首页> 外文期刊>Exploration Geophysics >Discussion: On 'Magnetization structure of Aogashima Island using vector magnetic anomalies obtained by a helicopter-borne magnetometer' (Isezaki, N., and J. Matsuo, 2009, Exploration Geophysics, 40,17-26; Butsuri-Tansa, 62,17-26; Mulli-Tamsa, 12, 17-26).
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Discussion: On 'Magnetization structure of Aogashima Island using vector magnetic anomalies obtained by a helicopter-borne magnetometer' (Isezaki, N., and J. Matsuo, 2009, Exploration Geophysics, 40,17-26; Butsuri-Tansa, 62,17-26; Mulli-Tamsa, 12, 17-26).

机译:讨论:关于“使用直升飞机磁强计获得的矢量磁异常对青岛的磁化结构”(伊泽崎,N。和J.松尾,2009,勘探地球物理学,40,17-26; Butsuri-Tansa,62,17 -26; Mulli-Tamsa,12,17-26)。

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摘要

In 'Magnetization structure of Aogashima Island using vector magnetic anomalies obtained by a helicopter-borne magnetometer', Isezaki and Matsuo discussed a source of inaccuracy in the inversion of total intensity magnetic anomalies, and presented an example of a helicopter three-component magnetic survey and its inversion. In their paper, I consider there to be some problems and points to be discussed. Here I refer to the figures in their paper by the original figure numbers, and use the label D-l for the new figure in this discussion. Isezaki and Matsuo described the algebra of the total intensity anomaly (TIA), and discussed the error introduced by the assumption that TIA is approximated by the projected total intensity anomaly (PTA). Their figures 3 and 4 are correct although the description of the horizontal axis of figure 4 could be clearer. It is obvious that the relative error ε_T/TIA ( = (TIA- PTA)/ TIA) becomes infinite where 7X4 = 0. However, the situation is not as severe as their assertion implies, because such a large error occurs only in a quite limited region near PTA = 0, but the result of analyses of magnetic anomalies is commonly more dependent on the locations and values of the high and low anomaly peaks, where the approximation above is fully valid. To illustrate this, I show a simple synthetic model.
机译:Isezaki和Matsuo在“使用直升机磁力计获得的矢量磁异常使用的青岛岛的磁化结构”中,讨论了总强度磁异常反演中的误差源,并举例说明了直升机三分量磁测和它的反转。在他们的论文中,我认为存在一些问题和要讨论的要点。在这里,我通过原始图形编号引用其论文中的图形,并在此讨论中为新图形使用标签D-1。 Isezaki和Matsuo描述了总强度异常(TIA)的代数,并讨论了由TIA近似于预计的总强度异常(PTA)的假设所引入的误差。尽管图4的水平轴的描述可能更清楚,但它们的图3和图4是正确的。显然,相对误差ε_T/ TIA(=(TIA-PTA)/ TIA)在7X4 = 0处变为无限。但是,这种情况并不像它们的断言所暗示的那样严重,因为如此大的误差仅发生在PTA = 0附近的有限区域,但是磁异常的分析结果通常更多地取决于高低异常峰的位置和值,其中上述近似值完全有效。为了说明这一点,我展示了一个简单的综合模型。

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  • 来源
    《Exploration Geophysics》 |2011年第1期|p.121-122|共2页
  • 作者

    Tadashi Nakatsuka;

  • 作者单位

    Geological Survey of Japan, AIST, 1-1-1 Higashi, Tsukuba, 305-8567, Japan;

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