Kui Zhang* and Kurt J. Marfurt 2008 AASPI Consortium annual meeting Migration-driven velocity analysis for anisotropy/stress analysis.

Slides:



Advertisements
Similar presentations
Feasibility Study of Fracture Detection Using Seismic Data in Karachaganak Xiang-Yang Li 1, Enru Liu 1 and Tim Pointer 2 1 Edinburgh Anisotropy Project,
Advertisements

Multi-Component Seismic Data Processing
Introduction to GeoProbe
3-D Fault Visualization with Fracture Swarms
Adaptive Grid Reverse-Time Migration Yue Wang. Outline Motivation and ObjectiveMotivation and Objective Reverse Time MethodologyReverse Time Methodology.
Workplan Kurt J. Marfurt Tim Kwiatkowski Marcilio Matos Attribute-Assisted Seismic Processing and Interpretation AASPI.
1 Xuyao Zheng Institute of Geophysics of CEA. 2 Outline 1.Motivation 2.Model and synthetic data 3.Calculation of Green functions 4.Pre-stack depth migration.
AASPI Workplan Kurt J. Marfurt Kurt J. Marfurt Jamie Rich Vikram Jayaram Marcilio Matos OU AASPI Team Attribute-Assisted Seismic Processing and.
First Arrival Traveltime and Waveform Inversion of Refraction Data Jianming Sheng and Gerard T. Schuster University of Utah October, 2002.
Imaging Multiple Reflections with Reverse- Time Migration Yue Wang University of Utah.
Wavepath Migration versus Kirchhoff Migration: 3-D Prestack Examples H. Sun and G. T. Schuster University of Utah.
Primary-Only Imaging Condition Yue Wang. Outline Objective Objective POIC Methodology POIC Methodology Synthetic Data Tests Synthetic Data Tests 5-layer.
CROSSWELL IMAGING BY 2-D PRESTACK WAVEPATH MIGRATION
Joint Migration of Primary and Multiple Reflections in RVSP Data Jianhua Yu, Gerard T. Schuster University of Utah.
Earth Study 360 Technology overview
MD + AVO Inversion Jianhua Yu, University of Utah Jianxing Hu GXT.
Prestack Migration Deconvolution in Common Offset Domain Jianxing Hu University of Utah.
Wave Imaging Technology Inc. PSDM for “Easy” Unconventional Reservoirs? Morgan Brown Rocky Mountain Section, AAPG September 10, 2012.
4. Spectral Decomposition
2015 Workplan for “VVAz” Analysis of Prestack Migrated Data
Multisource Least-squares Reverse Time Migration Wei Dai.
Raanan Dafni,  Dual BSc in Geophysics and Chemistry (Tel-Aviv University).  PhD in Geophysics (Tel-Aviv University).  Paradigm Geophysics R&D ( ).
Overview of AASPI accomplishments and software development Kurt J. Marfurt Kurt J. Marfurt Attribute-Assisted Seismic Processing and Interpretation AASPI.
Weighted Stacking of 3-D Converted-wave Data for Birefringent Media Richard Bale.
Attribute- Assisted Seismic Processing and Interpretation 3D CONSTRAINED LEAST-SQUARES KIRCHHOFF PRESTACK TIME MIGRATION Alejandro.
AASPI Workplan Kurt J. Marfurt Kurt J. Marfurt Jamie Rich Marcilio Matos Bo Zhang Brad Wallet OU AASPI Team Attribute-Assisted Seismic Processing.
© 2013, PARADIGM. ALL RIGHTS RESERVED. Long Offset Moveout Approximation in Layered Elastic Orthorhombic Media Zvi Koren and Igor Ravve.
Statistical measures of instantaneous spectra Kui Zhang* and Kurt J. Marfurt 2008 AASPI Consortium annual meeting Not Gaussian!
Migration In a Nutshell Migration In a Nutshell Migration In a Nutshell D.S. Macpherson.
Impact of MD on AVO Inversion
Fractures play a major role in many tight reservoirs such as shale, carbonate, and low permeability sand by providing fluid flow conduits, for this reason.
Seismic Imaging in GLOBE Claritas
1 RPSEA Project – Facies probabilities from seismic data in Mamm Creek Field Reinaldo J Michelena Kevin Godbey Patricia E Rodrigues Mike Uland April 6,
EXPLORATION GEOPHYSICS. EARTH MODEL NORMAL-INCIDENCE REFLECTION AND TRANSMISSION COEFFICIENTS WHERE:  1 = DENSITY OF LAYER 1 V 1 = VELOCITY OF LAYER.
The Experimental Comparison of Conventional and Differential Semblance on several data sets Jintan Li Rice University.
Multiples Waveform Inversion
Migration Velocity Analysis 01. Outline  Motivation Estimate a more accurate velocity model for migration Tomographic migration velocity analysis 02.
Mapping the P-S Conversion Point in VTI Media * Jianli Yang Don C. Lawton.
Multisource Least-squares Migration of Marine Data Xin Wang & Gerard Schuster Nov 7, 2012.
Tao Zhao and Kurt J. Marfurt University of Oklahoma
Data QC and filtering Bryce HutchinsonSumit Verma Objective: Consider the frequency range of different seismic features Look for low frequency and high.
Efficient Geophysical Research in Julia
Pitfalls in seismic processing : The origin of acquisition footprint Sumit Verma, Marcus P. Cahoj, Bryce Hutchinson, Tengfei Lin, Fangyu Li, and Kurt J.
4. Spectral Decomposition
Computing Attributers on Depth-Migrated Data Name : Tengfei Lin Major : Geophysics Advisor : Kurt J. Marfurt AASPI,The University of Oklahoma 1.
Wave-Equation Migration in Anisotropic Media Jianhua Yu University of Utah.
Velocity Estimation by Waveform Tomography in the Canadian Foothills: A Synthetic Benchmark Study Andrew J. Brenders 1 Sylvestre Charles 2 R. Gerhard Pratt.
1 Prestack migrations to inversion John C. Bancroft CREWES 20 November 2001.
TGS-NOPEC Geophysical Company Seismic Imaging: How we use waves to see the interior of the earth Apache Symposium on Imaging November 6, 2008 Y. C. Kim,
Raanan Dafni,  PhD in Geophysics (Tel-Aviv University)  Paradigm R&D ( )  Post-Doc (Rice University) Current Interest: “Wave-equation based.
Geology 5660/6660 Applied Geophysics 10 Feb 2016 © A.R. Lowry 2016 Last Time: Seismic Reflection Travel-Time Cont’d Dix Equations for multiple layers:
Lee M. Liberty Research Professor Boise State University.
MD+AVO Inversion: Real Examples University of Utah Jianhua Yu.
Migration-driven azimuthal velocity analysis
4. Spectral Decomposition
Imaging (and characterisation) of diffractors
M-OSRP 2006 Annual Meeting, June 6, 2007
Haiyan Zhang and Arthur B. Weglein
INTRODUCTION STRF: 50m reflection line with dx=1.0m
Non-local Means (NLM) Filter for Trim Statics
Han Yu, Bowen Guo*, Sherif Hanafy, Fan-Chi Lin**, Gerard T. Schuster
Azimuthally varying velocity is probably the most significant property of the seismic data that affects the seismic interpretation. A stacking velocity.
High Resolution Velocity Analysis for Resource Plays
Non-local Means (NLM) Filter for Trim Statics
Welcome from all of us.
EXPLORATION GEOPHYSICS
Velocity and anisotropy parameter scan
Unit 4 – Energy Learning target 4.3 – Define and relate wavelength, frequency, amplitude, period, and wave speed.
Least Squares Migration
Wave Equation Dispersion Inversion of Guided P-Waves (WDG)
Presentation transcript:

