Occurs when wave encounters sharp discontinuities in the medium important in defining faults generally considered as noise in seismic sections seismic.

Slides:



Advertisements
Similar presentations
Understanding Seismic Events
Advertisements

Tom Wilson, Department of Geology and Geography Environmental and Exploration Geophysics II tom.h.wilson Department of Geology.
Seismic Reflection Processing Illustrations The Stacking Chart and Normal Moveout Creating a seismic reflection section or profile requires merging the.
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.
Multichannel Analysis of Surface Waves (MASW)
Reflection Seismic Processing
Seismic Reflection Ground Roll Filtering Ted Bertrand SAGE 2004.
Multiple Removal with Local Plane Waves
Processing and Binning Overview From chapter 14 “Elements of 3D Seismology” by Chris Liner.
Introduction to GeoProbe
Processing: zero-offset gathers
GG450 April 22, 2008 Seismic Processing.
I. Basic Techniques in Structural Geology
Seismic waves. When an earthquake occurs shockwaves of energy, called seismic waves, are released from the earthquake focus. They shake the Earth and.
Seismic reflection Seismic reflection profiling basically same principle as echo sounding But lower frequency used for greater subbottom penetration Trade.
  The word comes from the Greek word seismic, for shaking.  It is the branch of Geology which has provided the most comprehensive interpretation of.
SOES6004 Data acquisition and geometry
Reflection Field Methods
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.
Basic Seismic Processing INPUT FILTER CMP Gather NMO STACK MIGRATE DISPLAY GEOM VEL ANAL STATICS MUTE.
Filters  Temporal Fourier (t f) transformation  Spatial Fourier (x k x ) transformation applications  f-k x transformation  Radon (-p x ) transformation.
GG 450 April 16, 2008 Seismic Reflection 1.
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.
Geology 5660/6660 Applied Geophysics 18 Feb 2014 © A.R. Lowry 2014 For Wed 20 Feb: Burger (§ ) Last Time: Reflection Data Processing Step.
General Reflection (and some Refraction) Theory Andrew Goodliffe University of Alabama Socorro, NM, Tuesday May 27.
Seismic Reflection Data Processing and Interpretation A Workshop in Cairo 28 Oct. – 9 Nov Cairo University, Egypt Dr. Sherif Mohamed Hanafy Lecturer.
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.
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.
The main instrument used is called the sonde. A basic sonde consists of a source and two receivers one-foot apart. The sonde is lowered down the borehole.
Tom Wilson, Department of Geology and Geography Environmental and Exploration Geophysics II tom.h.wilson Department of Geology.
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.
Tom Wilson, Department of Geology and Geography Environmental and Exploration Geophysics II tom.h.wilson Department of Geology.
Introduction to Seismology
Radon Transforms in Tau-P space and Multiple Removal
Data QC and filtering Bryce HutchinsonSumit Verma Objective: Consider the frequency range of different seismic features Look for low frequency and high.
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
Tom Wilson, Department of Geology and Geography Environmental and Exploration Geophysics II tom.h.wilson Department of Geology.
Seismic Resolution of Zero-Phase Wavelets Designing Optimum Zero-Phase Wavelets R. S. Kallweit and L. C. Wood Amoco Houston Division DGTS January 12, 1977.
Geology 5660/6660 Applied Geophysics 22 Jan 2016 © A.R. Lowry 2016 For Mon 25 Jan: Burger (Ch 2.2.2–2.6) Last time: The Seismometer A seismometer.
Geology 5660/6660 Applied Geophysics Last time: The Refraction Method Cont’d Multiple Horizontal Layers: Using Snell’s law, generalizes simply to: Dipping.
Does It Matter What Kind of Vibroseis Deconvolution is Used? Larry Mewhort* Husky Energy Mike Jones Schlumberger Sandor Bezdan Geo-X Systems.
Lee M. Liberty Research Professor Boise State University.
Geology 5660/6660 Applied Geophysics 12 Feb 2016
Seismic Methods Geoph 465/565 Vertical Seismic Profiling– Nov 2, 2015
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
I. Basic Techniques in Structural Geology Field measurements and mapping Terminology on folds and folds Stereographic projections From maps to cross-sections.
Stacked sections are zero offset sections
Seismic Refraction Interpretation
I. Basic Techniques in Structural Geology
Reflection velocity analysis
Reflection Seismic Method
Applied Geophysics Fall 2016 Umass Lowell
SEISMIC DATA GATHERING.
Environmental and Exploration Geophysics II
Understanding Seismic Events
Active Source Seismology
From Raw Data to an Image
Making CMP’s From chapter 16 “Elements of 3D Seismology” by Chris Liner.
—Based on 2018 Field School Seismic Data
Processing and Binning Overview
EXPLORATION GEOPHYSICS
Medium effects on waves Reflection/refraction
Reflected, Refracted and Diffracted waves
Presentation transcript:

