All Days 1980
DOI: 10.2118/9041-ms
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Advancements in Electromagnetic Propagation Logging

Abstract: The basic theory upon which the microwave Electromagnetic Propagation Tool (EPT) has been founded is reviewed, and the measurement technique is discussed in terms of a functional block diagram. Two methods of interpreting the propagating wave's measured phase and attenuation are reviewed. Specific log examples which distinguish between hydrocarbon and water-bearing zones in several lithologies are presented..

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Cited by 39 publications
(8 citation statements)
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“…After bandpass filtering (frequency range between 3 and 9 MHz), the data were migrated to account for off-angle reflections from sloped interfaces (e.g., the lateral walls of the subglacial conduit/ice-shelf channels) using Kirchoff-Depth migration implemented in the open-source software Seismic Unix. The required radio-wave velocity model varies with depth using a depth–density parameterization 53 and a density–velocity relation 54 . The grounding-zone of Roi Baudouin Ice Shelf is characterized by an extensive blue-ice belt so that the radio-wave velocity is close to the pure-ice velocity (1.68·10 8 m s −1 ) everywhere.…”
Section: Methodsmentioning
confidence: 99%
“…After bandpass filtering (frequency range between 3 and 9 MHz), the data were migrated to account for off-angle reflections from sloped interfaces (e.g., the lateral walls of the subglacial conduit/ice-shelf channels) using Kirchoff-Depth migration implemented in the open-source software Seismic Unix. The required radio-wave velocity model varies with depth using a depth–density parameterization 53 and a density–velocity relation 54 . The grounding-zone of Roi Baudouin Ice Shelf is characterized by an extensive blue-ice belt so that the radio-wave velocity is close to the pure-ice velocity (1.68·10 8 m s −1 ) everywhere.…”
Section: Methodsmentioning
confidence: 99%
“…Using this expression, v was expressed as a ε r(b) and used as input to the Complex Refractive Index Model (CRIM) to calculate gas content [e.g., Huisman et al ., ]. The CRIM is a volumetric three‐phase mixing model for the soil [ Wharton et al ., ], εrnormalbα=θεrnormalwα+()1nεrnormalsα+()nθεrnormalaαwhere ε r(a) , ε r(w) , and ε r(s) are the relative dielectric permittivity of gas (= 1), water (temperature dependent), and soil particles (= 2; after Comas et al . []), respectively, n is the porosity, θ is the volumetric soil water content, and α is a factor accounting for the orientation of the electrical field and the geometrical arrangement of minerals (typically 0.35 for peat soils [ Kellner et al ., ; Parsekian et al ., ]).…”
Section: Methodology and Experimental Setupmentioning
confidence: 99%
“…Assuming peat soil is a low loss medium, the EM wave velocity ( v ) can be expressed as: where ɛ r(b) is the relative dielectric permittivity of the peat soil and c = 3 × 10 8 m/s. In order to estimate gas content from v we applied the Complex Refractive Index Model (CRIM) [e.g., Huisman et al , 2003], which is a volumetric mixing model for a soil [ Wharton et al , 1980]: where ɛ r(a) , ɛ r(w) , and ɛ r(s) are the relative dielectric permittivity of gas (1), water (80 at 21 °C) and the soil particles respectively, n is the porosity, θ is the volumetric soil water content and α is a factor accounting for the orientation of the electrical field and the geometrical arrangement of peat fibers (typically 0.35 for peat soils [ Kellner et al , 2005]). As later explained in the results section, gas content estimation using the CRIM accounted for: (1) changes in porosity as a function of time due to peat surface deformation; (2) changes in ɛ r(w) due to temperature variation of the peat column; and (3) changes in water table elevation concurrently monitored during GPR data acquisition.…”
Section: Experimental Field Design and Methodologymentioning
confidence: 99%