Mrinal Sinha

and 3 more

Carbon capture and storage (CCS) is forecast to play a significant role towards CO2 emissions reduction. Cost-effective and simplified monitoring will be essential for rapid adoption and growth of CCS. Seismic imaging methods are regularly utilized to monitor low-velocity anomalies generated by injection of CO2 in the subsurface. In this study we generate active and passive synthetic seismic datasets at different stages of CO2 injection in the subsurface based on geologically constrained subsurface models of the Pelican storage site in the Gippsland Basin, Australia. We apply full waveform inversion (FWI) and wave-equation dispersion (WD) inversion to seafloor deployed distributed acoustic sensing (DAS) data to reconstruct the low-velocity anomalies. We model both strain (DAS) and displacement datasets for the active data component of the study and show that they result in similar reconstruction of the CO2 anomaly. FWI based time-lapse imaging of active data yields the most accurate results. However, this approach is expensive and also suffers from complex issues because of the near-onshore location of the storage site. Alternatively inverting passive data results in only minor differences, but can still effectively monitor changes in the subsurface, and assist in monitoring the CO2 plume at the reservoir depth. Furthermore, we demonstrate the capability of WD for inverting Scholte-waves derived from ambient noise for shallow detection of CO2 in the unlikely event of a leakage. Therefore, we propose a mixed mode monitoring strategy where passive data is utilised for routine monitoring while active surveys are deployed only when further investigation is required.

Peng Guo

and 2 more

Mehdi Tork Qashqai

and 1 more

The sensitivity of seismic compressional and shear waves and their velocity ratios to rock lithology, pore fluids, and high-temperature materials makes these parameters very useful for constraining the physical state of the crust. In this study, we develop a joint inversion approach utilizing both radial and vertical components’ autocorrelations of tele seismic P-wave coda for imaging the crust by simultaneously characterizing the crustal Vp, Vs and Vp/Vs ratio. Autocorrelations of the radial and vertical components contain P and S waves that are reflected from the subsurface. Therefore, joint inversion of them can account for the variations of both Vp and Vs, and consequently, the Vp/Vs ratio. Synthetic inversions show significant improvement in the estimation of these parameters com pared to those from the inversion of either, receiver functions or the autocorrelation of the vertical component. The velocity models inferred from the application of the approach to teleseismic data recorded along a north-south passive seismic profile (BILBY experiment) in central Australia reveal a distinct pattern of the Moho and the Vp/Vs variations across the crustal blocks/domain. The general trend of the Moho structure corresponds well with the change of the reflectivity that can normally be seen at the base of the crust and also with the Moho estimated from the previous studies including the deep seismic reflection profiling method. The Vp/Vs structure at depths greater than 10 km shows dominant high values beneath locations where the crustal domains interact (e.g., at transition from one domain to another).

yuqing chen

and 1 more

Ambient noise seismic data are widely used by geophysicists to explore subsurface properties at crustal and exploration scales. Two-step dispersion inversion schema is the dominant method used to invert the surface wave data generated by the cross-correlation of ambient noise signals. However, the two-step methods have a 1-D layered model assumption, which does not account for the complex wave propagation. To overcome this limitation, we employ a 2-D wave-equation dispersion inversion (WD) method which reconstructs the subsurface shear (S) velocity model in one step, and elastic wave-equation modeling is used to simulate the subsurface wave propagation. In the WD method, the optimal S velocity model is obtained by minimizing the dispersion curve differences between the observed and predicted surface wave data. This dispersion curve misfit makes the WD method less prone to getting stuck to local minima compared with full waveform inversion. In our study, the observed Scholte waves are generated by cross-correlating continuous ambient noise signals recorded by ocean-bottom nodes (OBN) in the 3-D Gorgon OBN survey, Western Australia. For every two OBN lines, the WD method is used to retrieve the 2-D S velocity structure beneath the first line. We then use a robust neural network based method to interpolate the inverted 2-D velocity slices to a continuous 3-D velocity model and also obtain a corresponding 3-D uncertainty model. Overall, a robust waveform and dispersion match between the observed and predicted data is observed across all of the Gorgon OBN lines both on inverted and interpolated velocity models.