3D depth-to-basement and density contrast estimates using gravity and borehole data Cristiano Mendes Martins Valéria C. F. Barbosa National Observatory.

Slides:



Advertisements
Similar presentations
Satellite gravity gradients for lithospheric structure R. Hackney, H.-J. Götze, S. Schmidt Institut für Geowissenschaften, Abteilung Geophysik Christian-Albrechts-Universität.
Advertisements

SPP 1257 Modelling of the Dynamic Earth from an Integrative Analysis of Potential Fields, Seismic Tomography and other Geophysical Data M. Kaban, A. Baranov.
Problem 1 The corrections can be larger than the anomaly Stat.Time T Dist. (m) Elev. (m) Reading (dial units) Base reading at time T Drift corr’d anom.
The general equation for gravity anomaly is: where:  is the gravitational constant  is the density contrast r is the distance to the observation point.
Gravitational Attractions of Small Bodies. Calculating the gravitational attraction of an arbitrary body Given an elementary body with mass m i at position.
Interpretation of Seafloor Gravity Anomalies. Gravity measurements of the seafloor provide information about subsurface features. For example they help.
Visualization of dynamic power and synchrony changes in high density EEG A. Alba 1, T. Harmony2, J.L. Marroquín 2, E. Arce 1 1 Facultad de Ciencias, UASLP.
Isopach and Isochore Maps
INFLUENCE OF CAPILLARY PRESSURE ON CO 2 STORAGE AND MONITORING Juan E. Santos Work in collaboration with: G. B. Savioli (IGPUBA), L. A. Macias (IGPUBA),
PIVETTA T., BRAITENBERG C. Dipartimento di Geoscienze, Università di Trieste, Italy, THE LITHOSPHERE STRUCTURE BENEATH.
Title Stephan Husen Institute of Geophysics, ETH Zurich, Switzerland,
Aspects of Conditional Simulation and estimation of hydraulic conductivity in coastal aquifers" Luit Jan Slooten.
Tom Wilson, Department of Geology and Geography Environmental and Exploration Geophysics II tom.h.wilson Department of Geology.
Inversion of Z-Axis Tipper Electromagnetic (Z-TEM)‏ Data The UBC Geophysical Inversion Facility Elliot Holtham and Douglas Oldenburg.
Total Variation Imaging followed by spectral decomposition using continuous wavelet transform Partha Routh 1 and Satish Sinha 2, 1 Boise State University,
Nyack - Geophysical Characterization Problem - determine subsurface parameters, relevant to fluid flow and basin evolution, from non-invasive observations.
Gravity: Gravity anomalies. Earth gravitational field. Isostasy. Moment density dipole. Practical issues.
Seismic refraction surveys
Prof. David R. Jackson Dept. of ECE Fall 2013 Notes 19 ECE 6340 Intermediate EM Waves 1.
Length Scale analysis of the transition from shallow to deep convection João Paulo A. Martins (1) Pedro M. A. Miranda (1) Pedro M. M. Soares (1) João Teixeira.
The aim of the presented research activities Is to develop new interpretation techniques for potential fields exploration methods (gravity, magnetic,
Gravity I: Gravity anomalies. Earth gravitational field. Isostasy.
Model of the theoretical gravity Normal gravity Elevation effect The effect of material beneath the station - the plate effect Topographic or terrain effect.
Radial gravity inversion constrained by total anomalous mass excess for retrieving 3D bodies Vanderlei Coelho Oliveira Junior Valéria C. F. Barbosa Observatório.
A spherical Fourier approach to estimate the Moho from GOCE data Mirko Reguzzoni 1, Daniele Sampietro 2 2 POLITECNICO DI MILANO, POLO REGIONALE DI COMO.
SOES6002: Modelling in Environmental and Earth System Science Geophysical modelling Tim Henstock School of Ocean & Earth Science University of Southampton.
3D gravity inversion incorporating prior information through an adaptive learning procedure Fernando J. S. Silva Dias Valéria C. F. Barbosa National Observatory.
GOCE OBSERVATIONS FOR DETECTING UNKNOWN TECTONIC FEATURES BRAITENBERG C. (1), MARIANI P. (1), REGUZZONI M. (2), USSAMI N. (3) (1)Department of Geosciences,
Polynomial Equivalent Layer Valéria C. F. Barbosa* Vanderlei C. Oliveira Jr Observatório Nacional.
Practical issues (This lecture is based largely on: The shape of the gravity anomaly depends not on the absolute.
