Theory of compressional and transverse wave propagation in consolidated porous media

Authors
Citation
Mj. Buckingham, Theory of compressional and transverse wave propagation in consolidated porous media, J ACOUST SO, 106(2), 1999, pp. 575-581
Citations number
31
Categorie Soggetti
Multidisciplinary,"Optics & Acoustics
Journal title
JOURNAL OF THE ACOUSTICAL SOCIETY OF AMERICA
ISSN journal
00014966 → ACNP
Volume
106
Issue
2
Year of publication
1999
Pages
575 - 581
Database
ISI
SICI code
0001-4966(199908)106:2<575:TOCATW>2.0.ZU;2-H
Abstract
A theory of compressional and shear wave propagation in consolidated porous media (rocks) is developed by extending ideas already introduced in: conne ction with unconsolidated marine sediments. The consolidated material is tr eated as an elastic medium which exhibits a specific form of stress relaxat ion associated with grain boundaries and microcracks. The stress relaxation , which is linear in the sense that it obeys superposition, shows hysteresi s, as characterized by a material response function. Two linear wave equati ons are derived, one for compressional and the second for shear waves, from which expressions for the wave speeds and attenuations are established. In both cases, the attenuation is found to scale with the first power of freq uency, consistent with many observations of attenuation in sandstones, lime stones, and shales; the wave speeds show weak logarithmic dispersion. These expressions for the wave speeds and attenuations satisfy the Kronig-Kramer s dispersion relationships, as they must if the response of the medium to d isturbances is to be causal. Some comments are offered on the nature of the material response, notably that it appears to be primarily associated with grain-boundary interactions: occurring at a molecular level, rather than b eing related to the macroscopic properties of the material, such as density or porosity. (C) 1999 Acoustical Society of America. America. [S0001-4966( 99)02106-2].