HR: 1320h
AN: S43A-0973 [Abstracts]
TI: Estimation of Gas-hydrate Saturation at the Hydrate Ridge, Offshore Oregon
AU: * Kumar, D
EM: dhananjay@mail.utexas.edu
AF: University of Texas Institute for Geophysics, 4412 Spicewood Springs Rd., Bldg. 600, Austin, TX 78759
AU: Sen, M K
EM: mrinal@ig.utexas.edu
AF: University of Texas Institute for Geophysics, 4412 Spicewood Springs Rd., Bldg. 600, Austin, TX 78759
AU: Bangs, N L
EM: nathan@ig.utexas.edu
AF: University of Texas Institute for Geophysics, 4412 Spicewood Springs Rd., Bldg. 600, Austin, TX 78759
AB:
Multicomponent seismic data were acquired in summer 2002, offshore Oregon, on the Hydrate Ridge of the Cascadia convergent
margin. The primary goal of the experiment was to map the gas hydrates and free gas (methane) and understand the mechanism of
fluid migration. Our analysis estimated the compressional- (P-wave) and shear-wave (S-wave) interval velocities with the
final goal of relating these velocities to the presence and quantification of gas hydrate and free gas. We performed interval
velocity analysis in the tau-p (intercept time - ray parameters) domain following three main steps: 1) P-wave velocity
analysis, 2) P- to S-wave (converted S-wave) event correlation, and 3) S-wave velocity analysis. We correlated P- to S-wave
event for a reflector using synthetic seismograms (generated with reflectivity method) and traveltime tables. A traveltime
table contains the arrival times of different wavetypes for a reflector and is calculated using the sonic logs or modeled
velocities. Seismic velocities are correlated to gas hydrate saturation using a Modified Wood equation. We found that maximum
saturation of gas hydrate is 7% of pore space. The P-wave velocity is lower down to 50m below the sea floor at the south
summit, probably because of the presence of free gas within the gas hydrate stability zone (GHSZ). Gas probably migrated from
below GHSZ up to sea floor through near-vertical fractures. We identified hydrate-bearing- and free-gas-bearing sediments
with anomalous increase and decrease of P-wave velocity, respectively (with a reference velocity calculated in water
saturated sediments). However, S-wave velocity does not show anomalous increase in the hydrate-bearing sediments. Thus, we
interpret that hydrate does not cement sediment grains enough to affect shear properties. It is more likely that hydrates
form within pore spaces.
DE: 5102 Acoustic properties
DE: 5104 Fracture and flow
DE: 7203 Body wave propagation
DE: 3210 Modeling
DE: 0902 Computational methods, seismic
SC: Seismology [S]
MN: 2004 AGU Fall Meeting