Time-space varying spectra for seismic processing

• US 8,185,316 B2
• Filed: 05/21/2008
• Issued: 05/22/2012
• Est. Priority Date: 05/25/2007
• Status: Expired due to Fees

• Current Assignee: Prime Geoscience Corporation
• Original Assignee: Prime Geoscience Corporation
• Inventors: Alam, Aftab, Taylor, James D.
• Primary Examiner(s): Dunn, Drew A
• Assistant Examiner(s): PARK, HYUN D
• Application Number:
  US12/124,439
• Publication Number:
  US 20090292475A1
• Time in Patent Office: 1,462 Days
• Field of Search: 702/14
• US Class Current: 702/14
• CPC Class Codes: G01V 1/34 Displaying seismic recordings or visualisation of seismic data or attributes
• CPC Class Codes: G01V 1/36 Effecting static or dynamic corrections on records, e.g. correcting spread; Correlating seismic signals; Eliminating effects of unwanted energy

Abstract

A method and visualization apparatus for spectral analysis of time-and-space varying signals enables high resolution investigation of 3D seismic data for the exploration of oil and gas. The method extrapolates multi-resolution short windows into an average long window then computes its FFT. Extrapolation uses the continuity relationship between data inside and outside of short windows. Applications of the method are illustrated with graphical screen 3D volume displays of amplitude spectra, dip and azimuth, curvature and faults (figure below). Aside from high resolution these displays improve the productivity of a seismic interpreter.

Claims

1. A method for estimating amplitude and phase spectra of data consisting of time-varying sensor signals sampled continuously in time with uniform high frequency-resolution, comprising:

(a) obtaining a representation of said data sampled at an input (Δ

T) time-rate wherein the data are acquired by deploying a plurality of seismic sensors proximate a surface of the earth or in a body of water, the data representing seismic amplitude detected by the sensors with respect to time in response to actuation of a seismic energy source;

(b) specifying an output sample time-rate (Δ

T′

) that is an integer multiple of Δ

T;

(c) specifying a data analysis window Δ

t that is larger than the output sample time rate (Δ

T′

), wherein the analysis window is an integer multiple of Δ

T;

(d) specifying a frequency sample rate (Δ

f);

(e) computing in a processor a time window (2/Δ

f) that would produce the frequency sample rate and that is an integer multiple of the input time rate (Δ

T);

(f) generating in the processor a model that extrapolates data inside the data analysis window to fill the frequency sample rate (2/Δ

f) window, wherein

(g) the model uses a continuity relationship between data within and data outside of the data analysis (Δ

t) window,

(h) wherein the model has the property that forward and backward extrapolated values decrease in amplitude with respect to time from edges of the data analysis (Δ

t) window,

(i) capturing data in the processor within the data analysis (Δ

t) window at a start of data time;

(j) extrapolating in the processor in forward and backward directions the captured data to fill the (2/Δ

f) time window;

(k) computing fast Fourier transform (FFT) coefficients in the processor for the data in the (2/Δ

f) time window;

(l) incrementing in the processor by the output sample time (Δ

T′

) from the start time of data capture for a next FFT computation;

(m) repeating (i) through (l) until an end of data time is reached; and

at least one of

(n) saving in a storage medium the FFT coefficients sampled at (Δ

T′

, Δ

f) intervals, and

(o) saving in the storage medium a transformation of the FFT coefficients into amplitude and phase spectra sampled at (Δ

T′

, Δ

f) intervals.

2. The method of claim 1 wherein:

(a) the mathematical model is a statistical Linear Prediction Filter (LPF) model;

(b) the continuity relationship is an autocorrelation function with a maximum lag, Lmax, of said data in a time window of length, (2/Δ

f), that is symmetrically centered relative to a moving data time window of length Δ

t; and

(c) the forward extrapolation is done with repeated application of a minimum phase filter derived via Levinson recursion from the autocorrelation function and backward extrapolation is done with repeated application of the time reversed version of the minimum phase filter.

3. The method of claim 2 further comprising:

(a) computing the auto-correlation function in the processor of the signal in a (2/Δ

f)-window to determine statistical correlation between the signal within and outside of a signal analysis window,

(b) using the auto-correlation function to compute LP coefficients in the processor via Levinson recursion and linearly combining said coefficients with analysis window in a recursive loop for extrapolations in the forward direction and then repeating said linear combination with the reversed sequence of said coefficients for extrapolations in the backward direction,

(c) specifying a plurality of multi-resolution data analysis windows, where each such multi-resolution data analysis window has a different length, the length being in a range from said Δ

t to a selected fraction of said (2/Δ

f);

(d) initializing the start of spectral computation time;

(e) capturing data within said plurality of multi-resolution signal analysis windows, each centered at the spectral computation time;

(f) computing a sequence of LP coefficients in the processor for each multi-resolution window;

(g) extrapolating captured data in the processor in each multi-resolution window in forward and backward directions to fill said (2/Δ

f)-window;

