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Seismic View: 2 km Deep Meandering River. Aerial View Eucalyi River, Peru. Overview of Seismic Imaging. Jerry Schuster KAUST. Outline. Forward Acoustic Problem. Inverse Acoustic Problem. Seismic Experiment. Seismic Migration. c r. c r. 2. 1. 2. 1. ZO Seismic Section.
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Seismic View: 2 km Deep Meandering River Aerial View Eucalyi River, Peru
Overview of Seismic Imaging Jerry Schuster KAUST
Outline • Forward Acoustic Problem • Inverse Acoustic Problem • Seismic Experiment • Seismic Migration
c r c r 2 1 2 1 ZO Seismic Section Depth Time
Monterey Seismic Image 0 km 2 km 0 km 0.1 km Monterey Optical Image
Acoustic Forward Problem Pressure Source r r ( r r ) o ( r ) k = w/c Given: r d(r) Find: dr Soln: c 1 2 2 d + k d = o r c ò = g d ( r ) 2 Depth
r r r r ( ( r r r r ) ) o o ( ( r r ) ) c r c r 1 2 1 2 dr Depth Time r r ò = = g g d d ( ( r r ) ) Goal: Compute ZO Seismic Section
Common Shot Gather Time Depth
Common Midpoint Gather Midpoint Time Depth
Normal Moveout Correction Midpoint Time Depth
Stacked Trace Midpoint Time Depth
Stacked Seismic Section Time Depth
Outline • Forward Acoustic Problem • Inverse Acoustic Problem • Seismic Experiment • Seismic Migration
What is the Problem? Incorrect location. You think events originated directlybelow geophones. Events Can Originate Updip V/2 D=VT/2 Depth Time
What is another Problem? Events Originate Pt. Diffractors Depth Time
corner 0 km 30 m 0 m 30 m
ZO Data Migration (Relocates Reflections back to Place of Origin) ZO Data 0 km 3 km 0 km 7 km
Seismic Inverse Problem 2 Soln: min || Lo-d || ‘ waveform inversion -1 T T migration o = [L L] L d T L d Given: d= Lo Find: o(x,y,z)
Outline • Forward Acoustic Problem • Inverse Acoustic Problem • Seismic Experiment • Seismic Migration
ZO Migration Smear Reflections along Fat Circles rs + T rs o 2-way time r x s 2 2 (x-x ) + y = d(x , ) s rs .5c s
ZO Migration Smear Reflections along Fat Circles rs & Sum 2-way time x d(x , ) s
ZO Migration Smear Reflections along Circles rs & Sum 2-way time r d(x , ) s
ZO Migration Resolution Intersection of Fresnel Zones Intersection of Fresnel Zones Vertical Res. = Near-Offset Traces
ZO Migration Resolution Intersection of Fresnel Zones Intersection of Fresnel Zones Horiz. Res. = Far-Offset Traces
Why is Pt. Scatterer Response of Migration a Blurred Version of Point? Lr d = Lr but Migration: Migration Section = Blured Imageof r Migrated Section Data T m = L d
Seismic Section 12 km Time
0 km 3 km 0 km 7 km
Migration Least Squares Migration 0 km 3 km 0 km 7 km
Seismic Imaging Course • Kirchhoff & Beam Migration • Phase Shift-Like Methods • Reverse-Time Migration • Full Waveform Inversion