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Seismic studies of the northern Cascadia accretionary prism: sediment consolidation and gas hydrates

This thesis work was directed at aspects of two related problems: (1) sediment
compaction and fluid expulsion processes in a subduction margin accretionary prism, and (2)
the nature and concentration of gas hydrates that form bottom-simulating reflectors (BSRs)
observed in the accretionary prism sediments of the northern Cascadia margin. The formation
of the gas hydrate and the occurrence of BSRs in the study area are believed to be mainly a
consequence of upward fluid expulsion in the accretionary prism. Therefore, the two study
objectives are closely correlated. Most of this thesis work was carried out analyzing
multichannel seismic data and incorporating available information including downhole and
other geophysical measurements. Seismic techniques, such as velocity analysis, forward
modelling, and waveform velocity inversion, were used in analyzing the data to advance our
understanding of the tectonic and geophysical processes in a dynamic accretionary prism
environment.
The velocity structure and the inferred porosity variations across the frontal region
of the accretionary prism have been quantitatively assessed by a detailed seismic velocity
analysis. Within the Cascadia basin sediments approaching the deformation front, and within
the frontal thrust zone of the accretionary prism, seismic velocities increase landward as a
result of sediment consolidation. An important conclusion is that more than one third of the
pore fluid content of the incoming sediment is lost by the time they are incorporated into the
accretionary prism. In the lower slope region of the deformation front, a pronounced velocity
decrease is evident. This low-velocity zone is explained by underconsolidation resulting from
rapid horizontal shortening and vertical thickening of the sediment column, accommodated
by displacements along thrust faults or by distributed deformation.
A prominent BSR becomes visible immediately landward of the deformation front in
the accreted sediment, and is developed over much of the low-to-mid continental slope. The
upward pore-fluid migration is believed to play an important role in the formation of a gas
hydrate BSR. From the estimated fluid loss of 35% over the 3-km-thick Cascadia Basin
sediments with an average sediment porosity of 30%, the quantity of the expelled fluid
reaches 315 m3/m2 over a distance of 12 km before the basin sediments are incorporated into
the accretionary prism. Assuming that 100 mmol/L of methane is removed from the expelled
fluid as it moves into the hydrate stability field, a 90-m-thick layer with an average hydrate
saturation of 10% of the pore space can be formed by the rising fluids.
A velocity-depth function in the lower slope region, representing a no-hydrate/no-gas
reference profile, has been established from the detailed semblance velocity analyses and the
ODP log data. The observed and measured sediment velocities near the ODP drill sites
increase downward more rapidly than the reference profile above the BSR. Based on the
reference profile, the velocity inversion results imply that the velocity increase due to hydrate
above the BSR accounts for ~2/3 of the impedance contrast required to produce the BSR
reflection amplitudes. The remainder of the impedance contrast appears to come from the
velocity decrease associated with small concentrations of free gas below the BSR.
The integrated analysis of the multichannel seismic and ODP downhole velocity data
has allowed the velocity enhancement associated with the formation and concentration of gas
hydrate to be estimated. If the BSR is overlain by a 100 m zone of sediment with a mean
porosity of 50% in which the hydrate saturation increases linearly from zero at the top of the
zone to 20% at the BSR, the estimated hydrate concentration-depth profiles indicate a total
hydrate amount of about 5 m3/m2 of ocean floor or methane amount of 820 m3/m2 at STP.
Throughout the Vancouver Island continental margin, where the clear BSR have been
observed in an area of 30x200 km, the total methane gas estimated can amount to about 175 Tcf (trillion cubic feet) or 2.6 Gt of carbon. / Graduate

Identiferoai:union.ndltd.org:uvic.ca/oai:dspace.library.uvic.ca:1828/9749
Date19 July 2018
CreatorsYuan, Tianson
ContributorsSpence, G. D.
Source SetsUniversity of Victoria
LanguageEnglish, English
Detected LanguageEnglish
TypeThesis
Formatapplication/pdf
RightsAvailable to the World Wide Web

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