ĐĎॹá>ţ˙  ŘÚţ˙˙˙ĐŃŇÓÔŐÖ×Ü€ŕD˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙ěĽÁ`řż$gbjbjËsËsI0ŠŠÓ\˙˙˙˙˙˙¤       ¤ Č(Č(Č(8)44-Ĥ P‡Ň2‚†D4şDşDşDwH‘cLÝh¨W†Y†Y†Y†Y†Y†Y†"‰hŠ‹zY†ą ŹnH^wHŹnŹnY†  şDşD_ ‡ÔtÔtÔtŹnć şD şDW†ÔtŹnW†ÔtÔt‚‡‚„  ť…şDř1 0œrFW6ČČ(’q …Fű…\ ‡0P‡Q…jŒŚsÖŒŒť…Œ ť…@…kŽ3l|ÔtŻldm™…k…k…kY†Y†|tX…k…k…kP‡ŹnŹnŹnŹn¤ ¤ ¤ $Č(¤ ¤ ¤ Č(¤ ¤ ¤       ˙˙˙˙  Russian State Geology Prospecting University COMPLEX OF SPECTRAL-CORRELATION ANALYSIS OF GEOPHYSICAL EVIDENCE ŤCOSCAD 3Dtť USER’S MANUAL PART I Version 2007.1  TOC \o "1-3" \h \z \u   HYPERLINK \l "_Toc59514593" 1. Computer technology COSCAD 3Dt.  PAGEREF _Toc59514593 \h 4  HYPERLINK \l "_Toc59514594" 1.1. Program overview  PAGEREF _Toc59514594 \h 4  HYPERLINK \l "_Toc59514595" 1.2. About Authors  PAGEREF _Toc59514595 \h 8  HYPERLINK \l "_Toc59514596" 1.3. How to install "Coscad 3Dt"?  PAGEREF _Toc59514596 \h 9  HYPERLINK \l "_Toc59514597" 1.4. FAQ and Error's handling  PAGEREF _Toc59514597 \h 10  HYPERLINK \l "_Toc59514598" 2. SERVICE  PAGEREF _Toc59514598 \h 13  HYPERLINK \l "_Toc59514599" 2.1. Data input...  PAGEREF _Toc59514599 \h 13  HYPERLINK \l "_Toc59514600" 2.1.1. Inputting data from “COSCAD 3Dt” - formats  PAGEREF _Toc59514600 \h 13  HYPERLINK \l "_Toc59514601" 2.1.2. Inputting data from SURFER format  PAGEREF _Toc59514601 \h 15  HYPERLINK \l "_Toc59514602" 2.1.3. Inputting data from GEOSOFT format  PAGEREF _Toc59514602 \h 15  HYPERLINK \l "_Toc59514603" 2.1.4. Inputting data from SEGY format  PAGEREF _Toc59514603 \h 15  HYPERLINK \l "_Toc59514604" 2.1.5. Inputting data from INTEGRO format  PAGEREF _Toc59514604 \h 15  HYPERLINK \l "_Toc59514605" 2.1.6. Inputting data from RADAR format  PAGEREF _Toc59514605 \h 15  HYPERLINK \l "_Toc59514606" 2.2. Data output...  PAGEREF _Toc59514606 \h 16  HYPERLINK \l "_Toc59514607" 2.2.1. Outputting data into COSCAD 3Dt format  PAGEREF _Toc59514607 \h 16  HYPERLINK \l "_Toc59514608" 2.2.2. Outputting data into SURFER format  PAGEREF _Toc59514608 \h 17  HYPERLINK \l "_Toc59514609" 2.2.3. Outputting data into GEOSOFT format  PAGEREF _Toc59514609 \h 18  HYPERLINK \l "_Toc59514610" 2.2.4. Outputting data into SEGY format  PAGEREF _Toc59514610 \h 18  HYPERLINK \l "_Toc59514611" 2.2.5. Outputting data into INTEGRO format  PAGEREF _Toc59514611 \h 18  HYPERLINK \l "_Toc59514612" 2.2.6. Outputting data into GRAPHER format  PAGEREF _Toc59514612 \h 18  HYPERLINK \l "_Toc59514613" 2.2.7. Outputting data as a common text table X,Y,Z,F (for EXCEL)  PAGEREF _Toc59514613 \h 19  HYPERLINK \l "_Toc59514614" 2.3. Irregular grids input...  PAGEREF _Toc59514614 \h 19  HYPERLINK \l "_Toc59514615" 2.3.1. Inputting of 2D irregular grids  PAGEREF _Toc59514615 \h 19  HYPERLINK \l "_Toc59514616" 2.3.2. Inputting of 2D irregular grids (2D-spline)  PAGEREF _Toc59514616 \h 20  HYPERLINK \l "_Toc59514617" 2.3.3. Inputting of 3D irregular grids  PAGEREF _Toc59514617 \h 21  HYPERLINK \l "_Toc59514618" 2.4. Interpolation of grids...  PAGEREF _Toc59514618 \h 22  HYPERLINK \l "_Toc59514619" 2.4.1. Liner interpolation  PAGEREF _Toc59514619 \h 22  HYPERLINK \l "_Toc59514620" 2.4.2. Profile spline interpolation  PAGEREF _Toc59514620 \h 22  HYPERLINK \l "_Toc59514621" 2.4.3. 2D Spline interpolation  PAGEREF _Toc59514621 \h 22  HYPERLINK \l "_Toc59514622" 2.4.4. Profile Fourier interpolation  PAGEREF _Toc59514622 \h 23  HYPERLINK \l "_Toc59514623" 2.5. Extrapolation of grids  PAGEREF _Toc59514623 \h 23  HYPERLINK \l "_Toc59514624" 2.6. Filling of absent data  PAGEREF _Toc59514624 \h 23  HYPERLINK \l "_Toc59514625" 2.7. Fragmentation of grids  PAGEREF _Toc59514625 \h 24  HYPERLINK \l "_Toc59514626" 2.8. Inserting of grids  PAGEREF _Toc59514626 \h 24  HYPERLINK \l "_Toc59514627" 2.9. Rotating of grids  PAGEREF _Toc59514627 \h 24  HYPERLINK \l "_Toc59514628" 2.10. Uniting of grids  PAGEREF _Toc59514628 \h 25  HYPERLINK \l "_Toc59514629" 2.11. Some transformations of data  PAGEREF _Toc59514629 \h 25  HYPERLINK \l "_Toc59514630" 2.11.1. Transformations with one sign  PAGEREF _Toc59514630 \h 25  HYPERLINK \l "_Toc59514631" 2.11.2. Transformations with two signs  PAGEREF _Toc59514631 \h 26  HYPERLINK \l "_Toc59514632" 2.11.3. Imposition of dummy-code  PAGEREF _Toc59514632 \h 26  HYPERLINK \l "_Toc59514633" 2.12. Gluing of grids  PAGEREF _Toc59514633 \h 27  HYPERLINK \l "_Toc59514634" 2.13. Printing information into file  PAGEREF _Toc59514634 \h 27  HYPERLINK \l "_Toc59514635" 2.14. Adaptive equalization of seismic traces  PAGEREF _Toc59514635 \h 27  HYPERLINK \l "_Toc59514636" 3. VISUALIZATION  PAGEREF _Toc59514636 \h 29  HYPERLINK \l "_Toc59514637" 3.1. Raster map  PAGEREF _Toc59514637 \h 29  HYPERLINK \l "_Toc59514638" 3.2. Plotting of classification  PAGEREF _Toc59514638 \h 30  HYPERLINK \l "_Toc59514639" 3.3. Graphics  PAGEREF _Toc59514639 \h 31  HYPERLINK \l "_Toc59514640" 3.4. Inverse problem  PAGEREF _Toc59514640 \h 32  HYPERLINK \l "_Toc59514641" 3.5. Viewing in projections X, Y, Z  PAGEREF _Toc59514641 \h 32  HYPERLINK \l "_Toc59514642" 3.6. Classification viewing in projections X, Y, Z  PAGEREF _Toc59514642 \h 33  HYPERLINK \l "_Toc59514643" 3.7. 3D Surface view  PAGEREF _Toc59514643 \h 34  HYPERLINK \l "_Toc59514644" 3.8. Graphic’s map  PAGEREF _Toc59514644 \h 35  HYPERLINK \l "_Toc59514645" 4. STATISTICS  PAGEREF _Toc59514645 \h 36  HYPERLINK \l "_Toc59514646" 4.1. Statistical characteristics...  PAGEREF _Toc59514646 \h 36  HYPERLINK \l "_Toc59514647" 4.1.1. Statistical characteristics of field fragments  PAGEREF _Toc59514647 \h 36  HYPERLINK \l "_Toc59514648" 4.1.2. Statistical characteristics in the slithering window  PAGEREF _Toc59514648 \h 37  HYPERLINK \l "_Toc59514649" 4.1.3. Statistical characteristics in the one-dimensional dynamic window  PAGEREF _Toc59514649 \h 38  HYPERLINK \l "_Toc59514650" 4.1.4. Statistical characteristics in the two-dimensional dynamic window  PAGEREF _Toc59514650 \h 38  HYPERLINK \l "_Toc59514651" 4.1.5. Statistical characteristics in the window of “alive form”  PAGEREF _Toc59514651 \h 39  HYPERLINK \l "_Toc59514652" 4.1.6. Estimation of the factor dispersion in the slithering window  PAGEREF _Toc59514652 \h 39  HYPERLINK \l "_Toc59514653" 4.2. Correlation characteristics...  PAGEREF _Toc59514653 \h 40  HYPERLINK \l "_Toc59514654" 4.2.1. Autocorrelation function  PAGEREF _Toc59514654 \h 40  HYPERLINK \l "_Toc59514655" 4.2.2. Cross-correlation function between profiles  PAGEREF _Toc59514655 \h 41  HYPERLINK \l "_Toc59514656" 4.2.3. Cross-correlation function between fields  PAGEREF _Toc59514656 \h 41  HYPERLINK \l "_Toc59514657" 4.2.4. Two-dimensional autocorrelation function  PAGEREF _Toc59514657 \h 42  HYPERLINK \l "_Toc59514658" 4.2.5. Two-dimensional cross-correlation function  PAGEREF _Toc59514658 \h 42  HYPERLINK \l "_Toc59514659" 4.2.6. Three-dimensional autocorrelation function  PAGEREF _Toc59514659 \h 42  HYPERLINK \l "_Toc59514660" 4.2.7. Correlation coefficient in the slithering window  PAGEREF _Toc59514660 \h 43  HYPERLINK \l "_Toc59514661" 4.3. Spectral characteristics...  PAGEREF _Toc59514661 \h 44  HYPERLINK \l "_Toc59514662" 4.3.1. Univariate spectrum  PAGEREF _Toc59514662 \h 44  HYPERLINK \l "_Toc59514663" 4.3.2. Two-dimension spectrum  PAGEREF _Toc59514663 \h 44  HYPERLINK \l "_Toc59514664" 4.4. Gradient characteristics  PAGEREF _Toc59514664 \h 45  HYPERLINK \l "_Toc59514665" 4.5. Sounding...  PAGEREF _Toc59514665 \h 45  HYPERLINK \l "_Toc59514666" 4.5.1. Statistical sounding  PAGEREF _Toc59514666 \h 46  HYPERLINK \l "_Toc59514667" 4.5.2. Correlation sounding  PAGEREF _Toc59514667 \h 46  HYPERLINK \l "_Toc59514668" 4.5.3. Cross-correlation sounding  PAGEREF _Toc59514668 \h 47  HYPERLINK \l "_Toc59514669" 4.5.4. Gradient sounding  PAGEREF _Toc59514669 \h 48  HYPERLINK \l "_Toc59514670" 4.6. Estimation of anomalous object’s parameters.  PAGEREF _Toc59514670 \h 48  HYPERLINK \l "_Toc59514671" 4.6.1. Estimation by I.I. Priezzhev  PAGEREF _Toc59514671 \h 48  HYPERLINK \l "_Toc59514672" 4.6.2. Estimations by A.V. Petrov  PAGEREF _Toc59514672 \h 49  HYPERLINK \l "_Toc59514673" 4.6.3. Tracing of axes of anomaly  PAGEREF _Toc59514673 \h 49  HYPERLINK \l "_Toc59514674" 4.6.4. Depth estimation of the main anomalous surfaces  PAGEREF _Toc59514674 \h 50  HYPERLINK \l "_Toc59514675" 5. FILTERING  PAGEREF _Toc59514675 \h 51  HYPERLINK \l "_Toc59514676" 5.1. One-dimension filtering...  PAGEREF _Toc59514676 \h 51  HYPERLINK \l "_Toc59514677" 5.1.1. One-dimension filtering in the fixed window  PAGEREF _Toc59514677 \h 51  HYPERLINK \l "_Toc59514678" 5.1.2. One-dimensional polynomial filtering  PAGEREF _Toc59514678 \h 52  HYPERLINK \l "_Toc59514679" 5.1.3. One-dimensional adaptive filtration  PAGEREF _Toc59514679 \h 52  HYPERLINK \l "_Toc59514680" 5.2. Two-dimension filtering...  PAGEREF _Toc59514680 \h 53  HYPERLINK \l "_Toc59514681" 5.2.1. Two-dimension filtering in the fixed window  PAGEREF _Toc59514681 \h 53  HYPERLINK \l "_Toc59514682" 5.2.2. Two-dimensional polynomial filtering  PAGEREF _Toc59514682 \h 53  HYPERLINK \l "_Toc59514683" 5.2.3. Two-dimension adaptive filtration  PAGEREF _Toc59514683 \h 54  HYPERLINK \l "_Toc59514684" 5.2.4. Two-dimension filtering in the window of “alive form”  PAGEREF _Toc59514684 \h 55  HYPERLINK \l "_Toc59514685" 5.3. Three-dimensional filtering...  PAGEREF _Toc59514685 \h 55  HYPERLINK \l "_Toc59514686" 5.3.1. Three-dimension entropy filtering  PAGEREF _Toc59514686 \h 55  HYPERLINK \l "_Toc59514687" 5.4. Decomposition of fields  PAGEREF _Toc59514687 \h 55  HYPERLINK \l "_Toc59514688" 5.5. Compensating filtering  PAGEREF _Toc59514688 \h 56  HYPERLINK \l "_Toc59514689" 5.6. Calculation of instantaneous power  PAGEREF _Toc59514689 \h 56  HYPERLINK \l "_Toc59514690" 6. DETECTION  PAGEREF _Toc59514690 \h 57  HYPERLINK \l "_Toc59514691" 6.1. Detection of weak linear anomalies...  PAGEREF _Toc59514691 \h 57  HYPERLINK \l "_Toc59514692" 6.1.1. Method of interprofiles correlation  PAGEREF _Toc59514692 \h 57  HYPERLINK \l "_Toc59514693" 6.1.2. Method of self-tuning filtering  PAGEREF _Toc59514693 \h 58  HYPERLINK \l "_Toc59514694" 6.1.3. Detection of multi-signs linear anomalies  PAGEREF _Toc59514694 \h 58  HYPERLINK \l "_Toc59514695" 6.2. Detection of weak free form anomalies...  PAGEREF _Toc59514695 \h 59  HYPERLINK \l "_Toc59514696" 6.2.1. Method of inverse probability  PAGEREF _Toc59514696 \h 59  HYPERLINK \l "_Toc59514697" 6.2.2. Automatic variant of the method of inverse probability  PAGEREF _Toc59514697 \h 60  HYPERLINK \l "_Toc59514698" 7. COMPLEX  PAGEREF _Toc59514698 \h 61  HYPERLINK \l "_Toc59514699" 7.1. Classification...  PAGEREF _Toc59514699 \h 61  HYPERLINK \l "_Toc59514700" 7.1.1. Method of the common distance  PAGEREF _Toc59514700 \h 61  HYPERLINK \l "_Toc59514701" 7.1.2. Method of the dynamic thickenings (-mean-value method)  PAGEREF _Toc59514701 \h 62  HYPERLINK \l "_Toc59514702" 7.1.3. Classification by A.V. Petrov  PAGEREF _Toc59514702 \h 62  HYPERLINK \l "_Toc59514703" 7.1.4. Sign classification  PAGEREF _Toc59514703 \h 63  HYPERLINK \l "_Toc59514704" 7.2. Detection of multi-signs anomalies  PAGEREF _Toc59514704 \h 63  HYPERLINK \l "_Toc59514705" 7.3. Components data analysis  PAGEREF _Toc59514705 \h 64  1. Computer technology COSCAD 3Dt. 1.1. Program overview COMPLEX OF SPECTRAL-CORRELATION ANALYSIS OF THREE-DIMENSIONAL GEOPHYSICAL EVIDENCE ŤCOSCAD 3Dtť. The efficiency of the modern geological prospecting production is defined by the introduction degree to the process of the manufacturing and interpretation of geology-geophisical information of new computer technologies. At the same time the specific of geological branch predestines the usage of the most varied technologies covering practically all main trends of the modern computer industry. The enormous amounts and variety of space-indexed geology-geophisical information requires introducing of the most modern computer systems for its collection, keeping, systematization and organization of the efficient searching. Geographical data binding expects the usage of geographical searching and cartographic computer systems as well as visualization devices spatially coordinated digital information. The modern space, air, overland and deep geophysical investigations including measurements, processing and interpretation of the most varied geophisical fields is impossible without using of special computer technologies. Here with on a measurement stage the adequate software for the measuring equipment is necessary. Each geophisical method requires the own software for undertaking the qualitative processing of the primary observations. Besides the range of problems solved by means of computer technologies in the step of interpretation are very broad. Amongst them it is possible to select two main blocks. The former includes software directed to solve the inverse problems using the classical deterministic approach. The latter is based on a method of probabilistic-statistical approach and the other sections of modern applied mathematics. The original usage of these methods allow to get additional information for solving of the primary interpretation task - construction of qualitative and greatly explicated geology-geophisical model of the concrete geological object. And it is possible to continue the unlimited list of specific problems solved in the process of geological production on the base of the modern computer technologies. * * * Regrettably, recently the share of Russian computer developments in the field of geological studies is vastly decreased. First of all, this pertains to areas where traditionally the lag is existed - in the development of the geographical information systems and global databases, cartographic systems and visualization facilities. On the other hand, the colossal amount of the domestic theoretical developments in different areas of the interpretation gatherer for previous ten years are partly realized in the modern computer technologies not yielding to west analogues by quality and contents. Herewith recently it is exist the increase of amount developments solving the determined range of problems of data interpretation of gravel-magnetometry, electrometry, electromagnetic observations, processing of nucleus- radiometric data, where the Russian school is traditionally occupied the leading positions. One of such developments is a computer technology of the statistical and spectral-correlation analysis of geophysical evidence "COSCAD 3Dt", intended for analysis of three-dimensional digital geographic information by probabilistic-statistical approaches. Works of G.A.Tarhov, A.A.Nikitin, V.I.Aronov, S.A.Serkerov, D.A.Rodionov, G.V.Demura, O.A.Demidovich and others lie at the heart of the functional filling of this technology. For the first time a spectrum of the original geological problems, solved by means of probabilistic-statistical methods was marked exactly in these works. The analysis of methods and results (got by means of their first programme realisation) described in these works has allowed to work out the efficient scheme of the processing of geological-geophysical observations by probabilistic-statistical approach. In the middle eightieth the improvement and working out of algorithms of the geophisical information processing had brought to the unique computer technology "COSCAD 3Dt" and occupied determined place in the crude structure of probabilistic-statistical approach to interpretation of geophisical information. First versions of "COSCAD 3Dt" were intended just for analysis of potential geophisical fields and processing of ore-geophisical methods. At the same time a part of algorithms contained in the complex and their theoretical motivation were adopted from seismics with conversion for correct usage in data processing of the ore-geophysics. At present time the inverse process is occurred. The programme complex "COSCAD 3Dt" finds more and more usage at analysis of 2D-3D seismic information by original algorithms of statistical analysis, finding of weak anomalies, artificial perceptions and classifications. Using instruments of the weak signal finding, created for analysis of potential fields, adaptive filters, analysis and calculation of the statistic performances in sliding-scale windows, both on the whole seismic profile and on the separate horizon are of interest of seismic parameter fields analysis. The programme complex of spectral-correlation data analysis "COSCAD 3Dt" is intended for processing on digital three-dimensional regular networks of geophisical information by methods of statistical, spectral and correlation analysis, linear optimum filtering, weak anomaly finding, classifications and artificial perceptions. "COSCAD 3Dt" enables to conduct full spectral-correlation and statistical analysis of given geophisical data, calculate the Fourier spectrum, correlation functions and gradient characteristics of the geophisical data. There is wide range of linear optimum filters in this complex. Using them you can present the source field by set forming with consequent reduction of the share of the low frequencies. Unique algorithms of adaptive linear filtering are intended for processing of non-stationary fields. A programme realisation of the methods of cross-profile correlation, self-adjusting filtering, inverse probability and their multivariate analogue allows solving the problems of the weak signal finding on the background of the commensurable hindrances on amplitude. The algorithms of the complex analysis of several geology-geophisical signs and their derived on basis of the recognition and classification of complex geophisical, geochemical and geological observations methods are intended for decision of the geological zoning and mapping problems. The original database of the complex allows effectively working with digital space-portioned information, organized in three-dimensional regular grids. Service functions of the database provide information exchange between different processing modules, carry out input/output operations, allow to fragment, unite and complement of grids, fill missing values, realize the different algebraic transformations on signs etc. The graphic interface of the complex "COSCAD 3Dt" is intended for screen visualisation of information from the database in the manner of separate graphs, graphic sets, raster maps, three-dimensional objects etc. MAIN STRUCTURED AND PITHY COMPONENTS OF THE COMPLEX This software uses the original database intended for storage of the 3D (multilayer and multilevel) geology-geophisical information. For all functional procedures of the complex the input and output digital information is organized as three-dimensional regular grids. Each three-dimensional grid in the database is characterized by following parameters (shown on Fig.1.1): An amount of pickets on profile N; An amount of profiles M and number of layers NS; Distance between pickets (picket’s step) Dx, profiles (profile’s step) Dy and layers (layer’s step) Dz; Number of digital signs Kp (this parameter is use like fourth discrete dimension); The coordinates of bottom-left corner of the 3D grid X0,Y0,Z0. Except this for grid orientation in space it is possible to assign two angles U1 and U2. Accepted definition: Grid is a 3D-cube of digital regular information (possibly has several signs). Layer is identified the horizontal-plane cut of the three-dimensional grid. Vertical cut is a cut oriented in planes of the same named profiles. The parallelepiped-shaped cut in grid with size smaller then the size of full grid is called the grid fragment. Layers can be presented as data measured on different height or depth. A number of pickets, profiles and layers in grid are limited just only by resources of concrete computer. On Fig.1.1 is shown direction of right-handed coordinate system (accepted in software complex) and numbering order of pickets, profiles and layers. EMBED Word.Picture.8 Fig.1.1 The separate point in grid can be described by vector of geology-geophisical digital signs, which maximum dimensionality is limited (maximum 128 signs). For identification of the profiles and pickets in grid are used their sequence numbers. Herewith the uppermost profile of the layer always has number 1, either as extreme-left picket on profile. Any grid in the database can be described by free-form additional text information, containing not more than 56 symbols (for example area or method name). Additional information is asked by all programme modules which form (as a result of work) new grids can be filled or disregard. So, this is optional information, but its presence helps at identifications of the grid. All enumerated parameters of grids are defined by user in time of creation, but there is a possibility to edit existing grids too. The file system of “COSCAD 3Dt” database is built to minimize the average access time to data for computing and service procedures. Herewith quick access is provided to information referring to concrete profile or layer of a grid owing to increase of access time to information on the same-name pickets of the different profiles or layers in one grid. That allows optimizing the process of the access to information for the functional procedures of the program complex. Also structure of the database provides very quick access to separate sign of the grid owing to increase of access time to vector of signs in separate point of the grid. It is important that the orientation of processing procedures of the complex on analysis data organized in three-dimensional grids does not exclude efficient information handling organized in two-dimensional and one-dimensional grids (areal mapping and profiles observations). The software of the complex includes six functional blocks (modules) uniting procedures on nature of the problems solved with their help. For most processing programs of the complex "COSCAD 3Dt" the sign value of grid or several grids are input information. Such grids and signs are called input data (input grid or input sign). The grids that are formed as a result of module working are identified as output data (output grid). After successful installation of the complex "COSCAD 3Dt" it is necessary to create one or several work directories on hard disk for information accommodation. In each directory it is possible to keep up to 99 grids. It is not recommended to place data in directory where the software is situated. With information keeping in each directory it is possible to work using software of the complex keeping in chosen during installation directory (for instance in C:\COSCAD3Dt). In the main program window numbers of the networks in databank are flashed (herewith if network is exist a button corresponding to her is active, otherwise a button is disarmed). Choosing the button of existing grid it is possible to get grid’s information on parameters, edit the separate parameters and (in case of necessary) delete the grid. Required functioning program block is chosen from the main menu whereupon appears the program list containing names of the selected block functional modules. After choice of the module the dialog box with a list of start parameters will appear in the right part of the screen. Start parameters is identified as information sent to the processing program for its correct execution (as example, number of input an output grids, number of the processed sign, value of the key parameter of the program and etc.). For detailed information on start parameters of the module it is possible (at moment of their filling) to use the help (using "Help" button). Editing of start parameters is realized by keyboard keys and mouse cursor and ends when the "Start" button is pressed. Whereupon the window with messages from executing program is appeared. If as a result of working of the program the new grid is created then before termination of the messages box user will be offered enter additional symbol information about output grid. All programs of the complex of spectral-correlation data analysis "COSCAD 3Dt" are divided into six sections: service, visualization, statistics, filtering, detection and complex. In the name of each section the information about nature of the problems solved by means of falling modules is kept. SERVICE The programs given in this section are intended for database administration and provide some standard data management system functions. With help of these programs you can realize input/output of information, association and fragmentation of the grids, filling unmeasured points of the sign, interpolation and extrapolation of the grid, different data transformations etc. VISUALIZATION The complex of spectral-correlation data analysis "COSCAD 3Dt" is equipped by suitable graphic interface allowing to view 1D, 2D and 3D information from the database on the screen in the manner of separate graphs, raster maps, cubes of data etc. Except visualization programs the program for decision of the inverse problem of gravity-magnetic survey enters in the graphic block. Detailed description of these modules you can find in chapter “Visualization”. STATISTICS