Kui Zhang* and Kurt J. Marfurt 2008 AASPI Consortium annual meeting Migration-driven velocity analysis for anisotropy/stress analysis

Motivation  Our industry is acquiring more and more wide azimuth data.  Traditional seismic processing often ignores the azimuth information and implements on the full azimuth gathers.  The presence of azimuthal velocity anisotropy can degrade image quality.  The analysis of azimuthal velocity anisotropy and/or azimuthal AVO provides valuable information about fracture densities and stress orientation. Current leaders are: Axis (NMO-based), Weinman (migration-based).

Motivation  Challenges: Statics caused by different elevations and the LVL zone.(short wavelength and long wavelength) Structural dip can bias the anisotropic analysis. Measured elliptical NMO velocities is usually converted to interval velocity by Dix equation. (ambiguity)  We use Kirchhoff prestack migration-driven approach to generate: More accurate NMO azimuthal velocities High resolution imaging

New azimuth binning method V fast V slow Fault plane xixi xsxs xgxg (x i -x s)+ (x i -x g ) (x i -x s) (x i -x g ) 11° 34° 56° 79° 101° 124° 146° 281° 304° 326° 349° E W N 169°191° 214° 236° 259° S

1 km Amplitude Positive Negative 0 N Conventional Binning

km Amplitude Positive Negative 0 N New Binning (Perez and Marfurt, 2008)

New P wave azimuthal velocity analysis approach Coarse grid selectionNMO velocity V nmo Choose α and φ V=V nmo + α cosφ Migrate and compute semblance more α or φ Yes Scan for maximum semblance over α m and φ m migrate over α m and φ m α +10% 0% Maximum semblance

New converted wave azimuthal velocity analysis approach t 1 p =(t 0 2 +x si 2 /v p 2 ) 1/2 t 2 p =(t 0 2 +x gi 2 /v p 2 ) 1/2 t 2 s =(t 0 2 +x gi 2 /v s 2 ) 1/2 t=0 P P S For P wave migration: For PS wave migration: Vs/Vp Maximum semblance

Acknowledgement We thank all sponsors of AASPI consortium for their support.