Improving gravity anomalies over China marginal sea from retracked Geosat and ERS-1 data

The quality of altimeter data and ocean tide model is critical to the recovery of coastal gravity anomalies. In this contribution, three retracking methods (threshold, improved threshold and Beta-5) are investigated with the aim of improving the altimeter data over a shallow water area. Comparison indicates that the improved threshold is the best retracking method over China Sea. Two ocean tide models, NAO99b and CSR4.0, are analyzed. Results show that different tide models used in the processing of altimeter data may result in differences more than 10 mGal in recovered coastal gravity anomalies. Also, NAO99b is more suitable than CSR4.0 over the shallow water area of China Sea. Finally, gravity anomalies over China Sea are calculated from retracked Geosat/GM and ERS-1/GM data by least squares collocation. Comparison with shipborne gravimetry data demonstrates that gravity anomalies from retracked data are significantly superior to those from non-retracked data. Our results have the same order as the other two altimeter-derived gravity models: Sandwell&Smith(V16) and DNSC08.     

TL-1本安型陀螺罗盘的设计与研究

本文叙述了 Ｔ Ｌ１ 本安型陀螺罗盘的陀螺马达选型及设计中的几个问题,介绍仪器样机的测试情况。测试结果表明,仪器性能稳定,陀螺方位角一次测量中误差≤±３０′,可以替代磁罗盘,进行低精度的定向测量。     

2019-05-26秘鲁北部地震前低纬电离层变化分析北大核心CSCD

针对2019-05-26秘鲁北部M W8.0地震,利用CODE-TEC数据和GPS-TEC实测数据,分析此次地震前上空电离层总电子含量和电离层赤道异常变化。利用地震前2019-05-10~26总电子含量格网数据分析震前电离层赤道异常变化和电离层TEC随地理纬度的异常变化;然后利用RIOP和GLPS站的GPS-TEC数据,统计分析地震前电离层TEC日变化异常。结果表明,地震发生前3 d,电离层赤道异常“双峰”消失,且电离层TEC含量显著减少,可达10 TECu左右。在地震发生前3 d 16:00~20:00 UT,电离层TEC随纬度变化呈现双峰曲线特征,震中附近存在低谷,且在该期间RIOP和GLPS站电离层TEC也出现显著减少现象。     

简化磁力计非线性误差模型的快速校正算法

针对传统的磁力计校正算法中存在的误差模型复杂、计算时间长、需要保持水平姿态和已知航向信息等弊端,该文从磁力计误差特性入手,推导并建立了简化的磁力计非线性等效误差模型。基于动态调整策略对传统的LM算法进行改进,并利用改进的LM算法求解误差模型,减少计算过程中的迭代次数,实现了磁力计误差的快速估计。实验表明,该方法在有效保证磁力计校正精度的前提下,迭代次数减少25%,计算速度提高了65.59%。     

惯性测量系统中垂线偏差和重力异常的确定

本文对惯性测量各项系统误差及异常重力场进行了分析和研究,并在此基础上建立了两种用于惯性重力测量的估算模型;模拟计算的结果表明,所建模型在原理上是可靠的,结果是令人满意的;同时,本文较为详细地分析了各项系统误差对异常重力元素估计精度的影响,对卡尔曼滤波应用中的有关问题进行了讨论。     

Ellipsoidal geoid computation

Modern geoid computation uses a global gravity model, such as EGM96, as a third component in a remove–restore process. The classical approach uses only two: the reference ellipsoid and a geometrical model representing the topography. The rationale for all three components is reviewed, drawing attention to the much smaller precision now needed when transforming residual gravity anomalies. It is shown that all ellipsoidal effects needed for geoid computation with millimetric accuracy are automatically included provided that the free air anomaly and geoid are calculated correctly from the global model. Both must be consistent with an ellipsoidal Earth and with the treatment of observed gravity data. Further ellipsoidal corrections are then negligible. Precise formulae are developed for the geoid height and the free air anomaly using a global gravity model, given as spherical harmonic coefficients. Although only linear in the anomalous potential, these formulae are otherwise exact for an ellipsoidal reference Earth—they involve closed analytical functions of the eccentricity (and the Earths spin rate), rather than a truncated power series in e². They are evaluated using EGM96 and give ellipsoidal corrections to the conventional free air anomaly ranging from –0.84 to +1.14 mGal, both extremes occurring in Tibet. The geoid error corresponding to these differences is dominated by longer wavelengths, so extrema occur elsewhere, rising to +766 mm south of India and falling to –594 mm over New Guinea. At short wavelengths, the difference between ellipsoidal corrections based only on EGM96 and those derived from detailed local gravity data for the North Sea geoid GEONZ97 has a standard deviation of only 3.3 mm. However, the long-wavelength components missed by the local computation reach 300 mm and have a significant slope. In Australia, for example, such a slope would amount to a 600-mm rise from Perth to Cairns.     

