Method and system for generating geophysical data

US10788596B2 · US · B2

Patent metadata
FieldValue
Publication numberUS-10788596-B2
Application numberUS-201615764461-A
CountryUS
Kind codeB2
Filing dateSep 30, 2016
Priority dateOct 1, 2015
Publication dateSep 29, 2020
Grant dateSep 29, 2020

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Abstract

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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

Opening claim text (preview).

We claim: 1. A method of generating geophysical data using at least one airgun source, the method comprising: generating a geophysical wavefield with a varying signature using the at least one airgun source, wherein the signature of the geophysical wavefield is varied in a periodic pattern by using a deterministic variation of a signature of the at least one airgun source; and using a deterministic variation of the signature of the at least one airgun source comprises varying at least one of: the time at which the geophysical wavefield is generated by the at least one airgun source: the polarity of the at least one airgun source; the phase of the at least one airgun source; and the amplitude of the at least one airgun source. 2. A method as claimed in claim 1 , further comprising: recording geophysical energy to produce geophysical data using at least one receiver, the geophysical energy comprising a propagating geophysical wavefield generated at the at least one source; 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; 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. 3. A method as claimed in claim 2 , further comprising transforming the isolated geophysical data back into the domain in which the geophysical data was recorded. 4. A method as claimed in claim 2 , further comprising: conditioning the isolated data so as to effectively remove the varying signature pattern from the recorded geophysical data and/or regularizing the isolated data. 5. A method as claimed in claim 4 , wherein the conditioning step occurs in the other domain or in the domain in which the geophysical data was recorded. 6. A method as claimed in claim 2 , 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. 7. A method as claimed in claim 1 , further comprising: recording geophysical energy to produce geophysical data using at least one receiver, the geophysical energy comprising a 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. A 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. 9. A method as claimed in claim 1 , wherein the signature is varied by varying a polarity and varying polarity is that every second geophysical wavefield generated by the at least one source has opposite polarity. 10. A 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. 11. A method as claimed in claim 10 , wherein the other signal arises from noise, interference, or one or more other sources. 12. A method as claimed in claim 1 , wherein at least two sources are used to simultaneously generate geophysical wavefields, a first source having a varying signature in a periodic and a 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. 13. A 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, a 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. 14. A method as claimed in claim 13 , wherein the signature is varied using time dither, and wherein a 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. 15. A 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. 16. A method as claimed in claim 15 , 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. 17. A method as claimed in claim 15 , wherein the signature is varied by varying a 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, (+1, +1, -1, -1, +1, +1, -1, -1). 18. A method as claimed in claim 1 , wherein a 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 a receiver, the method comprising identifying the data in a given trace originating from a geophysical wavefield generated previously to a trigger time of the given trace, and adding this identified data to data on a previou

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Classifications

  • Controlled source electromagnetic [CSEM] surveying · CPC title

  • specially adapted for seismic systems using continuous agitation of the ground {, e.g. using pulse compression of frequency swept signals for enhancement of received signals} · CPC title

  • Slowness, e.g. tau-pi · CPC title

  • G01V1/005Primary

    with exploration systems emitting special signals, e.g. frequency swept signals, pulse sequences or slip sweep arrangements · CPC title

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

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What does patent US10788596B2 cover?
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.
Who is the assignee on this patent?
Statoil Petroleum As, Equinor Energy As
What technology area does this patent fall under?
Primary CPC classification G01V1/005. Mapped technology areas include Physics.
When was this patent published?
Publication date Tue Sep 29 2020 00:00:00 GMT+0000 (Coordinated Universal Time) (B2). Legal status and post-grant events are not shown on this page.
What related patents are in patentsdb?
We list 8 related publications on this page (citations in our corpus or others sharing the same primary CPC).