Land and Marine Seismic Acquisition from 2D to 3D

Slides:



Advertisements
Similar presentations
The Seismic Method Lecture 5 SLIDE 1
Advertisements

Survey Planning & Illumination with NORSAR-3D
Chapter 1- General Properties of Waves Reflection Seismology Geol 4068
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.
Fourier Theory in Seismic Processing
Tom Wilson, Department of Geology and Geography Environmental and Exploration Geophysics II tom.h.wilson Department of Geology.
Velocity Analysis Introduction to Seismic ImagingERTH 4470/5470 Yilmaz, ch
Chapter 2 Fundamentals of Data and Signals
8. Ocean Crustal Structure and Seismic Reflection William Wilcock (via Michelle W.) OCEAN/ESS 410.
Reflection Seismic Processing
Seismic Reflection Ground Roll Filtering Ted Bertrand SAGE 2004.
Processing and Binning Overview From chapter 14 “Elements of 3D Seismology” by Chris Liner.
Seismic Measurement-Systems And Data Acquisition LandMarine.
SIMS-201 Characteristics of Audio Signals Sampling of Audio Signals Introduction to Audio Information.
IT-101 Section 001 Lecture #8 Introduction to Information Technology.
CHAPTER 5 Discrete Sampling and Analysis of Time-Varying Signals Analog recording systems, which can record signals continuously in time, digital data-acquisition.
Fundamentals Introduction Seismic waves: Propagation Velocity and Amplitudes Seismogram Measurement systems Sources, receivers, Acquisition strategies.
Field layouts  Common-offset & Zero-offset  Common-midpoint method  Up-dip and down-dip shooting  Spread types  Singlefold / Multifold recording 
SOES6004 Data acquisition and geometry
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.
Receivers and Recording Systems. Geophones String of Geophones 3 component Typical exploration geophone Various casings.
Reflection Field Methods
Bedrock Delineation by a Seismic Reflection/Refraction Survey at TEAD Utah David Sheley and Jianhua Yu.
Chapter 2: Fundamentals of Data and Signals. 2 Objectives After reading this chapter, you should be able to: Distinguish between data and signals, and.
Filters  Temporal Fourier (t f) transformation  Spatial Fourier (x k x ) transformation applications  f-k x transformation  Radon (-p x ) transformation.
 Principles of Digital Audio. Analog Audio  3 Characteristics of analog audio signals: 1. Continuous signal – single repetitive waveform 2. Infinite.
Fourier Theory in Seismic Processing (From Liner and Ikelle and Amundsen) Temporal aliasing Spatial aliasing.
Chapter 1- General Properties of Waves Reflection Seismology Geol 4068 Elements of 3D Seismology, 2nd Edition by Christopher Liner.
GG450 March 20, 2008 Introduction to SEISMIC EXPLORATION.
Time Series Analysis of Elephant Acoustic and Seismic Signals Alex Williamson Physics Dept.
Seismometry Seismology and the Earth’s Deep Interior Seismometer – The basic Principles u x x0x0 ugug umum xmxm x x0x0 xrxr uground displacement x r displacement.
Seismic reflection Ali K. Abdel-Fattah Geology Dept.,
Geology 5660/6660 Applied Geophysics 18 Feb 2014 © A.R. Lowry 2014 For Wed 20 Feb: Burger (§ ) Last Time: Reflection Data Processing Step.
Weighted Stacking of 3-D Converted-wave Data for Birefringent Media Richard Bale.
Processing Lab 9 Objectives: - View a timeslice - Consider binning effects on migration - Post stack Migration Sumit VermaBryce Hutchinson.
Chapter 11 Vibrations and Waves Phy 2053 Conceptual Questions.
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.
Tom Wilson, Department of Geology and Geography Environmental and Exploration Geophysics II tom.h.wilson Department of Geology.
Noise and Sensitivity of RasClic 91
Tom Wilson, Department of Geology and Geography Environmental and Exploration Geophysics II tom.h.wilson Department of Geology.
SEISMIC INTERPRETATION
Processing Lab 2 – Geometry Bryce Hutchinson Objectives: Add a dictionary Gain a better understanding of header issues Display geometry correctly Visualize.
Tom Wilson, Department of Geology and Geography Environmental and Exploration Geophysics II tom.h.wilson Department of Geology.
EXPLORATION GEOPHYSICS. EARTH MODEL NORMAL-INCIDENCE REFLECTION AND TRANSMISSION COEFFICIENTS WHERE:  1 = DENSITY OF LAYER 1 V 1 = VELOCITY OF LAYER.
Introduction to Seismology
Environmental and Exploration Geophysics II tom.h.wilson Department of Geology and Geography West Virginia University Morgantown, WV.
Reflection seismograms
Introduction to Seismic Reflection Imaging References: J.M. Reynolds, An Introduction to Applied and Environmental Geophysics, John Wiley & Sons,
FIELD GEOMETRY FOR MULTICHANNEL SEISMIC (MCS) PROFILES Introduction to Seismic Reflection Imaging: Pt 2.
Lee M. Liberty Research Professor Boise State University.
Microtremor method Saibi. Dec, 18, 2014.
Lee M. Liberty Research Professor Boise State University.
Seismic Refraction Interpretation
Zero-Offset Data d = L o ò r ) ( g = d dr r ) ( g = d
Reflection Seismic Method
Land and Marine Seismic Acquisition from 2D to 3D
Applied Geophysics Fall 2016 Umass Lowell
SEISMIC DATA GATHERING.
Environmental and Exploration Geophysics II
MECH 373 Instrumentation and Measurements
New ProMAX modules for reflectivity calibration and noise attenuation
Seismic Acquisition A 3D survey is designed based on: Land Operations
Acoustic Reflection 2 (distance) = (velocity) (time) *
The Wave Equation Modeled
Review of Coherent Noise Suppression Methods
—Based on 2018 Field School Seismic Data
Processing and Binning Overview
EXPLORATION GEOPHYSICS
Position of first shot= 300 m to the west of the first geophone
Presentation transcript:

Land and Marine Seismic Acquisition from 2D to 3D From chapters 7-12 “Elements of 3D Seismology” by Chris Liner

Outline-1 CMP METHOD (Harry Mayne) Seismic sensors geophones hydrophones gimballed geophones and hydrophones accelerometers Sources Explosives Vibroseis SEGY data

Outline-2 Acquisition Parameters Time Sample Rate Offset Range Listen Time Sample Rate and Temporal Aliasing Geophone Spacing and Spatial Aliasing Shooting geometry inline cross-line

Common Midpoint Method (CMP Method) Please take a look at the powerpoint presentation for the radio-telemetry field trip at the following link: http://www.geol.lsu.edu/Faculty/Juan/ReflectSeismol05/labs/ppt/Radio-telemetry.ppt This link has information to complement the explanation on the CMP method.

Common Midpoint Method (CMP Method) Hydrophone groups Shotpoint # 1 #6 #5 #4 #3 #2 #1 Midpoints Separation between midpoints is 1/2 separation between hydrophone groups

Common Midpoint Method (CMP Method) Hydrophone groups Shotpoint # 2 #6 #5 #4 #3 #2 #1 Midpoints

Common Midpoint Method (CMP Method) Hydrophone groups Shotpoint # 3 #1 #2 #3 #4 #5 #6 Midpoints

Common Midpoint Method (CMP Method) Hydrophone groups Shotpoint # 4 #1 #2 #3 #4 #5 #6 Midpoints

Common Midpoint Method (CMP Method) Hydrophone groups Shotpoint # 5 #1 #2 #3 #4 #5 #6 Midpoints

