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APPLIED GEOPHYSICS  2017, Vol. 14 Issue (1): 165-174    DOI: 10.1007/s11770-017-0604-2
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Cone-shaped source characteristics and inductance effect of transient electromagnetic method
Yang Hai-Yan1,2, Li Feng-Ping1, Yue Jian-Hua3, Guo Fu-Sheng1, Liu Xu-Hua1, and Zhang Hua1
1. State Key Laboratory Breeding Base of Nuclear Resources and Environment, East China University of Technology, Nanchang 330013, China.
2. Fundamental Science on Radioactive Geology and Exploration Technology Laboratory, East China University of Technology, Nanchang 330013, China.
3. School of Resource and Earth Science, China University of Mining & Technology, Xuzhou 221006, China.
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Abstract Small multi-turn coil devices are used with the transient electromagnetic method (TEM) in areas with limited space, particularly in underground environments such as coal mines roadways and engineering tunnels, and for detecting shallow geological targets in environmental and engineering fields. However, the equipment involved has strong mutual inductance coupling, which causes a lengthy turn-off time and a deep “blind zone”. This study proposes a new transmitter device with a conical-shape source and derives the radius formula of each coil and the mutual inductance coefficient of the cone. According to primary field characteristics, results of the two fields created, calculation of the conical-shaped source in a uniform medium using theoretical analysis, and a comparison of the inductance of the new device with that of the multi-turn coil, show that inductance of the multi-turn coil is nine times greater than that of the conical source with the same equivalent magnetic moment of 926.1 A·m2. This indicates that the new source leads to a much shallower “blind zone.” Furthermore, increasing the bottom radius and turn of the cone creates a larger mutual inductance but increasing the cone height results in a lower mutual inductance. Using the superposition principle, the primary and secondary magnetic fields for a conical source in a homogeneous medium are calculated; results indicate that the magnetic behavior of the cone is the same as that of the multi-turn coils, but the transient responses of the secondary field and the total field are more stronger than those of the multi-turn coils. To study the transient response characteristics using a cone-shaped source in a layered earth, a numerical filtering algorithm is then developed using the fast Hankel transform and the improved cosine transform, again using the superposition principle. During development, an average apparent resistivity inverted from the induced electromotive force using each coil is defined to represent the comprehensive resistivity of the conical source. To verify the forward calculation method, the transient responses of H type models and KH type models are calculated, and data are inverted using a “smoke ring” inversion. The results of inversion have good agreement with original models and show that the forward calculation method is effective. The results of this study provide an option for solving the problem of a deep “blind zone” and also provide a theoretical indicator for further research.
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Key wordsTransient electromagnetic method   Cone-shaped source   Apparent resistivity   Mutual inductance   “Smoke ring&rdquo   inversion     
Received: 2016-04-19;
Fund:

This work was supported by the National Natural Science Foundation of China (Nos. 41564001 and 41572185) and the Natural Science Foundation of Jiangxi Province (No. 20151BAB203045).

Cite this article:   
. Cone-shaped source characteristics and inductance effect of transient electromagnetic method[J]. APPLIED GEOPHYSICS, 2017, 14(1): 165-174.
 