occurs when wave encounters sharp discontinuities in the medium important in defining faults generally considered as noise in seismic sections seismic migration usually corrects for this effect Diffraction

Diffractions generated by abrupt lateral changes in lithology T-X curve is a hyperbola Amplitude falls off rapidly away from the apex. attenuated by migration Seismic events Non-primary events

X Z Earth model X T Seismic Section Diffraction

generated by waves that have been reflected once from an interface formed by the convolution of the source wavelet with the RC of the interface considered the most important part of the seismic section comprise the “signal” while everything else on the section is considered “noise” Seismic events Primary reflections

Direct waves source-generated wave that travels directly from source to receiver usually first arrivals at near offsets T-X curve is a straight line with intercept = 0 attenuated by NMO muting and stacking Head waves (refractions) generated by critically refracted waves from near-surface layers Usually first arrivals at far offsets T-X curve is a straight line with intercept  0 attenuated by NMO muting and stacking Seismic events Non-primary events

Ground roll generated by source They are surface waves traveling along the ground surface. T-X curve is a straight line with intercept = 0. frequency content < 10 Hz low velocities ( m/s) attenuated by arrays, frequency filtering, or F-K filtering Seismic events Non-primary events

Multiples generated by waves reflected more than once T-X curve is a hyperbola. NMO correction does NOT flatten them. Very high reflection coefficients are needed to produce distinctive multiples on the seismic section. Most common type is water reverberation. attenuated by various advanced techniques Seismic events Non-primary events

Direct Ground roll Head wave XCXC XOXO Non-primary Linear Events

Primary Earth’s surface Subsurface reflector S R1R1 Ground roll Direct P-wave R2R2 Head wave (refraction) First multiple Seismic events Non-primary events

Direc t Ground roll Head wave (refraction) First multiple Primary R1R1 R2R2 Seismic events Non-primary events

Incoherent noise generated by near-surface effects (e.g., humans, animals, machines, equipment, wind, plants, scatterings, … etc) random in nature Signal-to-noise ratio (S/N) is the ratio between signal and noise energies in a specific portion of the section. Poor sections have S/N < 1.0. attenuated by stacking Stacking M traces enhances the S/N by M 1/2. Seismic events Non-primary events

Ideally, we want an impulse of zero width. Practically, the best we can attain is a narrow wavelet with minimum sidelobes. Examples of practical wavelets are: Ricker wavelet, which approximates that of a dynamite. Klauder wavelet, which approximates that of a Vibroseis. The seismic wavelet

Ideal wavelet Klauder wavelet (f = 20 – 80 Hz) Ricker wavelet (f = 30 Hz) The seismic wavelet

ability to distinguish two closely-spaced events on the seismic section We can distinguish two events: - - vertically, depending on: - -the signs and magnitudes of the events - -the separation between the events - -dominant frequency - - horizontally, depending on: - -the receiver spacing - -dominant frequency - -velocity - -dip angle Seismic resolution

Seismic resolution Vertical