Does AVO Inversion Really Reveal Rock Properties?

Slides:



Advertisements
Similar presentations
Surface Waves and Free Oscillations
Advertisements

Viscosity of Dilute Polymer Solutions
Surface Waves and Free Oscillations
The Asymptotic Ray Theory
Chapter 1- General Properties of Waves Reflection Seismology Geol 4068
Upper mantle of the Bohemian Massif (Central Europe) studied by surface waves from Kurile Islands M8.1 and M8.3 earthquakes Petr Kolinsky Jiri Malek Institute.
Net vibration at point P:
Identification of seismic phases
Reflection Coefficients For a downward travelling P wave, for the most general case: Where the first term on the RHS is the P-wave displacement component.
Wave spreads over a larger surface as it travels through the medium. For a spherical wave, the wave energy falls off as the square of the distance. Its.
Synthetic Study of Azimuthal AVO Analysis with Anisotropic Spreading Correction Ellen (Xiaoxia) & Ilya.
Lectures 11-12: Gravity waves Linear equations Plane waves on deep water Waves at an interface Waves on shallower water.
Processes altering seismic amplitudes
EE3321 ELECTROMAGNETIC FIELD THEORY
Chapter 33. Electromagnetic Waves What is Physics? Maxwell's Rainbow The Traveling Electromagnetic Wave, Qualitatively The Traveling.
Scattering and Attenuation Seismology and the Earth’s Deep Interior Scattering and Attenuation Propagating seismic waves loose energy due to geometrical.
Geology 5640/6640 Introduction to Seismology 18 Feb 2015 © A.R. Lowry 2015 Last time: Spherical Coordinates; Ray Theory Spherical coordinates express vector.
GG 450 March 19, 2008 Stress and Strain Elastic Constants.
Seismic reflection Ali K. Abdel-Fattah Geology Dept.,
4. Reflection/transmisson coefficients Introduction R/T coefficient – reflectivity/transmissivity Zoeppritz type equations Critical angles/complex R/T.
Kinematic Representation Theorem KINEMATIC TRACTIONS Time domain representation Frequency domain representation Green Function.
New Trends in AVO Brian Russell and Dan Hampson
1 Investigation of Optical Properties n, k … index of refraction and damping  1,  2 … polarization and absorption Problems: The penetration depth of.
SOES6002: Modelling in Environmental and Earth System Science CSEM Lecture 1 Martin Sinha School of Ocean & Earth Science University of Southampton.
© 2013, PARADIGM. ALL RIGHTS RESERVED. Long Offset Moveout Approximation in Layered Elastic Orthorhombic Media Zvi Koren and Igor Ravve.
The elastic wave equation Seismology and the Earth’s Deep Interior The Elastic Wave Equation Elastic waves in infinite homogeneous isotropic media Numerical.
Seismology Part VI: Surface Waves: Love Augustus Edward Hough Love
The elastic wave equationSeismology and the Earth’s Deep Interior The Elastic Wave Equation  Elastic waves in infinite homogeneous isotropic media 
So far, we have considered plane waves in an infinite homogeneous medium. A natural question would arise: what happens if a plane wave hits some object?
Feb 26, John Anderson: GE/CEE 479/679: Lecture 11 Earthquake Engineering GE / CEE - 479/679 Topic 11. Wave Propagation 1 John G. Anderson Professor.
IRIS Summer Intern Training Course Wednesday, May 31, 2006 Anne Sheehan Lecture 3: Teleseismic Receiver functions Teleseisms Earth response, convolution.
1 AVO INVERSION OF LONG-OFFSET SYNTHETIC PP DATA BASED ON EFFECTIVE REFLECTION COEFFICIENTS 10 April 2008 Lyubov Skopintseva Milana Ayzenberg, Martin Landrø.
Lecture 21-22: Sound Waves in Fluids Sound in ideal fluid Sound in real fluid. Attenuation of the sound waves 1.
Chapters 16, 17 Waves.
Seismology Part V: Surface Waves: Rayleigh John William Strutt (Lord Rayleigh)
A model of the Earthquake surface waves V.K.Ignatovich. FLNP JINR STI2011 June 8.
Reflection Coefficients For a downward travelling P wave, for the most general case: Where the first term on the RHS is the P-wave displacement component.
Light and Matter Tim Freegarde School of Physics & Astronomy University of Southampton Wave mechanics.
Propagation of stationary nonlinear waves in disordered media
Lithospheric Layering
Introduction to Seismology
GPR Simulations for pipeline oil drainage
Physics 114: Exam 2 Review Weeks 7-9
Ground Penetrating Radar using Electromagnetic Models
Introduction to Seismology
Hamiltonian formalism, seismic waves, and seismic barriers
Light Through a Single Slit
Chapter 33. Electromagnetic Waves
Haiyan Zhang and Arthur B. Weglein
High Resolution AVO NMO
ENE 325 Electromagnetic Fields and Waves
Upscaling of 4D Seismic Data
Environmental and Exploration Geophysics I
Kristopher Innanen and Arthur Weglein University of Houston
Some current research in P-S AVO and multicomponent OBS
Identification of seismic phases
A first step towards the P wave only modeling plan
ENE 325 Electromagnetic Fields and Waves
Haiyan Zhang and Arthur B. Weglein
Radio Propagation Review
Wireless Communications Chapter 4
Direct horizontal image gathers without velocity or “ironing”
High Resolution Velocity Analysis for Resource Plays
Estimation of True (Angle-Dependent) Reflection Coefficients in 3-D Prestack Depth Migration of Seismic Data George A. McMechan, Center for Lithospheric.
Challenges of Radio Occultation Data Processing
“Exploring” spherical-wave reflection coefficients
RANDOM AND COHERENT SOURCES
Antenna Theory Chapter.4.7.4~4.8.1 Antennas
1st Week Seminar Sunryul Kim Antennas & RF Devices Lab.
plane waves in lossy material
Presentation transcript:

Does AVO Inversion Really Reveal Rock Properties? NO! YES!

“ …the P-wave reflection coefficient at an interface separating two media is known to vary with angle of incidence. The manner in which it varies is strongly affected by the relative values of Poisson’s ratio of the media…” (Ostrander, W. J., 1982)

A list of parameters affecting amplitudes Geometrical spreading Source directivity and array effects Near surface velocity variation and velocity anisotropy Waveform interference, dispersion and phase distortion Propagation loss of high frequencies Processing effects (move-out stretch, timing varying scaling, etc.)

Objectives of study Estimate of a set of model parameters Estimate of uncertainties in the model parameters How sensitive is the solution to noise in the data? Is a more complicated (i.e., more model parameters) model significantly better than a simple model?

Method of study Performed generalized linear inversion to synthetic noise and noise-free AVO data of homogenous and isotropic two layer elastic media with a single horizontal interface. Used approximations of Zoeppritz plane wave equation derived by Hilterman (1990) with 6, 5, and 3 model parameters Shuey (1985) with 6 model parameters

Model AVO data Model AVO data based on the properties of carbonate-gas sandstone and carbonate wet sandstone at depth about 2.5-3.0 km.

Results Investigation of model parameters Hilterman (1990) with 6, 5, and 3 model parameters Shuey (1985) with 6 model parameters Investigation on unweighted and weighted generalized inversion Investigation on noise data Investigation on data geometry effect Investigation on wet sandstone model

Discussions and Recommendations Did AVO inversion reveal rock properties correctly? Yes/No Did we oversimplify our model? Since the inversion is only a process that can generate a lot of answers to fit the data. One may be right or none! Thus we should perform with regard of some reasonable solutions!

Conclusions Hilterman plane wave approximation with 5 model parameters are able to determined a perfect model parameter for a different Poisson’s ratio between the upper and lower media, although one of the fundamental problems of the inversion is a non-uniqueness solution. This perfect model did not depend on an initial guess.

Conclusions For noise data, random noise did not influence the model resolution, whereas a coherent noise did a little. Incorrect geometry of the AVO data did influence a great deal of model resolution. Any question!