The programs given in this section are intended for calculation statistical, spectral and correlation descriptions of geophisical information. The analysis of these features allows to get additional useful information on target field and it helps to choose the earl of the further processing. The programs falling into group "Sounding" and "Estimation of parameters of anomaly objects" allow to evaluate the parameters of anomaly by statistical methods. FILTERING In programs of this section marketed the most wide-spread in exploratory geophysics linear optimum filters allowing to solve the tasks of field decomposition, trend removal, estimations of the form of weak anomaly. Special interest presents the unique adaptive filters allowing correct processing of the nonstationary on spectral-correlation features geophisical fields. DETECTION With the help of these programs the user can solve problems of separation of weak anomaly commensurable on amplitude with level of the noise (with linear and isometric form) using one or several signs. COMPLEX Using the programs of this section allows to solve the problems of the partition of the analyzed area on uniform areas (classes) with equal average signs value, discernment of complex anomaly on reference anomaly. Besides it is possible to undertaking component-analysis of a multi-signs data. As input information for programs of this group the values of different geology-geophisical signs and their derived gotten by means of programs from the other sections of the complex can be used. We wish you success in work! 1.2. About Authors Moscow State Geology Prospecting University  Professor, Doctor of physico-mathematical sciences, Member of the Russian Academy of Natural Sciences A.A. Nikitin  Professor, Doctor of physico-mathematical sciences, A.V. Petrov  Senior staff scientist, A.S. Aleksashin Coscad 3Dt is Copyright Š 1998-2003, MSGPU, All Rights Reserved. Moscow 2003 1.3. How to install "Coscad 3Dt"? The installation of the complex of spectral-correlation data analysis "COSCAD 3D" includes the following steps: Put the installation CD-disc into the reading device of your computer; Start the setup module COSCAD3D.EXE. (The installation password is “ANDR2001”); After successful closedown of the module COSCAD3D.EXE, the directory C:\COSCAD3D (or other, chosen by you) will be created. In this directory the special security file “SEC.BIN” will be created. Before start working with program complex you have to send us this file on E-mail:  HYPERLINK mailto:Petrov@msgpa.msgpa.ru Petrov@msgpa.msgpa.ru or  HYPERLINK mailto:AlexPetrov76@mail.ru AlexPetrov76@mail.ru with mark in subject: “SEC.BIN file from …(put you company name here)”; Within 3 days you get the file “NEWSEC.BIN” which necessary to copy in the directory C:\COSCAD3D (or other, chosen by you at installation). You need this file for correct functioning of our program. For each computer you need a unique security file; After that you copy of program will be ready to work. With any questions apply to developers on the following address: RUSSIA, MOSCOW, Mikluho-Maklaya str., 23, Department of “/  8  , room 6-16, professor A.A. Nikitin OR by E-Mail:  HYPERLINK mailto:Petrov@msgpa.msgpa.ru Petrov@msgpa.msgpa.ru or  HYPERLINK mailto:AlexPetrov76@mail.ru AlexPetrov76@mail.ru OR by telephones: (095) 420-51-47, (095) 238-21-95 call for Alex Petrov fax: (095) 438-14-38 Yours faithfully, Alex Vladimirovich Petrov! P.S. (ATTENTION!!!): Any attempts of the goal-directed breaking in uncomplicated but multifunctional program protection can bring to misbehaviour of your operating system and destruction of FAT system at your hard disk. Besides, computer piracy is pursued under the law. 1.4. FAQ and Error's handling FREQUENTLY ASKED QUESTIONS LIST: Q: In case of some visualization modules starting appears the message that DLL is absent. A: In this case address to the developer. Q: After starting of the calculation program the message that percent of the execution is a zero on screen is saved very long time. A: Restart the calculation program. If the situation is repeated address to the developer. Q: If the source grid contains the null-codes always appears the message "Unknown error". A: Most computing modules are oriented on work just with filled grids. Q: At appearance of the message "Module is absent in given version" at start of all programs address to the developer. A: Maybe you did not register your copy of program. Send us the “SEC.BIN” security file. Please, do not start simultaneously more than five functional accounting modules. This can cause the deceleration in the program and in your operating system. ERROR'S HANDLING (E – Error, D – Error description, S - suggestions) E: When work with file of the exchange “INREPORT” D: The mistake of the operating system or low disk space. S: Try to start the program again or check presence of the free space on your disk. E: Out of memory D: The grid is too large for processing by this module or too many applications are working simultaneously. S: The actions are obvious. Unload some applications and rerun the program. E: In work with file of the input data D: The error appears at operations of the institution to information from file. S: Check correctness of the data in file and their correspondence to description of the format. E: In work with file of the output data D: The error appears most often at export of given data into the other formats and is connected with absence of free disk space. S: Try to enlarge the available disc space. E: The window size is less than zero D: Negative value of one of the window size parameters. S: Correct the window size. E: Incorrect number of points of irregular grid D: The Number of points in file containing information on irregular grid does not comply with number of points given at the start of the program "Institution of irregular grid". S: Define the amount of points in irregular grid. Repeat calling of the program module "Institution of irregular grid". E: Incorrect geometric parameters of the grid OR Incorrect size of output grid D: The error appears in the procedure of the institution of the information in the database and is connected with incorrect geometric parameters of given grid (N, M, Ns, Dx, Dy, Dz etc). S: Correct the parameters of the source grid. E: Incorrect factors A, B or inadmissible values of the field D: In the procedure "Different transformations with data" factors A or B is given incorrect that does not allow to realize the selected transformation. S: Correct the factor’s values. E: Source grids do not coincide on size D: Some modules require that sizes of two input grids must have the same number of pickets, profiles and layers. S: Choose the input grids with the same size. E: The sizes of given matrixes are too small for DACF calculation. (Double-dimensional AutoCorrelation Function) D: For DACF calculation it is necessary that sizes of the grid satisfied the following requirements: number of pickets more than 7, profiles > 3 (if it is chose processing by layers) or layers > 3 (if it is chose processing by profiles). S: Choose the source grid with greater sizes or interpolate the grid. E: The sizes of given matrixes are too small for CCF calculation. (Cross-Correlation Function) D: For CCF calculation it is necessary that sizes of the grid satisfied the following requirements: number of pickets more than 5, profiles > 2 (if it is chose processing by layers) or layers > 2 (if it is chose processing by profiles). S: Choose the source grid with greater sizes or interpolate the grid. E: The sizes of given matrixes are too small for calculation D: Some modules require the restriction on minimum number of pickets, profiles and layers of the input grid. S: Interpolate the given grid with enlarging number of pickets, profiles or layers. E: The window size is too small. OR The window size is less than 3 D: Window sizes are very small for functioning of the given module. S: Enlarge window size. E: Incorrect sizes of the grid D: Sizes of the grid are very small for functioning of the given module. S: Interpolate the grid. E: Discrepancy between parameters of the source and anomalous grids D: The amount of signs at the anomalous grid less than number of analyzed signs of the source grid or given wrong borders of the master anomaly. S: Try to elaborate the reasons of the error. Repeat calling the procedure. E: Incorrect sign’s numbers D: The widespread mistake appearing when processing multi-signs grids at choice of the number of processed signs. S: Try to elaborate the reasons of the error. Repeat calling the procedure. E: Incorrect number of the input grid D: Input grid is absent or does not correspond on size for concrete module. S: Try to elaborate the reasons of the error. Repeat calling the procedure. E: Low disk space D: Current disk is full. S: Enlarge the free disc space. E: The input grid does not exist D: Number of input grid is incorrect. S: Correct the error. Repeat calling the procedure. E: Number of output grid is incorrect D: The output grid is exist already or occurred the system malfunction. S: Elaborate the mistake. If the result of the repeated start of the procedure will be negative terminate the work with complex "COSCAD 3Dt" and repeat its call. E: The amount of layers or profiles of input grid is less than 3 D: The error meets just when calling the procedures of the three-dimensional grid analysis. S: Check that grid is three-dimensional and repeat calling the program module. E: The output grid is exist already D: The output grid is exist already or occurred the system malfunction. S: Elaborate the mistake. If the result of the repeated start of the procedure will be negative terminate the work with complex "COSCAD 3Dt" and repeat its call. E: Incorrect amount of output grid signs D: The amount of signs in the output grid less than 1 or more than 128. S: Correct the error. Repeat calling the procedure. E: Error in work with temporary file D: Low free disk space. S: Enlarge the free disc space. E: Incorrect Dx, Dy or Dz of the output grid D: The distance between nearby pickets, profile or layers is less than zero. S: Correct the error. Repeat calling the procedure. E: Selected layer or profile is absent in the grid D: The layer or profile is incorrect for processing. S: Choose existing in the grid layer or profile. E: Error! The input grid is a cube or profile D: This module works just with two-dimension grids. S: If you want to process the profile convert it into layer with the program "Rotation of the grid". E: In the input grid Dx is not equal to Dy D: For given program it is necessary that input grid has to be regular i.e. Dx=Dy. S: Convert the grid into regular using programs from section "Interpolation". !!! In case of message "Unknown error" please send the letter to  HYPERLINK mailto:alexpetrov76@mail.ru alexpetrov76@mail.ru with headline "ERROR". Please, send the detail description of the situation led to error. The correction will be send to you in the shortest period. 2. SERVICE The programs given in section “SERVICE” are intended for database administration and provide some standard data management system functions. With help of these programs you can realize input/output of information, association and fragmentation of the grids, filling unmeasured points of the sign, interpolation and extrapolation of the grid, different data transformations etc. 2.1. Data input... The programs of this section are intended for inputting of digital signs measured in points of the three-dimensional (possible in two-dimensional or profile) regular grids from data-files into the database of the complex. Regular grid is a grid with determined number of pickets, profiles and layers and constant distance between nearest pickets, profiles and layers. You can not input grids with less than two pickets. If your grid with observations is not strictly parallelepiped (regular grid) it is necessary to bring it to regular before inputting to the database of the complex. So, you should fill the empty elements of your grid by any unique values (so called the dummy-code). This value (dummy-code) is used in the program of the data filling (in section "SERVICE") for recovering lacking information. 2.1.1. Inputting data from “COSCAD 3Dt” - formats The module is intended for entering of information from file. Input parameters of the module: Output grid – the result grid which will be created in the database of the complex; Input file – the full name (with path) of the input data file. The module is intended for entering of information from files prepared in the following formats: by profiles, by layers, by signs It is the format where the data in the file are prepared in symbol type with gap or comma separators in the following structure: First line: 0 - < format code> Second line: N, M, Ns, NK - Third line: XO, YO, ZO - Fourth line: Dx, Dy, Dz - Fifth line: U1, U2 - Then follows directly digital information from the first picket of the first profile of the first layer of the first sign (profile by profile, layer by layer). After the information on the first sign directly follows (in the same order) the information on the second sign etc. The amount of information in the separate lines of the source file is free, but the information for the next layer has to start with a new line. by points, by profiles, by layers It is the format where the data in the file are prepared in symbol type with gap or comma separators in the following structure: First line: 1 - < format code> Second line: N, M, Ns, NK - Third line: XO, YO, ZO - Fourth line: Dx, Dy, Dz - Fifth line: U1, U2 - Then follows directly digital information from the first picket of the first profile of the first layer of the first sign (profile by profile, layer by layer), but in contrast to the first format for each point (if input information is multi-sign) all signs of the grid are written immediately. After the first sign directly follows the second sign for the each point etc. The amount of information in the separate lines of the source file is free, but the information for the next layer has to start with a new line. by pickets, by layers, by signs It is the format where the data in the file are prepared in symbol type with gap or comma separators in the following structure: First line: 2 - < format code> Second line: N, M, Ns, NK - Third line: XO, YO, ZO - Fourth line: Dx, Dy, Dz - Fifth line: U1, U2 - Then follows directly digital information but in contrast to the first format the information in the file is situated not on profiles, but on pickets – it means that at first all first picket’s values in the layer follows then second pickets etc. After the information on the first sign directly follows (in the same order) the information on the second sign etc. The amount of information in the separate lines of the source file is free, but the information for the next layer has to start with a new line. by points, by pickets, by layers It is the format where the data in the file are prepared in symbol type with gap or comma separators in the following structure: First line: 3 - < format code> Second line: N, M, Ns, NK - Third line: XO, YO, ZO - Fourth line: Dx, Dy, Dz - Fifth line: U1, U2 - Then follows directly digital information for the first layer (picket by picket, layer by layer) but in contrast to the third format the information contains all signs for each point immediately. The amount of information in the separate lines of the source file is free, but the information for the next layer has to start with a new line. by cubes, by signs It is the format where the data in the file are prepared in symbol type with gap or comma separators in the following structure: First line: 4 - < format code> Second line: N, M, Ns, NK - Third line: XO, YO, ZO - Fourth line: Dx, Dy, Dz - Fifth line: U1, U2 - This data format is the same with the first format (by profiles, by layers, by signs), but it allows to speed up the process of the inputting of the information for small grids. If the size of the grid is very large it can occurs errors connected with shortage of the operative memory which does not appears when you use formats described above. The amount of information in the separate lines of the source file is free. The requirement that information for the each layer has to start with a new line does not spread on this format. Archive COSCAD 3Dt format It is an original software format. The main purpose of this format is the data archiving from the database of the complex in the suitable structure to quick reconstruction in the base. Archiving is realized by the "Outputting data in COSCAD 3Dt format". 2.1.2. Inputting data from SURFER format The module is intended for entering of information from the data file. Input parameters of the module: Output grid – the result grid which will be created in the database of the complex; Input file – the full name (with path) of the input data file. The module is intended for input of information from the file prepared in the data format accepted in the program SURFER 6, SURFER 7 or SURFER 8 for keeping of the coarse observations (so called GRIDs). The file can have binary or text structure. 2.1.3. Inputting data from GEOSOFT format The module is intended for entering of information from the data file. Input parameters of the module: Output grid – the result grid which will be created in the database of the complex; Input file – the full name (with path) of the input data file. The module is intended for input of information from the file prepared in the data format accepted in the computer technology GEOSOFT for keeping of the coarse observations (so called GRIDs). 2.1.4. Inputting data from SEGY format The module is intended for entering of information from the file with data. Input parameters of the module: Output grid – the result grid which will be created in the database of the complex; Input file – the full name (with path) of the input data file. The module is intended for input of information from the file prepared in the widespread format of keeping 2D seismic information - SEGY. The module works just with I1, I2, I4, R4 formats in IBM standard. 2.1.5. Inputting data from INTEGRO format The module is intended for entering of information from the file with data. Input parameters of the module: Output grid – the result grid which will be created in the database of the complex; Input file – the full name (with path) of the input data file. The module is intended for input of information from the file prepared in the data format accepted in the computer technology INTEGRO for keeping of the coarse observations (so called TOS-format). 2.1.6. Inputting data from RADAR format The module is intended for entering of information from the file with data. Input parameters of the module: Output grid – the result grid which will be created in the database of the complex; Input file – the full name (with path) of the input data file. Operating mode – the format type I2 or I4 The module is intended for input of information from the file prepared in the data format accepted in the computer technology RADAR. 2.2. Data output... Modules of the given section are intended for output of information from the database of the complex "COSCAD 3Dt" in the file on your hard disk for further keeping and using in other systems. 2.2.1. Outputting data into COSCAD 3Dt format The module is intended for output of information from the database into the file. Input parameters of the module: Input grid – the grid which will be used as a source of information to create the output file; Input sign – the number of the outputting sign. Format code – one of the following format codes. The module is intended for information output from the database into the file with one of the following formats: by profiles, by layers, by signs It is the format where the data in the file are prepared in symbol type with gap or comma separators in the following structure: First line: 0 - < format code> Second line: N, M, Ns, NK - Third line: XO, YO, ZO - Fourth line: Dx, Dy, Dz - Fifth line: U1, U2 - Then follows directly digital information from the first picket of the first profile of the first layer of the first sign (profile by profile, layer by layer). After the information on the first sign directly follows (in the same order) the information on the second sign etc. The amount of information in the separate lines of the source file is free, but the information about each layer is started with a new line. by points, by profiles, by layers It is the format where the data in the file are prepared in symbol type with gap or comma separators in the following structure: First line: 1 - < format code> Second line: N, M, Ns, NK - Third line: XO, YO, ZO - Fourth line: Dx, Dy, Dz - Fifth line: U1, U2 - Then follows directly digital information from the first picket of the first profile of the first layer of the first sign (profile by profile, layer by layer), but in contrast to the first format for each point all signs of the grid are written immediately. After the first sign directly follows the second sign for the each point etc. The amount of information in the separate lines of the source file is free, but the information about each layer is started with a new line. by pickets, by layers, by signs It is the format where the data in the file are prepared in symbol type with gap or comma separators in the following structure: First line: 2 - < format code> Second line: N, M, Ns, NK - Third line: XO, YO, ZO - Fourth line: Dx, Dy, Dz - Fifth line: U1, U2 - Then follows directly digital information but in contrast to the first format the information in the file is situated not on profiles, but on pickets – it means that at first all first picket’s values in the layer follows then second pickets etc. After the information on the first sign directly follows (in the same order) the information on the second sign etc. The amount of information in the separate lines of the source file is free, but the information about each layer is started with a new line. by points, by pickets, by layers It is the format where the data in the file are prepared in symbol type with gap or comma separators in the following structure: First line: 3 - < format code> Second line: N, M, Ns, NK - Third line: XO, YO, ZO - Fourth line: Dx, Dy, Dz - Fifth line: U1, U2 - Then follows directly digital information for the first layer (picket by picket, layer by layer) but in contrast to the third format the information contains all signs for each point immediately. The amount of information in the separate lines of the source file is free, but the information about each layer is started with a new line. by cubes, by signs It is the format where the data in the file are prepared in symbol type with gap or comma separators in the following structure: First line: 4 - < format code> Second line: N, M, Ns, NK - Third line: XO, YO, ZO - Fourth line: Dx, Dy, Dz - Fifth line: U1, U2 - This data format is the same with the first format (by profiles, by layers, by signs), but it allows to speed up the process of information output for small grids. If the size of the grid is very large it can occurs errors connected with shortages of the operative memory which does not appears when you use formats described above. The amount of information in the separate lines of the source file is free. Archive COSCAD 3Dt format It is an original software format. The main purpose of this format is the data archiving from the database of the complex in the suitable structure to quick reconstruction in the base. Archiving is realized by the "Outputting data in COSCAD 3Dt format". 2.2.2. Outputting data into SURFER format The module outputs the information from the database into the file. Input parameters of the module: Input grid – the grid which will be used as a source of information to create the output file; Input sign – the number of the outputting sign. Layer – the number of the outputting layer Profile – the number of the outputting profile !!! If both previous parameters are zero the first layer of the grid is outputted. Dummy-code – It is a code of unmeasurement data with will be changed into dummy-code of the target format. Output file – the full name of the file to output. You can browse it using the “Browse…” button Format – one of the following format-codes. BINARY SURFER format. The binary data format accepted in the program SURFER 7,8 for keeping of the coarse observations (GRIDs). Such format is intended for keeping only two-dimensional data so in this format you can output just information on one sign of the grid or by one layer or profile. ASCII SURFER format. The symbol data format accepted in the program SURFER 7,8 for keeping of the coarse observations (GRIDs). Such format is intended for keeping only two-dimensional data so in this format you can output just information on one sign of the grid or by one layer or profile. 