Data modeling using Cagniardde Hoop method Jingfeng Zhang

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Data modeling using Cagniardde Hoop method Jingfeng Zhang and Arthur B. Weglein M-OSRP annual

Data modeling using Cagniardde Hoop method Jingfeng Zhang and Arthur B. Weglein M-OSRP annual meeting University of Houston May 10 th – 12 th, 2006 1

Outline • Background and Motivation • Theory: – Data generation using Cagniard-de Hoop method

Outline • Background and Motivation • Theory: – Data generation using Cagniard-de Hoop method • Numerical tests • Conclusions 2

Background and Motivation • Data modeling is important for: – Evaluation of new algorithms

Background and Motivation • Data modeling is important for: – Evaluation of new algorithms – Forward model matching methods • Conventional data processing techniques: – Arrival time; Amplitude 3

Background and Motivation • (Recently) developed new algorithms: – Deghosting – ISS free surface

Background and Motivation • (Recently) developed new algorithms: – Deghosting – ISS free surface multiple removal method – ISS internal multiple attenuation and elimination – Imaging without the velocity – Nonlinear inversion 4

Background and Motivation • Reasons to choose Cagniard-de Hoop method for deghosting: – 1.

Background and Motivation • Reasons to choose Cagniard-de Hoop method for deghosting: – 1. 5 D medium data will suffice for initial tests – “Perfect” data: regular integrand on a finite integral range – Quality control each processing step: deghosting performed in two steps 5

Background and Motivation Primary and S-G Receiver deghosting + R-G and S-R-G Source deghosting

Background and Motivation Primary and S-G Receiver deghosting + R-G and S-R-G Source deghosting Primary 6

Theory The 2 D acoustic constant density wave equation: The corresponding Green’s function equation:

Theory The 2 D acoustic constant density wave equation: The corresponding Green’s function equation: Relationship: 7

Theory Fourier Transform over and (layered medium): where Just need to solving 1 D

Theory Fourier Transform over and (layered medium): where Just need to solving 1 D wave equation and matching boundaries for layered medium. 8

Theory Even for the direct wave in homogeneous medium: 9

Theory Even for the direct wave in homogeneous medium: 9

Caniard-de Hoop Fourier Transform over and Laplace transform over : 10

Caniard-de Hoop Fourier Transform over and Laplace transform over : 10

Strategy: Manipulate the integral ( ) Aki & Richards (2 nd Edition) 11

Strategy: Manipulate the integral ( ) Aki & Richards (2 nd Edition) 11

Theory Direct wave: Primary: Pre-critical Pos-critical 12

Theory Direct wave: Primary: Pre-critical Pos-critical 12

Theory (1) Evaluation of the integration (direct wave): 13

Theory (1) Evaluation of the integration (direct wave): 13

Theory (2) Sign of : 14

Theory (2) Sign of : 14

Numerical Tests 15

Numerical Tests 15

Numerical Tests 16

Numerical Tests 16

Numerical Tests Correct data 17

Numerical Tests Correct data 17

Incorrect data 18

Incorrect data 18

Deghosting result using correct data 19

Deghosting result using correct data 19

Deghosting result using incorrect data 20

Deghosting result using incorrect data 20

Deghosting results Red Solid: Exact results; Blue Dash: Calculated results 21

Deghosting results Red Solid: Exact results; Blue Dash: Calculated results 21

FSMR results Red Solid: Before FSMR; Blue Dash: After FSMR 22

FSMR results Red Solid: Before FSMR; Blue Dash: After FSMR 22

Conclusions and Acknowledgments • Very high quality of data can be generated using Cagniard-de

Conclusions and Acknowledgments • Very high quality of data can be generated using Cagniard-de Hoop method. • It is demonstrated that using the generated data deghosting and FSMR algorithms produce very good results. • We appreciate the help from Adrian de Hoop. • The support of M-OSRP sponsors is much appreciated. 23