Adaptive learning gravity inversion for 3D salt body imaging Fernando J. S. Silva Dias Valéria C. F. Barbosa National Observatory João B. C. Silva Federal.
Graphical Separation of Residual
1 Formation et Analyse d’Images Session 7 Daniela Hall 25 November 2004.
Geology 5640/6640 Introduction to Seismology 24 Apr 2015 © A.R. Lowry 2015 Last time: Amplitude Effects Multipathing describes the focusing and defocusing.
29 September 2009WAIS/Pack Forest Conference Center Variation in Subglacial Roughness in West Antarctica: How do we interpret causality in the context.
Fractals, Multi-Fractals, Psuedo- Fractals and Non-Fractals in Energy Spectral Techniques Francis Vaughan (Archimedes Consulting) EAGE Workshop on Non.
Application of the two-step method for the solution of the inverse gravity problem for the Kolárovo anomaly.
Imaging Multiple Horizons with Spectral Techniques in the Sirt Basin, Libya Authors: Sam Yates, Irena Kivior, Shiferaw Damte, Stephen Markham, Francis.
Indications of an Underground “River” beneath the Amazon River: Inferences from Results of Geothermal Studies Elizabeth Tavares Pimentel-UFAM/ON Supervisor:
An E-W gravity profile across the La Bajada fault Zone in the Rio Grande Rift, North Central New Mexico Rajesh Goteti University of Rochester SAGE 2007.
Gravity IV: Dipole moment of density anomaly: the ambiguity
February 13-15, 2006 Hydromechanical modeling of fractured crystalline reservoirs hydraulically stimulated S. Gentier*, X. Rachez**, A. Blaisonneau*,
Interactive 2D magnetic inversion: a tool for aiding forward modeling and testing geological hypotheses Valéria C. F. Barbosa LNCC - National Laboratory.
Measuring the Gravity and Magnetic Anomaly of a Rising Lava Plume Chris Jaeger December 3, 2015.
Designing Matched Bandpass and Azimuthal Filters for the Separation of Potential-Field Anomalies by Source Region and Source Type Jeffrey D. Phillips U.S.
Exercise.04 Receiver functions will be determined Receiver functions will be inverted Receiver functions and surface-wave dispersion will be inverted jointly.
Geology 5670/6670 Inverse Theory 12 Jan 2015 © A.R. Lowry 2015 Read for Wed 14 Jan: Menke Ch 2 (15-37) Last time: Course Introduction (Cont’d) Goal is.
Tom Wilson, Department of Geology and Geography Environmental and Exploration Geophysics I tom.h.wilson Department of Geology and.
GOCE GRADIENT TENSOR CHARACTERIZATION OF THE COUPLED PARANÁ (SOUTH AMERICA) AND ETENDEKA (AFRICA) MAGMATIC PROVINCES Patrizia Mariani and Carla Braitenberg.
Shaking and Flooding by the Tohoku-Oki earthquake Shengji Wei*, Rob Graves**, Don Helmberger*, Jean-Philippe Avouac* and Junle Jiang* * Seismological Lab,
Environmental and Exploration Geophysics I tom.h.wilson Department of Geology and Geography West Virginia University Morgantown, WV.
Gravity Data Reduction
Analysis of ground-motion spatial variability at very local site near the source AFIFA IMTIAZ Doctorant ( ), NERA Project.
Geology 5660/6660 Applied Geophysics 23 Mar 2016 © A.R. Lowry 2016 For Fri 25 Mar: Burger (§ ) Last Time: Density; Gravity Anomalies & Modeling.
Gravity modeling as guidance for salt interpretation: a case study from the Western Gulf of Mexico Irina Filina* (formerly at Hess Corporation, currently.
3D structure of the Thuringian Basin, Germany
Gravity 3.
Advance Seismic Interpretation Project
1-6 Relations Goals: Represent relations as tables, ordered pairs, graphs and mappings. Eligible Content: A / A / A / A
Nils Holzrichter, Jörg Ebbing
4D Gravity Inversion Hyoungrea Bernard Rim
Gravity II: Gravity anomaly due to a simple-shape buried body
Geological map of the massifs of Lake Chudzjavr
The horizontal number line is called the ______. x-axis
Figure 1.1 The parabolic trajectory problem.
South China Sea crustal thickness and oceanic lithosphere distribution from satellite gravity inversion by Simon Gozzard, Nick Kusznir, Dieter Franke,
Lesson 2-4 The Coordinate Plane
1-6 Relations Goals: Represent relations as tables, ordered pairs, graphs and mappings. Eligible Content: A / A / A / A
by Alan M. Roberts, Andrew D. Alvey, and Nick J. Kusznir
Geological Society, London, Memoirs
Presentation transcript:

3D depth-to-basement and density contrast estimates using gravity and borehole data Cristiano Mendes Martins Valéria C. F. Barbosa National Observatory João B. C. Silva Federal University of Pará

Contents Objective Methodology Real Data Inversion Result Conclusions Synthetic Data Inversion Result

Objective z Depth Gravity data Estimate x y N E a 3D basement relief of a sedimentary basin Basement relief Homogeneous lower medium from gravity data and depth-to-basement information at few points: x y N E

The   and  Objective a 3D basement relief of a sedimentary basin Homogeneous lower medium Heterogeneous upper medium 1,0 2,0 3,0 4,0 5,0 6,0 -0,6 -0,2 0,0 Depth  (g/cm 3 ) -0,4 Rao et al. (1994)   z z       0  0   Estimate from gravity data and depth-to-basement information at few points: Parabolic decay of density contrast with depth

Methodology

Methodology y x z y x Gravity observations g o M R  Basement relief Depth

Methodology y x Gravity observations g o M R  z Depth y x Sedimentary pack Basement relief

Methodology y x z y x Gravity observations g o M R  Basement relief Prisms’ thicknesses are the parameters to be estimated Depth pjpj dx dy Sedimentary pack

Methodology The vertical component of the gravity field produced by M prisms:  .,...,1,' ' ' 2 3 Mizdds zz z g M j jj p i ij jo o SjSj i j            rr   Chakravarthi et al. (2002)  ) ( i r j   3 z jo o     The constrained nonlinear inversion obtains a 3D depth-to-basement estimate by minimizing: 2 Rp subject to and 2 2 ),,( 1  o M pgg o 2 B B zpW 

Methodology 2 Rp subject to and 2 2 ),,( 1  o M pg g o The constrained nonlinear inversion obtains a 3D depth-to-basement estimate by minimizing: The first-order Tikhonov regularizing function The borehole information about the basement depth The data misfit function 0   2 B B zpW  B z g o g  2

2 B B zpW  0 ),(    ^ Methodology To estimate the parameters defining the parabolic decay of the density contrast with depth   z z       0  0   2 Rp 2. We obtain a 3D depth-to-basement estimate by: 1. We fix a pair of (  ,  ) We get the pair (  ,   ) in the following way: subject to 2 2 ),,( 1  o M pg g o 3. We evaluate the functional: 4. We repeat this procedure for different pairs (  ,  ) to produce a discrete mapping of  (  ,  ) minimizing B z p ^

INVERSION OF SYNTHETIC DATA

Simulated 3D sedimentary basin Horizontal coordinate y (km) Horizontal coordinate x (km) mGal Noise-corrupted gravity anomaly

Simulated 3D sedimentary basin The true depths of the simulated basement relief Region I Region II

Simulated 3D sedimentary basin Region I Region II Horizontal coordinate y (km) Horizontal coordinate x (km) Region IRegion II The true depths of the simulated basement relief Gravity data

Simulated 3D sedimentary basin To estimate the parameters defining the parabolic decay of the density contrast with depth Depth (km) Region I Region II   (g/cm 3 ) Parabolic laws of density contrast variation with depth   z z       0  0   We evaluate the functional: 2 B B zpW  0 ),(    ^

Region I Region II To estimate the parameters defining the parabolic decay of the density contrast with depth Simulated 3D sedimentary basin We evaluate the functional: 2 B B zpW  0 ),(    ^ B z p ^

To estimate the parameters defining the parabolic decay of the density contrast with depth The contour maps of functional km Region I Region II Simulated 3D sedimentary basin 2 B B zpW  0 ),(    ^ + +

Estimated basement relief

Simulated 3D sedimentary basin True basement relief Estimated basement relief Horizontal coordinate x (km) Horizontal coordinate y (km)

INVERSION OF REAL GRAVITY DATA

Real Gravity Data Brazil Salvador Brasília Rio de Janeiro São Paulo Study area The onshore and part of the shallow offshore Almada Basin on Brazil’s coast.

Real Gravity Data GRAVITY ANOMALY Almada Basin (Brazil)

14 o 30’S 14 o 45’S 39 o 05’ W mGal Real Gravity Data The gravity data from Almada Basin (Brazil) corrected for the seawater and Moho effects. I Actual coastline Shallow offshoreOnshore IIIII

Real Gravity Data The parameters defining the parabolic decay of the density contrast with depth for Almada Basin (Brazil) The contour map of functional: km Functional    for the regions I-II  0 (g/cm 3 )  (g/cm 3 /km) Functional    for the regions II-III 2 B B zpW  0 ),(    ^

Real Gravity Data The 3D depth-to-basement estimate of Almada Basin (Brazil) A B C D E 14 o 30’S 14 o 45’S 39 o 05’ W km

Real Gravity Data The 3D depth-to-basement estimates of Almada Basin (Brazil) Estimated basement relief Gravity anomaly

Conclusions

Conclusions Estimates the 3D basement relief and the density contrast It is impossible to determine the density and the volume of the source from gravity data only. The gravity inversion method How did we overcome the fundamental ambiguity involving the product of the physical property by the volume ? depth-to-basement information at few points gravity data density volume

Inversion method for simultaneously estimating 3D basement relief and density contrast of a sedimentary basin using gravity data and depth control at few points The estimated basement relief is not just a scaled version of the gravity data The method works well even in the case of complex geologic setting Conclusions

Thank You I cordially invite you to attend the upcoming

Extra Figures

The contour maps of functional Region I B B zpW  0 ),(    ^ Depth (km) Horizontal coordinate x (km) N True basement S Horizontal coordinate x (km) Horizontal coordinate y (km) Gravity data Region IRegion II