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GCReflection Events and Their Polarities Defined by the Hilbert Transform*
Bob Hardage1
Search and Discovery Article #40564 (2010)
Posted July 30, 2010
*Adapted from the Geophysical Corner
column, prepared by the author, in AAPG Explorer, July, 2010, and entitled
“Complex Traces: There’s an ‘App’ for That”. Editor of Geophysical Corner is
Bob A. Hardage ([email protected]). Managing Editor of AAPG Explorer is
Vern Stefanic; Larry Nation is Communications Director. Please see closely related article “Instantaneous
Seismic
Attributes
Calculated by the Hilbert Transform”, Search and Discovery article #40563.
1Bureau of Economic Geology, The University of Texas at Austin ([email protected])
Previously we introduced
the concept of a complex
seismic
trace (“Instantaneous
Seismic
Attributes
Calculated by the Hilbert Transform”, Search and Discovery article #40563);
here we’ll show how a complex trace provides a rigorous way to set the
boundaries of data windows associated with distinct
seismic
reflections – and
we’ll define the polarities of each of those reflection events. This complex
trace application is important because it is necessary to determine the
polarity of every reflection event that spans a layered system in order to
determine whether impedance increases or decreases from layer to layer – which
in turn provides insight into the lithology, porosity and type of pore fluid in
each rock layer.
The
principal problem involved in determining the polarity of a
seismic
reflection
event is the challenge of deciding what part of the
seismic
response represents
the reflection event. Questions that have to be answered include:
· Where does the reflection event start and stop?
· How many peaks and troughs are embedded in the reflection event?
· Which peak or trough of a reflection event should be used to define reflection polarity?
The
amplitude-envelope function determined from a complex
seismic
trace provides a
way to define the start time, stop time, wavelet character and polarity of
overlapping – but distinct – reflection events.
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An
example
You
will get the definitive answer “13.” A wavelet packet such as any of those
defined on Figure 1 may be a reflection from
a single interface, or it may be a composite of several reflections from
closely spaced interfaces. In either case, a wavelet packet represents the
shortest-time concentration of reflection of energy that can be recognized in
a
When
a reflection event is defined by this energy packet concept, the polarity of
the reflection event can be defined as the algebraic sign of the real-trace
extremum (either peak or trough) that is closest to the maximum of the
amplitude-envelope that encompasses the energy packet. Using this concept,
the polarity of reflection events 5 and 10 on Figure
1 are positive, and the polarities of reflection events 7 and 12 are
negative. Thus a complex-trace allows
A second illustration of energy packets being used to define distinct reflection events and their polarities is provided as Figure 2. In this case, there are excellent examples of energy packets distinguishing overlapping reflection events (events 7 and 8, and events 11 and 12) and defining the data windows spanned by faint, low-amplitude reflections (events 2 and 3).
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