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تخمین میزان جابهجایی ایستا در دادههای مگنتوتلوریک با استفاده از تانسور مغناطیسی افقی | ||
فیزیک زمین و فضا | ||
مقاله 5، دوره 45، شماره 2، مرداد 1398، صفحه 313-324 اصل مقاله (1 M) | ||
نوع مقاله: مقاله پژوهشی | ||
شناسه دیجیتال (DOI): 10.22059/jesphys.2019.268558.1007055 | ||
نویسندگان | ||
احسان لیموپرورجهرمی1؛ بنفشه حبیبیان دهکردی* 2؛ بهروز اسکوئی3 | ||
1دانشآموخته کارشناسی ارشد، گروه فیزیک زمین، مؤسسه ژئوفیزیک، دانشگاه تهران، تهران، ایران | ||
2استادیار، گروه فیزیک زمین، مؤسسه ژئوفیزیک، دانشگاه تهران، تهران، ایران | ||
3دانشیار، گروه فیزیک زمین، مؤسسه ژئوفیزیک، دانشگاه تهران، تهران، ایران | ||
چکیده | ||
تفسیر دادههای مگنتوتلوریک در حضور اعوجاجهای گالوانی ناشی از ساختارهای کوچکمقیاس نزدیک سطحی میتواند به نتایج نادرست منجر شود. سادهترین شکل ظهور این اعوجاجها درحالیکه فقط به تغییر دامنه میدانهای الکتریکی محدود میشوند، جابهجایی قائم منحنیهای مقاومتویژه ظاهری یا همان پدیده جابهجایی ایستا (static shift) است؛ که مقدار آن تنها با استفاده از دادههای تانسور امپدانس قابل محاسبه نیست و در واقع جزء بخشهای غیرقابل تعیین ماتریس اعوجاج است. در این تحقیق از توابع تبدیل ژئومغناطیسی (تیپر و دادههای مغناطیسی افقی) برای برآورد نسبی میزان این جابهجایی و بازیافت مقاومتویژه ظاهری معوج نشده یا منطقهای مود TE بر اساس قانون القاء فاراده استفاده شده است. با لحاظ کردن تغییرات افقی مؤلفههای افقی میدان مغناطیسی، روش مورد نظر بر روی دو مدل مصنوعی اعمال شده است. به دو روش محاسباتی مختلف، اغتشاشات ناشی از ساختارهای کوچک مقیاس سهبعدی شبیهسازی شده و به مدلهای مورد استفاده اضافه شدند. نتایج بهدست آمده، مؤید دقیقتر بودن میزان جابهجایی برآورد شده نسبت به حالتی است که از توابع تبدیل مغناطیسی افقی صرفنظر و تنها توابع تبدیل مغناطیسی قائم مد نظر قرار گیرند. | ||
کلیدواژهها | ||
مگنتوتلوریک؛ توابع تبدیل؛ جابهجایی ایستا | ||
عنوان مقاله [English] | ||
Static shift estimation in magnetotelluric data using horizontal magnetic tensor | ||
نویسندگان [English] | ||
Ehsan Limooparvar Jahromi1؛ Banafsheh Habibian Dehkordi2؛ Behrooz Oskooi3 | ||
1M.Sc. Graduated, Department of Earth Physics, Institute of Geophysics, University of Tehran, Tehran, Iran | ||
2Assistant Professor, Department of Earth Physics, Institute of Geophysics, University of Tehran, Tehran, Iran | ||
3Associate Professor, Department of Earth Physics, Institute of Geophysics, University of Tehran, Tehran, Iran | ||
چکیده [English] | ||
Interpretation of magnetotelluric data in the presence of galvanic distortions, caused by small-scale near-surface structures, can lead to unreliable results. The simplest manifest of these distortions, while limited only to the changes in the amplitude of electric fields, is vertical displacement of the apparent resistivity curves or static shift phenomenon that constitutes non-determinable part of the distortion matrix. Due to the boundary conditions governing components of the electric and magnetic fields, the occurrence of charge accumulation and therefore the static shift of apparent resistivity curves, affects only TM-mode data in the case of two-dimensional models. Thus, we can use the information available in the TE-mode- impedance phase (tipper and horizontal magnetic data) which are independent of this phenomenon. In this study, geomagnetic transfer functions have been used to estimate this displacement and recover the undistorted TE-mode apparent resistivity based on the Faraday induction law. Ledo et al. (2002) show that tipper data can be used to estimate static shift of magnetotelluric data, if the horizontal variations of the horizontal components of the magnetic field can be ignored. This assumption may be violated in complex situations. We estimate static shift while incorporating such variations and taking into account the horizontal magnetic transfer functions. Estimation of static shift through mathematical methods is only relatively possible and requires the selection of a reference station that has the minimal effect of galvanic distortion. The relations between different components of electric and magnetic fields are integrated and characterized by their mean values. To incorporate the horizontal magnetic