TY - GEN
T1 - Experimental results on the combined effects of frequency, pressure and pore fluid on the dispersion of elastic waves in porous rock
AU - Fortin, Jerome
AU - Gueguen, Y.
AU - David, E.
AU - Adelinet, M.
AU - Piementa, L.
AU - Schubnel, A.
PY - 2013
Y1 - 2013
N2 - When cracks and pores are connected within a rock, stress can induce fluid flow from one inclusion to another one. Because cracks are more compliant than equant pores, a stress wave builds up a higher fluid pressure within a crack than within a pore and, consequently, fluid flows from crack to pore at a local scale. At low frequencies, fluid pressure has time to reach equilibrium. The elastic moduli are in that case relaxed moduli, those moduli are defined within the framework of poroelastic theory (drained or undrained moduli). Such a situation can be expected at seismic frequencies. However, in laboratory conditions, most of elastic waves data are obtained in the MHz range. Clearly, in such a high frequency range, there is no time for fluid pressure equilibrium to take place (even at local scale). The elastic moduli are unrelaxed moduli in that case. They are not those accounted for by poroelasticity, but they may be calculated from effective medium theory.
AB - When cracks and pores are connected within a rock, stress can induce fluid flow from one inclusion to another one. Because cracks are more compliant than equant pores, a stress wave builds up a higher fluid pressure within a crack than within a pore and, consequently, fluid flows from crack to pore at a local scale. At low frequencies, fluid pressure has time to reach equilibrium. The elastic moduli are in that case relaxed moduli, those moduli are defined within the framework of poroelastic theory (drained or undrained moduli). Such a situation can be expected at seismic frequencies. However, in laboratory conditions, most of elastic waves data are obtained in the MHz range. Clearly, in such a high frequency range, there is no time for fluid pressure equilibrium to take place (even at local scale). The elastic moduli are unrelaxed moduli in that case. They are not those accounted for by poroelasticity, but they may be calculated from effective medium theory.
UR - http://www.scopus.com/inward/record.url?scp=84887344902&partnerID=8YFLogxK
U2 - 10.1061/9780784412992.027
DO - 10.1061/9780784412992.027
M3 - Conference contribution
SN - 9780784412992
T3 - Poromechanics V - Proceedings of the 5th Biot Conference on Poromechanics
SP - 235
EP - 238
BT - Poromechanics V - Proceedings of the 5th Biot Conference on Poromechanics
T2 - 5th Biot Conference on Poromechanics, BIOT 2013
Y2 - 10 July 2013 through 12 July 2013
ER -