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publications > ofr > OFR-02-101 > dighem report products and processing techniques
PRODUCTS AND PROCESSING TECHNIQUES
The following products are available from the survey data. Those which are not part of the survey contract may be acquired later. Refer to Table 3-1 for a summary of the maps which accompany this report, some of which may be sent under separate cover. Most parameters can be displayed as contours, profiles, or in colour. Base MapsBase maps of the survey area have been produced from the 1:100,000 scale Cape Sable, Everglades City, Miami and Homestead topographic map sheets. These were joined and photographically reproduced to a scale of 1:48,000. The topographic base maps were hand digitized to produce the skeletal topography for the colour maps. ResistivityThe apparent resistivity in ohm-m was generated from the inphase and quadrature EM components for the 900 Hz, 7,200 Hz and 56,000 Hz frequencies, using a pseudo-layer halfspace model. A resistivity map portrays all the EM information for that frequency over the entire survey area. The large dynamic range makes the resistivity parameter an excellent mapping tool.
900 Hz resistivity contours The final prints display the geophysical parameter combined with the flight path on a screened topographic base. Two sets of black and white prints are supplied. 900 Hz resistivity colours (648K JPG file, 10.5 MB PDF file) The colour maps display superimposed contours, flight path, skeletal topography, Lat/Long's and UTM coordinates. Two sets of colour maps are supplied. Digital XYZ archives with documentation Note: The XYZ archives are supplied on a DOS compatible CD-ROM in Geopak ASCII format.
Multi-channel Stacked ProfilesDistance-based profiles of the digitally recorded geophysical data are generated and plotted by computer. These profiles also contain the calculated parameters which are used in the interpretation process. These are produced in the final corrected form after interpretation. Contour and Colour DisplaysThe geophysical data are interpolated onto a regular grid using a modified Akima spline technique. The resulting grid is suitable for generating contour maps of excellent quality. Colour maps are produced by interpolating the grid down to the pixel size. The parameter is then incremented with respect to specific amplitude ranges to provide colour "contour" maps. Conductivity-depth SectionsThe apparent resistivities for all frequencies can be displayed simultaneously as coloured conductivity-depth sections. Usually, only the coplanar data are displayed as the quality tends to be higher than that of the coaxial data. Conductivity-depth sections can be generated in two formats: (1) Sengpiel resistivity sections, where the apparent resistivity for each frequency is plotted at the depth of the centroid of the inphase current flow1; and, (2) Differential resistivity sections, where the differential resistivity is plotted at the differential depth2. Both the Sengpiel and differential methods are derived from the pseudo-layer halfspace model. Both yield a coloured conductivity-depth section which attempts to portray a smoothed approximation of the true resistivity distribution with depth. The Sengpiel method is most useful in conductive layered situations, but may be unreliable in areas of moderate to high resistivity where signal amplitudes are weak. In areas where inphase responses have been suppressed by the effects of magnetite, the computed resistivities shown on the sections may be unreliable. The differential technique was developed by Dighem to overcome problems in the Sengpiel technique. The differential resistivity section is more sensitive than the Sengpiel section to changes in the earth's resistivity and it reaches deeper.
1 Approximate Inversion of Airborne EM Data from Multilayered Ground: Sengpiel, K.P., Geophysical Prospecting 36, 446-459, 1988. 2 The Differential Resistivity Method for Multi-frequency Airborne EM Sounding: Huang, H. and Fraser, D.C., presented at Intern. Airb. EM Workshop, Tucson, Ariz., 1993.
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Last updated: 02 December, 2004 @ 02:05 PM (KP)