tensor, array magnetotelluric data are required, so that components of the magnetic field at the reference and measurement sites are simultaneously provided. Considering two consecutive sites, impedance tensor at one site is written in terms of tipper and horizontal magnetic tensor at that site and the impedance at the adjacent site. By ignoring other types of distortions that can generally exist and using some algebra, the problem of determining the frequency-independent static shift factor becomes a linear fit problem. A set of data points covering different frequency ranges is selected and the quality of their linear fitting is examined through soling procedure. Considering the horizontal variations of the horizontal components of the magnetic field, the method has been applied to two synthetic models. Using two different approaches, the distortions caused by small-scale three-dimensional structures are simulated and added to the model responses. In the first approach, the distortion matrix is considered as the product of four parameters of gain factor, anisotropy, and twist and shear angles in the decomposition model then the distortion simulation is performed by selecting some numerical values of these four parameters and multiplying the resulted distortion matrix by the impedance tensor. In the second approach, some part of the top-layer of the model is replaced by a Gaussian distribution of resistivity with known selected mean and standard deviation. In this way, the effects of various geological processes, such as weathering, erosion- and to some extent- the nature of the deposited sediments are involved. The obtained results confirm that the estimated static shift parameter is more accurate than that of the case in which horizontal magnetic transfer functions are ignored and only the vertical magnetic transfer functions are considered. | ||
کلیدواژهها [English] | ||
magnetotelluric, transfer functions, static shift | ||
مراجع | ||
Berdichevsky, M. N. and Dmitriev, I. V., 2008, Models and Methods of Magnetotellurics. Springer, Berlin. Groom, R. W. and Bailey, R. C., 1989, Decomposition of magnetotelluric impedance tensors in the presence of local three-dimensional galvanic distortion: J. Geophys. Res., 94, 1913–1925. Habibian, D., B. and Oskooi, B., 2014, A resolution comparison of horizontal and vertical magnetic transfer functions. Journal of the Earth and Space Physics, 40, 47-53. Ledo, J., Gaba's, A. and Marcuello, A., 2002, Static shift levelling using geomagnetic transfer functions. Earth Planets Space 54, 493–498. Ledo, J., 2006, 2D versus 3D magnetotelluric data interpretation. Surveys in Geophysics., 27, 111-148. Martí, A., Queralt, P. and Ledo, J., 2009, WALDIM: a code for the dimensionality analysisof magnetotelluric data using the rotational invariants of the magnetotellurictensor. Comp. Geosci., 35, 2295–2303. Mackie, R. L., Smith, J. T. and Madden, T. R., 1994, Three-dimensional electromagnetic modeling using finite difference equations: the magnetotelluric example, Radio Sci., 29, 923–935. McNeice, G. W. and Jones, A. G., 2001, Multisite, multifrequency tensor decomposition of magnetotelluric data: Geophysics., 66, 158–173. Sasaki, Y. and Meju, M. A., 2006, Three-dimensional joint inversion for magnetotelluric resistivity and static shift distributions in complex media, J. Geophys. Res-solid earth., 111, B0511. Siripunvaraporn, W. and Egbert, G., 2000, An efficient data-subspace inversion method for 2-D magnetotelluric data. Geophysics., 65, 791-803. Soyer, W., 2002, Analysis of geomagnetic variation in the central and southern Andes, Ph.D thesis, Free University of Berlin. Varentsov, I. V. M. and EMTESZ-Pomerania Working Group., 2005, Method of horrzontal magnetovariational sounding: techniques and application in the EMTESZ-POMERANIA project, Kolloquium Elektromagnetische Tiefenforschung, Haus Wohldenberg, Holle, 3.-7.10.2005, Hrsg. Vozoff, k., 1972, The magnetotelluric method in the exploration of sedimentary basins. Geophysics., 37, 98-141. | ||
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