(h) averaging data over plurality of multi-resolution extrapolated (2/Δ

f)-windows in the processor to compute an average (2/Δ

f)-window;

(i) computing FFT coefficients in the processor for the average (2/Δ

f)-window;

(j) incrementing spectral computation time by Δ

T′

,

(k) repeating (e) through (j) until an end of spectral computation time;

(l) at least one of storing said FFT coefficients as 2-dimensional arrays sampled at (Δ

T′

, Δ

f) intervals, saving in said storage medium a transformation of said FFT coefficients into amplitude and phase spectra as 2-dimensional arrays sampled at (Δ

T′

, Δ

f) intervals, and

(m) displaying the amplitude and phase spectra as 2-dimensional images on an interactive graphical screen.

4. A method for estimating amplitude and phase spectra of seismic data sampled continuously in time with uniform high frequency-resolution, comprising:

(a) obtaining a representation of the seismic data sampled at an input time rate (Δ

T), wherein the data seismic are acquired by deploying a plurality of seismic sensors proximate a surface of the earth or in a body of water, the data representing seismic amplitude detected by the sensors with respect to time in response to actuation of a seismic energy source;

(b) specifying an output time-rate (Δ

T′

) that is an integer multiple of the input time rate Δ

T;

(c) specifying a data analysis window (Δ

t) that is larger than the output time rate (Δ

T′

), wherein the analysis window is an integer multiple of said Δ

T;

(d) specifying a frequency sample rate (Δ

f);

(e) computing in a processor a time window (2/Δ

f) that would produce the frequency said sample and is an integer multiple of the input time rate (Δ

T);

(f) generating a model in a processor that extrapolates data inside the data analysis window to fill the (2/Δ

f) time window, wherein

(g) the model uses a continuity relationship between data within and outside of the data analysis (Δ

t) window,

(h) the model has the property that forward and backward extrapolated values decrease in amplitude with respect to time from edges of the data analysis (Δ

t) window;

(i) capturing data within the data analysis (Δ

t) window at a start of data time;

(j) extrapolating in forward and backward directions the captured data in the processor to fill the (2/Δ

f) time window;

(k) computing fast Fourier transform (FFT) coefficients in the processor of data in the (2/Δ

f) time window;

(l) incrementing by the output sample time (Δ

T)′

the start time of data capture for a next FFT computation;

(m) repeating (i) through (l) until and end of data time is reached; and

at least one of

(n) saving in a storage medium the FFT coefficients sampled at (Δ

T′

,Δ

f) intervals, and

(o) saving in the storage medium a transformation of the FFT coefficients into amplitude and phase spectra sampled at (Δ

T′

,Δ

f) intervals.

5. The method of claim 4 wherein:

(a) the mathematical model is a statistical Linear Prediction Filter (LPF) model,

(b) the continuity relationship is an autocorrelation function with a maximum lag, Lmax, of said seismic data in a time window of length, (2/Δ

f), that is symmetrically centered relative to a moving said data time window of length Δ

t, and

(c) the forward extrapolation is done with repeated application of a minimum phase filter derived via Levinson recursion from the autocorrelation function and backward extrapolation is done with repeated application of the time reversed version of the minimum phase filter.

6. The method of claim 5 further comprising:

(a) computing an auto-correlation function in the processor of the data in a (2/Δ

f) window to determine statistical correlation between the data within and outside of the signal analysis window,

(b) using the auto-correlation function to compute LP coefficients in the processor via Levinson recursion and linearly combining said coefficients with analysis window in a recursive loop for extrapolations in the forward direction and then repeating said linear combination with the reversed sequence of said coefficients for extrapolations in the backward direction,

(c) specifying a plurality of multi-resolution data analysis windows, where each of the multi resolution data analysis windows has a different length, wherein the length thereof is in a range from Δ

t to a fraction of (2/Δ

f),

(d) initializing a start of spectral computation time,

(e) capturing data in the processor within the plurality of multi-resolution signal analysis windows, each centered at the spectral computation time,

(f) computing a sequence of LP coefficients in the processor for each multi-resolution window,

(g) time extrapolating captured data in the processor in each of the multi-resolution windows in forward and backward directions to fill the (2/Δ

f)-window,

(h) averaging data in the processor over plurality of multi-resolution extrapolated (2/Δ

f)-windows,

(i) computing FFT coefficients in the processor of data in said average (2/Δ

f)-window,

(j) incrementing spectral computation time by said Δ

T′

,

(k) repeating steps (e) through (j) until an end of spectral computation time,

(l) at least one of storing said FFT coefficients as 2-dimensional arrays sampled at (Δ

T′

,Δ

f) intervals and saving in said storage medium a transformation of said FFT coefficients into amplitude and phase spectra as 2-dimensional arrays sampled at (Δ

T′

,Δ

f) intervals, and

(m) displaying the amplitude and phase spectra as 2-dimensional images on an interactive graphical screen.