Method and system for generating geophysical data

Patent metadata

Field	Value
Publication number	US-11269093-B2
Application number	US-202016998085-A
Country	US
Kind code	B2
Filing date	Aug 20, 2020
Priority date	Oct 1, 2015
Publication date	Mar 8, 2022
Grant date	Mar 8, 2022

Abstract

A method of generating geophysical data using at least one source. The method may include the steps of generating a geophysical wavefield with a varying signature using at least one source, wherein the signature is varied in a periodic pattern.

First claim

We claim:

1. A method of generating geophysical data using at least one source, the method comprising:
generating a geophysical wavefield with a varying signature using at least one source,
wherein the signature is varied in a periodic pattern;
recording geophysical energy to produce geophysical data using at least one receiver, the geophysical energy comprising the propagating geophysical wavefield generated at the at least one source; and
transforming the geophysical data into another domain;
wherein the other domain is a domain such that at least some of the geophysical data is shifted to a location that is different to the location in the other domain where the at least some of the geophysical data would have been had the varying signature not been used.

2. The method as claimed in claim 1 , wherein the at least one source is an airgun source, an airgun source array, a watergun source, a flip/flop source, or an electric and/or magnetic source.

3. The method as claimed in claim 1 , further comprising:
isolating the geophysical data originating from the propagating geophysical wavefield generated at the at least one source from any other geophysical data that may be present in the other domain.

4. The method as claimed in claim 3 , further comprising transforming the isolated geophysical data back into the domain in which the geophysical data was recorded.

5. The method as claimed in claim 3 , further comprising:
conditioning the isolated data so as to effectively remove the varying signature pattern from the recorded geophysical data.

6. The method as claimed in claim 5 , wherein the conditioning step occurs in the other domain or in the domain in which the geophysical data was recorded.

7. The method as claimed in claim 1 , further comprising:
recording geophysical energy to produce geophysical data using at least one receiver, the geophysical energy comprising the propagating geophysical wavefield generated at the at least one source; and
isolating the geophysical data originating from the propagating geophysical wavefield generated at the at least one source from any other geophysical data that may be present in the other domain.

8. The method as claimed in claim 1 , wherein the periodic pattern is such that, after transforming the recorded geophysical data into another appropriate domain, a first portion of the recorded geophysical data originating from the propagating geophysical wavefield generated by the at least one source would be shifted relative to a second portion of the recorded geophysical data originating from the propagating geophysical wavefield generated by the at least one source,
and the method comprises:
identifying the first portion; and
processing the data to calculate a full data signal at the shifted location of the first portion using the identified first portion and/or to remove the second portion of the data using the identified first portion.

9. The method as claimed in claim 1 , wherein the signature is varied using time dither and the varying time dither is that every second geophysical wavefield generated by the at least one source is triggered with a constant delay of time T.

10. The method as claimed in claim 1 , wherein the signature is varied by varying the polarity and the varying polarity is that every second geophysical wavefield generated by the at least one source has opposite polarity.

11. The method as claimed in claim 1 , comprising selecting the varying signature of the at least one source such that, once geophysical energy comprising the generated geophysical wavefield and another signal is recorded and the recorded geophysical data is transformed into another appropriate domain, the recorded geophysical data originating from the generated geophysical wavefield would be shifted away from recorded geophysical data originating from the other signal.

12. The method as claimed in claim 11 , wherein the other signal arises from noise, interference, or one or more other sources.

13. The method as claimed in claim 1 , wherein at least two sources are used to simultaneously generate geophysical wavefields, the first source having a varying signature in a periodic and the second source having no varying signature in a periodic, or having a different varying signature in a periodic pattern and/or wherein the method comprises selecting the varying signature such that, once the geophysical data is recorded and transformed into another domain, a pressure wave portion of the geophysical data will be at least partially shifted away from a shear wave portion of the geophysical data.

14. The method as claimed in claim 1 , the method comprising selecting the varying signature such that, once the recorded geophysical data is recorded and transformed into another domain, the portion of the recorded geophysical data originating from the generated wavefield would be at least partially shifted away from an interference portion of the recorded geophysical data.

15. The method as claimed in claim 14 , wherein the signature is varied using time dither, and wherein the interference portion has a dominant frequency, and the method comprises using a time dither of approximately the same as, a half of or a quarter of the period of the dominant frequency.

16. The method as claimed in claim 1 , the method comprising selecting the varying signature such that, once the geophysical data is recorded and transformed into another domain, a residual shot noise portion of the recorded geophysical data would be at least partially shifted away from the portion of the geophysical data originating from the generated geophysical wavefield.

17. The method as claimed in claim 16 , wherein the signature is varied using time dither, and wherein the residual shot noise portion has a dominant frequency, and the method comprises using a time dither of approximately the same as, a half of or a quarter of the period of the dominant frequency of the residual shot noise.

18. The method as claimed in claim 16 , wherein the signature is varied by varying the polarity, and wherein the residual shot noise portion has a dominant frequency, and the periodic pattern of the varying polarity of sequentially generated geophysical wavefields is: a second generated geophysical wavefield having the same polarity as a first generated geophysical wavefield, a third generated geophysical wavefield having opposite polarity to the second generated geophysical wavefield, a fourth generated geophysical wavefield having the same polarity as the third generated geophysical wavefield, a fifth generated geophysical wavefield having opposite polarity to the fourth generated geophysical wavefield, a sixth generated geophysical wavefield having the same polarity as the fifth generated geophysical wavefield, (i.e. +1, +1, −1, −1, +1, +1, −1, −1).

19. The method as claimed in claim 1 , wherein the time between generating subsequent geophysical wavefields is less than the time taken for the geophysical wavefield energy originating from each generated geophysical wavefield to be recorded by the receiver, the method comprising identifying the data in a given trace originating from a geophysical wavefield generated previously to the trigger time of the given trace, and adding this identified data to data on a previous trace originating from the same geophysical wavefield.

20. The method as claimed in claim 1 , comprising reducing the width of the data signal originating from the at least one source in the other domain.

21. The method

Assignees

• Equinor Energy As

Inventors

• Amundsen Lasse
• Robertsson Johan Olof Anders

Classifications

• G01V3/083

  Controlled source electromagnetic [CSEM] surveying · CPC title

• G01V1/364

  Seismic filtering (G01V1/37 takes precedence) · CPC title

• G01V3/00

  Electric or magnetic prospecting or detecting; Measuring magnetic field characteristics of the earth, e.g. declination, deviation · CPC title

• G01V11/00 Primary

  Prospecting or detecting by methods combining techniques covered by two or more of main groups G01V1/00 - G01V9/00 · CPC title

• G01V2210/46

  Radon transform · CPC title