Proceedings of the 10th Intl Conf. “Problems of Geocosmos” (Oct 6-10, 2014, St. Petersburg, Russia) TWO-DIMENSIONAL INVESTIGATION OF THE EARTH CRUST SUBSURFACE LAYER BY METHOD OF INTERNAL SLIDING CONTACT V.E. Kolesnikov1, A.A. Skorokhodov1 1 Geological Institute of the Kola Science Center of Russian Academy of Sciences, 184209 Apatity, Russia, e-mail: [email protected] Abstract. Method of internal sliding contact (MISC) is a DC investigation method of Earth crust subsurface, which combines elements of profiling and sounding. Variation of distance between current electrode A and receiver electrode M allows the carrying on the investigations of this kind. Media sounding is conducted when the signal on receiver electrodes is registered and AM distance is varied. The electrode array movement along a profile permits to carry on profile investigations.The variation of AM distance is realized using the multi-electrode array. Electric current is injected to the ground through current dipole AB, and multi-channel digital receiver system records the signal from the ground. The MISC modeling and data processing was done by using ZondRes2D software that was designed by A.E. Kaminskiy. The software permits to carry on 2D-interpretation (2D-inversion) of the DC resistivity and IP data taking into consideration topography and prior information. The efficiency of MISC was investigated by physical modelling in a tank installation. MISC field research equipment includes AB current dipole and receiver system: receiver lines, switch, AD-converter and mobile PC that registers the digital signal and saves the data obtained to HDD. Method of internal sliding contact may be useful in structural research and in search of ore bodies. Introduction Method of internal sliding contact (MISC) is a DC method of investigation of Earth crust subsurface which combines elements of profiling and sounding. It is known that registration of DC signal on receiver electrodes with variation of distance between current electrode A and receiver electrode N gives information about media properties variation to depth (sounding). Moving of fixed electrode distance array along a profile permits to carry out investigations on earth-air surface (profiling). Thus simultaneous Earth crust survey along a profile and depth investigation on each point of the profile allows to conduct two-dimensional research of geoelectric cross-section subsurface layer. Two-dimensional investigations of Earth crust subsurface using multi-electrode arrays were conducted at the first time in 1970-1980s. Manual and automatic switch multi-electrode survey systems are described in the works [Barker, 1981; Dahlin, 1989]. Further development of research technique is described in proceedings [Griffiths, D.H., Barker, R.D., 1993; Bobachev et al., 1996]. Summary overview of development of the method is presented in publication [Dahlin, 2001]. Method of internal sliding contact was designed by A.A. Zhamaletdinov. Features and application of the method are described in publications [Zhamaletdinov et al., 1976; Zhamaletdinov et al., 1995]. Field research technique Practical MISC geological media investigations are conducted with variation of distance between A and M electrodes in multi-electrode electrical profiling array. The array is current dipole AB and receiver array that includes N electrode and some M electrodes on different distances from N electrode. Electric current is injected to the ground through the current dipole; signal is registered by multi-channel receiver system. Field research equipment which applied in Geological Institute if KSC RAS includes current dipole and receiver system. Generator injects low-frequency pulse current to the ground through the AB current dipole. Signal is registered on multi-channel system that connected with receiver electrode array. The system includes switch, AD-converter and field PC that registers the signal and saves the data to HDD. 23 Proceedings of the 10th Intl Conf. “Problems of Geocosmos” (Oct 6-10, 2014, St. Petersburg, Russia) Fig.1. MISC field equipment for investigations by DC resistivity and IP methods (GI KSC RAS) MISC data interpretation technique The one of the means of MISC field data processing and numerical modeling of research process is ZondRes2D software that is designed by A.E. Kaminskiy. The software permits to carry on 2D-interpretation (2D-inversion) of the DC resistivity and IP data taking into consideration topography and prior information. Observed data interpretation by means of ZondRes2D is multi-stage process. Full interpretation process can be divided to three stages: data input, data interpretation, data output. At the stage of data input some actions are performed: 1) 2) 3) 4) data file creation; interpretation model mesh construction; prior information input; inversion parameters input; Observed data file contains information about electrode relative coordinates, apparent resistivity values, registered signal values related to the current value, apparent polarizability