Processing and Binning Overview From chapter 14 “Elements of 3D Seismology” by Chris Liner.

Slides:



Advertisements
Similar presentations
Basic Seismic Processing INPUT FILTER CMP Gather NMO STACK MIGRATE DISPLAY GEOM VEL ANAL STATICS MUTE.
Advertisements

Chapter 1- General Properties of Waves Reflection Seismology Geol 4068
Making CMP’s From chapter 16 “Elements of 3D Seismology” by Chris Liner.
Fourier Theory in Seismic Processing
Velocity Analysis Introduction to Seismic ImagingERTH 4470/5470 Yilmaz, ch
Accommodation space, Coluvial wedge. Even in this image, throw is hard to interpret however, there is still geologic insight to be gained. Surface expression.
Basic Seismic Processing INPUT FILTER CMP Gather NMO STACK MIGRATE DISPLAY GEOM VEL ANAL STATICS MUTE.
Reflection Seismic Processing
Seismic Reflection Ground Roll Filtering Ted Bertrand SAGE 2004.
Multiple Removal with Local Plane Waves
Multi-Component Seismic Data Processing
Processing: zero-offset gathers
Near-surface Imaging at Meteor Crater, Arizona Soumya Roy, Ph. D. Student Advisor: Dr. Robert R. Stewart AGL Annual Meeting University of Houston, 2 nd.
Chapter 1- General Properties of Waves Reflection Seismology Geol 4068 Elements of 3D Seismology, 2nd Edition by Christopher Liner.
I. Basic Techniques in Structural Geology
First Arrival Traveltime and Waveform Inversion of Refraction Data Jianming Sheng and Gerard T. Schuster University of Utah October, 2002.
Overview of Some Coherent Noise Filtering Methods Overview of Some Coherent Noise Filtering Methods Jianhua Yue, Yue Wang, Gerard Schuster University.
Occurs when wave encounters sharp discontinuities in the medium important in defining faults generally considered as noise in seismic sections seismic.
Primary-Only Imaging Condition Yue Wang. Outline Objective Objective POIC Methodology POIC Methodology Synthetic Data Tests Synthetic Data Tests 5-layer.
Moveout-Based Spreading Correction for Mode-Converted Waves Ellen (Xiaoxia) & Ilya.
Loading of the data/conversion Demultiplexing Editing Geometry Amplitude correction Frequency filter Deconvolution Velocity analysis NMO/DMO-Correction.
Reflection Field Methods
Joint Migration of Primary and Multiple Reflections in RVSP Data Jianhua Yu, Gerard T. Schuster University of Utah.
Bedrock Delineation by a Seismic Reflection/Refraction Survey at TEAD Utah David Sheley and Jianhua Yu.
Arbitrary Parameter Extraction, Stationary Phase Migration, and Tomographic Velocity Analysis Jing Chen University of Utah.
Autocorrelogram Migration of Drill-Bit Data Jianhua Yu, Lew Katz, Fred Followill, and Gerard T. Schuster.
Filters  Temporal Fourier (t f) transformation  Spatial Fourier (x k x ) transformation applications  f-k x transformation  Radon (-p x ) transformation.
Autocorrelogram Migration for Field Data Generated by A Horizontal Drill-bit Source Jianhua Yu, Lew Katz Fred Followill and Gerard T. Schuster.
4C Mahogony Data Processing and Imaging by LSMF Method Jianhua Yu and Yue Wang.
Chapter 1- General Properties of Waves Reflection Seismology Geol 4068 Elements of 3D Seismology, 2nd Edition by Christopher Liner.
Multisource Least-squares Reverse Time Migration Wei Dai.
Land and Marine Seismic Acquisition from 2D to 3D
Seismic reflection Ali K. Abdel-Fattah Geology Dept.,
The ray parameter and the travel-time curves P flat and P radial are the slopes of the travel time curves T-versus-X and T-versus- , respectively. While.
Fundamentals Introduction Seismic waves: Propagation Velocity and Amplitudes Seismogram Measurement systems Sources, receivers, Acquisition strategies.
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.
1 Outline Full space, half space and quarter space Traveltime curves of direct ground- and air- waves and rays Error analysis of direct waves and rays.
Migration In a Nutshell Migration In a Nutshell Migration In a Nutshell D.S. Macpherson.
Beach Energy Ltd Lake Tanganyika 2D Marine Seismic Survey
Impact of MD on AVO Inversion
EXPLORATION GEOPHYSICS. EARTH MODEL NORMAL-INCIDENCE REFLECTION AND TRANSMISSION COEFFICIENTS WHERE:  1 = DENSITY OF LAYER 1 V 1 = VELOCITY OF LAYER.
Review of Coherent Noise Suppression Methods Gerard T. Schuster University of Utah.
Introduction to Seismology
Radon Transforms in Tau-P space and Multiple Removal
Basic Seismic Processing INPUT FILTER CMP Gather NMO STACK MIGRATE DISPLAY GEOM VEL ANAL STATICS MUTE.
T 2 = T X 2 /V 2. It is a hyperbola with apex at X = 0 and T 0 = 2H/V. – –V and H are the layer velocity and thickness. T 2 -X 2 plot is a straight.
Reflection seismograms
Migration Velocity Analysis of Multi-source Data Xin Wang January 7,
Geology 5660/6660 Applied Geophysics Last time: The Refraction Method Cont’d Multiple Horizontal Layers: Using Snell’s law, generalizes simply to: Dipping.
Geology 5660/6660 Applied Geophysics 29 Feb 2016 © A.R. Lowry 2016 Last Time: Ground Penetrating Radar (GPR) Radar = electromagnetic radiation (light)
Lee M. Liberty Research Professor Boise State University.
Geology 5660/6660 Applied Geophysics 12 Feb 2016
Microtremor method Saibi. Dec, 18, 2014.
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.
Seismic Methods Geoph 465/565 ERB 5104 Lecture 7 – Sept 16, 2015
ADVANCED MARINE TUTORIAL
Susan L. Beck George Zandt Kevin M. Ward Jonathan R. Delph.
GDF Suez Holland E 16-4 VSP Part 1:
Reflection Seismic Method
Land and Marine Seismic Acquisition from 2D to 3D
1-D Mississippi embayment sediment velocity structure and anisotropy: constraint from ambient noise analysis on a dense array Chunyu,Liu1; Charles A. Langston1.
4C Mahogony Data Processing and Imaging by LSMF Method
Overview of Multisource and Multiscale Seismic Inversion
Han Yu, Bowen Guo*, Sherif Hanafy, Fan-Chi Lin**, Gerard T. Schuster
Making CMP’s From chapter 16 “Elements of 3D Seismology” by Chris Liner.
Review of Coherent Noise Suppression Methods
—Based on 2018 Field School Seismic Data
Processing and Binning Overview
Wave Equation Dispersion Inversion of Guided P-Waves (WDG)
Presentation transcript:

Processing and Binning Overview From chapter 14 “Elements of 3D Seismology” by Chris Liner

Outline Justification for Processing Processing Flow Bins

Justification Field data representation of the data is distant from a distance-depth representation of data.

Categories of Processing Adjustments to wavelets, or short-pulse adjustments e.g., frequency filtering phase shifts (rotation) vibroseis correlation Traveltime Corrections (fig. 14.1) : Statics Normal Moveout Dip Moveout Migration

Categories of Processing Amplitude Corrections Geometric spreading Automatic Gain Control Noise Reduction Vertical stack Muting CMP stack filtering (f, f-k, tau-p (or radon) multiple suppression

Xia et al., 2004 An example of analysis for near-surface seismic structure

Seismic data “Multiple universes for seismic data” Shotpoint gathers (distance versus time) CMP gathers (distance versus time) Tau-p (horizontal slowness versus intercept time) f-k (frequency versus wavenumber)

Distance between shot and the receiver (m) Two-way traveltime (s)

Distance between shot and the receiver (m) Two-way traveltime (s) dT/dx = 1/V (s/m) Velocity (m/s) T 2 = T x 2 / V 2 T0T0

Distance between shot and the receiver (m) Two-way traveltime (s) dT/dx = 1/V (s/m) Velocity (m/s) T 2 = T x 2 / V 2 T0T0

dT/dx = 1/V (s/m) x 1/V = 0 ( s/m) 1/V = p (ray parameter) V

Distance between shot and the receiver (m) Two-way traveltime (s) dT/dx = 1/V (s/m) Velocity (m/s) T 2 = T x 2 / V 2 T0T0

dT/dx = 1/V h (s/m) x 1/V h = 1/[V/ sin(angle) ] ( s/m) 1/V h = p (ray parameter) angle V

Distance between shot and the receiver (m) Two-way traveltime (s) dT/dx = 1/V (s/m) Velocity (m/s) T 2 = T x 2 / V 2 T0T0

x 1/V h = 1/[V/sin(angle) ]( s/m) 1/V h = p (ray parameter) angle V

x (m) Two-way traveltime (s) T0T0 p (s/m) p=0 tau (intercept time) s Add amplitude

x (m) Two-way traveltime (s) T0T0 p (s/m) p=0 tau (intercept time) s Add amplitude

x (m) Two-way traveltime (s) f (1/s) p=0 k (wavenumber - 1/m) V=f/k (m/s) 100 Hz 1000 m/s 1/10 m

x (m) Two-way traveltime (s) f (1/s) p=0 k (wavenumber - 1/m) V=f/k (m/s) 100 Hz 1000 m/s 1/10 m

x (m) Two-way traveltime (s) f (1/s) k (wavenumber - 1/m) V h =inf (m/s) V h =1000 (m/s) V h =inf (m/s) V h =1000 (m/s)

P-wave & Sv - wave SzSz SxSx

“skin depth” = 1/2 longest wavelength V h ~= 90% shear wave velocity

Dispersion t0t0 t1t1 t2t2 t1t1 t2t2

Xia et al., 2004

x (m) Two-way traveltime (s) f (1/s) p=0 k (wavenumber - 1/m) V=f/k (m/s) 100 Hz 1000 m/s

Outline Bins Calculated common midpoints “CMP bin center” Length and width of bin <= spatial aliasing dimensions

To prevent aliasing: max dimension = V/4f max For GOM: V = V x depth Rule of Thumb: 12.5m by 12.5 m for > 2000 m IDEAL BIN SIZE: 5m by 5m for seafloor and deeper

The “best” bin: SMALL ALL OFFSETS ALL AZIMUTHS LARGE FOLD

Outline Justification for Processing Processing Flow Bins