Common Midpoint Method (CMP Method) Hydrophone groups Shotpoint # 6 #1 #2 #3 #4 #5 #6 Midpoints

Common Midpoint Method (CMP Method) Hydrophone groups Shotpoint # 7 #1 #2 #3 #4 #5 #6 Midpoints

Common Midpoint Method (CMP Method) Hydrophone groups Shotpoint # 8 #1 #2 #3 #4 #5 #6 Midpoints

Common Midpoint Method (CMP Method) Hydrophone groups Shotpoint # 8 #1 #2 #3 #4 #5 #6 Midpoints

Common Midpoint Method (CMP Method) Hydrophone groups #6 #5 #4 #3 #2 #1 Shotpoint # 1 Midpoints

Common Midpoint Method (CMP Method) Hydrophone groups #6 #5 #4 #3 #2 #1 Shotpoint # 1 Shotpoint # 2 Shotpoint # 1 Shotpoint # 2 Midpoints

Common Midpoint Method (CMP Method) Hydrophone groups #6 #5 #4 #3 #2 #1 Shotpoint # 1 Shotpoint # 2 Shotpoint # 3 Shotpoint # 1 Shotpoint # 2 Shotpoint # 3 Midpoints

Common Midpoint Method (CMP Method) Hydrophone groups #6 #5 #4 #3 #2 #1 Shotpoint # 1 Shotpoint # 2 Shotpoint # 3 Shotpoint # 4 Shotpoint # 1 Shotpoint # 2 Shotpoint # 3 Shotpoint # 4 Midpoints

Common Midpoint Method (CMP Method) Hydrophone groups #6 #5 #4 #3 #2 #1 Shotpoints # 1-8 1 2 Midpoints 3 4 5 6 7 8 8 13

Common Midpoint Method (CMP Method) Fold or Multiplicity is the number of times that the same midpoint is sampled by different shots and different receivers Signal-to-Noise increases as the square root of the fold Fold 1 2 Midpoints 3 4 5 6 7 8 8 13

Common Midpoint Method (CMP Method) Maximum Fold is achieved after the 6th shot Fold 1 2 Midpoints 3 4 5 6 7 8 8 13

Common Midpoint Method (CMP Method) When shotpoint spacing and group spacing are equal then Maximum fold = number of geophones or hydrophones Midpoint separation = 1/2 distance between geophones In a more general case: Maximum Fold = #recording groups * distance between groups 2 * distance between shots Midpoint separation = 1/2 smaller of the two: receiver group spacing or shot spacing

Gather Types A gather i.e. “a subset of the traces from the entire data set” can be of different types: Shotpoint gather Common source-receiver offset gather (COS) Common midpoint gather

Shotpoint Gather e.g. Shotpoint gather #3 #6 #5 #4 #3 #2 #1

A shotpoint gather samples various midpoints and a variety of angles #6 #5 #4 #3 #2 #1 Hydrophone groups #1 #2 #3 #4 #5 #6 A shotpoint gather samples various midpoints and a variety of angles

A shotpoint gather samples various midpoints and a variety of angles What happens to the reflecting points in a shotpoint gather when the reflecting interrface dips? Shotpoint #3 #6 #5 #4 #3 #2 #1 Hydrophone groups #1 #2 #3 #4 #5 #6 A shotpoint gather samples various midpoints and a variety of angles

What happens to the reflecting points in a shotpoint gather when the reflecting interface dips? #6 #5 #4 #3 #2 #1 Hydrophone groups #1 #2 #3 #4 #5 #6 Reflecting points Midpoints A shotpoint gather samples different reflecting points at a variety of angles

Common Midpoint Method (CMP Method) Hydrophone group #4 Common source-receiver offset and common receiver, shotpoints 1-8 #6 #5 #4 #3 #2 #1

Common source-receiver offset and common receiver, shotpoints 1-8 Hydrophone group #4 Common source-receiver offset and common receiver, shotpoints 1-8 #6 #5 #4 #3 #2 #1 COS means equal reflection angle Midpoints