values if IP measurements were conducted, weight values for each measurement. The file can also contain the topography and media reference model data. Interpretation model is divided to horizontal layers according to array geometry. Lower model boundary fits the maximum depth of investigation. Number of layers is equal to number of AM distances of array. First layer thickness is the depth of investigation on minimal AM distance. Thickness of the rest layers is increased so that the sum of all layer thicknesses will be equal to maximum depth of investigation. Prior information input is well-logging and lithology data addition. Inversion parameters are inversion algorithm, iterative process stop criteria, smoothing. The parameters are entered immediately before inversion process start. The second stage, or interpretation stage, begins from calculation of apparent resistivity values on each point of profile over the model. This is forward problem solution. This solution is followed by calculation of difference between observed and model apparent resistivity values (misfit), correction of model according to misfit values, new calculation of model apparent resistivity. The iterative process continues until the misfit value required to all the profile is reached. If the inversion results don’t correspond to the prior information, it is necessary to correct the inversion parameters. If the inversion process doesn’t bring to required misfit value, or the misfit value is decreased very slowly, inversion parameters should also be corrected. 24 Proceedings of the 10th Intl Conf. “Problems of Geocosmos” (Oct 6-10, 2014, St. Petersburg, Russia) If the inversion results are in accordance to all requirements, they are imaged as a resistivity cross-section; also they can be saved to HDD as ZondRes2D special file or exported to external software data file such as text file and Microsoft Excel file. Numerical modeling process also contains of several stages. At the first stage it is necessary to create data file that contains information about all electrode positions over a model medium. At the second stage the model mesh is constructed. To create the mesh it is necessary to enter horizontal and vertical relative coordinates of mesh nodes, and also to note whether a node is matched a coordinate of any electrode on profile. After the mesh construction the matrix of cell resistivity values is entered. The last stage is forward problem solution. It should be noted that the model can be constructed by two ways: addition the model information to the data file or creation the model immediately in software window. One of the main field data interpretation problems is non-linear electrode arrangement on terrain and, as a consequence, distortions in array geometry. Distortions in geometric factor values are a cause of apparent resistivity or polarizability calculation mistakes. In order to solve this problem the ZondRes2D opportunity to appoint the weight values to observed data is used. Observed geometric factor values are calculated from registered electrode absolute coordinates, and then the residual between theoretical and observed values for each measurement is calculated. The reverse value of the residual is appointed to each measurement as a weight value. Other problem is inversion process parameters selection. This problem is solved by multiple conduction of test inversion process with different algorithms until the required misfit value is reached. Also, knowingly false values should be deleted from observed data. Physical and mathematical modeling of MISC investigations During the ZondRes2D preparation for field data interpretation, its opportunities testing and adapting were conducted in the context of MISC investigation. The data of MISC physical modeling in test layout were used as test data. The layout is an electrolyte-filled tank with models of structural geological objects. This layout was used to prepare the electrical prospecting equipment EMAK-1 to field investigations and to study the MISC investigation efficiency in search of conductive objects and structural mapping. Fig.2. Installation for physical modeling and testing of DC resistivity and IP multi-electrode survey systems During the physical modeling four models were created – three models of conductive steeply dipping dike on different depths, and one model of two steeply dipping dikes on some distance between them. Physical models was created by means of metal plates buried to the tank. Models of single dikes were constructed to determine the maximum depth of investigation with the array. The 25 Proceedings of the 10th Intl Conf. “Problems of Geocosmos” (Oct 6-10, 2014, St. Petersburg, Russia) aim of construction two dikes model was to determine an opportunity of their separate allocation on resistivity cross-section. The studying MISC array is not symmetrical, therefore the location of conductivity or resistivity anomalies related to structural elements differs from elements’ true location. To compensate the