2.2.3. Outputting data into GEOSOFT format The module outputs the information from the database into the file. Input parameters of the module: Input grid – the grid which will be used as a source of information to create the output file; Input sign – the number of the outputting sign. Layer – the number of the outputting layer Profile – the number of the outputting profile !!! If both previous parameters are zero the first layer of the grid is outputted. Dummy-code – It is a code of unmeasurement data with will be changed into dummy-code of the target format. Output file – the full name of the file to output. You can browse it using the “Browse…” button Geosoft format – the format of the GEOSOFT system for keeping 2D information 2.2.4. Outputting data into SEGY format The module outputs the information from the database into the file. Input parameters of the module: Input grid – the grid which will be used as a source of information to create the output file; Input sign – the number of the outputting sign. Layer – the number of the outputting layer Profile – the number of the outputting profile !!! If both previous parameters are zero the first layer of the grid is outputted. Dummy-code – It is a code of unmeasurement data with will be changed into dummy-code of the target format. Output file – the full name of the file to output. You can browse it using the “Browse…” button Format code – the SEGY format with IMB(I2) or IBM(R4) standard. During the process of the output it is possible to conduct online correction by some flaps of the final SEGY file. !?! Do not forget to convert the seconds into milliseconds (it is required by the format). 2.2.5. Outputting data into INTEGRO format The module outputs the information from the database into the file. Input parameters of the module: Input grid – the grid which will be used as a source of information to create the output file; Input sign – the number of the outputting sign. Layer – the number of the outputting layer Profile – the number of the outputting profile !!! If both previous parameters are zero the first layer of the grid is outputted. Dummy-code – It is a code of unmeasurement data with will be changed into dummy-code of the target format. Output file – the full name of the file to output. You can browse it using the “Browse…” button INTEGRO format – the format of the system INTEGRO for keeping 2D information (so called TOS). 2.2.6. Outputting data into GRAPHER format The module outputs the information from the database into the file. Input parameters of the module: Input grid – the grid which will be used as a source of information to create the output file; Input sign – the number of the outputting sign. Layer – the number of the outputting layer Profile – the number of the outputting profile !!! If both previous parameters are zero the first layer of the grid is outputted. Dummy-code – It is a code of unmeasurement data with will be changed into dummy-code of the target format. Output file – the full name of the file to output. You can browse it using the “Browse…” button Grapher format – it is intended for output of the one-dimension realizations being the result of the profile and the layer crossing into the popular system Grapher (the text file X,Y,F). 2.2.7. Outputting data as a common text table X,Y,Z,F (for EXCEL) The module outputs the information from the database into the file. Input parameters of the module: Input grid – the grid which will be used as a source of information to create the output file; Input sign – the number of the outputting sign. Output file – the full name of the file to output. You can browse it using the “Browse…” button EXCEL format – in the tabular text format are outputted coordinates of all points of the processed sign in the grid (X,Y,Z,F). The file of such format is easy to load from EXCEL. 2.3. Irregular grids input... Modules of this section are intended for input of any digital geology-geophisical information measured in points of the irregular grid of observations into the database of the complex. 2.3.1. Inputting of 2D irregular grids The module inputs any digital geology-geophisical information measured in points of the two-dimensional irregular grid of observations. In this module the algorithm of searching for the nearest point in the moving window is used. Input parameters of the module: You have give all coordinates and steps in metres. Output grid – the number of the result grid which will be created in the database of the complex; Minimum coordinate X – the minimum coordinate X of the formed regular grid; Maximum coordinate X – the maximum coordinate X of the formed regular grid; Minimum coordinate Y – the minimum coordinate Y of the formed regular grid; Maximum coordinate Y – the maximum coordinate Y of the formed regular grid; !!! Attention! You may leave minimum and maximum coordinates with zero values. In that case all border coordinates will be chosen automatically on the basis of the analysis of the input information. Step for X – the distance (Dx) between pickets of the created regular grid; Step for Y – the distance (Dy) between profiles of the created regular grid; !!! Attention! You may put zero values of the step. In that case this parameter will be chosen automatically. Size of the window on X – the maximum removing at the searching for the nearest point on X-axis; Size of the window on Y – the maximum removing at the searching for the nearest point on Y-axis; !!! Attention! If this parameter is a zero then restriction is not taken, but if it is -1 so the restriction is chosen automatically. Number of averaging points – minimum amount of nearest points. Usually this parameter will assign from 3 up to 25. The bigger this parameter the more time of the functioning of the program and more smoothing the result. Input file – the full name (with path) of the input file with irregular grid. Method – having regard to low-frequency components; – having regard to mid-range-frequency components; – having regard to high-frequency components; – taking into consideration just high-frequency components; The selected method has influence upon the result of the adduction of data to the regular grid. In the first case some low-frequency components of the given data will be reflected in the resulting grid, in the second case - mid-range-frequency components will be reflected and etc. It is recommended to conduct the operation of the reduction by different methods and then choose the best one. In the same way it is possible to use the module "Inputting of 2D irregular grids (2D spline)" or similar procedures from the other systems (for example, SURFER). Mode of work – allows to smooth the final result. It is recommended. The input text file must consist of three values in each line - X, Y and F separated by gaps or commas. X, Y - point coordinates of two-dimensional irregular grid and F is a value of the sign in this point (first five lines in this file may have any free text information). As a result of the program in the database of the complex the regular two-dimensional grid with fixed amount of pickets and profiles is formed. If the window size is small the created by the program regular grid can contain the dummy-code. In this case it is necessary to enlarge the window size or using the program "Filling of absent data" from the section “SERVICE” fill them out. After it (for better smoothing of information) it is possible to use the module "Adaptive filtering in the window of the alive form" from the section "FILTERING" with small basic window (3E3) for improvement quality of the filling process. Working with the start parameter window (located in the right part) it is possible to examine the point s location of your irregular grid and choose the borders for future regular grid. 2.3.2. Inputting of 2D irregular grids (2D-spline) The module inputs any digital geology-geophisical information measured in points of the two-dimensional irregular grid of observations. This module uses the algorithm of 2D spline-interpolation. Input parameters of the module: You have give all coordinates and steps in metres. Output grid – the number of the result grid which will be created in the database of the complex; Minimum coordinate X – the minimum coordinate X of the formed regular grid; Maximum coordinate X – the maximum coordinate X of the formed regular grid; Minimum coordinate Y – the minimum coordinate Y of the formed regular grid; Maximum coordinate Y – the maximum coordinate Y of the formed regular grid; !!! Attention! You may leave minimum and maximum coordinates with zero values. In that case all border coordinates will be chosen automatically on the basis of the analysis of the input information. Step for X – the distance (Dx) between pickets of the created regular grid; Step for Y – the distance (Dy) between profiles of the created regular grid; !!! Attention! You may put zero values of the step. In that case this parameter will be chosen automatically. Input file – the full name (with path) of the input file with irregular grid. Mode of work – allows to smooth the final result. It is recommended. The input text file must consist of three values in each line - X, Y and F separated by gaps or commas. X, Y - point coordinates of two-dimensional irregular grid and F is a value of the sign in this point (first five lines in this file may have any free text information). As a result of the program in the database of the complex the regular two-dimensional grid with fixed amount of pickets and profiles is formed. Working with the start parameter window (located in the right part) it is possible to examine the point’s location of your irregular grid and choose the borders for future regular grid. 2.3.3. Inputting of 3D irregular grids The module inputs any digital geology-geophisical information measured in points of the three-dimensional irregular grid of observations. In this module the algorithm of searching for the nearest point in the moving window is used. Input parameters of the module: You have give all coordinates and steps in metres. Output grid – the number of the result grid which will be created in the database of the complex; Size of the window on X – the maximum removing at the searching for the nearest point on X-axis; Size of the window on Y – the maximum removing at the searching for the nearest point on Y-axis; Size of the window on Z – the maximum removing at the searching for the nearest point on Z-axis; !!! Attention! If this parameter is a zero then restriction is not taken, but if it is -1 so the restriction is chosen automatically. Minimum coordinate X – the minimum coordinate X of the formed regular grid; Maximum coordinate X – the maximum coordinate X of the formed regular grid; Minimum coordinate Y – the minimum coordinate Y of the formed regular grid; Maximum coordinate Y – the maximum coordinate Y of the formed regular grid; Minimum coordinate Z – the minimum coordinate Z of the formed regular grid; Maximum coordinate Z – the maximum coordinate Z of the formed regular grid; !!! Attention! You may leave minimum and maximum coordinates with zero values. In that case all border coordinates will be chosen automatically on the basis of the analysis of the input information. Step for X – the distance (Dx) between pickets of the created regular grid; Step for Y – the distance (Dy) between profiles of the created regular grid; Step for Z – the distance (Dz) between layers of the created regular grid; !!! Attention! You may put zero values of the step. In that case this parameter will be chosen automatically. Number of averaging points – minimum amount of nearest points. Usually this parameter will assign from 5 up to 15. The bigger this parameter - the more time of the functioning of the program. Input file – the full name (with path) of the input file with irregular grid. Method – having regard to low-frequency components; – having regard to mid-range-frequency components; – having regard to high-frequency components; – taking into consideration just high-frequency components; The selected method has influence upon the result of the adduction of data to the regular grid. In the first case some low-frequency components of the given data will be reflected in the resulting grid, in the second case - mid-range-frequency components will be reflected and etc. It is recommended to conduct the operation of the reduction by different methods and then choose the best one. In the same way it is possible to use the module "Inputting of 2D irregular grids (2D spline)" or similar procedures from the other systems (for example, SURFER). Mode of work – is not used in the given module. The input text file must consist of four values in each line - X, Y, Z and F separated by gaps or commas. X, Y, Z - point coordinates of three-dimensional irregular grid and F is a value of the sign in this point (the first line in this file may have text information. Not more than five words). As a result of the program in the database of the complex the regular two-dimensional grid with fixed amount of pickets, profiles and layers is formed. If the window size is small the created by the program regular grid can contain the dummy-code. In this case it is necessary to enlarge the window size or using the program "Filling of absent data" from the section “SERVICE” fill them out. After it (for better smoothing of information) it is possible to use the module "3D Entropy filtration" from the section "FILTERING" with small window (5-7 points. 2.4. Interpolation of grids... Programs of the given section allow to interpolate of the regular grids (without dummy-code) using methods of linear, one- and two-dimensional spline and Fourier interpolations. 2.4.1. Liner interpolation The program allows to interpolate values of one or several signs of the grid by pickets, profiles and layers. In the program the method of linear interpolation is used. The new distances (steps) must be more than zero. Input parameters of the module: Input grid – the source grid; Sign of input grid – the processed sign of the grid; New distance between pickets – the new distance between pickets (Dx) of the output grid; New distance between profiles – the new distance between profiles (Dy) of the output grid; New distance between layers – the new distance between layers (Dz) of the output grid; Output grid – the grid containing the result of interpolation. 2.4.2. Profile spline interpolation The program allows to interpolate values of one or several signs of the grid by pickets or by profiles. In the program the method of spline interpolation is used. The new distances (steps) must be more than zero. Input parameters of the module: Input grid – the source grid; Sign of input grid – the processed sign of the grid; New distance between pickets – the new distance between pickets (Dx) of the output grid; Output grid – the grid containing the result of interpolation. Spline type – it is possible the interpolation with use of following splines: Compute the cubic spline interpolant with the 'not-a-knot' condition; Compute the Hermite cubic spline interpolant; Compute the Akima cubic spline interpolant; Compute a cubic spline interpolant that is consistent with the concavity of the data; Compute the B-spline interpolant with order 2; Compute the B-spline interpolant with order 3; Compute the B-spline interpolant with order 4; Compute the B-spline interpolant with order 5; Compute the B-spline interpolant with order 6; Evaluate a piecewise polynomial; Evaluate a function defined on a set of points using quadratic interpolation. 2.4.3. 2D Spline interpolation The program allows to interpolate values of one or several signs of the grid by pickets and profiles. In the program the method of 2D-spline interpolation is used. The new distances (steps) must be more than zero. Input parameters of the module: Input grid – the source grid; Sign of input grid – the processed sign of the grid; New distance between pickets – the new distance between pickets (Dx) of the output grid; New distance between profiles – the new distance between profiles (Dy) of the output grid; Output grid – the grid containing the result of interpolation. 2.4.4. Profile Fourier interpolation The program allows to interpolate values of one or several signs of the grid by pickets or by profiles. In the program the method of Fourier-interpolation is used. The module is very efficient at building of geological cuts. The new distances (steps) must be more than zero. Input parameters of the module: Input grid – the source grid; Sign of input grid – the processed sign of the grid; New distance between pickets – the new distance between pickets (Dx) of the output grid; Output grid – the grid containing the result of interpolation. 2.5. Extrapolation of grids This program allows to extrapolate grids on the along-profile direction and transversely of the profile strike. Input parameters of the module: Input grid – the source grid; Sign of input grid – the processed sign of the grid; Amount of points on the left – the number of extrapolated pickets on the left; Amount of points on the right – the number of extrapolated pickets on the left; Amount of points from above – the number of extrapolated profiles from above; Amount of points from below – the number of extrapolated profiles from below; Output grid – the grid containing the result of extrapolation. In the program an original algorithm to extrapolation is used. The good results are got if number of extrapolated points on the left, on the right, from below and overhand does not exceed 5-15% from the total number of pickets or profiles of the grid. For exception of edge effect appearing after usage of different modules the preliminary grid extrapolation is recommended. After undertaking of some calculations the resulting grid can be bring to the source size with the help of "Grid fragmentation" module. 2.6. Filling of absent data The program is intended for filling being absent values (so called dummy-code) in the grid. The program uses the original filling algorithm that does not cause profound changes of the spectral-correlation attributes of the field. The program works correct if the share of dummy values does not exceed 25%. Input parameters of the module: Input grid – the source grid; Sign of input grid – the processed sign of the grid; Filling value – the number complying with the dummy-code of the grid; Output grid – the full grid without dummy values. 2.7. Fragmentation of grids The program makes a new fragment-grid from any existing in the database of the complex grid. Input parameters of the module: Input grid – the source grid; Left picket – left border for a new grid by pickets; Right picket – right border for a new grid by pickets; Upper profile – upper border for a new grid by profiles; Bottom profile – bottom border for a new grid by profiles; Upper layer – upper border for a new grid by layers; Bottom layer – bottom border for a new grid by layers; Output grid – the grid containing the result of fragmentation. Amount of signs in the input and output grids are equal. Numbers of the first and last picket and the first and last profile of the input grid define fragment boundaries. 2.8. Inserting of grids This program is intended for "insertions" in the grid of the other grid with smaller size. Changing the key parameter of the method it is possible to simply impose the information being kept in the grid of the smaller size or take the average between values of the signs in the corresponding points in both grids. Input parameters of the module: Input grid – the source grid in which the fragment will be inserted; Sign of input grid – the processed sign of the source grid; Second input grid – the grid which will be implanted; Second sign of input grid – the processed sign of the second grid; Bottom-left picket – the picket defining position of the insertion in the source grid; Upper profile – the profile defining position of the insertion in the source grid; Upper layer – the layer defining position of the insertion in the source grid; Output grid – the full grid without dummy values; Insertion method – there are four ways of the fragment insertion: The First one is to completely substitutes values in the source grid with values of the fragment. The Second one is to change values of the source grid on to average between signs of both source and fragment grids. The Third one allows to realize the operation of the insertion with provision for dummy-code. It means that if the dummy-code (13131313) is present in the source grid then this point does not subject to operation of the insertion. The Last one allows filling the certain fragment by the dummy-code (131313E13). The operation of the insertion reasonable to conduct just after detailed analysis of the fragment or if the certain area is required to be filled by the dummy-code. 2.9. Rotating of grids The program allows conducting the different geometric transformations with location of pickets, profiles and layers of the source grid. Input parameters of the module: Input grid – the source grid; Output grid – the rotated grid; Rotation direction – the way of the rotation. The last parameter defines concrete transformation method: The rotation of the grid in plane of the profiles and pickets from right to left. The program realizes exactly tumbling of the source grid but not the transposition. The rotation of the grid in plane of the profiles and pickets from left to right. The program realizes exactly tumbling of the source grid but not the transposition. Changing lower profiles onto upper profiles. Changing left pickets onto right pickets. Changing lower layers onto upper layers. Changing profiles onto layers. Changing layers onto profiles. 2.10. Uniting of grids This program allows uniting some signs of different grids into one general grid. It is expected that sizes of the input grids coincide otherwise the size of the resulting grid will be determined by minimum number of pickets, profiles and layers out of two grids. Input parameters of the module: Input grid – the first uniting grid; Second input grid – the second uniting grid; Third input grid – the third uniting grid; Fourth input grid – the fourth uniting grid; Fifth input grid – the fifth uniting grid; Output grid – the result grid; The amount of the united grids can not be more than five. The concrete amount of the united grids is defined by the following rule: If, for example, the number of the third source grid equals zero then just first and second source grids will be united. The amount of united signs in each grid and their numbers are defined in the dialogue after starting of the program. The amount of signs in the resulting grid equals to total of chosen signs in all input grids. Most often the program is used before using the algorithm of multi-signs analysis of information from the section "COMPLEX" for which is necessary that all analyzed signs were found in one source grid. 2.11. Some transformations of data Different algebraic operations with one or two signs of the grid are provided in the program complex. Except algebraic transformations with data the module allows to change one definite value of the sign onto any another assigned by user. For example, it is possible to create the grid containing dummy-code in determined points from existing in the database grid (so called mask-grid) with dummy-code. Creation of the grid with dummy-code is necessary when you want to remove the results of the calculations from the grid originally putted in the database with dummy-code. 2.11.1. Transformations with one sign This module is intended for realization of the algebraic transformations with one sign of the grid. Input parameters of the module: Input grid – the source grid; Sign of input grid – the processed sign of the source grid; Output grid – the result grid; Coefficient A – the value of factor A of chosen transformation; Coefficient B – the value of factor B of chosen transformation; Coefficient C – the value of factor C of chosen transformation; Transformation type – one of the following types: Liner Ax+B; Inverse A/(x-B); Logarithmical Aln(x); Exponential Aexp(x); Power Ax^B; Changing the values equals to A onto C; Changing the values greater than A onto C; Changing the values smaller than A onto C; Absolute value |x|; Projection of grid values onto range [A,B]. It means that it is used the common linear transformation allowing to bring size of parameter changing of given data into given interval. 2.11.2. Transformations with two signs This module is intended for realization of the algebraic transformations with two signs of one or two grids. Input parameters of the module: Input grid – the source grid; Sign of input grid – the processed sign of the first source grid; Second input grid – the second grid (optional); Sign of second input grid – the processed sign of the second source grid (optional); Coefficient A – the value of factor A of chosen transformation; Coefficient B – the value of factor B of chosen transformation; Output grid – the result grid; Transformation type – one of the following types: Sum Ax + By; Product Ax * By; Division Ax / By; If in the second grid “A” is kept then on this place of the first grid will be “B”. 