相比,本文结果的横向分辨率有明显改进,在安宁河-则木河断裂带可达20km左右,在其它区域可以达到20~40km。成像结果表明,安宁河-则木河断裂地区上地壳的速度结构存在明显横向不均匀性,速度分布特征与地表地质构造基本一致,不同周期的速度分布变化较小。盐源盆地、西昌盆地和四川盆地西南缘表现为低速异常。九龙附近和南部的德昌-盐边-巧家附近表现为高速异常,分别与出露的花岗岩体和峨眉山玄武岩有关。在安宁河断裂南段和则木河断裂北段能观测到断裂两侧的速度存在明显差异,其余断裂带两侧的速度对比不明显。贡嘎山附近的中上地壳表现为明显的低速异常,其东侧和西南侧高速体的阻挡,以及鲜水河-安宁河断裂带走向的变化,在贡嘎山区形成一个挤压弯曲段,使得川滇菱形块体的东南向水平运动转换为垂直于断裂的挤压作用和垂直隆升,导致了贡嘎山的快速隆起。     

3D P-WAVE VELOCITY STRUCTURE AT THE NORTHEASTERN MARGIN OF ORDOS BLOCK

Using the 7 100 absolute first arrivals of P waves and 91 513 relative P arrival times of 726 events at the northeastern margin of the Ordos block since 2009, the 3D fine structure of P wave velocity within the depth of 15km in the crust was inverted by the double difference seismic tomography method. The results show that there exist obvious high-speed continuous bodies in the northwest of the study area, and their lateral areas increase gradually with depth, while the velocity of east and south is relatively low. The velocity inhomogeneity exists and differs at different depths. The lateral differences of velocity are related to seismicity and faults. The 5~15km depth profile shows that earthquakes tend to occur in the area with relatively high velocity or high speed transition zones, which to some extent reflects the fragility of regional crustal media and the strong differential movement of faults in vertical and horizontal directions where the crust body is easy to absorb and store strain energy and generate major earthquakes. A "Y"-shape low-velocity channel is present in the lower crust around Liangcheng, corresponding to the NW-trending Heilaoyao-Shahukou fault set, which may reveal the migration path of the Late Tertiary-Quaternary basalt eruption. The Helingeer M6.2 earthquake in 1976 was related to the formation of the locking section of the thermal welding in this area. The three-dimensional fine structure of P wave velocity presented in this paper provides intuitive seismological evidence for physical and chemical properties of crustal media and the deep tectonic environment of earthquake preparation.     

基于背景噪声研究青藏高原东北缘瑞利波相速度和方位各向异性

本研究收集了甘肃、青海、宁夏等118个宽频带数字地震台站的连续波形资料,利用噪声互相关,经过计算和筛选,在5~38 s范围内,共得到5773条瑞利波相速度频散曲线.然后采用1°×1°的网格划分,反演获得青藏高原东北缘相速度和方位各向异性分布.结果表明：短周期8~12 s内,鄂尔多斯从低速异常变为高速异常;该周期范围内各向异性结果与区域断裂走向有很好的一致性.18~25 s周期内,祁连地块、松潘-甘孜地块、羌塘地块低速异常范围逐渐变大,随周期增加地壳低速异常与人工探测结果相符;鄂尔多斯表现为速度随周期增加逐渐变大,说明其中下地壳速度相对偏高,不存在低速异常;该周期范围内的各向异性特征表现为,祁连地块和松潘甘孜地块大致呈NW-SE方向,而青藏高原内部快波方向显示了顺时针旋转的形态.在30~35 s范围内面波速度主要受莫霍面深度和莫霍面附近介质速度的影响,与地壳厚度分布有非常好的吻合.综合不同方法获得的各向异性研究结果,支持印度-欧亚板块的碰撞使青藏高原东北缘地壳发生缩短和逐渐隆升的观点,认为整个岩石圈的垂直缩短变形是青藏高原东北缘的主要形成机制.

     

医用CT仪上基于衰减的曝光量和峰值电压自动控制基本等式

为了给患者以最少的辐射剂量而不影响诊断,现行医用CT仪都有基于噪声指标的自动曝光量控制。峰值电压对于图像质量和辐射剂量影响都很大,因此自动峰值电压控制很重要。本文从图像质量和辐射剂量优化的第一原理出发,给出基于衰减的曝光量和峰值电压同时自动控制的一般等式。此等式可用于单独曝光量自动控制或者单独峰值电压自动控制。对于单独暴光量自动控制,此等式要求对患者体厚度毎增加一厘米,曝光量要增加3.8%。对于单独峰值电压自动控制,此等式要求对患者体厚度每增加一厘米,峰值电压要平均增加1.53%。如果患者体厚度是常数,此等式要求平均百分比曝光量增加是百分比峰值电压减少的2.49倍。这些等式应该可以在现行医用CT仪上用于曝光量和峰值电压的自动控制。     

