Down-Hole Geophysical Testing for Rock Sockets Dennis R. Hiltunen
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Down-Hole Geophysical Testing for Rock Sockets Dennis R. Hiltunen
Down-Hole Geophysical Testing for Rock Sockets Dennis R. Hiltunen Pengxiang Jiang University of Florida FDOT GRIP August 17, 2012 Ft. McCoy ■ Surface array: 31 geophones at 1-m spacing ■ Borehole array: geophones 4-18 m at 1-m spacing ■ Sledgehammer source: 1,2,3,4,5,6,8,10,12,15 m each side of well Ft. McCoy 60 Observed Estimated 50 -4 -6 -8 Depth (m) Arrival time (ms) 40 30 20 -10 -12 Observed Estimated -14 10 -16 0 -18 5 -10 0 5 10 15 Distance (m) 20 25 30 10 15 20 Arrival time (ms) 25 30 35 Ft. McCoy -2 1800 -4 1600 -6 1400 1200 -8 1000 -10 800 -12 600 -14 P_wave velocity (m/s) Depth (m) 0 400 -16 -18 0 5 10 15 20 25 30 Distance (m) d) -2 55 50 -4 45 40 Depth (m) -6 35 -8 30 25 -10 20 -12 15 10 -14 5 0 -16 -18 0 5 10 15 Distance (m) 20 25 30 Coefficient of Variation (%) 0 Workplan ■ Task 1: Review Literature and State of Practice Single-well borehole logging devices ■ Task 2: Computer and Synthetic Model Studies Borehole instrumentation, full waveform analysis Preliminary array design: geometry, instrumentation ■ Task 3: Array Experiments Test/modify preliminary array design In-house instrumentation ■ Task 4: Design Borehole Tool Mechanical design of array, analysis software ■ Task 5: Report Chabot (2003) University of Calgary Sonic logging tool in fluid-filled borehole Seismic reflectionstyle processing Full waveform analysis of body waves (P and S) No surface waves Kalinski (1998) University of Texas (Stokoe) SASW along axis of borehole (1-D) Concrete, rock, and soil Geometry-induced dispersion Normalized magnitude Full Waveform: FD vs. FEM 0 300 m/s 5 10 200 m/s 1 25 400 m/s 30 35 0 20 40 X, m 60 80 FDM FEM 0.5 0 -0.5 -1 20 Normalized magnitude Y, m 15 Receiver @ 30m 0 0.2 0.4 0.6 0.8 1 Receiver @ 60m 1 FDM FEM 0.5 0 -0.5 -1 0 0.2 0.4 0.6 time in sec 0.8 1 Full Waveform: LVL at TAMU SV-Wave Velocity (m/s) 0 100 200 300 400 0 500 Standard Penetration Resistance (SPT N-Value) 0 2 12 15 18 4 15 14 Tan Sand 6 13 17 Tan Silty Fine Sand Tan Silty Fine Sand 6 Tan Sandy Clay 10 10 60 12 70 Dark Gray Clay w/Gravel 52 12 14 62 16 4 8 20 14 2 Gravel 16 8 Depth (m) Soil Profile 0 10 20 30 40 50 60 70 80 90 Dark Gray Clay 16 18 18 Crosshole test 20 22 20 Full wave inversion of 3 layers + half space Full wave inversion of 4 layers + half space 22 24 24 EOB 15.2m Full Waveform: Seg 2D at TAMU FWI: Layer 2D finite difference model Simulated annealing and genetic algorithm Surface array Array and source design FWI: Block FWI: Block in Gradient FWI: 5x5 Grid, 0.5 m Forward Model Questions ■ Original premise: Can we slice a radial plane from the borehole, put a source and array of receivers along the vertical borehole axis edge, and then model with a 2D, plane-strain, flatground model? ■ Under investigation: Or, do the actual surroundings of the borehole geometry significantly influence the wavefield and the waveforms collected along the borehole axis? Geometry-Induced Dispersion 2D, Flat-Ground Models Plane-strain: FD, Plaxis, Abaqus