COS means equal reflection angle In the case of a COS gather where are the true midpoints when the reflecting, geological interface has a dip? #6 #5 #4 #3 #2 #1 COS means equal reflection angle Midpoints

COS NO LONGER implies equal reflection angles #6 #5 #4 #3 #2 #1 Actual reflecting points Midpoints

Common Midpoint Method (CMP Method) Hydrophone group #4 Common mid-points and shotpoints 1-8 #6 #5 #4 #3 #2 #1 Midpoints

CMP gathers sample varying angles but a common geological midpoint Hydrophone group #4 Common mid-point and shotpoints 1-8 #6 #5 #4 #3 #2 #1 group 8 7 6 5 4 3 2 1 Midpoint #6 CMP gathers sample varying angles but a common geological midpoint

CMP gathers sample varying angles but a common geological midpoint What happens to a common midpoint gather when the reflecting interface has a dip? #6 #5 #4 #3 #2 #1 group 8 7 6 5 4 3 2 1 Midpoint #6 CMP gathers sample varying angles but a common geological midpoint

CMP gathers SAMPLE varying angles but with a relatively smaller spread of reflecting points than the shotpoint and common-offset gathers #6 #5 #4 #3 #2 #1 group 8 7 6 5 4 3 2 1 Midpoint #6 True Reflecting Points

A common midpoint gather minimizes the effect of dip while it helps increase the signal-to-noise ratio

Outline-1 CMP METHOD (Harry Mayne) Seismic sensors geophones hydrophones gimballed geophones and hydrophones accelerometers Sources Explosives Vibroseis SEGY data

Convert ground motion into electricity Geophones Convert ground motion into electricity at a rate of about 1 Volt/inch/sec Natural Resonance Frequency 100 Hz GS-100 from Geospace

Geophone layout

Geophone layout

Hydrophones convert changing pressure into Volts (Volts/bar) Seismic Sensors Hydrophones convert changing pressure into Volts (Volts/bar) e.g. Preseis 2517 from I/O 1V/microPascal

Gimballed Geophone-hydrophone combinations for sea-bottom work Sea-Array 4 from Geospace

Streamer layout

Convert ground acceleration into Volts d(dx/dt) dt Accelerometers Convert ground acceleration into Volts d(dx/dt) dt E.g. VectorSeis from I/O 3-component digital accelerometer (requires battery) full-scale at 3.3 m/s2; noise level 0.44 microm/s2 140db = 20 log (3.3/4*10^-7)

Outline-1 CMP METHOD (Harry Mayne) Seismic sensors geophones hydrophones gimballed geophones and hydrophones accelerometers Sources Explosives Vibroseis SEGY data

Vibroseis Method (Liner, 2004; p.157, para. 4, ) An output sweep (e.g., 10-80 Hz) enters the earth …..and undergoes various reflections

+ + = ...something too complicated to draw Field correlation “unravels” the raw data into ….

Vibroseis images from the Lithoprobe Project, Canada www.lithoprobe.ca A vibrator truck “12 elephants dancing in unison” (LITHOPROBE, CANADA)

Noble Explochem Limited Explosives Noble Explochem Limited

NSF R/VIB NBPalmer- February/March 2003 GI Watergun Array NSF R/VIB NBPalmer- February/March 2003

Sercel G. GUN 150 cu. In. firing at 2,000 p.s.i. Link to movie of this G. Gun working in a pool

Outline-1 CMP METHOD (Harry Mayne) Seismic sensors geophones hydrophones gimballed geophones and hydrophones accelerometers Sources Explosives Vibroseis SEGY data

SEGY data 3200 byte EBCDIC header 400 byte tape header One line at a time 400 byte tape header 240 byte trace header DATA 240 byte tape header DATA 240 byte tape header DATA

Outline-2 Acquisition Parameters Time Sample Rate Offset Range Listen Time Sample Rate and Temporal Aliasing Geophone Spacing and Spatial Aliasing Shooting geometry inline cross-line

Sample Rates What is the fewest number of times I need to sample this waveform per second? ? ? ?

