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Wide field electromagnetic sounding using y-component magnetic field with horizontal current dipole source |
LUO Wei-Bin1(), DING Zhi-Jun2, GAO Shu-De3, ZHANG Xing2 |
1. Lanzhou Resources & Environment Voc-Tech College, College of Geology and Jewelry, Lanzhou 730000, China 2. Gansu Nonferrous Geological Survey Institute, Lanzhou 730000, China 3. Earthquake Administration of Gansu Province, Lanzhou 730000, China |
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Abstract Based on the formula system of the electromagnetic field of the horizontal electric dipole source on the layered earth surface, this paper proposes the wide field apparent resistivity of y-component magnetic field (Hy) using the modulus of impedance. The field components Ex, Hy, and Hz of the electromagnetic field with multiple source-receiver separations on the surface of layered geoelectric model are calculated. The wide field apparent resistivity with these three field components and Ex/Hy cagniard resistivity are calculated, and compared with the MT Cagniard resistivity spectrum curve of the model. It is suggested that the wide field apparent resistivity of Hy has a good response to the geoelectric model in the vast area of the equatorial array and the axial array of the horizontal electric dipole source, and it can be used for single component wide field electromagnetic sounding. The axial array wide field apparent resistivity of Hy is similar to that of the equatorial array wide field of the vertical magnetic field of Hz. In the low frequency band, the wide field apparent resistivity of Hy is similar to that of the Cagniard resistivity of the magnetotelluric sounding of the layered model. Under the condition of small source-receiver separation, the axial array wide field apparent resistivity of Hy can have a better response to the deep basement. The equatorial array and the axial array wide field apparent resistivity of the Ex component of the horizontal electric field will wholly enter "saturated area" in the low frequency band. For each resistivity definition method, the appropriate source-receiver separation is the premise to reflect the geoelectric characteristics better, and the multi source-receiver separation measurement is more conducive to reflecting the deep electrical characteristics.
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Received: 30 March 2020
Published: 01 March 2021
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Layered geoelectricity model with horizontal electric dipole source
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层参数 | 第一层 | 第二层 | 电阻率/(Ω·m) | 200 | G型[10000,5000,2000,1000,400,300,220];D型[180, 100, 50, 25, 20, 10] | 层厚/m | 1100 | Inf |
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Two layers type geoelectricity model parameters
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Whole zone apparent resistivity spectrum of two layers type geoelectricity model
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层参数 | 第一层 | 第二层 | 第三层 | 电阻率/(Ω·m) | 200 | 30 | 700 | 层厚/m | 1100 | 120 | Inf |
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H-type geoelectricity model parameters
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Apparent resistivity spectrum of H-type geoelectricity model with different method
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层参数 | 第一层 | 第二层 | 第三层 | 电阻率/(Ω·m) | 300 | 1200 | 100 | 层厚/m | 1300 | 310 | Inf |
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K-type geoelectricity model parameters
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Apparent resistivity spectrum of K-type geoelectricity model with different T-R offset
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层参数 | 第一层 | 第二层 | 第三层 | 第四层 | 电阻率/(Ω·m) | 200 | 30 | 700 | 20 | 层厚/m | 1100 | 120 | 300 | Inf |
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HK-type geoelectricity model parameters
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Comparison of frequency curves with different definitions of equatorial resistivity (distance between transceiver and transmitter is 7 000 m)
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Whole zone apparent resistivity spectrum of HK-type geoelectricity model with multi T-R distance (frequency at 50.12 Hz)
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层参数 | 第一层 | 第二层 | 第三层 | 第四层 | 电阻率/(Ω·m) | 300 | 2000 | 60 | 750 | 层厚/m | 1100 | 450 | 200 | Inf |
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KH-type geoelectricity model parameters
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Whole zone apparent resistivity spectrum of KH-type geoelectricity model with multi transmit-receive distance
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