Williamson, J.P.; Chadwick, R.A.; Rowley, W.J.; Eiken, O.. 2001 Saline aquifer CO2 storage : a demonstration project at the Sleipner Field : Work Area 5 (Geophysics) : gravity modelling of the CO2 bubble. Nottingham, UK, British Geological Survey, 25pp. (CR/01/063N) (Unpublished)
Abstract
A principal aim of the SACS project is to monitor the injected CO2 by geophysical
methods and to develop a robust and repeatable monitoring and verification
methodology for future CO2 sequestration operations. This report evaluates the
applicability of microgravity surveys as a means of monitoring the future subsurface
distribution and migration of the Sleipner CO2 bubble.
Time-lapse seismic data acquired in 1999, after 2.3 MT of CO2 injection, show an
exceptionally clear image of the CO2 bubble, characterised by very high reflection
amplitudes. The outer envelope of the amplitude anomaly roughly defines an elliptical
cylindrical ‘bubble envelope’, ~ 225 m high, with a major axis of ~ 1500 m oriented
NNE and a minor axis of ~ 600 m.
Gravity modelling was based on a number of scenarios. Two ‘in situ’ scenarios
assume that the CO2 is entirely contained within the bubble envelope. The 1999 and
2001 in situ models assume respectively that 2.3 MT and 4MT of CO2 are contained
within the envelope. Two migration scenarios are also modelled. The first assumes
that 2.3MT of CO2 migrate vertically upwards into the overlying caprock succession
to between depths of 375 and 600 m. The second migration model looks further ahead
to the situation where 3 x 107 m3 (~ 10.5 – 21.0 MT depending on the density) of CO2
have been injected, and migrate laterally beneath the caprock at the top of the
reservoir.
Results depend strongly on the assumed density of the injected CO2 at reservoir
conditions, which is subject to significant uncertainty. Only one, poorly-constrained,
reservoir temperature measurement of 37 ° C is available. A density-depth profile
based on this suggests that the density of CO2 in the reservoir is ~ 700 kgm-3.
However the possibility of significantly lower densities cannot be discounted and
modelling also includes a lower density case of 350 kgm-3.
The 1999 and 2001 in situ cases produce anomalies which would be barely detectable
if the higher density of CO2 is assumed. With the lower density however anomalies
should be readily detectable with a modern seabed gravimeter. The vertical migration
scenario indicates that large-scale vertical migration into the caprock, to depths where
densities would be unequivocally lower, would be readily detected. The lateral
migration scenario, whereby a single thin layer of CO2 migrates beneath the top
reservoir seal, produces small anomalies which may be locally detectable but with
insufficient resolution to enable effective migration mapping. However if lateral
migration is via several layers, beneath intra-reservoir shales, then anomalies should
be more usefully measurable.
Obtaining time-lapse gravimeter readings directly above the bubble would appear to
offer the best chance of obtaining useful information. Coupled with geometric
information provided by the time-lapse seismic data, the gravity should be able to
discriminate between the low and high CO2 density scenarios. This would provide
important constraints on future reservoir modelling and also the volume estimates
based on the seismic velocity pushdown effect. Related to this, gravity data would
offer the potential to provide independent verification of the amount of CO2 sequestered. In addition gravimetric surveys above the bubble could provide an
effective ‘early warning’ of major caprock breaching.
Information
Programmes:
A Pre-2012 Programme
Library
Statistics
Downloads per month over past year
Share
![]() |
