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PETR8510 RECAP LAST WEEK Seismic reflection method Acoustic based method which provides high resolution images of the sub- surface Data recorded as shot gathers – many receivers for each source Arrivals in data are identified from their character and moveout Once identified their travel times can be used to determine depth to features in the sub-surface (within the errors of the input parameters)

Intro to seismic 2

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Introduction to Seismic

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Page 1: Intro to seismic 2

PETR8510

RECAP LAST WEEK• Seismic reflection method

– Acoustic based method which provides high resolution images of the sub-surface

– Data recorded as shot gathers – many receivers for each source

– Arrivals in data are identified from their character and moveout

– Once identified their travel times can be used to determine depth to features in the sub-surface (within the errors of the input parameters)

Page 2: Intro to seismic 2

PETR8510

ZERO OFFSET DATA• Shot gathers

– Numerous receivers, one source– Data are recorded at ‘finite offset’

• Zero offset– Equivalent of one source,

one receiver at eachlocation, but in lots of places

– Much easier to interpret

TWT

TWT

zhongwei
Note
Normal instance data or zero offset
Page 3: Intro to seismic 2

PETR8510

STACKING• Acquisition involves creating a series of shot gathers

– Move-up rate – source vs receiver spacing

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Line
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Note
Color represents different color positions.
Page 4: Intro to seismic 2

PETR8510

STACKING

• Acquisition involves an inherent data redundancy– Data recorded as shot

gathers are sorted in to common mid point (CMP) gathers

zhongwei
Rectangle
zhongwei
Note
we can get the time (t0 in the graph) for zero offset.
Page 5: Intro to seismic 2

PETR8510

STACKING• CMP gathers are

corrected for normal moveout (NMO)– This creates equivalent

zero offset traces

• Zero offset traces are plotted so centred on the equivalent source-receiver location

TWT

Location

Page 6: Intro to seismic 2

PETR8510

STACKING• NMO corrections in

practice– Function of reflector

depth, average velocity and source-receiver offset

– Only offset is known

• Resort to trial and errors and statistics

zhongwei
Note
this way to try which the velocity is for each layer.
zhongwei
Rectangle
zhongwei
Rectangle
zhongwei
Rectangle
Page 7: Intro to seismic 2

PETR8510

STACKING• The zero offset section is

not a depth section and its representation of sub-surface geometry is flawed– It needs to be ‘migrated’

• Post-stack migration only here

Page 8: Intro to seismic 2

PETR8510

MIGRATION• A reflector is the equivalent of a

series of closely spaced diffractors– Migration = series of diffractor

response corrections

Page 9: Intro to seismic 2

PETR8510

MIGRATION• Diffraction migration

– Sum along diffraction travel time curve

Page 10: Intro to seismic 2

PETR8510

MIGRATION• Time migration

– Based on a series of 1D velocity variations

• Depth migration– Based on 2D velocity function

Time Depth

Page 11: Intro to seismic 2

PETR8510

MIGRATION• Post-stack migration works

provided dips are shallow• If not require pre-stack

migration– More expensive– Based on ellipse rather than

circle (in 2D)

Page 12: Intro to seismic 2

PETR8510

MIGRATION• Places features in their correct

relative positions• Requires perfect knowledge of the

sub-surface velocity field• Many methods• Pre- or post-stack

– Depends on geological complexity

– dips, lateral velocity variation• Computational intensive

(expensive)

Page 13: Intro to seismic 2

PETR8510

SUMMARY• Stacking and migration

– Improve SNR– Place features in ‘correct’ relative positions – Depth conversion difficult

Page 14: Intro to seismic 2

PETR8510

NEXT TIME• Well logging – measurements in a

drill hole– Acoustic and density logging and

synthetic seismograms• Other kinds of logging

– Radioactivity (gamma), electrical (SP, resistivity)