Predictive deconvolution is a method that uses the autocorrelation of seismic trace data to design a filter that can predict reverberations and multiples in the data. This prediction is then subtracted from the original trace, leaving behind the trace with multiples removed while primaries remain. Spiking deconvolution aims to concentrate the energy of seismic pulses near the front of the wavelet. Adaptive deconvolution is based on adaptive linear filtering to remove multiples that have varying periods with travel time while preserving primary reflections.
Predictive deconvolution is a method that uses the autocorrelation of seismic trace data to design a filter that can predict reverberations and multiples in the data. This prediction is then subtracted from the original trace, leaving behind the trace with multiples removed while primaries remain. Spiking deconvolution aims to concentrate the energy of seismic pulses near the front of the wavelet. Adaptive deconvolution is based on adaptive linear filtering to remove multiples that have varying periods with travel time while preserving primary reflections.
Predictive deconvolution is a method that uses the autocorrelation of seismic trace data to design a filter that can predict reverberations and multiples in the data. This prediction is then subtracted from the original trace, leaving behind the trace with multiples removed while primaries remain. Spiking deconvolution aims to concentrate the energy of seismic pulses near the front of the wavelet. Adaptive deconvolution is based on adaptive linear filtering to remove multiples that have varying periods with travel time while preserving primary reflections.
Predictive deconvolution is a method that uses the autocorrelation of seismic trace data to design a filter that can predict reverberations and multiples in the data. This prediction is then subtracted from the original trace, leaving behind the trace with multiples removed while primaries remain. Spiking deconvolution aims to concentrate the energy of seismic pulses near the front of the wavelet. Adaptive deconvolution is based on adaptive linear filtering to remove multiples that have varying periods with travel time while preserving primary reflections.
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PREDICTIVE DECONVOLUTION
• Autocorrelation of a trace to ascertain periodicity within data
• Filter designed from the autocorrelation when convolved with data
trace predicts reverberations and multiples.
• Predicted trace is subtracted from observed trace to give prediction
error.
• Which should be the trace with the predicted reverberations and
multiples removed.
• Primaries are considered as unpredictable so they remain.
Autocorrelation is the cross correlation of a trace with itself Amplitude
Multiple period
Time
Primary energy Multiple energy Multiple energy
The autocorrelation function of a seismic signal is an effective tool for
determining the presence and time lag (duration) of reverberations/multiples. Given the input x(t), we want to predict its value at some future time (t+a), where ‘a’ is prediction lag.
• Type of predictive deconvolution in which the operator is to predict
energy within a sample or two, or at the first zero crossing , after the zero lag value of autocorrelation.
• Concentrate the energy of the pulse as near as possible to the front
of wavelet - turns a wavelet into spike.
• Data assumed to be minimum phase.
• Earths reflectivity series is assumed to be random and earth’s
impulse response to be minimum phase. VIBROSEIS DECONVOLUTION
• Vibroseis produces chirp signal which when convolved
with earths reflectivity series gives a complicated wavelet from which earths reflectivity series is hard to interpret.
• Cross correlate this observed signal with the chirp signal
to get the approximate of earths reflectivity series. ADAPTIVE DECONVOLUTION
• Based on adaptive linear filtering techniques in
which the operator coefficients are updated using a simple adaptive algoritm. • Applicable for use in preprocessing reflection seismic data which contains multiples with periods that vary with travel time. So it removes multiples with varying periods while leaving primary reflections relatively undistorted. Simplified diagram of a hard water-bottom model showing the raypathsfor some of the arrivals Plot showing near-offsets traces for several adjacent shotpoints from lina A with offset equal to 914 ft and water depth equal to 300 ft
Tp=traveltime of primary reflection
Tm1=traveltime of first water-bottom arrival REFERENCES