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Near field CSAMT resistivity and model parameter determination

机译:近场CSAMT电阻率和模型参数确定

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Cagniard resistivity approach in controlled source audiofrequency magnetotellurics/magnetotellurics (CSAMT/MT) data handling assumes a plane wave ER I source. Hence, near field Cagniard's resistivity does not permit the determination of model parameters. This paper presents the study of near/transition field apparent resistivity over multi-layered media by resorting to near field apparent resistivity and examines the possibility of extracting model parameters from near field CSAMT data, which hitherto has been ignored or corrected, using the well-known Marquardt algorithm. The per cent deviation (Delta alpha%) between the true and fitted geoelectric parameters for a two-layer case increases with increase in rho(2)/rho(1) when (rho(2) < rho(1)) for all values of r/h(1), h(1) being the thickness of the first-layer and r the distance between the transmitter and receiver. When r/h(1) 1, Delta alpha% is well below 15%. In case rho(2) > rho(1), the per cent deviation is within 5% when rho(2)/rho(1) > 20 and r/h(1) greater than or equal to 1. Over a three-layer geoelectric section the per cent deviation is within the 'acceptable' limits for the geoelectric parameters studied. Thus, this paper shows a way to invert the near zone CSAMT data which is a necessity to probe deeper layers. However, the scheme has poorer resolvability in the case of three-layer A-type geoelectric section. [References: 35]
机译:受控源音频大地电磁/大地电磁(CSAMT / MT)数据处理中的卡格纳德电阻率方法假定使用平面波ER I源。因此,近场卡格纳德的电阻率不允许确定模型参数。本文借助近场视在电阻率,介绍了多层介质上的近场/过渡场视在电阻率的研究,并探讨了从近场CSAMT数据中提取模型参数的可能性,迄今为止,该数据已被忽略或使用井眼校正。已知的Marquardt算法。当(rho(2) rho(1),则当rho(2)/ rho(1)> 20且r / h(1)大于或等于1时,偏差百分比在5%之内。层地电部分的百分比偏差在所研究的地电参数的“可接受”范围内。因此,本文显示了一种反转近区CSAMT数据的方法,这是探查更深层的必要条件。但是,在三层A型地电段的情况下,该方案的可分辨性较差。 [参考:35]

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