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4D Gravity Inversion Hyoungrea Bernard Rim

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Presentation on theme: "4D Gravity Inversion Hyoungrea Bernard Rim"— Presentation transcript:

1 4D Gravity Inversion Hyoungrea Bernard Rim
Korea Institute of Geoscience and Mineral Resources (KIGAM) Gravity Workshop in KRISS December 1, 2016

2 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

3 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)

4 Research question: How should the multiple sets of time-lapse data be interpreted coherently?

5 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

6 Vector gravity: synthetic examples
Expanding plumes Simulate vector gravity due to expanding plumes

7 Expanding plumes Injection vertical borehole 500 m expanding plumes
discrete representation with cubes

8 Expanding plumes vertical borehole Injection 500 m expanding plumes

9 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

10 Model representation Distance from a reference point
Function of azimuth angle

11 Inversion Regularized approach Data misfit
Two different model objective functions

12 Model objective function-1
Generic regularization over azimuth and time

13 Model objective function-2
Regularization over arc length and time

14 synthetic example

15 Single-hole Single-time inversions

16 Single-hole 4D inversion

17 Data comparison Time-1 Time-2 Time-3 Time-4 observed single-time inv
4D inv

18 Vertical- components gravity 3-component gravity

19 Data comparison (3-component data) Time-1 Time-2 Time-3 Time-4 gx gy
gz

20 Comparison of model objective functions
Time-3 Time-4 Model obj. function-1 Model obj. function-2: Better accommodates rapid changes

21 Data comparison - 3 wells - vertical component Time-1 Time-2 Time-3
observed

22 Time-lapse vector gravity Prudhoe Bay

23 Time-lapse gravity inversion
vertical gravity only vector gravity 3 monitoring wells 4 monitoring wells

24 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

25 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

26 Thank You!


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