2.11.3. Imposition of dummy-code This module is intended for imposition of the dummy-code in the grid. Input parameters of the module: Input grid – the source grid; Sign of input grid – the processed sign of the source grid; Second input grid – the second source grid with dummy-code (so called “mask-grid”); Sign of second input grid – the processed sign of the second source grid; Dummy-code of input grid – the dummy-code of the source grid; Dummy-code of mask-grid – the dummy-code of the second source grid – “mask-grid”; Output grid – the result grid; The result grid containing dummy-code in some determined points is being built on existing in the database grid with dummy-code (so called "mask-grid"). Obviously that the grid with dummy-code and the source grid which is superimposed by dummy-code have to be equal by size (i.e. contain the alike numbers of pickets and profiles). If you had interpolate the grid during calculation then for reception of a new "mask-grid" (with new interpolated size) you have to interpolate the source grid containing dummy-code. Creation of the grid with dummy-code is necessary when you want to remove the results of the calculations from the grid originally putted in the database with dummy-code. For example, to print the result grid from SURFER. If the source grid has three-dimensions then as a result of the module functioning you will get the three-dimensional grid which will contain the dummy-code in accordance with the "mask-grid" at all layers, herewith the "mask-grid" has to be two-dimensional. 2.12. Gluing of grids This program is intended for joining (gluing or splicing) of one sign of the grid with another. Grids can stick together on profiles, pickets or layers (i.e. with front- or right- or bottom-side of the grid). Input parameters of the module: Input grid – the source grid which will be added by other; Sign of input grid – the processed sign of the source grid; Second input grid – the second source grid that will be added to the source grid; Sign of second input grid – the processed sign of the second source grid; Output grid – the result grid; Gluing method – the second grid can be glued to the first by deferent ways - to the right, below and behind. When gluing it is necessary that component parts having corresponding geometric sizes. So if you are gluing grids "on the right" it is necessary that number of profiles and layers in both grids coincided. In case of “from below”-gluing grids have to be equal by pickets and profiles. The "Gluing of unequal grids"- mode allows to stick together two-dimensional grids with different situation and size. In this case the Dx and Dy parameters of sources grids must to be equal. Grids must to be “comparable”. This means that grid with X-coordinates 100,200,300… can not be glued with grid having X-coordinates 450,550,650… Therefor for gluing these grids it is necessary that second grid had to have X-coordinates 400,500,600… or the first grid must have X-coordinates like 150,250,350… Grids can be both overlap and non-overlap. The program is used when some additional information on the under investigation territory is appeared. 2.13. Printing information into file This program is outputting values of one sign of the given grid into the print-file “printer.mga”. This file is situated in the current directory. Input parameters of the module: Input grid – the source grid; Left picket – lest border for the fragment to print by pickets; Right picket – right border for the fragment to print by pickets; Upper profile – upper border for the fragment to print by profiles; Bottom profile – bottom border for the fragment to print by profiles; Upper layer – upper border for the fragment to print by layers; Bottom layer – bottom border for the fragment to print by layers; Language – the label’s language (Russian or English). Information of the print-file can be viewed by "Viewing the print-file "-module from the section "SERVICE". 2.14. Adaptive equalization of seismic traces This program corrects defective seismic information when on different seismic traces there is different dispersion’s level. Input parameters of the module: Input grid – the source grid; Sign of input grid – the processed sign of the source grid; Output grid – the result grid; Width of base-window for estimation of dispersion – the amount of traces for average level of dispersion estimation. It is being chosen in accordance with concrete data. 3. VISUALIZATION The complex of spectral-correlation data analysis "COSCAD 3Dt" is equipped by suitable graphic interface allowing to view 1D, 2D and 3D information from the database on the screen in the manner of separate graphs, raster maps, cubes of data etc. 3.1. Raster map The program allows to view information from the database as common raster map. This module works in multiple-document interface (MDI) allowing view of information in several windows simultaneously. The grid for viewing is being selected from grid’s catalogue (main program form) before starting the program "Raster map" or immediately after module start. The module "Raster map" allows following things: You can open a new window for viewing of the grid. Choose the submenu "Select the grid" from menu "Service". Change the viewing range. Choose submenu "Viewing range" from "Service" menu. Herewith if the “Fill”-mode is selected then data with values smaller than chosen range will be filled with color corresponding to the minimum value while data with values greater than maximum range-value will be filled with color corresponding to the maximum value. If “Fill”-mode is not chosen that data out of the chosen range does not plot at all. Creation, selection and loading of a color-palette. Choose submenu "Palette" from menu "Service". The dialog of the color-palette choice will be loaded. In this dialog you may choose among existed standard palettes or build and save your own one. For making of new palette assign several white rectangles located under the current palette with any colors from the list below. For this fix the rectangle by the mouse cursor and choose the necessary color with double-click. Assigned several rectangles with colors and choose the button "Build" for viewing the palette. Changing of axial labels. Choose submenu "Coordinates" from menu "Service". Axes possible to have labels in pickets and profiles or in real coordinates. Close the current window. Choose item "Close the window" from menu "Service". Choose the concrete sign of the grid for viewing. The point "Sign" of the main menu is using for sign choice. View any cut or layer of any three-dimensional grid. For layer or cut choosing use the point "Layer/Profile" of the main menu. If the grid is two-dimensional this menu-item is not available. Map scaling. In the current window choose the area of the viewing having pressed left mouse key. After appearance of the selected area boarded with stroke line press the right button (!!! holding the left button). The selected area will be boarded with solid line. If you want to correct the fragment repeat actions described above. Then choose the point "Scale" of the main menu and choose “zoom in”. Build the graphs along the current coordinate line or along any directions. In the current window choose the spread direction of graphics having pressed left button. After appearance of the selected area boarded with stroke line holding the left button press the right button (for area fixing). The selected direction (diagonal of the chosen area) will be plotted with solid line. If you want to correct the direction repeat actions described above. Then choose the point "Graphs" from the main menu and choose item “Along the direction”. The separate window for the graphic will be appeared. Using this window you may save the text file with coordinates X,Y and values of the field F. Plotting of the chosen layer or cut of the grid. Choose the point "Visualization" of the main menu. In some cases (for example, at the beginning or at opening of a new window) the program expects the choice of the point "Visualization" before plotting of the raster map. Choosing the current window of disposing of the opened windows on the screen. The submenu "Window" from the main menu. Get the help. The point "Help" of the main window. To move between layers and profiles use following keys: PageUp, PageDown, Home and End. Edit the separate points in the interactive-mode. Choose the point to edit by mouse or by arrow-keys (Left, Right,Up,Down). Then press the “Enter” key and enter a new point value. For corrections viewing choose the point "Visualization" from the main menu. If you want to save changes to the database it is necessary to choose the point " Save changes" from the section "Service". Filling with the dummy-code of chosen squared area. In the current window choose the squared area (rectangular fragment) of the graphic having pressed left button. After appearance of the selected area boarded with stroke line holding the left button press the right button (for area fixing). The selected area will be plotted with solid line. If you want to correct the direction repeat actions described above. Then press the “Enter” key. For corrections viewing choose the point "Visualization" from the main menu. If you want to save changes to the database it is necessary to choose the point " Save changes" from the section "Service". Saving of the current profile or layer into the separate grid of the database or SURFER-format. Use the corresponding items from the section "Service" from the main menu. If the grid is two-dimensional this item does not work. Show the field gradient. Choose the point "Gradients" from the section "Service". On the plotted curve (raster map) lines are appeared. Their directions will coincide with the direction of the full gradient of given field and thier length will be corresponded with the value of the full gradient. Imposing of points onto the raster map. First of all it is necessary to prepare the text file with lines containing number triplet separated with gaps – X,Y coordinates and F value in the point. Then choose the corresponding menu item. Fragment saving allows to save the examined fragment in any chosen grid of the database. It works only when you see the fragment. Saving with new range. If you had changed the color-range it is possible (without exiting from theraster map window) to create the grid in which the information within the chosen range will be kept. Also you can make the screen shot using “Print Screen” key. During viewing process you may get values of the coordinates of any point and values of the sign in this point. You can find this information at the bottom information line under the raster map. You just have to choose the point by the mouse cursor and in the lower part of the screen coordinates X,Y,Z and importance of the sign F will be flashed. For calculation of the statistical parameters of the examined fragment choose the point "Statistics” from the section "Service". 3.2. Plotting of classification This module allows plotting and editing the grids that are created by classification programs. Besides using this module it is possible to visualize grids containing directions of anomaly strikes which are got as a result of following modules usage: the module "Two-dimensional adaptive filtering" from the section "Filtering" and "Self-tuning filtering" from the section "Detection". This module works in multiple-document interface (MDI) allowing view of information in several windows simultaneously. The grid for viewing is being selected from grid’s catalogue (main program form) before starting the program "Plotting of classification" or immediately after module start. The module "Plotting of classification" allows following things: You can open a new window for viewing of the grid. Choose the submenu "Select the grid" from menu "Service". Changing of axial labels. Choose submenu "Coordinates" from menu "Service". Axes possible to have labels in pickets and profiles or in real coordinates. Close the current window. Choose item "Close the window" from menu "Service". Change the color palette. Double click on the chosen color from rectangles at the bottom of the screen. Choose the concrete sign of the grid for viewing. The point "Sign" of the main menu is using for sign choice. View any cut or layer of any three-dimensional grid. For layer or cut choosing use the point "Layer/Profile" of the main menu. If the grid is two-dimensional this menu-item is not available. Map scaling. In the current window choose the area of the viewing having pressed left mouse key. After appearance of the selected area boarded with stroke line holding the left button press the right button. The selected area will be boarded with solid line. If you want to correct the fragment repeat actions described above. Then choose the point "Scale" of the main menu and choose “zoom in”. Build the graphs along the current coordinate line or along any directions. In the current window choose the spread direction of graphics having pressed left button. After appearance of the selected area boarded with stroke line holding the left button press the right button (for area fixing). The selected direction (diagonal of the chosen area) will be plotted with solid line. If you want to correct the direction repeat actions described above. Then choose the point "Graphs" from the main menu and choose item “Along the direction”. The separate window for the graphic will be appeared. Using this window you may save the text file with coordinates X,Y and values of the field F. Plotting of the chosen layer or cut of the grid. Choose the point "Visualization" of the main menu. In some cases (for example, at the beginning or at opening of a new window) the program expects the choice of the point "Visualization" before plotting of the raster map. Choosing the current window of disposing of the opened windows on the screen. The submenu "Window" from the main menu. To move between layers and profiles use following keys: PageUp, PageDown, Home and End. Edit the separate points in the interactive-mode. Choose the point to edit by mouse or by arrow-keys (Left, Right,Up,Down). Then press the “Enter” key and enter a new point value. For corrections viewing choose the point "Visualization" from the main menu. If you want to save changes to the database it is necessary to choose the point " Save changes" from the section "Service". Get the help. The point "Help" of the main window. Filling with the dummy-code of chosen squared area. In the current window choose the squared area (rectangular fragment) of the graphic having pressed left button. After appearance of the selected area boarded with stroke line holding the left button press the right button (for area fixing). The selected area will be plotted with solid line. If you want to correct the direction repeat actions described above. Then press the “Enter” key. For corrections viewing choose the point "Visualization" from the main menu. If you want to save changes to the database it is necessary to choose the point " Save changes" from the section "Service". Save current or choose preserved palette. Use the corresponding items from the section "Service" of the main menu. Build histograms on classes and signs. Choose the point "Building of histograms" from the section "Service". Then in right part of screen will appear K windows (K – an amount of signs on which the classification was realized). In each window the sign’s sharing in classes is expressed by colors corresponding to classes on the screen. It is possible to examine sign’s distribution in all class immediately or apart in each class - refer to point "Service". You can use the key “Print Screen” or any screen invader to make a screen shot. 3.3. Graphics The module "Graphics" builds one or several graphs on the same-name profile from several grids. It is possible to plot up to 12 different graphs simultaneously. This module works in multiple-document interface (MDI) allowing view of information in several windows simultaneously. Module’s menu has following items: Grid selection - allows to open a new window for viewing the certain sign or signs of the chosen grid. Type - allows to change the thickness of graphic’s line and to switch on/off “draw points” mode. Close the window - close the current window. Visualization - updates drawings. Scale - allows zooming in the picture and drawing graphs in the individual scale. For detailing of the viewing stretch (holding the left mouse button pressed) rectangle in the field of the plot and not releasing left button press the right mouse button. For recovering of the initial scale choose "Source scale" mode. Add - allows adding a graph of the certain sign of the chosen grid. Delete - if you are examining more than one graphics this function allows to exclude the chosen in the table graph from viewing area. Select in the table any graph and delete it. The color rounded button allows to realize dynamic (animated) viewing i.e. sequential viewing of graphs from profile to profile. The upwards/downwards arrows allow to change the current profile. The right/left arrows allow changing graphics to the right or to the left. Motion is possible only if you see just a fragment of the graph (not all profile). Getting information about the grid. Press the left mouse button in the corresponding line of the table. 3.4. Inverse problem The module "Inverse problem" solves the inverse problem of a gravimetric and magnetometric prospecting for chosen profile of the grid by means of the analytical continuation of the field in the lower half-space up to the depth of 1/3 lengths of the profile. Program’s menu has following points: Grid selection  - allows to open a new window for viewing the certain sign of the chosen grid. Parameters  - allows to choose the type of the field - magnetic field Z, magnetic field T, gravitational field and to choose parameters for magnetic field: the angle of full magnetization vector T with horizon and the angle of the vector of the magnetizing J with horizon. Visualization - updates drawings. The color rounded button allows to realize dynamic (animated) viewing i.e. sequential viewing of graphs from profile to profile. The upwards/downwards arrows allow to change the current profile. The right/left arrows allow changing graphics to the right or to the left. Motion is possible only if you see just a fragment of the graph (not all profile). Pressing left mouse button on the cut you may get the value of the depth of the current point in units of the measurement between pickets. 3.5. Viewing in projections X, Y, Z The module "3D raster cube" allows to display 3D data of the format of "COSCAD 3Dt" technology in the manner of a raster cube in projections X,Y,Z and to slice any parallelogram-fragment of the cube. The main window contains following menu items: Menu Service: Grid selection - for opening of a new grid; Points - plotting of the cube points (assigned in the file coordinates). Coordinates - axes possible to have labels in pickets and profiles or in real coordinates. Menu View: Control panel - the panel on/off switcher. Hide the cursor - hides the cursor in the visualization window; Cube boarders - boarder on/off switcher (viewing the cut); Cursor coordinates - displays the current coordinates of the mouse cursor in the visualization window; Menu management: Build the grid - builds the cube in raster mode (by default) in accordance with chosen matrix; Rebuild/Update - reconstructs the cube reflecting last change made in the active window. Update all - reconstructs all cubes in all opened window; Cut out - cuts the part of the cube in accordance with selected values of pickets, profiles, layers; Viewing range - allows: - to see the histogram of values by colors; - to change the color-palette range of the current matrix having chosen a new minimum and maximum values; Filter/range - data out of the range are not drawn / are drawn; Cuts - switch to “Cuts viewing” mode; The “Cuts viewing” mode: Palette - choose or create the palette. Plane - choose the direction to viewing planes (projection plane). Step - choose the step between plotted profiles. Growth - choose the direction of the plane’s moving (on increasing of profiles or otherwise). Animation - change the view mode (with conservation of all planes or otherwise). Play - start animation. Pause - pause animation. Stop - finish animation. When all child windows are locked the menu contains just two items: "Grid selection" and "New window". Each child window contains: - a possibility of the matrix choice by the item "Matrix" and "Sign" (the current matrix is being showed in the window’s headline); - a possibility to choosing the place of the cut in the cube ("Picket", "Profile", "Layer"); - a possibility of ready palettes choice (only in “raster”-mode); - a possibility of the building quality choice (as for “raster” so and for “class” mode): high (Hi), average (Med), low (Low). In the “raster” mode the legend shows maximum and minimum values of the displayed planes and corresponding color of the selected palette. In the “class” mode the legend shows colors of corresponding classes allowing changing the color of any classes (double click) and to look the amount of values in each class. The coordinates of the point (the cursor) inside the cube - values were provided corresponding to units of the measurement and with a provision for coordinates of the left lower corner of the grid. In the visualization window some actions can be realized by means of keyboard: Right, Left - moving between profiles; Up, Down - moving between layers; Shift+Left, Shift+Right - moving along a profile (between pickets); Enter - build the cut; Space - hide the cursor. The same actions can be realized with mouse: Moving between profiles, pickets, layers - drag over the active plain cursor (thick white line) into necessary point; Build the cut - a double click on the cube; Hide the cursor - a click outside of the cube. 3.6. Classification viewing in projections X, Y, Z The module "Classification viewing in projections X, Y, Z" allows to display 3D data of the format of "COSCAD 3Dt" technology in the manner of a raster cube in projections X,Y,Z and to slice any parallelogram-fragment of the cube. The main window contains following menu items: Menu Service: Grid selection - for opening of a new grid; Points - plotting of the cube points (assigned in the file coordinates). Coordinates - axes possible to have labels in pickets and profiles or in real coordinates. The screen invader - for conservation of the scene in the buffer (so called “screen shot”). Menu View: Control panel - the panel on/off switcher. Hide the cursor - hides the cursor in the visualization window; Cube boarders - boarder on/off switcher (viewing the cut); Cursor coordinates - displays the current coordinates of the mouse cursor in the visualization window; Menu management: Build the grid - builds the cube in raster mode (by default) in accordance with chosen matrix; Rebuild/Update - reconstructs the cube reflecting last change made in the active window. Update all - reconstructs all cubes in all opened window; Cuts - switch to “Cuts viewing” mode; Cut out - cuts the part of the cube in accordance with selected values of pickets, profiles, layers; The “Cuts viewing” mode: Palette - choose or create the palette. Plane - choose the direction to viewing planes (projection plane). Step - choose the step between plotted profiles. Growth - choose the direction of the plane’s moving (on increasing of profiles or otherwise). Animation - change the view mode (with conservation of all planes or otherwise). Play - start animation. Pause - pause animation. Stop - finish animation. When all child windows are locked the menu contains just two items: "Grid selection" and "New window". Each child window contains: - a possibility of the matrix choice by the item "Matrix" and "Sign" (the current matrix is being showed in the window’s headline); - a possibility to choosing the place of the cut in the cube ("Picket", "Profile", "Layer"); - a possibility of ready palettes choice (only in “raster”-mode); - a possibility of the building quality choice (as for “raster” so and for “class” mode): high (Hi), average (Med), low (Low). In the “raster” mode the legend shows maximum and minimum values of the displayed planes and corresponding color of the selected palette. In the “class” mode the legend shows colors of corresponding classes allowing changing the color of any classes (double click) and to look the amount of values in each class. In the visualization window some actions can be realized by means of keyboard: Right, Left - moving between profiles; Up, Down - moving between layers; Shift+Left, Shift+Right - moving along a profile (between pickets); Enter - build the cut; Space - hide the cursor. The same actions can be realized with mouse: Moving between profiles, pickets, layers - drag over the active plain cursor (thick white line) into necessary point; Build the cut - a double click on the cube; Hide the cursor - a click outside of the cube. 3.7. 