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TERRACING POTENTIAL FIELD DATA

G. R. J. Cooper, D.R. Cowan

First published: 2009DOI pendingView metrics

Abstract

Terracing (Cordell and McCafferty, 1989, Philips, 1992) is an operator that is applied to potential field data to produce regions of constant field amplitude that are separated by sharp boundaries. Magnetic data is usually transformed into pseudogravity data (Baranov, 1957) prior to the application of terracing. The objective of terracing is ’to recast potential field maps into a geologic map like format’ (Cordell and McCafferty, 1989). Terracing is performed by moving a window through the data and computing the curvature at each point.

Publication details

Title
TERRACING POTENTIAL FIELD DATA
Authors
G. R. J. Cooper, D.R. Cowan
Proceedings
9th International Multidisciplinary Scientific GeoConference SGEM2009
Publisher
SGEM Scientific GeoConference
Year
2009
Pages
717-720
ISSN
1314-2704
ISBN
954-91818-1-2
Language
en
Publication type
Conference Paper
References17
  1. Baranov., V.,

  2. 1957. A new method for the inte gravimetric anomalies. Geophysics 22, 359-383. Blakely, R.J.,

  3. 1995. Potential Theory in Gravit University Press. Blakely. R. J., and

  4. W., 1986, Locat gravity anomalies: Geophysics 51, 1494-1498.

  5. Cordell, L., and McCafferty,

  6. A.E., 1989, A mapping with potential field data: Geophysics 54

  7. Mitasova, H., and Jarosalav, H.,

  8. 1993. Int Tension: II. Application to Terrain Mode Mathematical Geology 25 (6) 657-669. Philips, J.D.,

  9. 1992. TERRACE: A terracing p programs, and VAX Command Procedure implementations. Department of the interior, U

  10. 5. FIGUR Function values at data point x at the n+1st maximum or minimum of the nth iteration v Applied and Environmental Geophysics thanked for permission to use the gravity data e interpretation of aeromagnetic maps: pseudo-

  11. 9-383. Gravity and Magnetic Applications. Cambridge Locating edges of source bodies for magnetic or

  12. 9, A terracing operator for physical property sics 54 (5) 621-634.

  13. 3. Interpolation by Regularized Spline with Modeling and Surface Geometry Analysis, cing procedure for gridded data, with Fortran edure, Unix C-Shell, and DOS batch file ior, U.S. geological survey open file report 92- GURE 1 n+1st iteration are kept the same or set to the ion values of the function within the narrow International Multidisciplinary Scientific GeoConfe window w (centered on x ) on the basis of the and McCafferty,

  14. 1989). FIGUR a) Gravity data from the three rectangular bod is 200x200 units in size and the depth of the body and 15 units for the other bodies. The function is plotted as a thin black line, while th plotted as a thick black line. The density contra b) Gravity data terraced using the Laplacian used. c) Gravity data terraced using the profile curva FIGUR a) Gravity data from a portion of the Witwate

  15. 300x300km in size, and the gravity values ran (blue). b) Gravity data terraced using the Laplacian used. c) Gravity data terraced using the profile curva of the direction of the curvature (from Cordell GURE 2 r bodies whose outlines are shown. The image of the bodies is 25 units for the northernmost The zero contour of the Laplacian derivative hile the zero contour of the profile curvature is contrasts used were

  16. 0.1, -0.1, and

  17. 0.05g.cm-3. acian derivative function. 20 Iterations were curvature. 20 Iterations were used. GURE 3 twatersrand basin, South Africa. The image is es range from -80 mGals (red) to -180 mGals acian derivative function. 20 Iterations were curvature. 20 Iterations were used.

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