[1] Anderson, W. L., and Chave, A. D., 1979, Numerical integration of related Hankel transforms of order 0 and 1 by adaptive digital filtering: Geophysics, 44(7), 1287−305.
[2] Asten, M. W., and Price, D. G., 1985, Transient EM sounding by the in/out-loop method: Exploration Geophysics, 16(3), 165−168.
[3] Chen, M. S., and Tian, X. B., 1999, Study on the transient electromagnetic (TEM) sounding with electric dipole.V. The measured induced voltage transformed to the vertical magnetic field: Goal Geology and Exploration, 27(5), 63−65.
[4] Christian, H., Rainer, S., and Siegfried, S., 2003, Efficient inductance calculation in interconnect structures by applying the Monte Carlo method: Microelectronics Journal, 34(9), 815−821.
[5] Christian, P., and Yiannos, M., 2008, Inductance calculation of planar multi-layer and multi-wire coils:An analytical approach: Sensors and Actuators, S145−146, 394−404.
[6] Fan, T., Zhao, Z., Wu, H., et al., 2014, Research on inductance effect removing and curve offset for mine TEM with multi small loops: Journal of China Coal Society, 39(5), 932−940.
[7] Fitterman, D. V., and Anderson, W. L., 1987, Effect of Transmitter Turn-off Time on Transient Soundings: Geoexploration, 24(2), 131−146.
[8] Guptasarma, D., and Singh, B., 1997, New digital linear filters for Hankel J0 and J1 transforms: Geophysical Prospecting, 45, 745−762.
[9] Harlander, C., Sabelka, R., and Selberherr, S., 2003, Efficient inductance calculation in interconnect structures by applying the Monte Carlo method: Microelectronics Journal, 34, 815−821.
[10] Jiang, B. Y., 1998, Applied near zone magnetic source Transient Electromagnetic Exploration: Geological Publishing House, Beijing.
[11] Jiang, Z. H., Yue, J. H., and Liu, S. C., 2007, Mine transient electromagnetic observation system of small multi-turn coincident configuration: Journal of China Coal Society (in Chinese), 32(11), 1152-1156.
[12] KANAHTAPOB, П. N., and ЦEHTNHH, N. А., 1986, Handbook of inductance calculation: Mechanical Industry Press, Beijing.
[13] Kaufman, A. A., and Eaton, P. A., 2001, The Theory of Inductive Prospecting: Elsevier.
[14] Li, W. Y., and Wu, Z. H., 2010, A compute formula of self-inductance coefficient of rectangular coil in transient electromagnetic methods: Geology and Exploration, 46(1), 160−164.
[15] Li, X., 2002, Theory and application of transient electromagnetic method: Science and Technology Press, Shanxi.
[16] Li, X., Xue, G. Q., Song, J. P., et al., 2005, Application of the adaptive shrinkage genetic algorithm in the feasible region to TEM conductive thin layer inversion: Applied Geophysics, 2(4), 204−210.
[17] Li, Y. Q., 2002, Equivalent self inductance of mutual coils in series: Journal of Liaoning Teachers College, 4(2), 23−25.
[18] Liu, Y., Wang, X. B., and Wang, Y., 2013, Numerical modeling of the 2D time-domain transient electromagnetic secondary field of the line source of the current excitation: Applied Geophysics, 10(2), 134−144.
[19] Morrison, H. F., Phillips, R. J., O’Brien, D. P., et al., 1969, Quantitative interpretation of transient electromagnetic fields over a layered half-space: Geophysical prospecting, 17(1), 82−101.
[20] Nabighian, M. N., 1979, Quasi-static transient response of a conducting half-space-An approximate representation: Geophysics, 44(10), 1700−1705.
[21] Ni, G. Z., 2010, Numerical calculation of engineering electromagnetic field: China Machine Press, Beijing.
[22] Peters, C., and Manol, Y., 2008, Inductance calculation of planar multi-layer and multi-wire coils: An analytical approach: Sensors and Actuators, A145−146, 394−404.
[23] Raiche, A. P., and Gallagher, R. G., 1985, Apparent resistivity and diffusion velocity: Geophysics, 50(10), 1628−1633.
[24] Rainey, J. K., DeVries, J. S., and Sykes, B. D., 2007, Estimation and measurement of flat or solenoidal coil inductance for radio frequency NMR coil design: Journal of Magnetic Resonance, 187(1), 27−37.
[25] Sijoy, C. D., and Chaturvedi S., 2008, Calculation of accurate resistance and inductance for complex magnetic coils using the finite-difference time-domain technique for electromagnetics: IEEE Transaction on Plasma Science, 36(1), 70−79.
[26] Tang, X. G., Hu, W. B., et al., 2011, Topographic effects on long offset transient electromagnetic response: Applied Geophysics, 8(4), 277−284.
[27] Wang, H. J., 2004, Digital filtering algorithm of sine and cosine transform: Engineering Geophysics, 51(6), 1936−1942.
[28] Xue, G. Q., 2004, On surveying depth by transient electromagnetic sounding method: Oil Geophysical Prospecting, 39(5), 575−57 8.
[29] Xue, G. Q., Song, J. P., Yan, S. N., et al., 2004, Analysis and estimation of the minimum depth of large loop transient electromagnetic method: Geotechnical Investigation Surveying, 2004(2), 63−65.
[30] Yang, H. Y., 2009, Study on numerical simulation and distribution regularity of transient electromagnetic field with Mine-used multi small loop: PhD. Thesis, China University of Mining Technology, Jiangsu Xuzhou.
[31] Yang, H. Y., Deng, J. Z., Tang, H. Z., et al., 2014, Translation algorithm of data Interpretation technique in full-Space transient electromagnetic method: Journal of Jilin University, 44(3), 1012−1017.
[32] Yang, H. Y., and Yue, J. H., 2015, The theory and technique of mine transient electromagnetic method: Science Press, Beijing.
[33] Yang, H. Y., Yue, J. H., and Liu, Z. X., 2006, Theoretical Stud y of inductance effect with multi-axial coils for TEM in underground mine: Journal of Jilin University (Earth Science Edition), 36(sup), 168−171.
[34] Yu, C. T., Liu, H. F., Zhang, X. J., et al., 2013, The analysis on IP aignals in TEM response based on SVD: Applied Geophysics, 10(1), 79−87.
[35] Yu, J. C., Liu, Z. X., Liu, S. C., et al., 2007, Theoretical analysis of mine transient electromagnetic method and its application in detecting water burst structures in deep coal stope: Journal of China Coal Society, 32(8), 818−821.
[36] Zhou, N. N., Xue, G. Q., and Wang, H. Y., 2013, Comparison of the time-domain electromagnetic field from an infinitesimal point charge and dipole source: Applied Geophysics, 10(3), 349−356.
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