3D Surface view The program allows viewing information from the database as three-dimensional surfaces. This module works in multiple-document interface (MDI) allowing view of information in several windows simultaneously. The grid for viewing is being selected from grid’s catalogue (main program form) before starting this program or immediately after loading. The module "Raster map" allows following things: You can open a new window for viewing of the grid. Choose the submenu "Select the grid" from menu "Service". Creation, selection and loading of a color-palette. Choose submenu "Palette" from menu "Service". The dialog of the color-palette choice will be loaded. In this dialog you may choose among existed standard palettes or build and save your own one. Close the current window. Choose item "Close the window" from menu "Service". Choose the concrete sign of the grid for viewing. The point "Sign" of the main menu is using for sign choice. View any cut or layer of any three-dimensional grid. For layer or cut choosing use the point "Layer/Profile" of the main menu. If the grid is two-dimensional this menu-item is not available. Plotting of the chosen layer or cut of the grid. Choose the point "Visualization" of the main menu. In some cases (for example, at the beginning or at opening of a new window) the program expects the choice of the point "Visualization" before plotting of the raster map. Choosing the current window of disposing of the opened windows on the screen. The submenu "Window" from the main menu. Get the help. The point "Help" of the main window. Hide the color scale. Hide axes labels. Change the viewing form. For using of other possibilities press the right mouse button at the surface plot. 3.8. Graphic’s map This module allows viewing information from the database in the manner of a map of graphics. This module works in multiple-document interface (MDI) allowing view of information in several windows simultaneously. The grid for viewing is being selected from grid’s catalogue (main program form) before starting the program "Graphic‘s map" or immediately after module start. The module "Plotting of classification" allows following things: You can open a new window for viewing of the grid. Choose the submenu "Select the grid" from menu "Service". Change the viewing range. Choose submenu "Viewing range" from "Service" menu. Creation, selection and loading of a color-palette. Choose submenu "Palette" from menu "Service". The dialog of the color-palette choice will be loaded. In this dialog you may choose among existed standard palettes or build and save your own one. For making of new palette assign several white rectangles located under the current palette with any colors from the list below. For this fix the rectangle by the mouse cursor and choose the necessary color with double-click. Assigned several rectangles with colors and choose the button "Build" for viewing the palette. Changing of axial labels. Choose submenu "Coordinates" from menu "Service". Axes possible to have labels in pickets and profiles or in real coordinates. Close the current window. Choose item "Close the window" from menu "Service". Choose the concrete sign of the grid for viewing. The point "Sign" of the main menu is using for sign choice. Map scaling. In the current window choose the area of the viewing having pressed left mouse key. After appearance of the selected area boarded with stroke line holding the left button press the right button. The selected area will be boarded with solid line. If you want to correct the fragment repeat actions described above. Then choose the point "Scale" of the main menu and choose “zoom in”. Build the graphs along the current coordinate line or along any directions. In the current window choose the spread direction of graphics having pressed left button. After appearance of the selected area boarded with stroke line holding the left button press the right button (for area fixing). The selected direction (diagonal of the chosen area) will be plotted with solid line. If you want to correct the direction repeat actions described above. Then choose the point "Graphs" from the main menu and choose item “Along the direction”. The separate window for the graphic will be appeared. Using this window you may save the text file with coordinates X,Y and values of the field F. Plotting of the chosen layer or cut of the grid. Choose the point "Visualization" of the main menu. In some cases (for example, at the beginning or at opening of a new window) the program expects the choice of the point "Visualization" before plotting of the raster map. Choosing the current window of disposing of the opened windows on the screen. The submenu "Window" from the main menu. Get the help. The point "Help" of the main window. Also you can make the screen shot using “Print Screen” key. During viewing process you may get values of the coordinates of any point and values of the sign in this point. You can find this information at the bottom information line under the raster map. You just have to choose the point by the mouse cursor and in the lower part of the screen coordinates X,Y,Z and importance of the sign F will be flashed. 4. STATISTICS The programs given in this section are intended for calculation statistical, spectral, correlation and gradient descriptions of geophisical information. The analysis of these features allows to get additional useful information on target field and it helps to choose the earl of the further processing. Modules of this block are realized first stage of data processing on which following problems are being solved: Analysis of statistical and spectral-correlation characteristics of a geophisical field for estimation of parameters of anomalous forming of a field and complicating hindrances (frequency spectrum, statistical and correlation characteristics, amplitude, size, directions of anomaly strikes); Calculation of statistical characteristics of geophisical fields in so-called "slithering window" and gradient characteristics which are directly analyzed in the process of the interpretation as well as can be enclosed in processing of multi-signs data by the algorithms of the artificial perception and classification; With provision of estimated statistical and spectral-correlation characteristics the earl of the further processing of the under investigation geophisical field will have been chosen; Modules of the block "STATISTICS" allow to realize full and detailed analysis of spectral-correlation characteristics of geophisical fields by means of calculation of autocorrelation functions along each profile, cross-correlation functions between separate profiles and different signs of the grid, two-dimensional autocorrelation and cross-correlation functions as well as three-dimensional autocorrelation functions. There is possibility of the estimation of one-dimension spectrums along separate profiles and two-dimension spectrums for coarse data. Procedures of the calculation of statistical characteristics of geophisical fields in one- two- and three-dimensional slithering windows allow getting fields of average, dispersion, asymmetry, kurtosis, mode, median and entropy of the analyzed geophisical field. In interpreting by fields of high order statistical moments the main interest presents the area of their extreme values checking borders of geophisical field stationary areas. Their separation raises the efficiency of the solution of the actual problem of geological zoning and mapping of any under investigation territory. Different fields of statistical parameters emphasize different not obvious details of the source field, which can be effectively used in process of the interpretation. It is possible to calculate statistical parameters of geophisical fields in dynamic windows that automatically tuning on changing of spectral-correlation characteristics of the field along profiles, on area or in space. This approach raises the accuracy of the estimation of the statistical characteristics of non-stationary geophisical fields. It is become very important because practically all geophisical observations are not stationary. In the block "STATISTICS" is included some modules for calculation of gradient characteristics of geophisical fields (gradients of the field along profiles, between and layer of the grid, full gradient and its direction). Analysis of gradient characteristics allows getting additional information about field’s structure and enhancing borders of the stationary areas and anomalous areas. Except this, there is another one very interesting procedure in this section. It is a module of the under investigation territory partition onto areas uniformed by field values and its gradient characteristics. Thus, the functional filling of this block helps to conduct the detailed analysis of geophisical fields by means of study of their statistical and gradient characteristics, different correlation functions and spectrums. 4.1. Statistical characteristics... Programs comprised into this block are intended for estimation of the statistical characteristics by field fragments or in slithering windows with fixed or dynamic sizes and in windows of so called "alive form". 4.1.1. Statistical characteristics of field fragments The program estimate the statistical characteristics of the sign of the grid or its fragment. Input parameters of the module: Input grid – the source grid; Sign of input grid – the processed sign of the source grid; Left picket – left border of grid fragment by pickets; Right picket – right border of grid fragment by pickets; Upper profile – upper border of grid fragment by profiles; Bottom profile – bottom border of grid fragment by profiles; Upper layer – upper border of grid fragment by layers; Bottom layer – bottom border of grid fragment by layers. The procedure estimates following statistical characteristics by any grid fragment: Average of distribution  EMBED Equation.DSMT4 ; Dispersion  EMBED Equation.DSMT4 ; Asymmetry  EMBED Equation.DSMT4 ; Swing  EMBED Equation.DSMT4  of the correlation coefficient  EMBED Equation.DSMT4  (m - minimum value of the argument where the auto-correlation function is a zero  EMBED Equation.DSMT4 ); Mode  EMBED Equation.DSMT4 ; Median  EMBED Equation.DSMT4  (here  EMBED Equation.DSMT4  are a function of distribution density and a function of the probability distribution of the random variate accordingly). Information got by this module is used to choice an earl of further processing of geophisical field and to estimate the stationarity of statistical and correlation characteristics of the field. Except this, by the value of the correlation coefficient (radius of correlation) the width of the one-dimensional optimum filter is chosen. Results of calculations are showed on the screen by means of module "Viewing the print file" from the section “SERVICE”. 4.1.2. Statistical characteristics in the slithering window This program calculates central statistical moments (the average, dispersion, asymmetry, kurtosis and standard) in the two-dimensional slithering window of the fixed size. Input parameters of the module: Input grid – the source grid; Sign of input grid – the processed sign of the source grid; Width of window (in pickets) – the width of the slithering window; Height of window (in profiles) – the height of the slithering window; Depth of window (in layers) – the depth of the slithering window; First incline of window – slopping of three-dimensional window in planes of layers; Second incline of window – slopping of three-dimensional window in planes of cuts; Output grid – the result grid. The program creates the grid containing five signs. The first sign is an average, the second is dispersion, the third is an asymmetry, the fourth is a kurtosis and the fifth is an attitude of dispersion to average value (If in analyzed point the average is a zero that attitude will be filled with dummy-code 131313E13. In this case use the program "Filling of absent values" from the section “SERVICE”). Analysis of values of the main statistical moments enables to get additional useful information about nature of the distribution of sign’s values. Besides, (along with the other information) these distribution characteristics can be effectively used in tasks of geological zoning by classifications programs of the complex. 4.1.3. Statistical characteristics in the one-dimensional dynamic window The program calculates six characteristics of the field of the source grid in the dynamic one-dimensional slithering along profile window. Input parameters of the module: Input grid – the source grid; Sign of input grid – the processed sign of the source grid; Width of base window (in pickets) – the base window width (!!! If zero - defined automatically); Output grid – the result grid. The program creates the grid coinciding on size with the source grid and containing six signs: Field of in-window average values; Field of dispersion; Field of asymmetry; Field of kurtosis; Factor of linear regression of the field in window; Radius of correlation. Enumerated characteristics are calculated in the slithering along profile window with variable sizes. Window width changes depending on spectral-correlation characteristics of the field defined in the base window in the vicinity of each point of the profile. The size of the base window must be not less then the power-hungriest forming of the field on the profile. This parameter can be assigned by user for all profiles of the source grid or defined for each separate profile automatically. For automatic choice of the window size it is enough to assign its equal zero. Usage of the slithering window with variable size gives more proper estimation of the statistical characteristics of the field in conditions when field is non-stationary along the profile. Analysis of values of statistical characteristics allows to any researcher to get additional useful information about particularity of any geophisical field. So, in fields of dispersions, asymmetries and kurtosis borders of anomalous object are more contrasting. By the regression factor determines the slopping of graphics in the window. The radius of correlation defines the size of an anomaly in concrete point. Besides, these distribution characteristics can be effectively used in tasks of geological zoning by other programs of the complex. 4.1.4. Statistical characteristics in the two-dimensional dynamic window This program is intended for calculation of first four statistical moments on the field of the source grid in the dynamic two-dimensional slithering window. Input parameters of the module: Input grid – the source grid; Sign of input grid – the processed sign of the source grid; Width of base window (in pickets) – the base window width (!!! If zero - defined automatically); Height of base window (in profiles) – the base window height (!!! If zero - defined automatically); Step by pickets – the parameter that allows reducing time of the calculations. If assign value of this parameter equal 2 - time of the calculations decreases in abt two times and etc. Step by profiles (or by layers) – the parameter that allows reducing time of the calculations. If assign value of this parameter equal 2 - time of the calculations decreases in abt two times and etc. Output grid – the result grid. As a result of functioning the program is formed a grid containing following characteristics of the geophisical field in each point of the grid: Field of average values; Field of dispersion; Field of asymmetry; Field of kurtosis. Enumerated characteristics are calculated in the slithering two-dimensional window with variable sizes. Window width and height changes depending on spectral-correlation characteristics of the field defined in the base two-dimensional window in the vicinity of each point of the profile. The size of the base window must be not less then the power-hungriest forming of the field. This parameter can be assigned by user or defined for automatically. For automatic choice of the window size it is enough to assign geometric parameters equal zero. Usage of the slithering window with variable size gives more proper estimation of the statistical characteristics of the field in conditions when field is non-stationary on area. Analysis of values of statistical characteristics allows to any researcher to get additional useful information about particularity of any geophisical field. So, in fields of dispersions, asymmetries and kurtosis borders of anomalous object are more contrasting. By the regression factor determines the slopping of graphics in the window. The radius of correlation defines the size of an anomaly in concrete point. Besides, these distribution characteristics can be effectively used in tasks of geological zoning by other programs of the complex. 4.1.5. Statistical characteristics in the window of “alive form” This program is intended for calculation of first four statistical moments on the field of the source grid in the two-dimensional dynamic slithering window of “alive form”. The program computes the same characteristics as in the module "Statistical characteristics in the two-dimensional dynamic window", but with greater reliability and validity. Input parameters of the module: Input grid – the source grid; Sign of input grid – the processed sign of the source grid; Width of base window (in pickets) – the base window width; Height of base window (in profiles) – the base window height; Output grid – the result grid; Working mode – the window size is assigned by user or is chosen automatically; Processing mode – processing switcher: by layers / by profiles. As a result of functioning the program is formed a five-signed grid containing following characteristics of the geophisical field in each point of the grid: Field of average values; Field of dispersion; Field of asymmetry; Field of kurtosis; Field with the dispersion to average value ratio - a standard. (If in analyzed point the average is a zero that ratio will be filled with dummy-code 131313E13. In this case use the program "Filling of absent values" from the section “SERVICE”). The usage of slithering window of the “alive form” allows getting the most reliable estimations of the statistical moments of the field in conditions when field is non-stationary on area. Analysis of values of statistical characteristics allows to any researcher to get additional useful information about particularity of any geophisical field. So, in fields of dispersions, asymmetries and kurtosis borders of anomalous object are more contrasting. The radius of correlation defines the size of an anomaly in concrete point. Besides, these distribution characteristics can be effectively used in tasks of geological zoning by other programs of the complex. 4.1.6. Estimation of the factor dispersion in the slithering window This program is intended for calculation of factor and residual dispersion in the slithering window of the fixed sizes. Factor and residual dispersion is calculated using the following formulas:  EMBED Equation.DSMT4  Number of pickets in the window (window length) is associated with amount of factors, and number of profiles - with amount of observation points for each factor. Also, the program returns factor-to-residual dispersions ratio in each point of the grid.  EMBED Equation.DSMT4  Using this field it is possible to reveal the areas, where there is influence of the factor (i.e. possibility of anomalies presence). Input parameters of the module: Input grid – the source grid; Sign of input grid – the processed sign of the source grid; Width of the window (in pickets) – width of the window; Height of the window (in profiles) – height of the window; Window’s incline (in points) – incline of the window; Output grid – the result grid. As a result of functioning the program is formed a grid containing following four characteristics in each point of the grid: Factor-to-residual dispersions ratio F; Factor dispersion Dfact; Residual dispersion Dost; Common (or total – a sum of Dfact and Dost) dispersion D. 4.2. Correlation characteristics... In this block are united some modules allowing to estimate correlation characteristics of geophisical fields: one- and two-dimensional autocorrelation functions ACF(m) and DACF(m,p), one- and two-dimensional cross-correlation functions CCF(m) and DCCF(m,p), three-dimensional autocorrelation functions TACF(m,p,s) and etc. 4.2.1. Autocorrelation function The program calculates an autocorrelation function for each profile of the source grid. Input parameters of the module: Input grid – the source grid; Sign of input grid – the processed sign of the source grid; Maximum offset of ACF(m) – maximum of the argument value m (!!! If zero - defined automatically); Output grid – the result grid. This module calculates an autocorrelation function by the following formula:  EMBED Equation.DSMT4  By the autocorrelation function you can estimate a linear size of anomaly on profile and choose the parameters of the one-dimensional optimum filter. The program creates a grid containing values of the autocorrelation function for the argument from zero up to maximum offset. Since the autocorrelation function is even that the function calculates just for positive values of the argument. Amount of profiles and layers in the resulting grid complies with amount of profiles and layers in the source grid, but amount of pickets complies with amount of offsets m for which the autocorrelation function R(m) is calculated. The value of the autocorrelation function is corresponding to zero value of the argument. Viewing the autocorrelation function by means of graphic modules allows to select the area of non-stationary correlation characteristics of the field on area. By the radius of correlation the depth of anomaly objects. 4.2.2. Cross-correlation function between profiles This program is calculates a cross-correlation function CCF(m) between neighboring profiles of the source grid layers. Input parameters of the module: Input grid – the source grid; Sign of input grid – the processed sign of the source grid; Maximum offset of CCF(m) – maximum of the argument value m of CCF(m) by pickets (!!! If zero - defined automatically); Output grid – the result grid; Processing mode – processing switcher: between neighbor profiles of layers / of cuts. Usage of this module allows to estimate the correlation relationship between observations on two neighbor profiles to a grid ( EMBED Equation.DSMT4  and  EMBED Equation.DSMT4 ) by means of estimation of their cross-correlation function:  EMBED Equation.DSMT4  Using the cross-correlation function it is possible to emphasize areas of the stationarity breach of correlation characteristic of the field, which are often connected with tectonic breaches. On values of the argument  EMBED Equation.DSMT4  corresponding to extreme values  EMBED Equation.DSMT4  it is possible to estimate the correlation directions of the field from profile to profile and energy of signal-to-noise merit  EMBED Equation.DSMT4 . It is also provided estimation of the cross-correlation function between two signs of the grid. The analysis of the cross-correlation function in this case allows to separate the areas with presence and absences of correlation between two different signs. The program creates a grid containing values of the cross-correlation function. Amount of profiles in the resulting grid is less than in the source by one. The first profile of the output grid contains values of cross-correlation function between the first and the second profile of input grid, the second profile contains values of cross-correlation function between the second and the third profile and etc. Values of the cross-correlation function are written into the output grid in following order: B(-max), B(-max+1), …, B(0), B(1), …, B(max-1), B(max), where max is the maximum of the argument value m of CCF(m) determined by user. 4.2.3. Cross-correlation function between fields This program calculates a cross-correlation function between two different signs of two grids B(m). Input parameters of the module: Input grid – the source grid; Sign of input grid – the processed sign of the source grid; Second input grid – the second source grid; Sign of second input grid – the processed sign of the second source grid; Maximum offset of CCF(m) – maximum of the argument value m of CCF(m) by pickets (!!! If zero - defined automatically); Output grid – the result grid; After functioning the program creates the grid containing values of cross-correlation function. Each profile of the resulting grid contains cross-correlation function between two signs on each of profiles. Values of the cross-correlation function between signs (by each profile) are written into the output grid in following order: B(-max), B(-max+1), …, B(0), B(1), …, B(max-1), B(max), where max is the maximum of the argument value m of CCF(m) determined by user. The analysis of the cross-correlation function allows separating the areas with presence and absences of correlation between two different signs. Except this, the big interest presents the value of the offset under which the correlation between signs on the separate profile is existed. 