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3D Multisource Full-Waveform Inversion using Quasi-Monte Carlo Phase Encoding. Chaiwoot Boonyasiriwat Jan. 7, 2010. Outline. Introduction to Multisource Technology Phase Encoding Multisource Full-Waveform Inversion Quasi-Monte Carlo Phase Encoding Numerical Results
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3D Multisource Full-Waveform Inversion using Quasi-Monte Carlo Phase Encoding Chaiwoot Boonyasiriwat Jan. 7, 2010
Outline • Introduction to Multisource Technology • Phase Encoding • Multisource Full-Waveform Inversion • Quasi-Monte Carlo Phase Encoding • Numerical Results • 3D SEG/EAGE Overthrust Model • Summary • Future Work • Acknowledgment 1
Introduction: Multisource Tech. • Migration • Delayed-shot migration (Zhang et al., 2005) • Random phase encoding (Romero et al., 2000) • Plane-wave migration (Liu et al., 2006; Shan and Biondi, 2008; Shan et al., 2009) • Full-Waveform Inversion (FWI) • Plane-wave FWI (Vigh and Starr, 2008) • Random phase encoding (Krebs et al., 2009; Zhan et al., 2009) 2
Multisource Method Linear Phase Encoding—Planewave Decomposition 4
Multisource Method Random Phase Encoding 5
CSG vs SSG CSG SSG 6
Outline • Introduction to Multisource Technology • Phase Encoding • Multisource Full-Waveform Inversion • Quasi-Monte Carlo Phase Encoding • Numerical Results • 3D SEG/EAGE Overthrust Model • Summary • Future Work • Acknowledgment 7
Conventional FWI Model Observed Data Evaluate misfit function and compute gradient Perturb Model Evaluate misfit function No Search criterion Yes Yes No Convergence criterion Done 8
Multisource FWI Model Encoded Data Evaluate misfit function and compute gradient Perturb Model Evaluate misfit function No Search criterion Yes Yes No Convergence criterion Done 9
2D Multisource FWI Krebs Method (ExxonMobil): one SSG, random source polarity, dynamic encoding 8
2D Multisource FWI Zhan Method (UTAM): multiple SSGs, random time shift, static encoding, deblurring filter 9
3D Multisource FWI Krebs Source Configuration 10
3D Multisource FWI Closely Packed Source Configuration 11
3D Multisource FWI Loosely Packed Source Configuration 12
3D Multisource FWI Quasi-Monte Carlo Source Configuration 13
Static vs Dynamic Configuration Static Dynamic Iteration 1 2 14
Outline • Introduction to Multisource Technology • Phase Encoding • Multisource Full-Waveform Inversion • Quasi-Monte Carlo Phase Encoding • Numerical Results • 3D SEG/EAGE Overthrust Model • Summary • Future Work • Acknowledgment 15
Numerical Results True Velocity Model 17
Numerical Results Initial Velocity Model 18
Numerical Results Velocity Model from Static QMC 19
Numerical Results Velocity Model from Dynamic QMC 20
Numerical Results Velocity Model from Krebs Method 21
Outline • Introduction to Multisource Technology • Multisource Full-Waveform Inversion • Numerical Results • 3D SEG/EAGE Overthrust Model • Summary • Future Work • Acknowledgment 22
Summary • 3D multisource FWI using multiple SSGs is compared with multisource FWI using one SSG. • Using multiple SSGs and a dynamic QMC phase encoding provides a better-quality velocity model than a static QMC phase encoding and Krebs method. • Theoretical speedups need to be verified. • More reliable timing results will be presented later. 23
Outline • Introduction to Multisource Technology • Multisource Full-Waveform Inversion • Numerical Results • 3D SEG/EAGE Overthrust Model • Summary • Future Work • Acknowledgment 24
Future Work • Compare various multisource configurations. • Compare random phase encoding with plane-wave encoding. • Apply random time shifts and deblurring filter. • Apply 3D multisource FWI to field data. 25
Acknowledgment • Sponsors of 2009 UTAM consortium • HPC: AronAhmadia and Mark Cheeseman • Shaheen: Iain Georgeson and Jonathan Anderson • Multisource: Ge Zhan and Wei Dai • Workstation: Benoit Marchand • KAUST: Jerry Schuster 26