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Title Effects of single fractures on seismic wave propagation
Creator/Author Myer, L.R. (Lawrence Berkeley Lab., CA (USA)) ; Pyrak-Nolte, L.J. (Purdue Univ., Lafayette, IN (USA). Dept. of Earth and Atmospheric Sciences) ; Cook, N.G.W. (Lawrence Berkeley Lab., CA (USA) California Univ., Berkeley, CA (USA). Dept. of Materials Science and Mineral Engineering)
Publication Date1990 Jan 01
OSTI IdentifierOSTI ID: 7041898; Legacy ID: DE90009191
Report Number(s)LBL-28442; CONF-900640--4
DOE Contract NumberAC03-76SF00098
Other Number(s)Other: ON: DE90009191
Resource TypeConference
Specific TypeTechnical Report
Resource RelationConference: International conference on rock joints, Loen (Norway), 4-6 Jun 1990
Research OrgLawrence Berkeley Lab., CA (USA)
Sponsoring OrgDOE/ER; DOE/RW
Subject02 PETROLEUM; 03 NATURAL GAS; 58 GEOSCIENCES; 99 GENERAL AND MISCELLANEOUS//MATHEMATICS, COMPUTING, AND INFORMATION SCIENCE; GEOLOGIC FRACTURES; MATHEMATICAL MODELS; ROCKS; WAVE PROPAGATION; SEISMIC WAVES; FLUID FLOW; OIL FIELDS; SEISMIC EFFECTS; STRESSES; VISCOSITY; GEOLOGIC DEPOSITS; GEOLOGIC STRUCTURES; MINERAL RESOURCES; PETROLEUM DEPOSITS; RESOURCES
Description/AbstractDetection and characterization of fractures, joints and faults remains an important problem in mining and geotechnical engineering, as well as in petroleum reservoir engineering. A theoretical model has been developed which predicts the amplitude and group time delay of the transmitted, reflected, and converted waves resulting from a plane wave incident upon a single fracture. It is assumed that seismic stresses are continuous across the interface. Seismic particle displacements, however, are assumed to be discontinuous. For completely dry conditions, the magnitude of the displacement discontinuity is given by the ratio of the seismic stress to the stiffness, {kappa}, of the fracture. If a fluid is present in the fracture, we postulate that, in addition to the displacement discontinuity, a velocity discontinuity exists which is equal to the ratio of the seismic stress to specific viscosity, {eta}. The wave equation has been solved for two sets of boundary conditions, with each set incorporating both specific stiffness and specific viscosity. These boundary conditions have been designated as Kelvin and Maxwell models. 12 refs., 5 figs.
Country of PublicationUnited States
LanguageEnglish
FormatMedium: X; Size: Pages: (8 p)
AvailabilityNTIS, PC A02/MF A01 - OSTI; GPO Dep.
System Entry Date2008 Feb 12

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