4.2.4. Two-dimensional autocorrelation function The module estimates correlation characteristic of the field on area by calculation of a two-dimensional autocorrelation function. Input parameters of the module: Input grid – the source grid; Sign of input grid – the processed sign of the source grid; Maximum offset of DACF(m,p) by pickets – maximum step m between pickets for the two-dimensional autocorrelation function DACF(m,p) (!!! If zero - defined automatically); Maximum offset of DACF(m,p) by profiles – maximum step p between profiles for the two-dimensional autocorrelation function DACF(m,p) (!!! If zero - defined automatically); Output grid – the result grid; Processing mode – processing switcher: calculate by layers / by cuts. This module calculates an autocorrelation function by the following formula:  EMBED Equation.DSMT4  By the two-dimensional autocorrelation function the correlation directions of the field is estimated. These directions usually comply with the spread of the most power-hungry anomaly. Analysis of the structure of the two-dimensional autocorrelation function allows to do a motivated choice of the size and slopping of window to filtering for two-dimensional linear filters. The program allows to calculate the two-dimensional autocorrelation function DACF(m,p) for signs of the grid (fully or by the cut). The two-dimensional autocorrelation function is the most important correlation function describing correlation characteristics of the field on area. By the two-dimensional autocorrelation function it is possibly to judge about presented correlation directions, which comply with spreads of the most power-hungry anomaly. 4.2.5. Two-dimensional cross-correlation function This module calculations the two-dimensional cross-correlation function between two  EMBED Equation.DSMT4  and  EMBED Equation.DSMT4  signs of the grid:  EMBED Equation.DSMT4  Input parameters of the module: Input grid – the source grid; Sign of input grid – the processed sign of the source grid; Maximum offset of DCCF(m,p) by pickets – maximum step m between pickets for the two-dimensional cross-correlation function DCCF(m,p) (!!! If zero - defined automatically); Maximum offset of DCCF(m,p) by profiles – maximum step p between profiles for the two-dimensional cross-correlation function DCCF(m,p) (!!! If zero - defined automatically); Output grid – the result grid; Processing mode – processing switcher: calculate between layers / between cuts. By means of the two-dimensional cross-correlation function are estimated the correlation relationship between two signs on the area. 4.2.6. Three-dimensional autocorrelation function This program is intended for calculation of a three-dimensional autocorrelation function TACF(m,p,k) for a sign of a grid. Input parameters of the module: Input grid – the source grid; Sign of input grid – the processed sign of the source grid; Maximum offset of TACF(m,p,k) by pickets – maximum step m between pickets for the three-dimensional autocorrelation function TACF(m,p,k) (!!! If zero - defined automatically); Maximum offset of TACF(m,p,k) by profiles – maximum step p between profiles for the three-dimensional autocorrelation function TACF(m,p,k) (!!! If zero - defined automatically); Maximum offset of TACF(m,p,k) by layers – maximum step k between layers for the three-dimensional autocorrelation function TACF(m,p,k) (!!! If zero - defined automatically); Output grid – the result grid; The three-dimensional autocorrelation function allows to study the correlation characteristics of the field in space. On the base of TACF(m,p,k) the calculation of weighting coefficients of three-dimensional filters is realized. 4.2.7. Correlation coefficient in the slithering window The Program calculations the usual correlation coefficient and the rank correlation coefficient of Spirmen between two signs in a slithering three-dimensional window with the fixed size. The window height (amount of profiles or layers) can be is 1 (to work with two-dimensional grids). Input parameters of the module: Input grid – the source grid; Sign of input grid – the processed sign of the source grid; Second input grid – the second source grid; Sign of second input grid – the processed sign of the second source grid; Window width – the window width in pickets for correlation coefficient counting; Window height – the window height in profiles (or layers) for correlation coefficient counting; Step by pickets – the parameter that allows reducing time of the calculations. If assign value of this parameter equal 2 - time of the calculations decreases in abt two times and etc. Step by profiles (or by layers) – the parameter that allows reducing time of the calculations. If assign value of this parameter equal 2 - time of the calculations decreases in abt two times and etc. Output grid – the result grid. Working mode – you may calculate the usual correlation coefficient and the rank correlation coefficient of Spirmen; Processing mode – processing switcher: by layers / by cuts. Module allows to estimate the value of the usual correlation coefficient:  EMBED Equation.DSMT4  ( EMBED Equation.DSMT4  are estimations of average values and mean square deviation of signs X and Y accordingly) and the rank correlation coefficient of Spirmen:  EMBED Equation.DSMT4  ( EMBED Equation.DSMT4  are ranks corresponding to sign values X and Y) between two signs in the slithering two-dimensional window of the fixed size. Analysis of values of correlation coefficient on area enables to select the areas of presence or absences of correlation between signs that can be effectively used in problem of geological zoning and mapping. 4.3. Spectral characteristics... Spectral analysis occupies the central place in processing of geophisical data. The decomposition of the observed field onto different frequency components already gives much information about structure of the field. Herewith, it is important to emphasize the applicability of spectral analysis for description characteristics of geophisical fields given as deterministic or casual functions. Spectral analysis has very broad and varied possibilities in filtering of raw data, estimation of inaccuracy and comparison of data processing efficiency. This section contains the modules of calculation of the univariate Fourier spectrum and two-dimensional quick Fourier transformation. 4.3.1. Univariate spectrum The program calculates the Fourier spectrum for each profile of the grid. Input parameters of the module: Input grid – the source grid; Sign of input grid – the processed sign of the source grid; Output grid – the result grid. By means of this procedures it is possible to calculate the amplitude  EMBED Equation.DSMT4  and phase  EMBED Equation.DSMT4  Fourier spectrums on all profiles of the grid (where  EMBED Equation.DSMT4 ,  EMBED Equation.DSMT4  and m is a harmonica number, N is an amount of pickets of the grid profile). The program creates the two-signs grid: energy spectrum for frequencies from zero up to Naykvist frequency and phase spectrum for the same frequencies. Amount of profiles and layers in the resulting grid complies with amount of profiles and layers in the source grid, but amount of pickets is a half plus one concerning to amount of pickets in the source grid plus one. This complies with amount of harmonicas in a spectrum. The first picket in the resulting grid corresponds to the first (zero) spectrum harmonica and etc. 4.3.2. Two-dimension spectrum This program realizes the algorithm of quick two-dimensional Fourier transformation in suggestion that number of pickets and profiles in the grid is multiple to degree of numbers two, three, five or seven. Input parameters of the module: Input grid – the source grid; Sign of input grid – the processed sign of the source grid; Output grid – the result grid; Processing mode – processing switcher: by layers / by cuts. If sizes of the grid do not satisfy to the putted condition than they will be automatically cut with minimum losses of information for estimation of the two-dimensional spectrum. The program creates the grid containing three signs: energy, phase and amplitude spectrums. The first picket of the first profile of the resulting grid contains values of the spectrum corresponding to zero frequency on pickets and zero frequency on profiles (layers). The last picket of the last profile in the resulting grid contains values of the spectrum corresponding to Naykvist frequency on pickets and profiles (layers). Analysis of the two-dimensional spectrum allows to estimate the spectral composition of the field, amplitudes composing its harmonicas and anomaly parameters presented by low-frequency part of spectrum and noise presented by high-frequency part of spectrum. 4.4. Gradient characteristics The given program calculates of the field gradient along profiles or transversely profiles spread, between layers of the grid, full gradient of the field and directions of the full gradient in plane of the layers or in cut’s plane. The direction of the full gradient calculates in radians. Input parameters of the module: Input grid – the source grid; Sign of input grid – the processed sign of the source grid; Output grid – the result grid. When the two-dimensional grid is processing the four-signs grid is formed: First sign – a gradient of the field along profiles. Second sign – a gradient of the field between profiles (layers). Third sign – a full gradient in a plane of profiles (layers) and pickets. Fourth sign – a direction of the full gradient When the three-dimensional grid is processing the grid with eight signs is formed: First sign – a gradient of the field along profiles. Second sign – a gradient of the field between profiles. Third sign – a full gradient in a plane of profiles and pickets. Fourth sign – a direction of the full gradient in a plane of profiles and pickets in degrees. The direction N-S corresponds to the 90 degrees angle and direction E-W corresponds to the angles 0 and 180 degrees. Fifth sign – a gradient of the field between layers. Sixth sign – a full gradient in a plane of layers and pickets. Seventh sign – a direction of the full gradient in a plane of layers and pickets in degrees. Eighth sign – a direction of the full gradient in the space XYZ. Analysis of gradient characteristics of the field enables to get for researcher additional useful information about particularity of a geophisical field. The borders of anomalous object on corresponding directions are risen above in gradient fields. When interpreting it is necessary to account following: Borders of anomalous objects are noted by extremums in the field gradient along axes and by maximums in the fields of the full gradient; By extremums in fields of gradient characteristics borders of anomalies with different amplitudes are noted, that allows to see simultaneously sidebars anomaly of different amplitudes during the visualization; Gradient characteristics along a certain direction allow to emphasize the borders of anomaly with perpendicular spread for this direction; The field of the full gradient direction allows to estimate anomaly spread in each point of the source grid of the observations, but contrasting transition from minimum values to maximum checks the position of the anomaly’s axes. Along with the other information these characteristics of the field can be used in tasks of geological zoning taxonomic programs of the complex. Most effectively, by means of gradient characteristics, dares tasks of the highlighting of the borders between anomalies or stationary areas. 4.5. Sounding... In this section are presented programs realizing original approach to estimation the changes in statistical and correlation characteristics (with depth) of the field on the base of their calculation in slithering windows with different sizes. The possibility of using of probabilistic-statistical methods at building of physico-geological models and estimation of geometric parameters anomalies object are considered. 4.5.1. Statistical sounding This program calculates first four central statistical moments in the window with different sizes with forming of the three-dimensional grids. Herewith, the first layer to the resulting grid is the result of moment’s calculation in the window with minimum size and the last layer - with maximum size of the window. Input parameters of the module: Input grid – the source grid; Sign of input grid – the processed sign of the source grid; Start window size – the initial size of the base slithering window in which the radius to correlation is estimated; (!!! If zero - defined as 3) Final window size – the final size of the base slithering window in which the radius to correlation is estimated; (!!! If zero - defined as 0.5*MIN[amount of pickets or profiles]); Step of detailing in points – the step of the window sizes changes (from initial to final size). Than the value of this parameter bigger than accounting time is less. Herewith the quality of the final result is falling. Output grid – the result grid. After calculations the three-dimensional grid coinciding on pickets and profiles with the source one is being formed. Amount of layers of the resulting grid is defined by expression: [final – initial window sizes]/2+1. Amount of signs in the resulting grid is 4. The first sign contains the average value in the window, the second – the dispersion, the third – the asymmetry and the fourth – the kurtosis. Each layer of the resulting grid contains values of the statistical moments calculated in windows with corresponding sizes. The first layer of the resulting grid corresponds to the window with "initial size", the last - "final size". The proposed statistical sounding allows to track the changes in statistical characteristics computed in slithering windows depending on the analyzed forming frequencies of the field. Thus, the first layer of will present values of the statistical moments of high-frequency forming of the field, the last one - an low-frequency forming. Considering the fact that extreme values of the field of dispersions, asymmetries and kurtosis is checking areas of stationary breaches, it is possible to track the position of these borders for different (on size and locations) geological objects. 4.5.2. Correlation sounding This program calculates the two-dimensional correlation radius of areal data. The correlation radius is written into the resulting grid with minus sign. For example the value r=-5090.3 follows to interpret as r=5090.3. The minus sign is putted because of orientation of the Z-axis. Thereby, for example, values r=-100.2 and r=-320.1 are indicative that in the second event anomaly source is situated deeper then in the first one. Input parameters of the module: Input grid – the source grid; Sign of input grid – the processed sign of the source grid; Start window size – the initial size of the base slithering window in which the radius to correlation is estimated; (!!! If zero - defined as 3) Final window size – the final size of the base slithering window in which the radius to correlation is estimated; (!!! If zero - defined as 0.5*MIN[amount of pickets or profiles]); Step of detailing in points – the step of the window sizes changes (from initial to final size). Than the value of this parameter bigger than accounting time is less. Herewith the quality of the final result is falling. Output grid – the result grid. After calculations the three-dimensional grid coinciding on pickets and profiles with the source one is being formed. Amount of layers of the resulting grid is defined by expression: [final – initial window sizes]/2+1. The each layer of the resulting grid contains the correlation radius value calculated in the window with corresponding sizes. The first layer of the resulting grid corresponds to the window with "initial size" and the last - "final size". The more size of the window the more depth of the sounding of anomalous sources. Thereby, assigning different values of the interval of the window’s size changing you are sounding the position of anomalous sources on the determined interval of the depths. It is recommended the joint interpretation of results got by means of the given module and by the program "Statistical estimation of anomalous object’s parameters". The question of the two-dimensional correlation radius determination is very actual because it allows to estimate the depth of the sources anomaly location by formulas gotten by S.A. SERKEROV for data of gravitational and magnetic explorations. For the estimation of the true depth of the sources multiply the location the field of the correlation radius on the corresponding factor (see S.A. SERKEROV) having used by program "Some transformations of data " from the section "SERVICE". Working with the program it is recommended to execute the following actions: Using the procedure "Interpolation of grids" from the section "SERVICE" bring the source grid to uniform (dx=dy) because the procedure works just with uniform grids; For increasing of the program efficiency extrapolate the grid with usage of the module "Extrapolation of grids" with zero value of amount points of extrapolations beforehand. Herewith the source grid will be added on the left and on the right by additional pickets and from above and from below by additional profiles. The amount of added points will be approximate 0.1 from the amount of pickets and profiles; The maximum window’s size for processing of the extrapolated grid must be not greater than 0.5*MIN[amount of pickets or of profiles] of the source (before extrapolation) grid; After processing of the extrapolated grid by this program (for reduction of the resulting grid to the source size) use the module "Fragmentation of grids " having sliced extrapolation points; The input parameter "Step of detailing in points" allows to reduce time of the calculations. Than the value of this parameter bigger than less the accounting time. Herewith the quality of the final result is falling. 4.5.3. Cross-correlation sounding This program calculates the correlation coefficient in the slithering window of the different size and forms the three-dimensional grid. Herewith, the first layer of the resulting grid is the calculation result of the correlation coefficient in the window with minimum size, the last layer - with maximum window size. Input parameters of the module: Input grid – the source grid; Sign of input grid – the processed sign of the source grid; Second input grid – the second source grid; Sign of second input grid – the processed sign of the second source grid; Start window size – the initial size of the base slithering window in which the radius to correlation is estimated; (!!! If zero - defined as 3) Final window size – the final size of the base slithering window in which the radius to correlation is estimated; (!!! If zero - defined as 0.5*MIN[amount of pickets or profiles]); Step of detailing in points – the step of the window sizes changes (from initial to final size). Than the value of this parameter bigger than accounting time is less. Herewith the quality of the final result is falling. Output grid – the result grid. After calculations the three-dimensional grid coinciding on pickets and profiles with the source one is being formed. Amount of layers of the resulting grid is defined by expression: [final – initial window sizes]/2+1. The each layer of the resulting grid contains the correlation coefficient calculated in the window with corresponding sizes. The first layer of the resulting grid corresponds to the window with "initial size" and the last - "final size". The step value is 1 by default. The proposed cross-correlation sounding allows to track the correlation relationship changes depending on analyzed frequency forming of the source field. The first layer of the resulting grid will characterize the correlation relationship between fields high-frequency forming, the last - an low-frequency forming. 4.5.4. Gradient sounding This program calculates gradient characteristics with consequent discharging of the source grid. Such procedure allows to research changes of gradient characteristics with depth. Herewith, the first layer of the resulting grid is a result of the gradient characteristics calculation with minimum source grid discharging, the last layer - with maximum discharging. Input parameters of the module: Input grid – the source grid; Sign of input grid – the processed sign of the source grid; Start grid discharging – the initial discharging in points; (!!! If zero - defined as 1) Final grid discharging – the final discharging in points; (!!! If zero - defined as 0.25*MIN[amount of pickets or profiles]); Step of discharging in points – the step of the discharging changes (from initial to final). Than the value of this parameter bigger than accounting time is less. Herewith the quality of the final result is falling. Output grid – the result grid. After calculations the three-dimensional grid coinciding on pickets and profiles with the source one is being formed. Amount of layers of the resulting grid is defined by expression: [final – initial window sizes]/2+1. After processing the four-signs grid is formed: First sign – a gradient of the field along profiles. Second sign – a gradient of the field between profiles (layers). Third sign – a full gradient in a plane of profiles (layers) and pickets. Fourth sign – a direction of the full gradient 4.6. Estimation of anomalous object’s parameters. This section contains modules allowing to estimate anomalous object’s parameters by means of usage probabilistic-statistical methods of the data analysis. 4.6.1. Estimation by I.I. Priezzhev The program calculates the equivalent sharing the masses of the sources at the depth. Input parameters of the module: Input grid – the source grid; Sign of input grid – the processed sign of the source grid; Layer of input grid – the processed layer of the source grid; Angle of T-vector with horizon – the angle of the full vector of the magnetic field T with horizon; Angle of J-vector with horizon – the angle of the vector of the magnetizing J with horizon; Output grid – the result grid; Field type – it is possible to solve the inverse problem for vertical forming magnetic field dZ, gravitational field or for the full vector of the magnetic field dT. After functioning the program forms the grid with N pickets, M profiles and N/3 layers (where N is amount of pickets and M is amount of the profiles of the source grid). In each point of the gotten cube the relative density of the sources magnetic or gravitational field is kept. The distance between layer of the resulting grid is a distance between pickets of the source grid that allows to estimate the position of outraging solids. 4.6.2. Estimations by A.V. Petrov This program is intended for estimation of the geometrical and relative sharing of masses of the anomalous sources. The program is based on integrated usage of statistical, spectral-correlation methods and the algorithm of adaptive filtering in the window of the “alive form”. Input parameters of the module: Input grid – the source grid; Sign of input grid – the processed sign of the source grid; Start window size – the initial size of the base slithering window in which the radius to correlation is estimated; (!!! If zero - defined as 3) Final window size – the final size of the base slithering window in which the radius to correlation is estimated; (!!! If zero - defined as 0.5*MIN[amount of pickets or profiles]); Step of detailing in points – the step of the window sizes changes (from initial to final size). Than the value of this parameter bigger than accounting time is less. Herewith the quality of the final result is falling. Output grid – the result grid; Method – it is possible to solve the problem using the adaptive energy filtering, entropic filtering, median filtering and simple averaging in a window. As a result of calculations the three-dimensional grid is formed. This grid contains 3 signs and coinciding on pickets and profile with the source one. Amount of layers of the resulting grid is defined by expression: [final – initial window sizes]/2+1. First sign – an equivalent masses sharing. Second sign – masses sharing located on small depth (similarly to downward recalculation). Third sign – an analogue of the upward recalculation. It is recommended the joint interpretation of results gotten by means of the given module and programs "Correlation sounding", "Statistical sounding" and "Cross-correlation sounding". 