Axisymmetric: Plaxis, Abaqus Waveforms similar for all three codes Movies 2.5D, Axisymmetric, Borehole Model Two models: Plaxis, Abaqus Ring load Waveforms similar for both codes 3D Borehole Model Abaqus Ring load Point load Movies 3D Borehole Model, 50 cm Radius Code: Abaqus Configuration: R=10 m, r=50 cm, L=20 m Properties: Vs=1000 m/s Array: 20 @ 0.25 m along borehole wall Source: point, triangular, center of cylinder, S=0.25 m 3D Borehole Model, 5 cm Radius Code: Abaqus Configuration: R=10 m, r=5 cm, L=20 m Properties: Vs=1000 m/s Array: 20 @ 0.25 m along borehole wall Source: point, triangular, center of cylinder, S=0.25 m Compare: Waveforms 2D 50 cm 2.5D 5 cm Compare: Waveforms at x=middle Compare: Dispersion Images 2D 50 cm 2.5D 5 cm Inversion with 2D, Plane-Strain, Flat-Ground Model: 3D Flat Ground Code: Abaqus synthetic Configuration: 20 m cube Properties: Vs=1000 m/s Array: 10 @ 0.5 m Source: point, triangular, S=0.5 m Inversion: 6 m x 6 m, 2 layers +half-space Waveforms not well matched, but return about 1000 m/s Inversion with 2D, Plane-Strain, Flat-Ground Model: 50 cm Radius Code: Abaqus synthetic Configuration: R=10 m, r=50 cm, L=20 m Properties Vs=1000 m/s Array: 10 @ 0.5 m along borehole wall Source: point, triangular, center of cylinder, S=0.5 m Inversion: 6 m x 6 m, 2 layers +half-space Waveforms not well matched, return stiffer than 1000 m/s Forward Model Questions ■ Summary: appears that borehole influence is significant, based on wavefield movies, dispersion curves, waveform comparisons, and inversions assuming 2D plane-strain, flatground model ■ Future: original premise does not appear feasible, require a forward model that includes borehole geometry, e.g., build a FD model, use existing FEM code Two Solutions ■ Have built two inversion models that use borehole model in Abaqus to invert waveforms collected along vertical wall of borehole ■ First inversion model uses simulated annealing ■ Second inversion model uses linearized, local inversion following recent work of Tran ■ 2.5D a few seconds, 3D an hour for each forward ■ Good for a ring experiment, 2.5D and 3D similar Abaqus FWI: Flat-Ground, 5x5 Grid 9 True model x 10 9 0.5 1 8 1.5 7 2 9 Inverted model x 10 9 0.5 1 8 1.5 7 2 6 2.5 6 2.5 3 5 3.5 4 4 3 5 3.5 4 4 3 4.5 2 5 5.5 3 4.5 1 2 3 4 5 1 2 5 5.5 1 2 3 4 5 1 Abaqus FWI: 2.5D Borehole, 5x5 Grid 9 True model x 10 5 0.5 1 4.5 1.5 9 Inverted model x 10 0.5 6 1 5.5 1.5 4 2 5 2 3.5 2.5 4.5 2.5 4 3 3 3 3.5 3.5 2.5 4 3.5 3 4 2.5 2 4.5 4.5 5 5.5 2 1.5 5 1 2 3 4 5 1 5.5 1.5 1 1 2 3 4 5 Array Experiments ■ Test multi-sensor array concept and full waveform inversion on experimental data ■ Use existing instrumentation ■ Flat surface and borehole ■ Do we use fluid-filled or dry hole? ■ How to do tests on a model with correct-scale array and instruments? Effects of boundaries? ■ How to design/construct a model with properties of Florida limerock? Synthetic Limerock Specimen data fit 1 0.8 0.6 0.4 0.2 0 -0.2 -0.4 -0.6 -0.8 -1 data fit 0 1 2 3 4 5 6 8 7 -4 x 10 Synthetic Limerock Specimen Preliminary results Vs = 935 m/s from FWI Free-free resonant column tests Vp = 1500 m/s Poisson’s ratio = 0.2 Thank You!