双低技术在腹主动脉联合下肢动脉CTA中的可行性探讨

目的:比较腹主动脉联合下肢动脉CT成像中两种不同对比剂注射方案对对比剂剂量的影响。方法:搜集临床上怀疑腹主-下肢动脉疾病行CT血管成像(CTA)的患者50例,随机分为A、B组,对比剂(350 mg I/m L),A组:男16例,女9例,平均年龄(58.53±9.39)岁,平均体质量(67.86±11.65)kg,平均扫描范围(124.65±8.28)cm。B组:男17例,女8例,平均年龄(60.87±9.76)岁,平均体质量(66.23±12.42)kg,平均扫描范围(122.59±9.12)cm。A组注射流率4 m L/s,对比剂用量1.5 m L/kg。B组第1期5 m L/s注射20 m L,第2期3 m L/s注射剩余量;B组对比剂总量=1.5 m L/kg×体重-4 m L/s×(B方案对比剂注射时间-A方案对比剂注射时间)。对比剂注射完毕两组均以3 m L/s流率无缝隙注射生理盐水30 m L。两组均选择智能触发技术,监测平面为腹主动脉(右膈肌水平),阈值≥150 HU。对两组5个动脉段图像质量进行评分;测量5个动脉段CT值,记录两组对比剂剂量。均进行独立样本0.05)。A、B组对比剂剂量分别为(93.79±13.68)m L和(74.61±14.76)m L,差异有统计学意义(相似文献   

西太平洋俯冲板块对中国东北构造演化的影响及其动力学意义

中国东北地区在古生代期间以众多微陆块的拼合以及古亚洲洋的闭合为特征,其后又经历了中-新生代太平洋构造域及中生代蒙古-鄂霍茨克构造域的叠加与改造,以致东北地区的构造行迹显得极为复杂,而大兴安岭重力梯级带及其西部地区构造演化是否与西太平洋俯冲有关仍然存在争议.本研究利用分布于中国东北、华北地区以及韩国、日本等部分台网所接收的近震与远震走时数据获得了中国东北地区壳幔精细的三维P波速度结构.成像结果显示,太平洋板块持续西向俯冲,俯冲板片的前缘停滞在大兴安岭-太行山重力梯度带以东区域的地幔转换带之中;长白山火山区上地幔存在着显著的低速异常体,推测西太平洋板块的深俯冲脱水导致了上地幔底部岩石的熔点降低,从而形成了大范围的部分熔融物质上涌.通过分析上地幔的速度结构,我们认为由于太平洋板块的大规模西向深俯冲,在大地幔楔中发生板片脱水、低速热物质上涌等复杂的地球动力学过程;俯冲板片前缘带动上地幔中不均匀分布的地幔流强烈作用于上部的岩石圈,这对东北地区深部壳幔结构乃至大兴安岭重力梯级带的形成、演化有着重要的影响.

     

(ϖμ/ϖT) P of the lower mantle

We estimate (/T) _P of the lower mantle at seismic frequencies using two distinct approaches by combining ambient laboratory measurements on lower mantle minerals with seismic data. In the first approach, an upper bound is estimated for |(/T) _P | by comparing the shear modulus () profile of PREM with laboratory room-temperature data of extrapolated to high pressures. The second approach employs a seismic tomography constraint ( lnV _S / lnV _P ) _P =1.8–2, which directly relates (/T) _P with (K _S /T) _P . An average (K _S /T) _P can be obtained by comparing the well-established room-temperature compression data for lower mantle minerals with theK _S profile of PREM along several possible adiabats. Both (K _S /T) and (/T) depend on silicon content [or (Mg+Fe)/Sil of the model. For various compositions, the two approaches predict rather distinct (/T) _P vs. (K _S /T) _P curves, which intersect at a composition similar to pyrolite with (/T) _P =–0.02 to –0.035 and (K _S /T) _P =–0.015 to –0.020 GPa/K. The pure perovskite model, on the other hand, yields grossly inconsistent results using the two approaches. We conclude that both vertical and lateral variations in seismic velocities are consistent with variation due to pressure, temperature, and phase transformations of a uniform composition. Additional physical properties of a pyrolite lower mantle are further predicted. Lateral temperature variations are predicted to be about 100–250 K, and the ratio of ( lnp/ lnV _S ) _P around 0.13 and 0.26. All of these parameters increase slightly with depth if the ratio of ( lnV _S / lnV _P ) _P remains constant throughout the lower mantle. These predicted values are in excellent agreement with geodynamic analyses, in which the ratios ( ln / lnV _S ) _P and ( / lnV _S ) _P are free parameters arbitrarily adjusted to fit the tomography and geoid data.