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Istituto Nazionale di Oceanografia e di Geofisica Sperimentale (OGS), Trieste, Italy
Corresponding author: utinivella@ogs.trieste.it
| The first 20% of the full text of this article appears below. |
When no direct measurements are available, detailed knowledge of the compressional- and/or shear-wave velocity fields is essential for quantitative estimation of gas hydrate and free gas in bottom-simulating reflectors (BSR). Discrepancies between experimental velocity profiles and the velocity for water-filled sediments reveal the presence of gas hydrate (positive anomalies) and free gas (negative anomalies).
We use the model developed by Carcione and Tinivella (2000), based on a three-phase Biot-type theory, to obtain wave velocities of sediments saturated with water and gas hydrate, and the theory of Santos et al. (1990) to calculate the wave velocities of a porous medium saturated with a mixture of water and free gas. This model assumes that the free gas is uniformly distributed in the pore space. We use a second approach to model patchy saturation of free gas (Dvorkin et al., 1999).
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Figure 2 compares the theoretical P-wave velocity of water-saturated sediments (broken line) and the VSP wave velocity (solid line). The curves indicate that it is possible to estimate the presence of gas hydrate and free gas from the velocity anomaly. As observed by Guerin et al. (1999), compressional- and shear-wave velocity gradients
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