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4C Mahogony Data Processing and Imaging by LSMF Method

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Presentation on theme: "4C Mahogony Data Processing and Imaging by LSMF Method"— Presentation transcript:

1 4C Mahogony Data Processing and Imaging by LSMF Method
Jianhua Yu and Yue Wang

2 Outline Motivation and Objective LSMF Method
Examples Graben Model Mahogany Field Data Summary

3 Outline Motivation and Objective LSMF Method
Examples Graben Model Mahogany Field Data Summary

4 Geological Objectives
Image Complex Structure Detect Gas Reservoir Over Salt

5 Problems Strong Guided Waves P-SV Conversion at Reflector ?
How to Get “Pure” P-P and P-SV Strong Guided Waves

6 Problems for F-K Use only wave moveout Strong guided waves
Near offset distortion

7 P-P and P-SV Waves Source P-P P-SV Point Scatterer

8 Least Squares Migration Filtering
Moveout Particle Motion Direction Time + offset Separation

9 Separate P-P & P-S Suppress Guide Waves Improve Migration Image
Objective Separate P-P & P-S Suppress Guide Waves Improve Migration Image

10 Outline Motivation and Objective LSMF Method
Examples Graben Model Mahogany Field Data Summary

11 LSMF with Moveout m p = L m = [ Lp Lps ] m m [L L] L d m = moveout PS
-1 T = m ps PS P

12 LSMF with Moveout+2-Comp.
Particle Motion P PS q (cos q , sin q ) (sin q , -cos q ) u = u + u p ps v = v + v total 2-component particle motion data p = L m = [ Lp Lps ] m p ps Scalar moveout m u = [ cos(q)Lp sin(q) Lps ] p ps Vector moveout + particle motion v = [ sin(q)Lp -cos(q) Lps ]

13 LSMF Method = > Dpp + Dp-s Lpp mpp P-P wave Time Lp-s mp-s P-S wave
Observed data Dp-s Lp-s mp-s Lpp mpp Reflectivty Modeling Operator P-P wave Time P-S wave Offset

14 LSMF Filtering Step dpp = Lppmpp dp-s = Lp-smp-s P-P wave Time Time
P-S wave Offset Time P-P wave Offset Time

15 LSMF Method Operators are constructed based on moveout and particle-motion direction The migration operators are the transposes of the modeling operators

16 Outline Motivation and Objective LSMF Method
Examples Graben Model Mahogany Field Data Summary

17 Examples Graben Model Mahogony Field Data

18 Graben Velocity Model 5000 X (m) Depth (m) 3000 V1=2000 m/s
X (m) V1=2000 m/s V2=2700 m/s V3=3800 m/s Depth (m) V4=4000 m/s V5=4500 m/s 3000

19 FD Synthetic Data P-P P-S P-S P-P Horizontal Component
Offset (m) Offset (m) 5000 5000 P-P P-S Time (s) P-S P-P 1.4 Horizontal Component Vertical Component

20 LSMF Separation P-P P-S Horizontal Component Vertical Component
Offset (m) 5000 Offset (m) 5000 P-P P-S Time (s) 1.4 Horizontal Component Vertical Component

21 F-K Filtering Separation
Offset (m) 5000 Offset (m) 5000 P-S P-P Time (s) P-S P-P 1.4 Horizontal Component Vertical Component

22 Test Results Indicate:
LSMF works well for separating P-P and P-SV LSMF is superior to F-K filtering

23 Examples Graben Model Mahogony Field Data

24 Acquisition Survey Shot Line OBC 9 km 29 km

25 Main Processing Flow Geometry assignment, datuming and so on
Trace edit, noise elimination, dual-sensor summation Amplitude Recovery Static correction, (F-K filtering), multiple suppression LSMF, velocity analysis Migration Output

26 Raw CSG Hydrophone component Vertical component Offset(m) Offset(m)
-750 725 -750 725 Continuous events Continuous events Time (s) 4 Hydrophone component Vertical component

27 Raw CSG Radial component Transverse component Offset(m) Offset(m)
-750 725 -750 725 Wormy events Wormy events Time (s) 4 Radial component Transverse component

28 Raw CRG Hydrophone component Vertical component X (m) X (m) Time (s)
3750 3750 Continuous events Continuous events Time (s) 4 Hydrophone component Vertical component

29 Raw CRG Radial component Transverse component X (m) X (m) Time (s)
3750 3750 Continuous events Continuous events Time (s) 4 Radial component Transverse component

30 Rough Estimate of Static Shift
Source Receiver 12 p s Receiver static Static shift (ms) Source Receiver p s Shot static -4 100 Station Number

31 Data Analysis Indicates:
The Shear static shifts exist These shifts mainly come from receivers and one-way Shear path from deeper reflector P-S waves originate from reflectors

32 CRG1 Data before Using LSMF
Guided wave and P-S Time (s) 4 CRG1 (Vertical component)

33 CRG1 Data after Using F-K Filtering
Unwanted waves remain Time (s) 4 CRG1 (Vertical component)

34 CRG1 Data after Using LSMF
Less Noise remains Time (s) 4 CRG1 (Vertical component)

35 Prestack Migration Image With F-K Separation
Midpoint (Km) 4.6 c Time (s) 3.5

36 Prestack Migration Image With LSMF Separation
Midpoint (Km) 4.6 c Time (s) 3.5

37 A Zoom View of Box A Time (s) Midpoint (Km) Midpoint (Km) FK+Mig.
0.6 1.4 0.6 1.4 2.0 Time (s) 3.2 FK+Mig. LSMF+Mig.

38 A Zoom View of Box C Time (s) Midpoint (Km) Midpoint (Km) FK+Mig.
3.4 4.6 3.4 4.6 0.2 Time (s) 0.8 FK+Mig. LSMF+Mig.

39 Outline Motivation and Objective LSMF Method
Examples Graben Model Mahogany Field Data Xwell Data Summary

40 SSP Synthetic

41 Xwell

42 Outline Motivation and Objective LSMF Method
Examples Graben Model Mahogany Field Data Summary

43 Summary and improves the migration image P-SV waves in Mahogony data
originate from the deep reflectors LSMF gives better separation results and improves the migration image

44 Summary LSMF can eliminate unwanted noise, such as guided waves
LSMF has negative impact on the fidelity of data to some extent

45 Summary Future Research: Multiple Elimination Prestack Depth Migration
Converted Wave Imaging

46 Acknowledgement We are grateful to the 1999 sponsors
of the UTAM consortium for financial support


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