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    空间模式的广义自相似性分析与矿产资源评价

    成秋明

    成秋明, 2004. 空间模式的广义自相似性分析与矿产资源评价. 地球科学, 29(6): 733-743.
    引用本文: 成秋明, 2004. 空间模式的广义自相似性分析与矿产资源评价. 地球科学, 29(6): 733-743.
    CHENG Qiu-ming, 2004. Quantifying the Generalized Self-Similarity of Spatial Patterns for Mineral Resource Assessment. Earth Science, 29(6): 733-743.
    Citation: CHENG Qiu-ming, 2004. Quantifying the Generalized Self-Similarity of Spatial Patterns for Mineral Resource Assessment. Earth Science, 29(6): 733-743.

    空间模式的广义自相似性分析与矿产资源评价

    基金项目: 

    国家科技司“863”项目“非线性空间信息获取” 2002AA135090

    安大略矿产勘查计划 OMET

    自然科学和工程基金会 NSERC

    详细信息
      作者简介:

      成秋明(1960-), 男, 教授, 1994年毕业于加拿大渥太华大学, 获博士学位, 主要从事矿产与勘探、数学地质、地理信息系统、矿产资源与环境评价的教学和研究.E-mail: qiuming@yorku.ca

    • 中图分类号: P628

    Quantifying the Generalized Self-Similarity of Spatial Patterns for Mineral Resource Assessment

    • 摘要: 尺度不变性(scaleinvariance) 包括自相似性(各向同性)、自仿射性(成层结构)、广义自相似性(各向异性标度不变性), 是由各种地质过程和地质事件所产生的地质特征和模式的本质属性.尺度不变性可用分形和多重分形模型来表征.这些尺度特征的定量化可为刻画地质空间模式和模式识别提供有力的工具.例如, 热液矿床的群聚现象可以用局部分形特征(局部奇异性) 来刻画.通过在特征空间中(如频率空间) 识别空间模式的广义自相似性, 可以将空间混合模式进行分解或异常的识别.介绍了几种相关的分形模型和方法, 包括度量空间模式广义尺度独立性(GSI) 的线性模型; 基于广义尺度独立性的异常分解S-A方法; 度量空间模式的局部奇异性方法; 以及如何利用分形特征预测未发现矿床的2种方法.有些方法已应用于许多矿产资源评价实例中.给出了对加拿大Nova Scotia省西南部湖泊沉积物样品中的4种元素As、Pb、Zn和Cu的地球化学数据处理分析结果, 证明了局部奇异性分析和S-A异常分解方法对地球化学异常的增强和分离的有效性.研究表明: 由S-A方法分解的异常往往具有多重分形的特点, 而且普遍具有局部奇异性.研究区内具有明显奇异性的地区(元素含量富集区) 是金矿异常区域, 它们与金矿成矿作用和已知矿床的赋存密切相关.

       

    • 图  1  加拿大Nova Scotia省西南部地区地质简图和已知矿床分布(Chatterjee, 1983)

      Fig.  1.  Simplified geology and distribution of known mineral deposits in southwestern Nova Scotia, Canada

      图  2  加拿大Nova Scotia省西南部地区湖泊沉积物地球化学取样点分布(N=1 948)

      (数据来自加拿大Nova Scotia省能源部矿产资源处)

      Fig.  2.  Location of the lake sediment geochemical samples (N=1 948), southwestern Nova Scotia, Canada

      图  3  砷的奇异性指数α值分布

      圆点表示金矿床, 多边形表示SMB和早期和晚期的花岗岩相

      Fig.  3.  Estimated singularity values (α) for As

      图  4  在GeoDAS GSI (Cheng, 2000b) 软件中使用快速傅立叶变换(FFT) 计算所得的能谱密度分布(图的中心处波数为0)

      Fig.  4.  Power energy spectrum calculated using fast Fourier transform (FFT) implemented in GeoDAS GSI (Cheng, 2000b). The center of the map is where wave number equals zero. It is a two-dimensional function of wave numbers in horizontal and vertical axes

      图  5  能谱密度-面积(S-A) 双对数图

      本结果由GeoDAS软件(Cheng, 2000b) 计算所得.在能谱密度的3个区间(-125 284), (125 284-178 129)和(178 129-) 上使用最小二乘法拟合直线段.这3条直线段的斜率分别为-1.966, -2.85, -1.17, 截距分别为26.6, 36.9和16.6.以125 284为阀值定义2个滤波器: 异常滤波器, S < 125 284;背景滤波器, S > 125 284

      Fig.  5.  S-A plot showing relationship between power energy spectrum S and A (> S) on log-log paper

      图  6  图 5中所定义的背景滤波器滤波并经傅立叶逆变换得到的砷背景分布

      图中圆点表示金矿床(点), 暗色图案表示As高背景区

      Fig.  6.  Background component decomposed from the As power spectrum density map using inverse Fourier transform with background filter as defined in

      图  7  图 5中所定义的异常滤波器滤波并经傅立叶逆变换所得到的砷异常

      图中圆点表示金矿床, 暗色图案表示高异常(10-6)

      Fig.  7.  Anomalies decomposed from As power spectrum density map using inverse Fourier transform with anomaly filter as defined in

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    • 收稿日期:  2004-07-15
    • 刊出日期:  2004-11-25

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