Sample Rates

Sample Rates

Sample Rates

Sample Rates What is the fewest number of times I need to sample this waveform per second? At least twice per wavelength or period! OTHERWISE ….

Undersampled waveforms Amplitude Reconstructed frequency (f -aliased) True frequency (f -true)

Oversampled waveforms Nyquist frequency Amplitude Reconstructed frequency frequency is unaliased = True frequency (f -true) Nyquist frequency = 1 / twice the sampling rate Minimum sampling rate must be at least twice the desired frequency E.g., 1000 samples per second for 500Hz, 2000 samples per second for 1000 Hz

Oversampled waveforms Nyquist frequency Amplitude In practice we are best oversampling by double the required minimum i.e. 1000 samples per second for a maximum of 500 Hz i.e., 2000 samples per second for a maximum of 1000 Hz Oversampling is relatively cheap.

Outline-2 Acquisition Parameters Sample Rate and Temporal Aliasing Offset Range Listen Time Geophone Spacing and Spatial Aliasing

Offset Range Maximum shot-receiver offset Target depth One-layer earth of a semi-infinite layer Maximum shot-receiver offset >= target depth. Near critical distance

Maximum shot-receiver Offset Range Maximum shot-receiver offset Target depth Multi-layered earth

Outline-2 Acquisition Parameters Time Sample Rate Offset Range Listen Time Sample Rate and Temporal Aliasing Geophone Spacing and Spatial Aliasing Shooting geometry inline cross-line

….Twice target time to be sage Listen Time ….Twice target time to be sage

Outline-2 Acquisition Parameters Time Sample Rate Offset Range Listen Time Sample Rate and Temporal Aliasing Geophone Spacing and Spatial Aliasing Shooting geometry inline cross-line

Spatial aliasing Spatial frequency, or wavenumber (k) is the number of cycles per unit distance. One spatial cycle or wavenumber = frequency/velocity. Each wavenumber must be sampled at least twice per wavelength (two CMP’s per wavelength) IN PRACTICE each wavenumber must be sampled at least four times per minimum wavelength (two CMP’s per wavelength)

Spatial aliasing However, dip (theta) as well as frequency and velocity event changes the number of cycles per distance, so Liner, 9.7,p.192

For aliasing NOT to occur, delta(t) must be less than T/2 Spatial aliasing For aliasing NOT to occur, delta(t) must be less than T/2

Spatial aliasing

Geophone Spacing and Spatial Aliasing K=0

1/4 wavelength shift per trace total shift across array=3/4 wavelength K=+ or -ve?

1/4 wavelength shift per trace total shift across array=3/4 wavelength K=?

1/2 wavelength shift per trace total shift across array=3/2 wavelength K=0

3/4 wavelength shift per trace total shift across array=2 1/4 wavelength

Spatial aliasing Degrades (“string of pearls”) stacked sections Degrades migration

Signal-to-Noise Improves with stacking: greater fold greater repetition of shots

Outline-2 Acquisition Parameters Time Sample Rate Offset Range Listen Time Sample Rate and Temporal Aliasing Geophone Spacing and Spatial Aliasing Shooting geometry inline cross-line

Fundamental Parameters for land 3D shooting

Common Midpoint

Source-Receiver Offset 2D 3D

Azimuth (3D)

Inline geometry Matlab code

Outline-2 Acquisition Parameters Time Sample Rate Offset Range Listen Time Sample Rate and Temporal Aliasing Geophone Spacing and Spatial Aliasing Shooting geometry inline cross-line

Cross-line geometry Matlab code

Spatial aliasing Degrades (“string of pearls”) stacked sections Degrades migration