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An alternate and effective approach to Hilbert transform in geophysical applications

机译:地球物理应用中希尔伯特变换的另一种有效方法

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摘要

The Hilbert transform defined via the Hartley transform in contrast with the well-known Fourier transform is mathematically illustrated with a couple of geophysical applications. Although, the 1-D Fourier and Hartley transforms are identical in amplitude with a phase difference of 45°, the Hilbert transform effectively differs when defined as a function of the Hartley transform in certain geophysical applications. It may be noted here that the Hilbert transform defined through Fourier and Hartley transforms while possessing the same magnitude differs in phase by 270°. It is derived and shown mathematically that the evaluation of depth of subsurface targets is directly equal to the abscissa of the point of intersection of the gravity (magnetic) field and the Hartley-Hilbert transform; however, it is not the case with the Fourier-Hilbert transform. The practical applications are illustrated with the interpretation of gravity anomaly due to an inclined sheet-like structure across the Mobrun ore body, Noranda, Quebec, Canada, and the vertical magnetic anomaly due to a cylindrical structure over a narrow band of quartzite magnetite, Karimnagar, India. The entire process can be automated.
机译:通过Hartley变换定义的Hilbert变换与著名的Fourier变换形成对比,并通过几个地球物理应用进行了数学说明。尽管一维傅立叶变换和Hartley变换的幅度相同,但相位差为45°,但是在某些地球物理应用中,将Hilbert变换定义为Hartley变换的函数时,实际上是不同的。在这里可以注意到,通过傅立叶变换和哈特利变换定义的希尔伯特变换在具有相同幅度的同时相位相差270°。从数学上得出并显示,对地下目标深度的评估直接等于重力(磁场)与Hartley-Hilbert变换的交点的横坐标。但是,傅立叶-希尔伯特变换并非如此。实际应用通过对重力异常的解释来说明,这是由于横跨加拿大魁北克省诺兰达的莫布伦矿体上的倾斜片状结构,以及由于在窄带石英岩磁铁矿上的圆柱形结构Karimnagar造成的垂直磁异常。 ,印度。整个过程可以自动化。

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