Wavefield imaging and tomography with the energy norm

Slides:



Advertisements
Similar presentations
Patrick Smith Academic History PhD Project Title: Combining magma flow modelling and seismicity on Montserrat Supervisor: Prof. Jürgen Neuberg (aka Locko)
Advertisements

Using Simulation to Address Challenges of Subsalt Imaging in Tertiary Basins with Emphasis on Deepwater Gulf of Mexico (Paper 23566) Michael Fehler SEG.
Multiple attenuation in the image space Paul Sava & Antoine Guitton Stanford University SEP.
Differential Semblance Optimization for Common Azimuth Migration
Overview of SEP research Paul Sava. The problem Modeling operator Seismic image Seismic data.
Three Worlds to Explore Look Up? (Astronomy) Look Down? (Geophysics) Look at Surface? (Geology)
Existing Infrastructure for International Exchange of Seismic Data Raymond J. Willemann GEM Technology, Washington, D.C. IASPEI:Includes commissions for.
Applied Geophysics An Introduction
Reverse-Time Migration
Paul Sava
TARGET-ORIENTED LEAST SQUARES MIGRATION Zhiyong Jiang Geology and Geophysics Department University of Utah.
Center for Wave Phenomena Department of Geophysics Colorado School of Mines Golden, Colorado.
Xi’an Jiaotong University 1 Quality Factor Inversion from Prestack CMP data using EPIF Matching Jing Zhao, Jinghuai Gao Institute of Wave and Information,
Slide 1 Light and telescopes Just by analyzing the light received from a star, astronomers can retrieve information about a star’s 1.Total energy output.
Youli Quan & Jerry M. Harris
Imaging a complex Earth… …with all available information… …to derive rock properties… …in a stochastic environment.
Seismic imaging using an inverse scattering algorithm Montclair State University Chapter of SIAM Bogdan G. Nita Dept. of Mathematical Sciences Montclair.
Robert L. Nowack Ph.D. Geophysics, MIT –Wave Propagation in Seismology Using Gaussian Beam Fields Postdoctoral Fellowship at MIT Earth Resources Laboratory.
Scattering and Attenuation Seismology and the Earth’s Deep Interior Scattering and Attenuation Propagating seismic waves loose energy due to geometrical.
Technical sessions 9am-noon Break for lunch (provided) Technical 1-4:00pm; discussion Cocktails and posters 4:30-6:00pm Dobrin 6 – Dr. Brian.
Surface wave tomography: part3: waveform inversion, adjoint tomography
Seismic wave Propagation and Imaging in Complex media: a European network Suggestions for synthetic data storage The SPICE project Expected seismic simulation.
Raanan Dafni,  Dual BSc in Geophysics and Chemistry (Tel-Aviv University).  PhD in Geophysics (Tel-Aviv University).  Paradigm Geophysics R&D ( ).
Manifestation of Fluid Saturation in Scattererd Waves – Numerical Experiments and Field Study 25 September 2014 II Russian-French Workshop "Computational.
University of Missouri - Columbia
Engineering Geology and Seismology
WAVES l wave = disturbance that propagates “disturbance” e.g., displacement of medium element from its equilibrium position; propagation can be in medium.
Uncertainty Maps for Seismic Images through Geostatistical Model Randomization Lewis Li, Paul Sava, & Jef Caers 27 th SCRF Affiliates’ Meeting May 8-9.
SOES6002: Modelling in Environmental and Earth System Science CSEM Lecture 1 Martin Sinha School of Ocean & Earth Science University of Southampton.
Remarks: 1.When Newton’s method is implemented has second order information while Gauss-Newton use only first order information. 2.The only differences.
Start Typical student project Advanced student project Level of final response.
The main instrument used is called the sonde. A basic sonde consists of a source and two receivers one-foot apart. The sonde is lowered down the borehole.
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
Seismological Analysis Methods Receiver FunctionsBody Wave Tomography Surface (Rayleigh) wave tomography Good for: Imaging discontinuities (Moho, sed/rock.
Least squares migration of elastic data Aaron Stanton and Mauricio Sacchi PIMS 2015.
Geology 5640/6640 Introduction to Seismology 09 Jan 2015 © A.R. Lowry 2015 Read for Mon 12 Jan: S&W 1-28 Last time: Course overview Discussed: syllabus,
Seismology Dylan Mikesell April 5, 2011 Boise State University.
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,
Fast Least Squares Migration with a Deblurring Filter 30 October 2008 Naoshi Aoki 1.
Estimation of True (Amplitude-Dependent) Reflection Coefficients in 3-D Prestack Depth Migration of Seismic Data George A. McMechan, Center for Lithospheric.
Fang Liu and Arthur Weglein Houston, Texas May 12th, 2006
Dr. Jing-Bo Chen Professor
ABSTRACT –Basic Principles and applications
Introduction to Seismology
Making Marchenko imaging work with field data and the bumpy road to 3D
6/11/2018 Finding Oil with Cells: Seismic Imaging Using a Cluster of Cell Processors Michael Perrone IBM Master Inventor Mgr, Multicore Computing, IBM.
I. Tutorial: ISS imaging
17-Nov-18 Parallel 2D and 3D Acoustic Modeling Application for hybrid computing platform of PARAM Yuva II Abhishek Srivastava, Ashutosh Londhe*, Richa.
Fang Liu, Arthur B. Weglein, Kristopher A. Innanen, Bogdan G. Nita
Passive Seismic Imaging
Skeletonized Wave-Equation Surface Wave Dispersion (WD) Inversion
Haiyan Zhang and Arthur B. Weglein
Paul Sava: WE seismic imaging
Acoustic Reflection 2 (distance) = (velocity) (time) *
Multiple attenuation in the image space
The FOCI method versus other wavefield extrapolation methods
Gary Margrave and Michael Lamoureux
Identification of seismic phases
Haiyan Zhang and Arthur B. Weglein
Typical Vertical Resolution
Some remarks on the leading order imaging series
Least-squares Joint Imaging of Primaries and Multiples
Estimation of True (Angle-Dependent) Reflection Coefficients in 3-D Prestack Depth Migration of Seismic Data George A. McMechan, Center for Lithospheric.
MCMC Inference over Latent Diffeomorphisms
Welcome from all of us.
Prestack depth migration in angle-domain using beamlet decomposition:
Wave Equation Dispersion Inversion of Guided P-Waves (WDG)
Bogdan G. Nita *University of Houston M-OSRP Annual Meeting
Presentation transcript:

Wavefield imaging and tomography with the energy norm Daniel Rocha & Paul Sava Center for Wave Phenomena Colorado School of Mines We seek to develop technology for imaging the interior of the Earth using seismic waves. Our work belongs to well-established technology in the exploration seismology community which has been proven to be effective at delineating deep Earth structure. Analogous technology is used in medical ultrasound imaging, with primary differences in the type of acoustic/elastic waves and the frequencies used for investigation. The two main types of structural imaging based on seismic imaging are: 1. Wavefield migration (slide 2): a process designed to identify and position in the subsurface the interfaces between rock formations characterized by different physical properties. 2. Wavefield tomography (slide 3): a process designed to characterize the physical properties (e.g. velocity and other elastic parameters) between the identified interfaces. Migration and tomorgraphy work together and iteratively, i.e advances in one facilitates advances in the other. Our specific implementation uses the so-called energy norm which closely matches the properties of the propagating elastic waves. For tomography, we also employ knowledge of physical observed in boreholes, thus constraining the inversion to feasible results throughout the investigated subsurface space. Both migration and tomography are computationally intensive. Typical datasets can be many TB in size and consist of multiple partially-redundant experiemnts (often tens of thousands). These experiments require expensive calculations of wavefields which can be best accomplied on a distributed computing infrastructure, as the experiments are independent of one-another. Moreover, modern processing uses iterative methods, and thus processing repeats multiple times over the same physical subsurface. It is not uncommon that least-squares migration or tomography take days/weeks of continuous processing over multiple compute nodes.

Wavefield migration Build high-resolution images with least-squares migration first iteration final iteration

conventional: recovered model with artifacts Wavefield tomography Constrain wavefield tomography using petrophysical information true model conventional: recovered model with artifacts new recovery method

Acknowledgements Center for Wave Phenomena Sponsors – research funding Shell Exploration and Production Company – field data Co-authors Jeffrey Shragge Antoine Guitton Nicolay Tanushev Ben Witten