大型斑岩铜矿的遥感信息探讨

遥感影像解译的不同规模级别的线性构造、不同类型的环形构造和线-环组合类型以及色彩异常影像是寻找斑岩铜矿,特别是大型斑岩铜矿床最有用的遥感标志。1.砂岩铜矿的规模直接与不同规模不同级别的线性构造相联系区域性斑岩铜矿带直接受大型区域线性构造带和它们的汇聚格局控制,这种区域线性构造带多为区域压性壳断裂或超壳断裂,在遥感图像上常显示为浅色带,其长度超过100km,被称为主干边缘线性构造带(处于隆起单元向坳陷单元过渡部位,靠近隆起单元一侧).此外,一系列次级线性构造往往与主干边缘线性构造成一定角度相交,共同形成一种贯通性构造,在遥感图像上也常显示为浅色线;并直接控制斑岩铜矿田的分布和矿床的定位,被称为横向线性构造,长度一般1km-100km,主要包括三种类型(略),均显示张性特征。事实上,与斑岩铜矿有关的蚀变矿化直接受控于更低级别的线性构造(断裂和裂隙),它们常构成统一的环状和放射状断裂、裂隙系统。2.不同组合的多层环形影像是斑岩铜矿的不同呈矿环块构造的映像几乎所有的斑岩铜矿都与环块构造有关,特别是Ⅲ或Ⅳ级环块(直径50km-500km,包括环隆、环陷及褶皱-断裂环块等).它们控制了斑岩铜矿的定位。     

浑江市幅区域化探异常遥感评价筛选研究

本文介绍了根据国家计委和地矿部的要求,应用遥感地质方法,即主要通过航卫片解译,结合本区已有地质矿产分布和物化探资料的综合分析,对吉林省浑江市幅区域化探异常进行遥感评价、筛选研究的概况。文中主要阐述了区内金、多金属矿成矿地质特征,论述了断裂构造和环状构造与金、多金属矿及化探异常的关系,简介了区域化探异常遥感评价筛选和野外验证结果以及圈定的若干找矿靶区的情况。     

波段选择协同表达高光谱异常探测算法

高光谱遥感影像具有光谱分辨率极高的特点,承载了大量可区分不同类型地物的诊断性光谱信息以及区分亚类相似地物之间细微差别的光谱信息,在目标探测领域具有独特的优势。与此同时,高光谱遥感影像也带来了数据维数高、邻近波段之间存在大量冗余信息的问题,高维度的数据结构往往使得高光谱影像异常目标类和背景类之间的可分性降低。为了缓解上述问题,本文提出了一种基于波段选择的协同表达高光谱异常探测算法。首先,使用最优聚类框架对高光谱波段进行选择,获得一组波段子集来表示原有的全部波段,使得高光谱影像异常目标类与背景类之间的可分性增强。然后使用协同表达对影像上的像元进行重建,由于异常目标类和背景类之间的可分性增强,对异常目标像元进行协同表达时将会得到更大的残差,异常目标像元的输出值增大,可以更好地实现异常目标和背景类的分离。本文使用了3组高光谱影像数据进行异常目标探测实验,实验结果表明,该方法与其他现有高光谱异常目标探测算法对比,曲线下面积AUC(Area Under Curve)值更高,可以更好地实现异常目标与背景分离,能够更有效地对高光谱影像进行异常目标探测。     

利用多元回归分析反演西南印度洋区域海底地形

针对海底地形与重力异常和重力异常垂直梯度在相应频段呈现强线性相关的特点,引入多元回归分析技术,提出并详细推导了联合多元重力数据的海底地形建模方法。然后,在西南印度洋SWIR(Southwest India Ridge)所在部分海域开展了海底地形反演试验及地形地貌分析研究。试验结果表明:6种海深模型中,基于多元回归分析技术构建的海深模型(BDVG模型)检核精度最高,相较于S&S V18.1模型和ETOPO1模型精度分别提高了11.51%和57.81%左右;2000 m以上水深海域,各个海深模型的检核精度较高,相对误差波动较小,反映了深海海域具有良好的反演效果;地形起伏剧烈海域或者浅海海域,BDVG海深模型,相较于以重力异常和重力异常垂直梯度作为单一输入源建立的BDG模型和BVGG模型相对误差及相对误差波动变化较小,反映了BDVG模型拥有更好的稳定性,从而体现了联合反演的必要性和优势。Indomed FZ—Gallieni FZ上唯一轴部缺失裂谷洋脊段(27洋脊段)目前属于岩浆供应充足阶段,构造作用的海底扩张对其影响较小;同时由于对称裂离方式影响,27洋脊段沿轴南北对称分布有地形隆...