P waves traveling in thermoelastic materials suffer attenuation and dispersion due to the existence of the thermal (T) wave, which is diffusive at low frequencies and is a propagation wave at high frequencies. Thus, this wave behaves similarly to the slow P wave in Biot (poroelastic) media. We presents a finiteelement (FE) procedure to determine an effective viscoelastic medium long-wave equivalent to a thermoelastic material, by applying compressibility and shear tests. Each test is defined by a boundary-value problem and the procedure is validated by comparison with an analytical solution for a periodic sequence of two layers of equal thickness and different Grüneisen ratios. The S wave is not sensitive to variations of this ratio, so that only the S-wave velocity is determined. Next, we consider a layered medium with varying Grüneisen ratios and random layer thicknesses, for which there is no analytical solution available. This case shows a decrease in the P-wave phase velocities and an increase in the dissipation factors, with respect to the previous case. Representations of the real an imaginary parts of the temperature illustrate the attenuation effects.
Effective P-and S-wave moduli in finely layered thermoelastic media
Carcione J. M.;
2020-01-01
Abstract
P waves traveling in thermoelastic materials suffer attenuation and dispersion due to the existence of the thermal (T) wave, which is diffusive at low frequencies and is a propagation wave at high frequencies. Thus, this wave behaves similarly to the slow P wave in Biot (poroelastic) media. We presents a finiteelement (FE) procedure to determine an effective viscoelastic medium long-wave equivalent to a thermoelastic material, by applying compressibility and shear tests. Each test is defined by a boundary-value problem and the procedure is validated by comparison with an analytical solution for a periodic sequence of two layers of equal thickness and different Grüneisen ratios. The S wave is not sensitive to variations of this ratio, so that only the S-wave velocity is determined. Next, we consider a layered medium with varying Grüneisen ratios and random layer thicknesses, for which there is no analytical solution available. This case shows a decrease in the P-wave phase velocities and an increase in the dissipation factors, with respect to the previous case. Representations of the real an imaginary parts of the temperature illustrate the attenuation effects.I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.