Joint 3D relocation of earthquakes by surface and borehole data

Slides:



Advertisements
Similar presentations
JOINT IMAGING OF THE MEDIA USING DIFFERENT TYPES OF WAVES A.V. Reshetnikov* Yu.A. Stepchenkov* A.A. Tabakov** V.L. Eliseev** * SPbSU, St-Petersburg, **
Advertisements

A Partition Modelling Approach to Tomographic Problems Thomas Bodin & Malcolm Sambridge Research School of Earth Sciences, Australian National University.
Time-Lapse Monitoring of CO2 Injection with Vertical Seismic Profiles (VSP) at the Frio Project T.M. Daley, L.R. Myer*, G.M. Hoversten and E.L. Majer.
Tom Wilson, Department of Geology and Geography Environmental and Exploration Geophysics II tom.h.wilson Department of Geology.
Body and Surface Wave Seismic Tomography for Regional Geothermal Assessment of the Western Great Basin Glenn Biasi 1, Leiph Preston 2, and Ileana Tibuleac.
Using 3D Seismic Imaging for Mine and Mineral Exploration G. Schuster University of Utah.
Lessons we have learned from seismological observations in the Taiwan region Jer-Ming Chiu CERI/Dept. of Earth Sciences University of Memphis March 19,
GG450 April 22, 2008 Seismic Processing.
What is a reflector? There are many reflectors on a seismic section. Major changes in properties usually produce strong, continuous reflectors as shown.
Sensitivity kernels for finite-frequency signals: Applications in migration velocity updating and tomography Xiao-Bi Xie University of California at Santa.
First Arrival Traveltime and Waveform Inversion of Refraction Data Jianming Sheng and Gerard T. Schuster University of Utah October, 2002.
Fine-scale structure of the San Andreas fault zone and location of the SAFOD target earthquakes Thurber, Roecker, Zhang, Baher, and Ellsworth Geophysical.
Wavepath Migration versus Kirchhoff Migration: 3-D Prestack Examples H. Sun and G. T. Schuster University of Utah.
Wave-Equation Interferometric Migration of VSP Data Ruiqing He Dept. of Geology & Geophysics University of Utah.
Wave-Equation Interferometric Migration of VSP Data Ruiqing He Dept. of Geology & Geophysics University of Utah.
Salt Boundary Delineation by Transmitted PS Waves David Sheley.
Advanced Seismic Imaging GG 6770 Variance Analysis of Seismic Refraction Tomography Data By Travis Crosby.
CROSSWELL IMAGING BY 2-D PRESTACK WAVEPATH MIGRATION
Bedrock Delineation by a Seismic Reflection/Refraction Survey at TEAD Utah David Sheley and Jianhua Yu.
Key Result Seismic CAT Scan vs Trenching.
Earthquake Seismology
Youli Quan & Jerry M. Harris
Midyear Overview of Year 2001 UTAM Results T. Crosby, Y. Liu, G. Schuster, D. Sheley, J. Sheng, H. Sun, J. Yu and M. Zhou J. Yu and M. Zhou.
Advanced Seismic Imaging GG 6770 Tomography Inversion Project By Travis Crosby.
Single station location Multiple station location
David von Seggern Joint Seismic Tomography/Location Inversion in the Reno/Carson City Area Leiph Preston & David von Seggern Nevada Seismological Laboratory.
Advances in Earthquake Location and Tomography William Menke Lamont-Doherty Earth Observatory Columbia University.
AN ORGANISATION FOR A NATIONAL EARTH SCIENCE INFRASTRUCTURE PROGRAM Capricorn Transect : Lithospheric Background B.L.N. Kennett Research School of Earth.
Earthquake Location The basic principles Relocation methods
Small is beautiful: AGL physical modeling and salt measurements N. Dyaur, R. Stewart, and L. Huang Houston May 16,
GG450 March 20, 2008 Introduction to SEISMIC EXPLORATION.
Multisource Least-squares Reverse Time Migration Wei Dai.
Geology 5660/6660 Applied Geophysics 17 Jan 2014 © A.R. Lowry 2014 Read for Wed 22 Jan: Burger (Ch 2.2–2.6) Last time: The Wave Equation; The Seismometer.
Automatic detection and location of microseismic events
How Shallow Earth Structure Is Determined A Classroom Exercise Demonstrating Seismic Refraction Use in the Real World NSTA, Boston, 2008 Michael Hubenthal,
U.S. Department of the Interior U.S. Geological Survey Earthquake Location by Annabel Kelly.
Passive Seismic ImagingStanford Exploration Project passive seismic imaging Brad Artman.
Last week’s problems a) Mass excess = 1/2πG × Area under curve 1/2πG = × in kgs 2 m -3 Area under curve = -1.8 ×10-6 x 100 m 2 s -2 So Mass.
Seismic reflections. Seismic waves will be reflected at “discontinuities” in elastic properties A new ray emerges, heading back to the surface Energy.
Lg Q Across the Continental US Dan McNamara and Rob Wesson with Dirk Erickson, Arthur Frankel and Harley Benz.
Evidence for a low-permeability fluid trap in the Nový Kostel Seismic Zone from double-difference tomography 3rd Annual AIM Workshop I October 10 – 12,
Environmental and Exploration Geophysics II tom.h.wilson Department of Geology and Geography West Virginia University Morgantown, WV.
EXPLORATION GEOPHYSICS. EARTH MODEL NORMAL-INCIDENCE REFLECTION AND TRANSMISSION COEFFICIENTS WHERE:  1 = DENSITY OF LAYER 1 V 1 = VELOCITY OF LAYER.
Fig 3) Crustal Structure using the tomography method, in the central part of Itoigawa- Shizuoka Tectonic Line (ISTL). The central part of the Itoigawa-Sizuoka.
Environmental and Exploration Geophysics II tom.h.wilson Department of Geology and Geography West Virginia University Morgantown, WV.
Seismological Analysis Methods Receiver FunctionsBody Wave Tomography Surface (Rayleigh) wave tomography Good for: Imaging discontinuities (Moho, sed/rock.
Introduction to Seismology
Migration Velocity Analysis 01. Outline  Motivation Estimate a more accurate velocity model for migration Tomographic migration velocity analysis 02.
Super-virtual Interferometric Diffractions as Guide Stars Wei Dai 1, Tong Fei 2, Yi Luo 2 and Gerard T. Schuster 1 1 KAUST 2 Saudi Aramco Feb 9, 2012.
Interferometric Traveltime Tomography M. Zhou & G.T. Schuster Geology and Geophysics Department University of Utah.
G. Schuster, S. Hanafy, and Y. Huang, Extracting 200 Hz Information from 50 Hz Data KAUST Rayleigh Resolution ProfileSuperresolution Profile Sinc function.
Wave-Equation Waveform Inversion for Crosswell Data M. Zhou and Yue Wang Geology and Geophysics Department University of Utah.
Migration Velocity Analysis of Multi-source Data Xin Wang January 7,
1 Geophysical Methods Data Acquisition, Analysis, Processing, Modelling, Interpretation.
A Fiber-Optic Borehole Seismic
Seismic phases and earthquake location
Fast Least Squares Migration with a Deblurring Filter 30 October 2008 Naoshi Aoki 1.
Lee M. Liberty Research Professor Boise State University.
2010/11/01 Workshop on "Earthquake Forecast Systems Based on Seismicity of Japan: Toward Constructing Base-line Models of Earthquake Forecasting" Seismicity.
Earthquake hypocentre and origin time
Zero-Offset Data d = L o ò r ) ( g = d dr r ) ( g = d
R. G. Pratt1, L. Sirgue2, B. Hornby2, J. Wolfe3
Sisgbee2b / Data Release
Modeling of free-surface multiples - 2
Microseisms at Turtle Mountain
Acoustic Reflection 2 (distance) = (velocity) (time) *
Overview of current and upcoming field projects
Integrated high-resolution tomography
Reflected, Refracted and Diffracted waves
Packing of uniform spheres
Presentation transcript:

Joint 3D relocation of earthquakes by surface and borehole data Aldo Vesnaver & Lara Lovisa Trieste, 7 October 2008 Annual Meeting of the Italian EAGE-SEG Section

Main topics Microseismicity caused by hydrocarbon production and storage, and by CO2 sequestration Wadati’s method in wells ... ... and joint 3D tomography by active and passive seismic, from well and surface receivers

Method Voxels in irregular grids Ray tracing for direct, reflected, refracted, diving and converted waves

Method 1. Time Zero by Wadati’s method (or Least Squares) 2. Initial model from 3D seismic, well data and geology 3. Hypocentre estimate by “Shrinking Grids” 4. 3D tomography 5. Iterations of steps 3 and 4, until convergence

Method 1. Time Zero by Wadati’s method (or Least Squares) 2. Initial model from 3D seismic, well data and geology 3. Hypocentre estimate by “Shrinking Grids” 4. 3D tomography 5. Iterations of steps 3 and 4, until convergence

Wadati in a well ?

Wadati in a well ?

Wadati in a well ?

Wadati in a well ? Rp, Rs = Recorded P or S time Tp, Ts = Actual P or S traveltimes Vp, Vs = Average P or S velocity To = Time Zero

Method 1. Time Zero by Wadati’s method (or Least Squares) 2. Initial model from 3D seismic, well data and geology 3. Hypocentre estimate by “Shrinking Grids” 4. 3D tomography 5. Iterations of steps 3 and 4, until convergence

Method - “Shrinking grids”

3D recording geometry 225 receivers at surface 28 receivers in 2 wells (Jervis and Dasgupta, 2006) (Dasgupta, 2006)

3D recording geometry Vertical arrays Area : 3 x 3 km Maximum depth : 2.015 km

Relocation – 1.5D model (“true” traveltimes, without Wadati) NonLinLoc Hypo3D

Relocation – 3D model Missing (“true” traveltimes, without Wadati) NonLinLoc Hypo3D

Method 1. Time Zero by Wadati’s method (or Least Squares) 2. Initial model from 3D seismic, well data and geology 3. Hypocentre estimate by “Shrinking Grids” 4. 3D tomography 5. Iterations of steps 3 and 4, until convergence

Synthetic model P velocity km km/s

Reflection tomography P velocity km km/s

Active + passive tomography P velocity km km/s

Synthetic model S velocity km km/s

Reflection tomography S velocity km km/s

Active + passive tomography S velocity km km/s

Conclusions Wadati’s Method does NOT work in wells and if the Vp/Vs ratio changes a lot along the ray-paths of recorded events Thus, surface and well data should be jointly processed for the Time Zero The joint 3D tomography of active + passive seismic can better image the reservoir Gualtiero (Walter) B