Gas saturation prediction and effect of low frequencies on acoustic impedance images at Foinaven Field

ABSTRACT Low frequencies are necessary in seismic data for proper acoustic impedance imaging and for petrophysical interpretation. Without lower frequencies, images can be distorted leading to incorrect reservoir interpretation and petrophysical predictions. As part of the Foinaven Active Reservoir...

Full description

Saved in:
Bibliographic Details
Published inGeophysical Prospecting Vol. 54; no. 1; pp. 75 - 87
Main Authors Wagner, Sean R., Pennington, Wayne D., MacBeth, Colin
Format Journal Article
LanguageEnglish
Published PO Box 1354, 9600 Garsington Road , Oxford OX4 2XG , UK Blackwell Science Ltd 01.01.2006
Blackwell
Subjects
Online AccessGet full text

Cover

Loading…
More Information
Summary:ABSTRACT Low frequencies are necessary in seismic data for proper acoustic impedance imaging and for petrophysical interpretation. Without lower frequencies, images can be distorted leading to incorrect reservoir interpretation and petrophysical predictions. As part of the Foinaven Active Reservoir Management (FARM) project, a Towed Streamer survey and an Ocean Bottom Hydrophone (OBH) survey were shot in both 1995 and 1998. The OBH surveys contain lower frequencies than the streamer surveys, providing a unique opportunity to study the effects that low frequencies have on both the acoustic impedance image along with petrophysical time‐lapse predictions. Artefacts that could easily have been interpreted as high‐resolution features in the streamer data impedance volumes can be distinguished by comparison with the impedance volumes created from the OBH surveys containing lower frequencies. In order to obtain results from the impedance volumes, impedance must be related to saturation. The mixing of exsolved gas, oil and water phases involves using the Reuss (uniform) or Voigt (patchy approximation) mixing laws. The Voigt average is easily misused by assuming that the end‐points correspond to 0% and 100% gas saturation. This implies that the patches are either 0% gas saturation or 100% gas saturation, which is never the case. Here, the distribution of gas as it comes out of solution is assumed to be uniform until the gas saturation reaches a sufficiently high value (critical gas saturation) to allow gas to flow. Therefore, at low gas saturations the distribution is uniform, but at saturations above critical, it is patchy, with patches that range from critical gas saturation to the highest gas saturation possible (1 minus residual oil and irreducible water saturation).
Bibliography:ArticleID:GPR517
ark:/67375/WNG-PBK6RSZV-B
istex:ADDB4AE9081EA87C0A51E4202627F930EF2ED1A5
ISSN:0016-8025
1365-2478
DOI:10.1111/j.1365-2478.2006.00517.x