4.6.3. Tracing of axes of anomaly This program is intended for tracing of anomaly with different energy from profile to profile. For tracing the original modification of the univariate adaptive filtering is used. Input parameters of the module: Input grid – the source grid; Sign of input grid – the processed sign of the source grid; Minimal anomaly size – the size in points of the most short selected anomalies; Threshold in % from mean square deviation – a parameter allowing to adjust the sensitivity of the algorithm. The less value of the parameter the bigger the sensitivity to weak anomaly. Output grid – the result grid; Working mode – a size of the selected anomaly can be assigned by user or chosen automatically. As a result of functioning the program is formed the grid containing two signs. The first sign contains the statistics with maximums correspond to the axes of positive anomalies and minimums - axes of negative anomalies. Second sign contains parameter which can takes three values: 1 – the positive anomaly is present; -1 – the negative anomaly is present; 0 – Nothing is present. Working with the program it is necessary to bear in mind that well tracing anomaly axes located across to the profile’s spread. For highlighting of anomaly spreads with the same direction as the profile’s spread it is recommended to turn the grid on 90 degrees left to right, or right to left using the module "Rotation of grids". 4.6.4. Depth estimation of the main anomalous surfaces This program is intended for evaluation of depths of the main gravel-magnetic surfaces on the base of the analysis of the logarithm of spectrum in slithering window and field’s correlation radius. Input parameters of the module: Input grid – the source grid; Sign of input grid – the processed sign of the source grid; Layer of input grid – the processed layer of the source grid; Radius of the window – the most important parameter of the algorithm, assigned in the grid’s points. It has to be assigned in 3-5 times greater than the expected depth of the main gravel-magnetic surfaces; Step of detalization – the step (in points of the grid) in which the estimation of the depth will be realized. It is recommended to conduct the estimation in each fifth point of the source grid; Working mode – with trend removing and without removing; Output grid – the result grid. It is recommended to choose the mode with trend removing. As a result of functioning the program is formed a grid, coinciding on size with the source one and containing 3 signs. The first sign contains the evaluation of an upper edge of the main gravel-magnetic surface on the base of analysis of the logarithm of the spectrum. The second one contains a lower edge. The last one contains the estimation of a lower edge of main gravel-magnetic surface on the base of analysis of the correlation radius. 5. FILTERING Trend-analysis and filtering of geophisical fields occupy the most important place in the processing of geology-geophisical data. Program modules realizing this stage of the processing are united in the block "FILTERING" of the computer technology "COSCAD3Dt". They allow to solve the following problems of the processing and interpretation of geology-geophisical observations: Separations of fields on components with estimation of the form and parameter separated component; Estimations of the form of low-frequency trend forming of geophisical fields; Separations and estimations of the form of weak anomalies with the amplitude commensurable or less than noise level. This block includes the original realizations of one-, two- and three-dimensional Viner’s, matched and energy optimum filtering, algorithms of entropy filtering solving a problem of the efficient processing of (geochemical, radiometric, ecological) geophisical fields with presence of hurricane values. In this block different modifications of one- and two-dimensional polynomial filters are broadly presented. The each module in the given block was developed with provision of following principle positions: Abilities of the correct functioning of the algorithm in conditions of the absence to a priori information on spectral-correlation characteristics of useful signals and noise that is corresponds to the most often existing situation when the real geology-geophisical observations are processing; Possibilities of the processing of very-large arrays of input information within the frames of real time intervals; The maximum account in the algorithm of non-execution of the requirement of data stationarity; Realizations of the program of the concrete filter in time area for the reason of exceptions of disadvantage effects connected with distortion of useful signal and noise parameters when turning into and out of the spectral area using the Fourier transformation. 5.1. One-dimension filtering... Different realizations of univariate filters are presented in this section. 5.1.1. One-dimension filtering in the fixed window This program is intended for on-profile filtering of data in the grid. Input parameters of the module: Input grid – the source grid; Sign of input grid – the processed sign of the source grid; Window size (in pickets) – the size of filtration window (!!! If zero - defined automatically); Output grid – the result grid; Working mode – the base window size can be assigned by user or chosen automatically; In this program there are several on-profile filters: Univariate energy filtering – this filter occupies the intermediate position between the Kolmogorov-Viner’s filter and the detection filter. The criterion of an optimal signal on output of this filter is a maximization of energy signal-to-noise merit. Univariate entropy filtering – allows to process fields with presence of hurricane values (geochemical, radiometric etc.) Univariate median filtering – calculates the median in slithering window. Univariate correlation filtering – is useful for estimation of the noise in the small-size window and least of all changes the data. Univariate trend filtering – efficient in problems of trend removing. Averaging in the univariate window – calculates average in the slithering window. After functioning the program creates the grid containing two signs: 1st is local (remaining) and 2nd - regional (trend) forming of the source grid. 5.1.2. One-dimensional polynomial filtering This program is intended for on-profile filtering of separate signs of the grid using approximation of field values on profile with polynomials (degrees from 1 up to 49). Input parameters of the module: Input grid – the source grid; Sign of input grid – the processed sign of the source grid; Window size (in pickets) – the size of filtration window (!!! If zero - defined automatically); Degree of polynomial P – the degree of approximating polynomial P<50; Output grid – the result grid; Working mode – the base window size can be assigned by user, taken equal to profile length or chosen automatically. There is a possibility to conduct filtering in the window mode (in slithering along profiles window) and in mode of the building approximating polynomial on all point of the profile. In the last case the window width is assigned equal to the profile length in pickets. Usage of this program is effectively in processing of any types of geophisical fields. The dignity of this algorithm is a possibility to change the frequency characteristics of the signal on outputting of the filter and to change the degree of approximating polynomial. So, the less the polynomial degree the less of high-frequency components remains in the output signal of this filter. The program creates the grid containing two signs: local (remaining) and regional components of the source field. 5.1.3. One-dimensional adaptive filtration This program is intended for on-profile filtering of geophisical fields by an adaptive filter. The univariate adaptive filter allows effectively processing the non-stationary along profile fields. Input parameters of the module: Input grid – the source grid; Sign of input grid – the processed sign of the source grid; Size of base window (in pickets) – the size of the base filtration window (!!! If zero - defined automatically); Step by pickets – the parameter that allows reducing time of the calculations. If assign value of this parameter equal 2 - time of the calculations decreases in abt two times and etc. Output grid – the result grid; Filter type – there are several filters in this program: correlation, energy, entropy, median filtering and simple time averaging. Working mode – the base window size can be assigned by the user or chosen automatically; In contrast to usual filters, which do not change their own parameters during the filtering process, the given filter automatically changes values of weighting coefficients and size of the filtering window depending on changes of spectral-correlation characteristics in a vicinity of the base window in each points of the field. This allows to process the non-stationary on spectral-correlation characteristics geophisical fields correctly. The size of the base window must be odd and not more than the lengths of the most power-hungry component of the field on profile and not less than three. This parameter can be assigned by user or be chosen automatically if assign its value equal zero. The program creates the grid containing two signs: 1st sign is a local (remaining) component and 2nd sign is a regional (the most power-hungry) component of the given field. 5.2. Two-dimension filtering... Different realizations of two-dimensional filters are presented in this section. 5.2.1. Two-dimension filtering in the fixed window This program is intended for two-dimensional filtering of the field for division reasons onto regional and local components by using of two-dimensional energy and entropy filtering. Input parameters of the module: Input grid – the source grid; Sign of input grid – the processed sign of the source grid; Window width (in pickets) – the width of the filtration window (!!! If zero - defined automatically); Window height (in profiles/layers) – the height of the filtration window (!!! If zero - defined automatically); Incline of filtration window – the slopping of the filtration window; Output grid – the result grid; Filtration type – energy filter, which is maximize the energy signal-to-noise merit on the output. The filter occupies intermediate position between the Kolmogorov-Viner’s filter and the detection filter; entropy filter, which is intended for filtering of fields with presence of hurricane values (geochemical, radiometric etc.); Processing mode – two-dimensional filtering can be provided by layers and by cuts of the source grid. The filtering window sizes are chosen on the base of the analysis of two-dimensional autocorrelation function of the source grid or are assigned coming from nature of the problem. Obviously that the more the window size the less the share of the high frequency in the trend component. The program creates the grid containing two signs: the local (remaining) and the regional components of the source field. 5.2.2. Two-dimensional polynomial filtering This program is intended for division of the field onto the regional and the local components by building of the two-dimensional polynomial (from zero up to ninth degree inclusive). This filtering is realized in two-dimensional slithering window with the fixed size. The window can move along the profile or by profiles with bigger than unit step that allows to enlarge the velocity of the performing the program. Input parameters of the module: Input grid – the source grid; Sign of input grid – the processed sign of the source grid; Window width (in pickets) – the width of the filtration window (!!! If zero - defined automatically); Window height (in profiles/layers) – the height of the filtration window (!!! If zero - defined automatically); Step by pickets – the parameter that allows reducing time of the calculations. If assign value of this parameter equal 2 - time of the calculations decreases in abt two times and etc. Step by profiles (or by layers) – the parameter that allows reducing time of the calculations. If assign value of this parameter equal 2 - time of the calculations decreases in abt two times and etc. Output grid – the result grid; Working mode – the base window size can be assigned by user, chosen automatically or taken equal to profile length. In the last case the window width is assigned equal to the profile length in pickets. Processing mode – two-dimensional filtering can be provided by layers and by cuts of the source grid. The filtering window sizes are chosen on the base of the analysis of two-dimensional autocorrelation function of the source grid or are assigned coming from nature of the problem. Obviously that the more the window size the less the share of the high frequency in the trend component. Usage of this program is effectively in processing of any types of geophisical fields. The dignity of this algorithm is a possibility to change the frequency characteristics of the signal on outputting of the filter and to change the degree of approximating polynomial. So, the less the polynomial degree the less of high-frequency components remains in the output signal of this filter. Except this the automatic orientation of approximating polynomial onto the correlation direction of the field in window, draws near this filter to adaptive in processing of non-stationary on area geophisical fields is processing. The program creates the grid containing two signs: the local (remaining) and the regional components of the source field. 5.2.3. Two-dimension adaptive filtration The program is intended for two-dimensional adaptive filtering of geophisical fields. Input parameters of the module: Input grid – the source grid; Sign of input grid – the processed sign of the source grid; Window width (in pickets) – the width of the filtration window (!!! If zero - defined automatically); Window height (in profiles/layers) – the height of the filtration window (!!! If zero - defined automatically); Step by pickets – the parameter that allows reducing time of the calculations. If assign value of this parameter equal 2 - time of the calculations decreases in abt two times and etc. Step by profiles (or by layers) – the parameter that allows reducing time of the calculations. If assign value of this parameter equal 2 - time of the calculations decreases in abt two times and etc. Output grid – the result grid; Filter type – there are several filters in this program: energy, entropy, median filtering and simple time averaging. Working mode – the base window size can be assigned by the user or chosen automatically; Processing mode – two-dimensional filtering can be provided by layers and by cuts of the source grid. Essentially the two-dimensional adaptive filtering of geophisical fields is reduced to automatic changing of filter parameters (width, height, slopping filtering window and weighting coefficient) when some spectral-correlation characteristics of the field is changing in vicinity of the base window for each point of the field. Base window sizes are assigned by a user and must be not less than sizes of the most power-hungry component of the field. Usually the size is chosen on the base of analysis of two-dimensional autocorrelation function of the source grid. The usage of this two-dimensional adaptive filter allows effectively processing the non-stationary on area (by spectral-correlation characteristics) fields. Since majority of real observed fields are non-stationary on area the usage of this program gives the more correct results than usage of usual two-dimensional filters with constant parameters. In the sense of optimum criterion of output signal in this module several filters are marketed: energy filter, which is maximize the energy signal-to-noise merit; entropy filter - intended for filtering of non-potential (the radiometric, geochemical fields with presence of hurricane values) and simple time averaging in window. The program creates the grid containing four signs: the local (remaining) field, the regional field (trend), the slop of filtering window (i.e. the direction of correlation of the field in the point) and the radius to correlation for estimation of occurrence depth of anomalous objects. The direction is defined by offset (expressed in pickets) of correlation directions on the following profile relatively to previous. The positive direction corresponds to increase of the sequence number of pickets, negative – to their reduction. 5.2.4. Two-dimension filtering in the window of “alive form” It is the BEST program for two-dimensional filtering of non-stationary geophisical fields. Input parameters of the module: Input grid – the source grid; Sign of input grid – the processed sign of the source grid; Base window width (in pickets) – the width of the base filtration window; Base window height (in profiles/layers) – the height of the base filtration window; Output grid – the result grid; Filter type – there are several filters in this program: energy, entropy, median filtering and simple time averaging in the window of “alive form”. Working mode – the base window size can be assigned by the user or chosen automatically; Processing mode – two-dimensional filtering can be provided by layers and by cuts of the source grid. The filtering window sizes are chosen on the base of the analysis of three-dimensional autocorrelation function of the source grid. The program creates the grid containing two signs: the local (remaining) and the regional components of the source field. 5.3. Three-dimensional filtering... In this section three-dimensional entropy and median filters are presented. 5.3.1. Three-dimension entropy filtering Program is intended for three-dimensional filtering of the field. Input parameters of the module: Input grid – the source grid; Sign of input grid – the processed sign of the source grid; Window width (in pickets) – the width of the filtration window (!!! If zero - defined automatically); Window height (in profiles/layers) – the height of the filtration window (!!! If zero - defined automatically); Window depth (in layers) – the depth of the filtration window (!!! If zero - defined automatically); First incline of filtration window – the slope of the filtration window in a plane of pickets and profiles; Second incline of filtration window – the slope of the filtration window in a plane of pickets and layers; Output grid – the result grid; Filter type – there are two adaptive filters in this program: energy and median filtering. The filtering window sizes are chosen on the base of the analysis of three-dimensional autocorrelation function of the source grid. The program creates the grid containing two signs: the local (remaining) and the regional components of the source field. 5.4. Decomposition of fields In the given program automatic technology of the field decomposition by means of two-dimensional adaptive filtering is marketed. The source information for this procedure is just the number to the source grid and the filter type. Input parameters of the module: Input grid – the source grid; Sign of input grid – the processed sign of the source grid; Output grid – the result grid; Filter type – decomposition methods are based on different filters: energy, entropy, median filtering and simple time averaging. The program creates the grid containing several signs depending on presence of anomalies with different energy in the source field. The first grid’s sign contains the most power-hungry forming (trend), the second sign contains the smaller energy component and etc. The last sign contains the field component with amplitude commensurable with noise level. !!! ATTENTION !!! The input grid must be two-dimensional consisting of one layer. The number of pickets and profiles must be more than 10! 5.5. Compensating filtering The program is intended for solving of the problem of the exception from one field of correlation effect of the other one. Input parameters of the module: Input grid – the source grid; Sign of input grid – the processed sign of the source grid; Second input grid – the second source grid; Sign of second input grid – the processed sign of the second source grid; Base window width (in pickets) – the width of the base filtration window; Base window height (in profiles/layers) – the height of the base filtration window; Frequency factor of the filter – the factor taking values from 0.5 up to 1.5; If this parameter equals to 1, that spectrum of the analyzed frequencies is defined just by size of base window and correlation score. Increasing of this parameter allows to enlarge correlation coefficient. Output grid – the result grid. The program forms the grid including five signs. The first sign keeps the component of the first field uncorrelated with the second one. The second sign (on the contrary) contains correlated component of the first field. The radius of correlation is kept in the third sign. The fourth and fifth sign contains offsets by pickets and profiles of the maximum two-dimensional cross-correlation functions accordingly. 5.6. Calculation of instantaneous power This program estimates the instantaneous power in the slithering window along seismic traces (along the same name pickets) i.e. across profile’s spreads. Input parameters of the module: Input grid – the source grid; Sign of input grid – the processed sign of the source grid; Second input grid – the second source grid; Sign of second input grid – the processed sign of the second source grid; Base width (in profiles) – the window width in profiles for the instantaneous power estimation; Output grid – the result grid. 6. DETECTION Procedures of the program block "DETECTION" are intended for separation of weak geophisical anomalies of linear and free form. In the terms of exploration geophysics the weak anomaly is accepted to consider as the signal which is commensurable by amplitude with noise level or below of this level and its reliable visual finding is practically impossible. Amongst methods of the detection of weak anomaly algorithms built on theories of the statistical decisions taking and checking of the statistical hypotheses are broadly used. Along with well-known algorithms of the detection: the method of the inverse probabilities and self-tuning filtering, in this block enters adaptive algorithms taking into account changing of parameters of anomalies and of the noise characteristics on area and in space. Except this, the block contains the program realization of multivariate analogues of the inverse probability method and self-tuning filtering increasing the separation possibility of weak geophisical signals onto several geophisical signs owing to the accumulation of energy signal-to-noise merit. Functional filling of the block "DETECTION" is effective for solving of the following geological problems: mapping of weakly shown tectonics in geophisical fields; separations of low-amperage lifting typical for hydrocarbon deposits; detection of weak anomalies conditioned by small-sizes geophisical objects located on small depth (archeological and engineering geophysics). 6.1. Detection of weak linear anomalies... Programs of detection of weak linear anomalies are enclosed in this block. 6.1.1. Method of interprofiles correlation Input parameters of the module: Input grid – the source grid; Sign of input grid – the processed sign of the source grid; Base width (in pickets) – the number of pickets in the base window; Base height (in profiles) – the number of profiles in the base window; Maximum slope of summation – the maximum offset within the extremum of CCF(m) is searching. This parameter adjusts the possible offset at summation between profiles; Incline of summation base – the slope of the summation base if it is assigned as constant; Algorithm of base window choosing – the window is assigned or chosen automatically; Algorithm of summation base choosing – the summation is assigned or chosen automatically; Algorithm of window incline choosing – the slope is assigned or chosen automatically; Output grid – the result grid. Working mode – the base window size can be assigned by the user or chosen automatically; Processing mode – summation can be provided by layers and by cuts of the source grid. The program realizes the method of interprofiles correlation in the slithering base window and is intended for revealing and tracing (from profile to profile) of weak linear anomalies with amplitude commensurable with noise level. This algorithm is concluded in a simple summation of field’s values by several neighboring profiles in the slithering window with offset from profile to profile and normalization of the gotten sum on the number of the profiles. The offset between profiles is chosen on values of the argument corresponding to the maximum of cross-correlation function between them. The number of profiles of the summation is defined by the base window height, which usually is taken to be equal from 5 to 31 profiles (or layers) depending on nature of the field and problems to be solved. When the seismic information is processing the base parameters are usually assigned and chosen in accordance with nature of the seismic cut. Such directed summation of field values allows to emphasize existing and correlated from profile to profile weak anomalies and reduce the influence of uncorrelated noise. The program creates the grid containing two signs - the result of the directed summation of the field and correlation direction (from profile to profile) in each point of the source field. 