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Published byTheodora Bernice Morton Modified over 6 years ago
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4D Gravity Inversion Hyoungrea Bernard Rim
Korea Institute of Geoscience and Mineral Resources (KIGAM) Gravity Workshop in KRISS December 1, 2016
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Outline Background Formulation 4D gravity inversion Numerical examples
Application to fluid fronts Two different model objective functions Numerical examples compare single-time versus 4D inversion compare single-component versus vector gravity Summary
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Time-Lapse Gravity Monitoring
Mimic Prudhoe Bay, GCWI Δρ = 0.12 g/cm3 Year 2 Year 5 Year 10 Year 15 Year 20 Brady et al, 2002 (Krahenbuhl et al. 2013)
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Research question: How should the multiple sets of time-lapse data be interpreted coherently?
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Separate single-time inversions
Layer-density distribution (e.g., Hare et al, 2008) Binary inversion (e.g., Krahenbuhl & Li, 2012) FCM inversion (Maag, 2014) 4D inversion for density change with time 4D inversion for reservoir properties Capriotti (2013) 4D inversion for fluid front
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Vector gravity: synthetic examples
Expanding plumes Simulate vector gravity due to expanding plumes
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Expanding plumes Injection vertical borehole 500 m expanding plumes
discrete representation with cubes
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Expanding plumes vertical borehole Injection 500 m expanding plumes
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Statement of problem Data: borehole gravity at multiple times
Model: fluid fronts at corresponding times Known top and bottom of the reservoir Known density contrast due to fluid substitution
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Model representation Distance from a reference point
Function of azimuth angle
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Inversion Regularized approach Data misfit
Two different model objective functions
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Model objective function-1
Generic regularization over azimuth and time
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Model objective function-2
Regularization over arc length and time
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synthetic example
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Single-hole Single-time inversions
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Single-hole 4D inversion
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Data comparison Time-1 Time-2 Time-3 Time-4 observed single-time inv
4D inv
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Vertical- components gravity 3-component gravity
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Data comparison (3-component data) Time-1 Time-2 Time-3 Time-4 gx gy
gz
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Comparison of model objective functions
Time-3 Time-4 Model obj. function-1 Model obj. function-2: Better accommodates rapid changes
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Data comparison - 3 wells - vertical component Time-1 Time-2 Time-3
observed
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Time-lapse vector gravity Prudhoe Bay
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Time-lapse gravity inversion
vertical gravity only vector gravity 3 monitoring wells 4 monitoring wells
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Summary 4D gravity inversion for fluid front
Better performance than single-time inversions Arc length-based model objective function better suited for detecting rapid change in the fluid front Vector gravity
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Work ahead Efficient modeling for reservoir with variable thickness and depth Consistent data misfit as a function of time Choice of time-dependent weighting coefficients Refine algorithm with field data
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Thank You!
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