distortions caused by array dissymmetry, profile observations in «two traverses» should be conducted: «forward traverse», in which the array moves from relative start of profile to relative finish, and «reverse traverse», in which the array moves from relative finish of profile to relative start. Observations over the physical model medium were conducted only in «forward traverse», that was a cause a mistake in horizontal localization of structural element. The mistake evaluation was not conducted because precise horizontal localization wasn’t aim of physical modeling. Results of interpretation for two models, in which the structural elements is localized, by means of ZondRes2D software are presented. Fig.3. Model of steeply dipping dike, depth to top 1 cm. ZondRes2D interpretation results. Upper part – observed apparent resistivity plot, medium part – calculated apparent resistivity pseudosection, lower part – interpretation model resistivity cross-section. Structural element is marked as a white stripe. Fig.4. Model of steeply dipping dike, depth to top 2.5 cm. ZondRes2D interpretation results. 26 Proceedings of the 10th Intl Conf. “Problems of Geocosmos” (Oct 6-10, 2014, St. Petersburg, Russia) Structural elements in other two models were not localized. Depth of model dike 4.5 cm is larger than the maximum depth of investigation. Two model dikes on distance 2.5 cm were not separated and formed an uniform conductivity anomaly. In addition to physical modeling material, numerical modeling by means of ZondRes2D for «two traverses» was conducted. Two models were created. Parameters of the models were matched to physical models. Also one additional model of two conductive dikes was created, with distance between dikes that larger than distance between two dikes in physical model. Background resistivity was 700 Ohm.m, elements’ resistivity was 50 Ohm.m. Fig.5. Forward problem solving results in ZondRes2D for model of steeply dipping dike, depth to top 1 cm. Upper part – calculated apparent resistivity pseudosection, lower part – model geoelectric cross-section. Fig.6. Forward problem solving results in ZondRes2D for model of steeply dipping dike, depth to top 2.5 cm. Fig.7. Forward problem solving results in ZondRes2D for model of two steeply dipping dikes, depth to top 1 cm, distance between the dikes 9 cm. Field data interpretation results MISC investigations were carried out during the field excursion research in the north part of Pechenga structure as a part of investigation works complex to search of homologues of Archaean section of Kola Superdeep Borehole on earth-air surface. 27 Proceedings of the 10th Intl Conf. “Problems of Geocosmos” (Oct 6-10, 2014, St. Petersburg, Russia) Fig.8. Field data interpretation results in ZondRes2D for MISC investigations in Pechenga area. Conclusions Combination of elements of profiling and sounding in the method of internal sliding contact permits to carry on two-dimensional investigation of Earth crust subsurface layer. This investigation allows to identify borders of structural geological elements and to localize the elements to depth, that is useful in structural research. Also, two-dimensional Earth crust subsurface studies with MISC array are less time-consuming than the same investigations with other DC resistivity method arrays. ZondRes2D software is useful for interpretation and modeling of two-dimensional investigations of Earth crust subsurface with MISC array or with other arrays. However, work with this software requires thorough analysis of the data observed and operator’s active participation in interpretation process. Gratitude Authors of this paper express a great appreciation and gratitude to Organizing Committee of the conference «Problems of Geocosmos» for opportunity given to submit the results of investigations, to participants of the Conference for discussion and criticism, and to scientific advisors Abdulkhay A. Zhamaletdinov and Aleksandr N. Shevtsov for overall aid and support and wise direction of research carrying out. References Glaznev V.N., Dyakov S.N., Raevskiy A.B., Tokarev A.D. (2004). Geophysical methods (Field geophysical surveys manual), 66 pp., MSTU press, Murmansk. Balkov, E.V., Panin, G.L., Mainshtein, Yu.A., Mainshtein, A.K., Beloborodov, V.A. (2010) Electrotomography: equipment, technique and using experience. [Electronic resource] www.nemfis.ru, 12. Kaminskiy, A.E. (2010), ZondRes2D. Two-dimensional DC resistivity and IP methods interpretation software. Zond geophysical software, Saint-Petersburg, 3, 18-62. Zhamaletdinov A.A., Ronning J.S. & Vinogradov (1995), Electrical profiling by the MISC and Slingram methods in the Pechenga-Pasvik area. Norges Geologiske Undersokelse, Special publication 7, 333-338. Skorokhodov, A.A. (2007) Using of multi-functional electrical prospecting equipment EMAK-1 in DC resistivity method. Book of abstracts of X International scientific conference, Apatity, April 5-6, 2007. Vol. 3., 126 pp., Kola Branch of PetrSU Press, Apatity. 28
© Copyright 2026 Paperzz