6.1.2. Method of self-tuning filtering This program realizes the so-called algorithm to self-tuning filtering, which is based on the calculation of the Hotteling statistics that estimates the energy signal-to-noise merit. Input parameters of the module: Input grid – the source grid; Sign of input grid – the processed sign of the source grid; Filtering window width – the width of the filtration window in pickets; Filtering window height – the height of the filtration window in profiles or layers; The width is assigned much less than the height. Approximately in ratio 1:7 or 1:15. Incline of filtering window – the slope of the filtering window; Output grid – the result grid. Method – it is possible to centralize data in the window (i.e. reduction to zero average); Working mode – the base window size can be assigned by the user or chosen automatically; Processing mode – filtration can be provided by layers and by cuts of the source grid; Modification of the algorithm – the calculation of the maximum statistics is provided on different directions or by total statistics. The last event is efficient when detecting star-shaped structures at the searching of kimberlite pipes. The Hotteling statistic is calculated in the slithering two-dimensional window of the fixed size with different slopping. The slopping of the slithering window is chosen automatically or is assigned by the user as constant. The assignment of the fixed slopping window is used when it is necessary to select anomalies with determined direction. The window width must be much less than the window height (optimum is ratio 3E31). The algorithm is efficient just for raw data in which the visual finding of anomalies does not possible. Otherwise, the usage of this algorithm can be inefficient. The program creates the grid in the database of the complex containing two signs: Hotteling statistic and correlation direction of the field. The statistic is interpreted in the following way: in points where its value is close to zero (less than 1.5) anomalies are absent. The more the statistic’s values the more the probability of the presence of anomalies. The correlation direction is possible to use at solving of the geological zoning problem using classification programs. 6.1.3. Detection of multi-signs linear anomalies This program is intended for revealing and tracing of weak complex linear anomalies commensurable by amplitude with the noise level in conditions when the information about the form of the anomalies is absent. Input parameters of the module: Input grid – the source grid; Amount of anomaly signs – the amount of signs in the multi-signs anomalies (concretely sign’s numbers will be required in the dialogue after starting of the program); Filtering window width – the width of the filtration window in pickets. It is assigned much less than window height. Usually it is 3-7 points; Filtering window height – the height of the filtration window in profiles or layers; Incline of filtering window – the slope of the filtering window; Output grid – the result grid; Method – it is possible to centralize data in the window (i.e. reduction to zero average); Slope mode – the slope can be assigned by the user or chosen automatically; Processing mode – filtration can be provided by layers and by cuts of the source grid. This program realizes the so-called multivariate analogue of self-tuning filtering, which is based on the calculation of the spur of covariance matrix statistic in the slithering two-dimensional window with different slopping. The Slope of the slithering window is chosen automatically in each point of the field or is assigned by the user as constant for all points of the field. The assignment of the fixed slopping window is used when it is necessary to select anomalies with determined direction. The window size is usually do not exceed seven pickets and nine profiles. The algorithm is efficient just for raw data in which the visual finding of anomalies does not possible. Otherwise, the usage of this algorithm can be inefficient. The program creates the grid containing two signs: spur of covariance matrix statistic and correlation direction of the field. The statistic is interpreted in the following way: in points where its value is close to zero (less than 1.5) anomalies are absent. The more the statistic’s values the more the probability of the presence of anomalies. The correlation direction is possible to use at solving of the geological zoning problem using classification programs. In contrast to univariate analogue of the method of self-tuning filtering the given algorithm possesses greater reliability of the correct detection of anomalies. So, in the processing by two signs the reliability of the detection increases not less than in four times, in the processing by three signs - increases not less than in nine times and etc. Analyzed signs must be united in the one grid using the module "Uniting of grids" from the section "SERVICE" of this program complex. 6.2. Detection of weak free form anomalies... In the given block the program on detection of weak free form anomalies are enclosed. 6.2.1. Method of inverse probability This program realizes the method of inverse probability and is used for detecting of weak one-signs or complex anomalies in conditions when there is information on their form (the model anomaly). As the model anomaly most often is taken the square-wave fragment to any grid from the database of the complex where the presence of the anomaly is realistically known. Input parameters of the module: Input grid – the source grid; Second input grid – the source of the model anomaly. The grid containing the anomaly fragment (may comply with the source grid); Left picket of anomaly – the left border of the anomaly by pickets; Right picket of anomaly – the right border of the anomaly by pickets; Upper profile (layer) of anomaly – the upper border of the anomaly by profiles (layers); Bottom profile (layer) of anomaly – the bottom border of the anomaly by profiles (layers); Amount of anomaly signs – the amount of signs in the multi-signs anomalies (concretely sign’s numbers will be required in the dialogue after starting of the program); Output grid – the result grid; Method – it is possible to centralize data in the window (i.e. reduction to zero average); Processing mode – filtration can be provided by layers and by cuts of the source grid. For each point of the field the spur of covariance matrix statistic F is computed, which is a multivariate analogue of the Fisher’s statistic. Values of the F-statistic is interpreted in the following way: If its values is located in the interval 0<=F<=0.5 that the model anomaly in the point is absent. 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WĂú0!g#„ô˙„]„ô˙^„a$„ô˙]„ô˙& Ć/tŸŮ M ˛ě&Q‹Ĺ˙*!d#„ô˙„„ň˙]„ô˙^„`„ň˙)$ Ć/tŸŮ M ˛ě&Q‹Ĺ˙*!d#„ô˙„„ň˙]„ô˙^„`„ň˙a$ cŮRŕYŕbŕ„ŕWáwá„ášá˛áDâ\âÖâďâ.ăKără€ă–ă ă÷ăäHäZä°äźä@ëoëĆëěëYíZízí‡íí°í"î9îiîî˛îŇî ď.ďiďďđ!đ7đAđ˜đŞđóđń7ń8ńńňęâęňŃÂňÂňÂňÂňÂňÂňÂňÂňÂň°ňęžęňŃÂňÂňÂňÂňÂňÂňÂňÂňÂňÂňňhĐq(CJOJQJmH sH #hĐq(B*CJOJQJmH phsH #hĐq(B*CJOJQJmH phsH hĐq(5CJOJQJmH sH  hĐq(5>*CJOJQJmH sH hΕmH sH hĐq(mH sH hĐq(CJOJQJmH sH 8VáWáwášáDâÖâ.ără–ă÷ăHäŁä۸¸‘jjj¸‘‘‘& Ć/tŸŮ M ¸ě&Q‹Ĺ˙*!d#„ô˙„„›ń]„ô˙^„`„›ń& Ć/tŸŮ M x˛ě&Q‹Ĺ˙*!d#„ô˙„„ń]„ô˙^„`„ń" Ć/tŸŮ M x˛ě&Q‹Ĺ˙*!d#„ô˙„]„ô˙^„$ Ć26mŁŮ F }łé VĂů0!f#„ô˙„]„ô˙^„ Łä†çŕčXé¸ę>ë?ë@ënëoëĹëĆëëëěëYíŘŽŽŽŘŘب¨››••Ř„ô˙]„ô˙ $„ô˙„´]„ô˙^„´a$„ô˙]„ô˙)$ Ć/tŸŮ M ˛ě&Q‹Ĺ˙*!d#„ô˙„„ň˙]„ô˙^„`„ň˙a$'$ Ć27mŁÚ G }łę WĂú0!g#„ô˙„]„ô˙^„a$YíZízíí"îiî˛î ďiďđ7đ˜đóđ۸¸‘¸¸¸¸‘¸‘‘& Ć/tŸŮ M x˛ě&Q‹Ĺ˙*!d#„ô˙„„ń]„ô˙^„`„ń" Ć/tŸŮ M x˛ě&Q‹Ĺ˙*!d#„ô˙„]„ô˙^„$ Ć26mŁŮ F }łé VĂů0!f#„ô˙„]„ô˙^„ óđ‚ń3ó7ôuôűôüôýô;ő<őDöEöeöˆöČöěöŘŘŘŘŘŘŘŇŇŘŽ‹‹‹‹" Ć/tŸŮ M x˛ě&Q‹Ĺ˙*!d#„ô˙„]„ô˙^„$ Ć26mŁŮ F }łé VĂů0!f#„ô˙„]„ô˙^„„ô˙]„ô˙'$ Ć27mŁÚ G }łę WĂú0!g#„ô˙„]„ô˙^„a$ń‘ńíńîńZň[ňąň˛ňrôsôuôüôýô<őEöeöröˆöœöČöÖöěöööH÷Z÷ć÷ç÷ŰřéřęřFůGůłů´ů ú úŒú˜ű™űšűŚűq‰/UnŽ›ąÂ7E[đâđâđâđâđâÔâĚÔťŹÔŹÔŹÔŹÔŹÔŹÔâđâđâđâđâԗ…ĚÔ̅ĚÔťŹÔŹÔŹÔ#hĐq(B*CJOJQJmH phsH )hΕhĐq(B*CJOJQJmH phsH hĐq(5CJOJQJmH sH  hĐq(5>*CJOJQJmH sH hĐq(mH sH hĐq(CJOJQJmH sH hĐq(CJOJQJmH sH hĐq(5CJOJQJmH sH 4ěöH÷Ł÷ŰřŒúű—ű˜űšűĽűŚű ţaţšţA˙˙ŘŘąąąąąŤĽĽ˜˜ƒƒƒ$ & F Ćhv„ô˙„v]„ô˙^„va$ $„ô˙„]„ô˙^„a$„ô˙]„ô˙„ô˙]„ô˙'$ Ć27mŁÚ G }łę WĂú0!g#„ô˙„]„ô˙^„a$& Ć/tŸŮ M x˛ě&Q‹Ĺ˙*!d#„ô˙„„ń]„ô˙^„`„ń˙Ř˙/popqˆ‰./TUmnęęÝÝÝÝ××ÝÝŃŃ­‰$ Ć26mŁŮ F }łé VĂů0!f#„ô˙„]„ô˙^„$ Ć27mŁÚ G }łę WĂú0!g#„ô˙„]„ô˙^„„ô˙]„ô˙„ô˙]„ô˙ $„ô˙„]„ô˙^„a$$ & F Ćhv„ô˙„v]„ô˙^„va$nŽą7[Żűœ  „ … † ÜܾܾŽŽŽŽŽj$ Ć27mŁÚ G }łę WĂú0!g#„ô˙„]„ô˙^„'$ Ć27mŁÚ G }łę WĂú0!g#„ô˙„]„ô˙^„a$& Ć/tŸŮ M x˛ě&Q‹Ĺ˙*!d#„ô˙„„ń]„ô˙^„`„ń" Ć/tŸŮ M x˛ě&Q‹Ĺ˙*!d#„ô˙„]„ô˙^„ [f›œŹ­% ' † r Tt—¨6^l‚ÂĂÓÔLN­Óô!7H˝Öţ "1 Tpsƒ‡xy¨ŠđâÓâÓâÄâźâŤđâđâđâđâđâÓâÓâÄâźâŤđâđâđâđâđâÄ⼜ŽœŽœŽœhĐq(CJOJQJmH sH hĐq(5CJOJQJmH sH  hĐq(5>*CJOJQJmH sH hĐq(mH sH hĐq(CJH*OJQJmH sH hĐq(CJH*OJQJmH sH hĐq(CJOJQJmH sH hĐq(5CJOJQJmH sH 2† p r STt—^‚Ö"ůůŇŽ‹‹d‹‹dŇ& Ć/tŸŮ M x˛ě&Q‹Ĺ˙*!d#„ô˙„„ń]„ô˙^„`„ń" Ć/tŸŮ M x˛ě&Q‹Ĺ˙*!d#„ô˙„]„ô˙^„$ Ć26mŁŮ F }łé VĂů0!f#„ô˙„]„ô˙^„'$ Ć27mŁÚ G }łę WĂú0!g#„ô˙„]„ô˙^„a$„ô˙]„ô˙ "Ă?ŤŹ­ŇÓóô7ŘŘŘŘŘŇŇŤ‡dd" Ć/tŸŮ M x˛ě&Q‹Ĺ˙*!d#„ô˙„]„ô˙^„$ Ć26mŁŮ F }łé VĂů0!f#„ô˙„]„ô˙^„'$ Ć2:tŸŮ M x˛ě&Q‹Ĺ˙*!d#„ô˙„]„ô˙^„a$„ô˙]„ô˙'$ Ć27mŁÚ G }łę WĂú0!g#„ô˙„]„ô˙^„a$ 7˝ţ"–âƒ˙RŘľľŽgggg'$ Ć27mŁÚ G }łę WĂú0!g#„ô˙„]„ô˙^„a$& Ć/tŸŮ M x˛ě&Q‹Ĺ˙*!d#„ô˙„„˙đ]„ô˙^„`„˙đ" Ć/tŸŮ M x˛ě&Q‹Ĺ˙*!d#„ô˙„]„ô˙^„& Ć/tŸŮ M x˛ě&Q‹Ĺ˙*!d#„ô˙„„ń]„ô˙^„`„ńRSTop‡ˆŹŐŽ¨¨Z'$ Ć27mŁÚ G }łę WĂú0!g#„ô˙„]„ô˙^„a$'$ Ć27mŁÚ J }łę WĂú0!g#„ô˙„Ü]„ô˙^„Üa$„ô˙]„ô˙'$ Ć2:tŸŮ M x˛ě&Q‹Ĺ˙*!d#„ô˙„]„ô˙^„a$)$ Ć/tŸŮ M x˛ě&Q‹Ĺ˙*!d#„ô˙„„˙đ]„ô˙^„`„˙đa$ŠŞŹ­ÍÚđ,‰—68Ű é ě !c!ƒ!!Ś!š!+"B"r"Š"ť"Ű"#7#r#Š#$*$@$J$Ą$°$% %(`cc2c4cEdedrdˆd™d&e4eÇfďáÓÂłÓłÓłÓłÓ¤ÓáÓáœÓ³ӳӳӳӳӳӳӳӳӳӳӚӏœÓÂłÓłÓłÓhΕhĐq(mH sH UhĐq(mH sH hĐq(CJH*OJQJmH sH hĐq(5CJOJQJmH sH  hĐq(5>*CJOJQJmH sH hĐq(CJOJQJmH sH hĐq(CJOJQJmH sH  hĐq(5CJH*OJQJmH sH 7Ź­Íđ‰­Űę ë ě !!۸¸‘¸jjjjdd„ô˙]„ô˙'$ Ć27mŁÚ G }łę WĂú0!g#„ô˙„]„ô˙^„a$& Ć/tŸŮ M x˛ě&Q‹Ĺ˙*!d#„ô˙„„ń]„ô˙^„`„ń" Ć/tŸŮ M x˛ě&Q‹Ĺ˙*!d#„ô˙„]„ô˙^„$ Ć26mŁŮ F }łé VĂů0!f#„ô˙„]„ô˙^„ !b!c!ƒ!Ś!+"r"ť"#r#$@$Ą$%i%ç&ňÎŤŤ„ŤŤŤŤ„Ť„„„ň& Ć/tŸŮ M x˛ě&Q‹Ĺ˙*!d#„ô˙„„ń]„ô˙^„`„ń" Ć/tŸŮ M x˛ě&Q‹Ĺ˙*!d#„ô˙„]„ô˙^„$ Ć26mŁŮ F }łé VĂů0!f#„ô˙„]„ô˙^„ $„ô˙„]„ô˙^„a$del, but their orientation differs from model. The program forms the grid with an amount of signs equals to an amount of directions assigned by the user. Each sign contains a spur of covariance matrix statistic corresponding to each direction. The statistic’s values are interpreted as follows: The more similar fields in the vicinity of the point onto the model the less the value of the statistic. Usually, the decision threshold about the presence of the model anomaly is not more than three. It is considered that in the vicinity of the point the probability of the model anomaly presence is high if the calculated statistic of this vicinity lies within the range from 0 up to 2.5. The algorithm is efficient in solving of problems of the forecasting, geological mapping and zoning. 7.3. Components data analysis This program is intended for carrying out of the classical components analysis of multi-signs geophisical information by means of covariance matrix calculation, searching for eigenvalues and eigenvectors and the further folding of multi-signs information by eigenvectors. Input parameters of the module: Input grid – the source grid; Amount of signs – the amount of signs in the multi-signs grid (concretely sign’s numbers will be required in the dialogue after starting of the program); Output grid – the result grid; Amount of signs in the resulting grid complies with amount of analyzed signs. The first sign (with the bigest dispersion) presents the folding of analyzed signs with the covariance matrix corresponding to the maximum eigenvalue, the second sign (with a little bit smaller dispersion) - presents the folding with eigenvectors corresponding to following in size eigenvalue and etc.     PAGE  PAGE 64 Coscad 3Dt Copyright Š 2003 MSGPU Page page64 ç&/`ô`Žbccc3c4cDdEdňÉÉÉÉÉŔŔšv$ Ć26mŁŮ F }łé VĂů0!f#„ô˙„]„ô˙^„%$ Ć/tŸŮ M x˛ě&Q‹Ĺ˙*!d#„ô˙„]„ô˙^„a$$„ô˙]„ô˙a$($ Ć5htŸŮ M x˛ě&Q‹Ĺ˙*!d#„ô˙„]„ô˙^„a$ $„ô˙„]„ô˙^„a$ Ededˆd&eJeĆfÇfÉfĘfĚfÍfĎfĐfŇfÓfÜfÜܵ܏„„ř˙„&`#$%$ Ć/tŸŮ M x˛ě&Q‹Ĺ˙*!d#„ô˙„]„ô˙^„a$& Ć/tŸŮ M x˛ě&Q‹Ĺ˙*!d#„ô˙„„ń]„ô˙^„`„ń" Ć/tŸŮ M x˛ě&Q‹Ĺ˙*!d#„ô˙„]„ô˙^„ÇfČfĘfËfÍfÎfĐfŃfÓfÔfÚfŰfÜfŢfßfĺfćfčféfęfôfůfggggggg g"g#g$g÷ó÷ó÷ó÷óéăéăßéăéÔéăÂß´ß´˘´˘˘ßóhĐq(CJOJQJmH sH %hБ5B*OJQJmHnHphu#jh ľ5B*OJQJUphh ľ5B*OJQJph"h ľ5B* OJQJmH ph€sH hБ0JmHnHuh ľ h ľ0Jjh ľ0JUhš'tjhš'tU ÜfÝfŢfęföf÷fřfůf!g"g#g$gů÷îäŢ÷÷Ţ÷÷¸%$ Ć/tŸŮ M x˛ě&Q‹Ĺ˙*!d#„ô˙„]„ô˙^„a$ Ć I Ć I„h]„h„ř˙„&`#$„h]„h 6 00&P P°ƒ. °ČA!°Ĺ"°Đ#Đ$‹%°°Đ°Đ Đ`!đÍK—“ Ů!sEcG2YŠaEĂ°ăÖc đ 8››KţxÚí}  =m=˙÷÷śżoŞ)*ŻAŮRŒ5$˛ŇŘEŞ!$ŠY˘he ƒ˛ocß ɒČcÉž=ö]†ěç?Ďwyžď33çžĺžsçöżsżťœ{î93Ÿůîë5¸Ŕ-~ďĺ7Ŕí_ăqŤń˙M7ČwˇżáQ7ţÎmn1~÷:üógßř˛ŰÄçčß<ĺĆkˇM˙zţœgߘ->gůŮĎ˝ńîž˝üw?|㽡ţťĺWxÁ÷Űă–_ëĽ7>ŕ\ŻľüŞxăƒôŞËŻ?ÜXüő—ßéżo|Äßiů=oÓ'\Č{.żűÝnzŇżűňyźÉMOťnçą|Fϟ銡ťţg´|nßpÓÓOęÜŚgy›ńó]oéĎ2Jďďťé9'zÎËgďĎ7žýűÜńyˇ?őł_žćń:Ţë.zÇËsËWäŻ!^чÜĺ—ňŠ–ŻÍ_ěŐÇ˙÷şőÇÇWăqKüůƒ˙„GßňŘG=áńO||ý)7űŸ ƒű^{\n âw÷˙żâ†ZĎş6~˛ˇ| Üůá}ÜcžxóCÓÜü°Ç?Ďы›Ž˙o~áK€űÁ-Ç'Ţç˝Ň ׎ńkŢ.ź:=v'ĆőŽˆ+ŕgüďřřýřŻosÍż–ˇAtǛÁŽß?ůÚýýĂ}Ż˝ĎęĆ˙ţ‘'˙ŻÁmńąßúÍkđjwü×řż˙2žď 7ܡ¸Ĺ-ŕ–ˇź%ÜęVˇ‚[ßúÖp›ŰÜn{ŰŰÂínw;¸ńĆᦛn‚ŰßţöđjŻöjp‡;ÜîxÇ;ît'Ȳ î|ç;Ă]îrxőWux×x ¸ë]ď wťŰÝŕîwż;źćkž&źÖk˝źökż6Üă÷€{Ţóžđ:Żó:đşŻűşpóÍ7Ăë˝ŢëAžçđúŻ˙úđođđ†oř†pŻ{Ý î}ď{Ă˝ŃÁżńÛźÉ›Ŕ›žé›Â›˝Ů›Á}îsxó7s¸ď}ď ÷ťßýŕ-Ţâ-ŕ-ßň-Ą( xŤˇz+xëˇ~kx›ˇyxۡ}[xťˇ{;xűˇ{¸˙ýďďđďďřŽďďôNďxŔŕßůá| źËťź źëťž+<čA‚˛,áÝŢíÝŕÝßýÝáÁ~0źÇ{źźç{ž'ź×{˝ź÷{ż7źĎűź<ä!‡>ôĄđžďűžđ~ď÷~đţď˙ţđ°‡= >ŕ>ţđ‡CUUđřđAôAđÁüÁđ!ň!đĄúĄđaöađáţáđńđˆG<>ň#?>ęŁ> ůČGÂGôGĂŁő(xôŁ yĚc Žkř˜ůř؏ýXxěc ÷q˙ńŸđ Ÿ{Üăŕ?ńáń<|Ň'}|ň'2<á O€'>ń‰đ)Ÿň)đŠŸúŠđ¤'= šŚOű´OƒO˙ôO‡ĎřŒĎ€'?ůÉđ™Ÿů™đYŸőYđٟýŮđ9Ÿó9đ”§<>÷s?>ďó>žúÔ§ÂӞö4řüĎ˙|ř‚/řxúӟmŰÂ~áÂ}ŃÁ3žń řâ/ţbř’/ůřŇ/ýRxć3Ÿ ĎzÖłŕËžěËŕËżüËá+žâ+ŕ+żň+áŮĎ~6|ŐW}|őW5|Í×| t]_űľ_ _÷u__˙ő_ĎyÎsŕšĎ}.|Ă7||ă7~#|Ó7}|ó73|ˡ| |ëˇ~+|ۡ}|űˇ;|Çw||çw~'|×w}ô}ßýÝß ßó=ßßű˝ß ß÷}ßß˙ýß?đ??řƒ??ôC??üĂ? ?ň#??úŁ? 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EFEquation.DSMT4ô9˛qřڐXęz&h0ęzDSMT5WinAllBasicCodePagesTimes New RomanSymbolCourier NewMT Extra!/ED/APô_1118610891"ÎŔF0+pFW6Č0+pFW6ČOle ˙˙˙˙˙˙˙˙˙˙˙˙CompObj˙˙˙˙iObjInfo˙˙˙˙˙˙˙˙Equation Native ˙˙˙˙˙˙˙˙˙˙˙˙Ź_1118611000˙˙˙˙˙˙˙˙ÎŔF0+pFW6Č0+pFW6ČOle ˙˙˙˙˙˙˙˙˙˙˙˙%CompObj ˙˙˙˙&iG_APňAPôAôEô%ôB_AôC_AôEô*_HôAô@ôAHôA*_D_Eô_Eô_A  ƒA†== ˆ1ƒnp ƒx ƒi †"-ƒm–(–) ˆ3 ƒD ˆ3‚/ˆ2ƒi†==ˆ1ƒn †"ĺA*_D_Eô_ţ˙ ˙˙˙˙ÎŔFMathType 5.0 Equation MathType EFEquation.DSMT4ô9˛qObjInfo˙˙˙˙!˙˙˙˙(Equation Native ˙˙˙˙˙˙˙˙˙˙˙˙)4_1118611072'$ÎŔF0+pFW6Č0+pFW6ČOle ˙˙˙˙˙˙˙˙˙˙˙˙.řÚXęz.h0ęzDSMT5WinAllBasicCodePagesTimes New RomanSymbolCourier NewMT Extra!/ED/APôG_APňAPôAôEô%ôB_AôC_AôEô*_HôAô@ôAHôA*_D_Eô_Eô_A  ƒR†==ƒX ‚m‚a‚x †"-ƒX ‚m‚i‚nA*ţ˙ ˙˙˙˙ÎŔFMathType 5.0 Equation MathTyCompObj#%˙˙˙˙/iObjInfo˙˙˙˙&˙˙˙˙1Equation Native ˙˙˙˙˙˙˙˙˙˙˙˙2_1118611200˙˙˙˙˙˙˙˙)ÎŔF0+pFW6Č0+pFW6Čpe EFEquation.DSMT4ô9˛qřÚčXęz.h0ęzDSMT5WinAllBasicCodePagesTimes New RomanSymbolCourier NewMT Extra!/ED/APôG_APňAPôAôEô%ôB_AôC_AôEô*_HôAô@ôAHôA*_D_Eô_Eô_A  ƒr ˆ0 †==ƒmOle ˙˙˙˙˙˙˙˙˙˙˙˙7CompObj(*˙˙˙˙8iObjInfo˙˙˙˙+˙˙˙˙:Equation Native ˙˙˙˙˙˙˙˙˙˙˙˙;ţ˙ ˙˙˙˙ÎŔFMathType 5.0 Equation MathType EFEquation.DSMT4ô9˛qřÚěXęz.h0ęzDSMT5WinAllBasicCodePagesTimes New RomanSymbolCourier NewMT Extra!/ED/APôG_APňAPôAôEô%ôB_AôC_AôEô*_HôAô@ôAHôA*_D_Eô_Eô_A  ƒRƒm–(–)†==ˆ0_1118611249^.ÎŔF0+pFW6Č0+pFW6ČOle ˙˙˙˙˙˙˙˙˙˙˙˙@CompObj-/˙˙˙˙AiObjInfo˙˙˙˙0˙˙˙˙Cţ˙ ˙˙˙˙ÎŔFMathType 5.0 Equation MathType EFEquation.DSMT4ô9˛qřÚ Xęz.h0ęzDSMT5WinAllBasicCodePagesTimes New RomanSymbolCourier NewMT Extra!/ED/APôG_APňAPôAôEô%ôB_AôC_AôEô*_HôAô@ôAHôA*_D_Eô_Eô_A  ƒM ˆ0 †==ƒxEquation Native ˙˙˙˙˙˙˙˙˙˙˙˙D<_1118611396˙˙˙˙˙˙˙˙3ÎŔF0+pFW6Č0+pFW6ČOle ˙˙˙˙˙˙˙˙˙˙˙˙ICompObj24˙˙˙˙Ji‚_ƒfƒx–(–)†==‚m‚a‚xţ˙ ˙˙˙˙ÎŔFMathType 5.0 Equation MathType EFEquation.DSMT4ô9˛qřÚ4Xęz.h0ęzDSMT5WinAllBasicCodePagesTimes New RomanSymbolCourier NewMT Extra!/ED/APôG_APňAPôAôEô%ôB_AôC_AôEô*_HôAô@ôAHôA*_D_Eô_EôObjInfo˙˙˙˙5˙˙˙˙LEquation Native ˙˙˙˙˙˙˙˙˙˙˙˙MP_11186114071E8ÎŔF0+pFW6Č0+pFW6ČOle ˙˙˙˙˙˙˙˙˙˙˙˙S_A  ƒMƒe_ƒPƒ(ƒxƒ<ƒMƒeƒ)ƒ=ƒPƒ(ƒxƒ>ƒMƒeƒ)ƒ=ƒ0ƒ.ƒ5erţ˙ ˙˙˙˙ÎŔFMathType 5.0 Equation MathType EFEquation.DSMT4ô9˛qřÚXęzh0ęzDSMT5WinAllBasicCodePagesCompObj79˙˙˙˙TiObjInfo˙˙˙˙:˙˙˙˙VEquation Native ˙˙˙˙˙˙˙˙˙˙˙˙W _1133084436@=ÎŔF0+pFW6Č0+pFW6ČTimes New RomanSymbolCourier NewMT Extra!/ED/APôG_APňAPôAôEô%ôB_AôC_AôEô*_HôAô@ôAHôA*_D_Eô_Eô_A  ƒfƒx–(–)‚,ƒPƒx–(–)ţ˙ ˙˙˙˙ÎŔFMathType 5.0 Equation MathType EFEquation.DSMT4ô9˛qOle ˙˙˙˙˙˙˙˙˙˙˙˙\CompObj<>˙˙˙˙]iObjInfo˙˙˙˙?˙˙˙˙_Equation Native ˙˙˙˙˙˙˙˙˙˙˙˙`ŘzÝźXęzh0ęzDSMT5WinAllBasicCodePagesTimes New RomanSymbolCourier NewMT Extra!/ED/APôG_APňAPôAôEô%ôB_AôC_AôEô*_HôAô@ôAHôA*_D_Eô_Eô_A  ƒD ƒfƒaƒcƒt †== ˆ1ƒN†"-ˆ1p ƒA ƒj †"- ƒA–(–) ˆ2ƒj†==ˆ1ƒN †"ĺ ‚;˜ďƒD ƒoƒsƒt †== ˆ1ƒNƒn†"-ˆ1–(–)ppƒA ƒiƒj †"- ƒA ƒj –(–) ˆ2ƒi†==ˆ1ƒn †"ĺ ƒj†==ˆ1ƒN †"ĺţ˙ ˙˙˙˙ÎŔFMathType 5.0 Equation MathType EFEquation.DSMT4ô9˛q_1133084473˙˙˙˙˙˙˙˙BÎŔF0+pFW6Č0+pFW6ČOle ˙˙˙˙˙˙˙˙˙˙˙˙lCompObjAC˙˙˙˙miObjInfo˙˙˙˙D˙˙˙˙oEquation Native ˙˙˙˙˙˙˙˙˙˙˙˙p@_1118743063˙˙˙˙˙˙˙˙GÎŔF0+pFW6Č0+pFW6ČOle ˙˙˙˙˙˙˙˙˙˙˙˙uCompObjFH˙˙˙˙vizÝ$Xęzh0ęzDSMT5WinAllBasicCodePagesTimes New RomanSymbolCourier NewMT Extra!/ED/APôG_APňAPôAôEô%ôB_AôC_AôEô*_HôAô@ôAHôA*_D_Eô_Eô_A  ƒF†== ƒD ƒfƒaƒcƒt ƒD ƒoƒsƒtţ˙ ˙˙˙˙ÎŔFMathType 5.0 Equation MathType EFEquation.DSMT4ô9˛qObjInfo˙˙˙˙I˙˙˙˙xEquation Native ˙˙˙˙˙˙˙˙˙˙˙˙yp_11187547236TLÎŔF0+pFW6Č0+pFW6ČOle ˙˙˙˙˙˙˙˙˙˙˙˙ƒÖÖTXęzh0ęzDSMT5WinAllBasicCodePagesTimes New RomanSymbolCourier NewMT Extra!/ED/APôG_APňAPôAôEô%ôB_AôC_AôEô*_HôAô@ôAHôA*_D_Eô_Eô_A  ƒRƒm–(–)†== ˆ1ƒN†"-ƒm–ě–ěpƒf ƒi †"-ƒf ƒaƒvƒeƒrƒaƒgƒe –(–)†Ĺ"׃f ƒi‚ţ˙˙˙ţ˙˙˙…ţ˙˙˙ţ˙˙˙ˆ‰Šţ˙˙˙ţ˙˙˙ţ˙˙˙ţ˙˙˙‘’ţ˙˙˙ţ˙˙˙•ţ˙˙˙ţ˙˙˙˜™š›œžŸ Ąţ˙˙˙ţ˙˙˙¤ţ˙˙˙ţ˙˙˙§¨Šţ˙˙˙ţ˙˙˙Źţ˙˙˙ţ˙˙˙Ż°ą˛ţ˙˙˙ţ˙˙˙ľţ˙˙˙ţ˙˙˙¸šşťź˝ţ˙˙˙ţ˙˙˙Ŕţ˙˙˙ţ˙˙˙ĂÄĹĆÇČÉĘËĚÍÎţ˙˙˙ţ˙˙˙Ńţ˙˙˙ţ˙˙˙ÔŐÖţ˙˙˙ţ˙˙˙Ůţ˙˙˙ţ˙˙˙ÜÝŢţ˙˙˙ţ˙˙˙áţ˙˙˙ţ˙˙˙äĺćçčéęëěíîďţ˙˙˙ţ˙˙˙ňţ˙˙˙ţ˙˙˙őö÷řůúűţ˙˙˙ţ˙˙˙ţţ˙˙˙ţ˙˙˙†++ƒm–ě–ě †"-ƒf ƒaƒvƒeƒrƒaƒgƒe –(–) ƒi†==ˆ1ƒN†"-ƒm–ě–ě †"ĺ_ţ˙ ˙˙˙˙ÎŔFMathType 5.0 Equation MathType EFEquation.DSMT4ô9˛qÖÖÜXęzh0ęzDSMT5WinAllBasicCodePagesCompObjKM˙˙˙˙„iObjInfo˙˙˙˙N˙˙˙˙†Equation Native ˙˙˙˙˙˙˙˙˙˙˙˙‡ř_1118754732˙˙˙˙˙˙˙˙QÎŔF0+pFW6Č0+pFW6ČTimes New RomanSymbolCourier NewMT Extra!/ED/APôG_APňAPôAôEô%ôB_AôC_AôEô*_HôAô@ôAHôA*_D_Eô_Eô_A  ƒf ˆ1ţ˙ ˙˙˙˙ÎŔFMathType 5.0 Equation MathType EFEquation.DSMT4ô9˛qÖÖÜXęzh0ęzDSMT5WinAllBasicCodePagesOle ˙˙˙˙˙˙˙˙˙˙˙˙‹CompObjPR˙˙˙˙ŒiObjInfo˙˙˙˙S˙˙˙˙ŽEquation Native ˙˙˙˙˙˙˙˙˙˙˙˙řTimes New RomanSymbolCourier NewMT Extra!/ED/APôG_APňAPôAôEô%ôB_AôC_AôEô*_HôAô@ôAHôA*_D_Eô_Eô_A  ƒf ˆ2ţ˙ ˙˙˙˙ÎŔFMathType 5.0 Equation MathType EFEquation.DSMT4ô9˛qÖÖlXęzh0ęzDSMT5WinAllBasicCodePages_1118754946OYVÎŔF0+pFW6Č0+pFW6ČOle ˙˙˙˙˙˙˙˙˙˙˙˙“CompObjUW˙˙˙˙”iObjInfo˙˙˙˙X˙˙˙˙–Equation Native ˙˙˙˙˙˙˙˙˙˙˙˙—ˆ_1118755573˙˙˙˙˙˙˙˙[ÎŔF0+pFW6Č0+pFW6ČOle ˙˙˙˙˙˙˙˙˙˙˙˙˘CompObjZ\˙˙˙˙ŁiTimes New RomanSymbolCourier NewMT Extra!/ED/APôG_APňAPôAôEô%ôB_AôC_AôEô*_HôAô@ôAHôA*_D_Eô_Eô_A  ƒBƒm–(–)†== ˆ1ƒN†"-ƒm–ě–ěpƒf ƒiˆ1 †"-ƒf ƒaƒvƒeƒrƒaƒgƒeˆ1 –(–)†Ĺ"׃f ƒi†++ƒm–ě–ěˆ2 †"-ƒf ƒaƒvƒeƒrƒaƒgƒeˆ2 –(–) ƒi†==ˆ1ƒN†"-ƒm–ě–ě †"ĺţ˙ ˙˙˙˙ÎŔFMathType 5.0 Equation MathType EFEquation.DSMT4ô9˛qÖÖäXęzÚh0ęzDSMT5WinAllBasicCodePagesTimes New RomanSymbolCourier NewMT Extra!/ED/APôObjInfo˙˙˙˙]˙˙˙˙ĽEquation Native ˙˙˙˙˙˙˙˙˙˙˙˙Ś_1118755603Jr`ÎŔF0+pFW6Č0+pFW6ČOle ˙˙˙˙˙˙˙˙˙˙˙˙ŞG_APňAPôAôEô%ôB_AôC_AôEô*_HôAô@ôAHôA*_D_Eô_Eô_A  ƒm ƒeƒxƒtţ˙ ˙˙˙˙ÎŔFMathType 5.0 Equation MathType EFEquation.DSMT4ô9˛qÖÖXęzÚh0ęzDSMT5WinAllBasicCodePagesTimes New RomanSymbolCourier NewMT Extra!/ED/APôCompObj_a˙˙˙˙ŤiObjInfo˙˙˙˙b˙˙˙˙­Equation Native ˙˙˙˙˙˙˙˙˙˙˙˙Ž_1118755792˙˙˙˙˙˙˙˙eÎŔF0+pFW6Č0+pFW6ČG_APňAPôAôEô%ôB_AôC_AôEô*_HôAô@ôAHôA*_D_Eô_Eô_A  ƒBƒm ƒeƒxƒt –(–)Aţ˙ ˙˙˙˙ÎŔFMathType 5.0 Equation MathType EFEquation.DSMT4ô9˛qÖÖlXęzÚh0ęzDSMT5WinAllBasicCodePagesOle ˙˙˙˙˙˙˙˙˙˙˙˙łCompObjdf˙˙˙˙´iObjInfo˙˙˙˙g˙˙˙˙śEquation Native ˙˙˙˙˙˙˙˙˙˙˙˙ˇˆTimes New RomanSymbolCourier NewMT Extra!/ED/APôG_APňAPôAôEô%ôB_AôC_AôEô*_HôAô@ôAHôA*_D_Eô_Eô_A  „Ár†== ƒBƒm ƒeƒtƒr –(–)ˆ1†"-ƒBƒm ƒeƒtƒr –(–)–[–]ţ˙ ˙˙˙˙ÎŔFMathType 5.0 Equation MathTy_1118760909cmjÎŔF0+pFW6Č0+pFW6ČOle ˙˙˙˙˙˙˙˙˙˙˙˙žCompObjik˙˙˙˙żiObjInfo˙˙˙˙l˙˙˙˙Ápe EFEquation.DSMT4ô9˛qâÚXęzh0ęzDSMT5WinAllBasicCodePagesTimes New RomanSymbolCourier NewMT Extra!/ED/APôG_APňAPôAôEô%ôB_AôC_AôEô*_HôAô@ôAHôA*_D_Eô_Eô_A  ƒDƒm‚,ƒp–(–)†== ˆ1ƒM†"-ƒp–ě–ě ˆ1ƒN†"-ƒm–ě–ěppEquation Native ˙˙˙˙˙˙˙˙˙˙˙˙Â,_1118762255˙˙˙˙˙˙˙˙oÎŔF0+pFW6Č0+pFW6ČOle ˙˙˙˙˙˙˙˙˙˙˙˙ĎCompObjnp˙˙˙˙Điƒf ƒi‚,ƒj †"-ƒf ƒaƒvƒeƒrƒaƒgƒe –(–)†Ĺ"׃f ƒi†++ƒm–ě–ě‚,ƒj†++ƒp–ě–ě †"-ƒf ƒaƒvƒeƒrƒaƒgƒe –(–) ƒi†==ˆ1ƒN†"-ƒm–ě–ě †"ĺ ƒj†==ˆ1ƒM†"-ƒp–ě–ě †"ĺXţ˙ ˙˙˙˙ÎŔFMathType 5.0 Equation MathType EFEquation.DSMT4ô9˛qâÚÜXęz6h0ęzDSMT5WinAllBasicCodePagesTimes New RomanSymbolCourier NewMT Extra!/ED/APôG_APňAPôAôEô%ôB_AôC_AôEô*_HôAô@ôAHôA*_D_Eô_Eô_A  ƒf ˆ1ObjInfo˙˙˙˙q˙˙˙˙ŇEquation Native ˙˙˙˙˙˙˙˙˙˙˙˙Óř_1118762265h†tÎŔF0+pFW6Č0+pFW6ČOle ˙˙˙˙˙˙˙˙˙˙˙˙×CompObjsu˙˙˙˙ŘiObjInfo˙˙˙˙v˙˙˙˙ÚEquation Native ˙˙˙˙˙˙˙˙˙˙˙˙Űř_1118762464˙˙˙˙˙˙˙˙yÎŔF0+pFW6Č0+pFW6Čţ˙ ˙˙˙˙ÎŔFMathType 5.0 Equation MathType EFEquation.DSMT4ô9˛qâÚÜXęz6h0ęzDSMT5WinAllBasicCodePagesTimes New RomanSymbolCourier NewMT Extra!/ED/APôG_APňAPôAôEô%ôB_AôC_AôEô*_HôAô@ôAHôA*_D_Eô_Eô_A  ƒf ˆ2Ole ˙˙˙˙˙˙˙˙˙˙˙˙ßCompObjxz˙˙˙˙ŕiObjInfo˙˙˙˙{˙˙˙˙âEquation Native ˙˙˙˙˙˙˙˙˙˙˙˙ă,ţ˙ ˙˙˙˙ÎŔFMathType 5.0 Equation MathType EFEquation.DSMT4ô9˛qâÚXęz6h0ęzDSMT5WinAllBasicCodePagesTimes New RomanSymbolCourier NewMT Extra!/ED/APôG_APňAPôAôEô%ôB_AôC_AôEô*_HôAô@ôAHôA*_D_Eô_Eô_A  ƒDƒCƒCƒFƒm‚,ƒp–(–)†== ˆ1ƒM†"-ƒp–ě–ě ˆ1ƒN†"-ƒm–ě–ěppƒf ƒi‚,ƒjˆ1 †"-ƒf ƒaƒvƒeƒrƒaƒgƒeˆ1 –(–)†Ĺ"׃f ƒi†++ƒm‚,ƒj†++ƒpˆ2 †"-ƒf ƒaƒvƒeƒrƒaƒgƒeˆ2 –(–) ƒi†==ˆ1ƒN†"-ƒm–ě–ě †"ĺ ƒj†==ˆ1ƒM†"-ƒp–ě–ě †"ĺ _1118769691w~ÎŔF0+pFW6Č0œrFW6ČOle ˙˙˙˙˙˙˙˙˙˙˙˙đCompObj}˙˙˙˙ńiObjInfo˙˙˙˙€˙˙˙˙óţ˙ ˙˙˙˙ÎŔFMathType 5.0 Equation MathType EFEquation.DSMT4ô9˛qâÚŘXęzh0ęzDSMT5WinAllBasicCodePagesTimes New RomanSymbolCourier NewMT Extra!/ED/APôG_APňAPôAôEô%ôB_AôC_AôEô*_HôAô@ôAHôA*_D_Eô_Eô_A  ƒr ƒxƒy †==Equation Native ˙˙˙˙˙˙˙˙˙˙˙˙ôô_1118769764˙˙˙˙˙˙˙˙ƒÎŔF0œrFW6Č0œrFW6ČOle ˙˙˙˙˙˙˙˙˙˙˙˙üCompObj‚„˙˙˙˙ýi ˆ1ƒn†Ĺ"ׄĂs ƒx „Ăs ƒy pƒx ƒi †"-ƒx–(–)†Ĺ"׃y ƒi †"-ƒy–(–) ƒi†==ˆ1ƒN †"ĺţ˙ ˙˙˙˙ÎŔFMathType 5.0 Equation MathType EFEquation.DSMT4ô9˛qObjInfo˙˙˙˙…˙˙˙˙˙Equation Native ˙˙˙˙˙˙˙˙˙˙˙˙,_1118770060|;ˆÎŔF0œrFW6Č0œrFW6ČOle ˙˙˙˙˙˙˙˙˙˙˙˙ţ˙˙˙ţ˙˙˙ţ˙˙˙ţ˙˙˙    ţ˙˙˙ţ˙˙˙ţ˙˙˙ţ˙˙˙ţ˙˙˙ţ˙˙˙ţ˙˙˙ţ˙˙˙ !"#ţ˙˙˙ţ˙˙˙&ţ˙˙˙ţ˙˙˙)*+,-.ţ˙˙˙ţ˙˙˙1ţ˙˙˙ţ˙˙˙456789ţ˙˙˙ţ˙˙˙<ţ˙˙˙ţ˙˙˙?@ABCDţ˙˙˙FGHIJKLţ˙˙˙Nţ˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙˙âÚXęz6h0ęzDSMT5WinAllBasicCodePagesTimes New RomanSymbolCourier NewMT Extra!/ED/APôG_APňAPôAôEô%ôB_AôC_AôEô*_HôAô@ôAHôA*_D_Eô_Eô_A  ƒx‚,ƒy‚,„Ăs ƒx „Ăs ƒyţ˙ ˙˙˙˙ÎŔFMathType 5.0 Equation MathType EFEquation.DSMT4ô9˛qCompObj‡‰˙˙˙˙iObjInfo˙˙˙˙Š˙˙˙˙Equation Native ˙˙˙˙˙˙˙˙˙˙˙˙ Ô_1118770114˙˙˙˙˙˙˙˙ÎŔF0œrFW6Č0œrFW6ČâÚ¸Xęzh0ęzDSMT5WinAllBasicCodePagesTimes New RomanSymbolCourier NewMT Extra!/ED/APôG_APňAPôAôEô%ôB_AôC_AôEô*_HôAô@ôAHôA*_D_Eô_Eô_A  „Ár ƒxƒy †==ˆ1†"- ˆ6pƒr ƒiƒx †"-ƒr ƒiƒy –(–) ƒi†==ˆ1ƒn †"ĺ ƒn ˆ3 †"-ƒn–(–)ţ˙ ˙˙˙˙ÎŔFMathType 5.0 Equation MathType EFEquation.DSMT4ô9˛qâÚXęzFh0ęzDSMT5WinAllBasicCodePagesTimes New RomanSymbolCourier NewMT Extra!/ED/APôG_APňAPôAôEô%ôB_AôC_AôEô*_HôAô@ôAHôA*_D_Eô_EôOle ˙˙˙˙˙˙˙˙˙˙˙˙CompObjŒŽ˙˙˙˙iObjInfo˙˙˙˙˙˙˙˙Equation Native ˙˙˙˙˙˙˙˙˙˙˙˙ _A  ƒr ƒiƒx ‚,ƒr ƒiƒyţ˙ ˙˙˙˙ÎŔFMathType 5.0 Equation MathType EFEquation.DSMT4ô9˛qâÚ,Xęzh0ęzDSMT5WinAllBasicCodePagesTimes New RomanSymbolCourier NewMT Extra!/ED/APô_1118779461‹š’ÎŔF0œrFW6Č0œrFW6ČOle ˙˙˙˙˙˙˙˙˙˙˙˙CompObj‘“˙˙˙˙iObjInfo˙˙˙˙”˙˙˙˙Equation Native ˙˙˙˙˙˙˙˙˙˙˙˙H_1118779574˙˙˙˙˙˙˙˙—ÎŔF0œrFW6Č0œrFW6ČOle ˙˙˙˙˙˙˙˙˙˙˙˙$CompObj–˜˙˙˙˙%iG_APňAPôAôEô%ôB_AôC_AôEô*_HôAô@ôAHôA*_D_Eô_Eô_A  ƒR ƒm †== ƒA ƒmˆ2 †++ƒB ƒmˆ2ţ˙ ˙˙˙˙ÎŔFMathType 5.0 Equation MathType EFEquation.DSMT4ô9˛qObjInfo˙˙˙˙™˙˙˙˙'Equation Native ˙˙˙˙˙˙˙˙˙˙˙˙(Ź_1118779676•ŸœÎŔF0œrFW6Č0œrFW6ČOle ˙˙˙˙˙˙˙˙˙˙˙˙/âڐXęzh0ęzDSMT5WinAllBasicCodePagesTimes New RomanSymbolCourier NewMT Extra!/ED/APôG_APňAPôAôEô%ôB_AôC_AôEô*_HôAô@ôAHôA*_D_Eô_Eô_A  ƒR ƒm †==ƒaƒrƒcƒtƒg †"-ƒB ƒm ƒA ƒm –(–)‚,˜ďƒm†==ˆ0‚,ˆ1‚,‹& K‚,ƒN‚/ˆ2CompObj›˙˙˙˙0iObjInfo˙˙˙˙ž˙˙˙˙2Equation Native ˙˙˙˙˙˙˙˙˙˙˙˙3Ź_1118779696˙˙˙˙˙˙˙˙ĄÎŔF0œrFW6Č0œrFW6Čţ˙ ˙˙˙˙ÎŔFMathType 5.0 Equation MathType EFEquation.DSMT4ô9˛qâڐXęzh0ęzDSMT5WinAllBasicCodePagesTimes New RomanSymbolCourier NewMT Extra!/ED/APôG_APňAPôAôEô%ôB_AôC_AôEô*_HôAô@ôAHôA*_D_Eô_Eô_A  ƒA ƒm †== ˆ1ƒNpƒf ƒi ‚c‚o‚s ˆ2„ŔpƒmƒiƒN–(–) ƒi†==ˆ1ƒN †"ĺ ţ˙ ˙˙˙˙ÎŔFMathType 5.0 Equation MathType EFEquation.DSMT4ô9˛qâڐXęzh0ęzDSMT5WinAllBasicCodePagesTimes New RomanSymbolCourier NewMT Extra!/ED/APôOle ˙˙˙˙˙˙˙˙˙˙˙˙:CompObj ˘˙˙˙˙;iObjInfo˙˙˙˙Ł˙˙˙˙=Equation Native ˙˙˙˙˙˙˙˙˙˙˙˙>ŹG_APňAPôAôEô%ôB_AôC_AôEô*_HôAô@ôAHôA*_D_Eô_Eô_A  ƒA ƒm †== ˆ1ƒNpƒf ƒi ‚s‚i‚n ˆ2„ŔpƒmƒiƒN–(–) 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