Method and device for acquisition of seismic data

• US 4,914,636 A
• Filed: 10/20/1988
• Issued: 04/03/1990
• Est. Priority Date: 10/20/1987
• Status: Expired due to Fees

• Current Assignee: Compagnie Generale De Geophysique
• Original Assignee: Compagnie Generale De Geophysique
• Inventors: Garrotta, Robert J.
• Primary Examiner(s): Tarcza, Thomas H.
• Assistant Examiner(s): Lobo, Ian J.
• Application Number:
  US07/260,279
• Time in Patent Office: 530 Days
• Field of Search: 367/20, 367/48, 367/23, 367/49, 367/56, 367/58, 367/62, 367/41, 181/111, 181/112
• US Class Current: 367/56
• CPC Class Codes: G01V 1/003 Seismic data acquisition in general, e.g. survey design G01V1/3808, G01V1/42 take precedence

Abstract

In a method of acquiring seismic data in a prospecting area, an array of excitation vibration receivers is placed on or over the terrestrial surface. A plurality of excitation vibration sources is disposed in the vicinity of the array, each source emitting excitation vibrations with a frequency spectrum in a specific frequency band. These bands are adjacent and together cover the frequency band of usable seismic data signals. When the excitation vibrations are emitted by the plurality of sources, the excitation vibration echoes reflected from strata beneath the terrestrial surface are registered by the receivers. The above steps are repeated for a plurality of successive trace increment displacements to produce an emission figure and to cover the prospecting area. The method and the device implementing it can be used for acquisition of terrestrial or marine seismic data.

Claims

1. Method of acquiring seismic data in a prospecting area comprising, in order to establish a trace, the steps of:

(a) disposing on or over the terrestrial surface in said prospecting area an array of vibration receivers, said array including at least one row of regularly spaced receivers,

(b) disposing in the vicinity of said array a plurality of vibration sources each adapted to emit vibrations with a frequency spectrum in a specific frequency band, the frequency bands of the spectra of said sources being adjacent and together covering the frequency band of seismic data signals, a high-frequency first source being placed at the center of said array and a low-frequency second source being placed near an end of said array, said first source emitting vibrations at a higher frequency than said second source, said first and second sources having adjacent vibration frequency spectra and being separated by a distance substantially equal to one half the length of said array,

(c) emitting vibrations with different frequency spectra from said first and second sources,

(d) recording said vibrations after reflection from strata beneath the terrestrial surface by means of said receivers,

(e) moving said sources relative to said array in an acquisition direction by a trace displacement increment, and

(f) repeated the above steps (c), (d) and (e) for a plurality of successive movements by said trace displacement increment.

2. Method according to claim 1, wherein said vibrations with different frequency spectra are emitted synchronously.

3. Method according to claim 1, wherein said second source is offset towards the exterior of said array.

4. Method according to claim 1, where said array is adapted for two-dimensional multirow acquisition and comprises a plurality of parallel rows of receivers and said vibration sources are in a line parallel to said rows of receivers.

5. Method according to claim 1, wherein said array is adapted for two-dimensional multisource acquisition and comprises a central row of receivers and parallel first and second source displacement lines.

6. Method according to claim 5, wherein a high-frequency first source is placed on said first line and a low-frequency second source is placed on said second line and said first and second sources are alternated after each trace displacement increment movement along said first and second lines.

7. Method according to claim 4, wherein said array is adapted for three-dimensional acquisition and comprises a plurality of parallel rows of receivers perpendicular to the direction in which said sources are moved.

8. Method according to claim 1, wherein to cover all or part of said prospecting area said array of receivers and said sources are moved by a displacement increment in a direction of advance.

9. Device for acquisition of seismic data in a prospecting area comprising on or over the terrestrial surface in said prospecting area:

an array of vibration receivers; and

a plurality of vibration sources each adapted to emit vibrations with a frequency spectrum in a specific frequency band, the frequency bands of the spectra of said sources being adjacent and together covering the frequency band of seismic data signals, said plurality of sources comprising a first source placed at the center of said array and a second source placed near an end of said array, said first source emitting vibrations at a higher frequency than said second source emissions, said first and second sources having adjacent vibration frequency spectra and being separated by a distance substantially equal to one half the length of said array.

10. Device according to claim 9, wherein said array comprises one or more rows of receivers.

11. Device according to claim 9, wherein said

first source is adapted to emit vibrations with a frequency spectrum in a frequency band between 20 Hz and 80 Hz;

and

said second source is adapted to emit vibrations with a frequency spectrum between 8 Hz and 20 Hz.

12. Device according to claim 9, wherein each receiver comprises a set of interconnected geophones and said receivers are spaced by a specific distance.

13. Device according to claim 9, further comprising means for capturing and processing in digitized form said reflected vibrations according to their corresponding emission frequency bands, in the form of a fire control and processing computer and associated peripheral devices.

14. Device according to claim 13, wherein said capture and processing means include a working memory of said computer and in said working memory:

a subroutine commanding recording of the reflected low-frequency vibrations with a first spatial sampling whereby the geophones or groups of geophones commanded to record said low-frequency vibrations are separated by a distance n×

e where e represents the distance between two adjacent groups of geophones and n is a specific integer,

a subroutine for commanding recording of the reflected high-frequency vibrations with a second spatial sampling, where said second spatial sampling is denser than said first spatial sampling, the geophones or groups of geophones commanded to record said high-frequency vibrations being separated by said distance e,

a subroutine for correlating said reflected low-frequency vibrations with the emission signal of said low-frequency vibrations with the emission signal of said low-frequency source to generate a plurality of low-frequency data, and

a subroutine for correlating said reflected high-frequency vibrations with the emission signal of said high-frequency source to generate a plurality of high-frequency data.

15. Device according to claim 14, wherein said capture and processing means further comprise in said working memory of said computer a subroutine for aligning phase spectra of said low-frequency data and said high-frequency data.

16. Device according to claim 14, wherein said capture and processing means further comprise a subroutine for aligning amplitude spectra of said low-frequency data and said high-frequency data to enable weighting of the amplitude spectra of said high-frequency data and said low-frequency data to re-establish the equilibrium of the total amplitude spectrum across the range of frequencies.

17. Device according to claim 16, wherein said weighting is applied allowing for the number NV_H of low-frequency sources, the effective emission lengths L_B and L_H of the low-frequency and high-frequency sources, respectively, and the order of additions S_H and S_B, a correction coefficient K being applied to the high-frequency amplitude weighting coefficient β

_H given by the equation;

space="preserve" listing-type="equation">β

.sub.H =NV.sub.H ×

L.sub.H ×

S.sub.H

whereby said correction coefficient K, said high-frequency amplitude weighting coefficient β

_H and said low-frequency amplitude weighting coefficient β

_B given by the equation;

space="preserve" listing-type="equation">β

.sub.B =NV.sub.B ×

L.sub.B ×

S.sub.B

satisfy the equation;

space="preserve" listing-type="equation">K×

β

.sub.H =β

.sub.B.

18. Device according to claim 14 further comprising in said working memory of said computer a subroutine for linear interpolation of (n-1) dummy low-frequency data acquisitions between two consecutive low-frequency acquisitions so as to be able to combine the interpolated stream of dummy data with the corresponding high-frequency data.

19. Device according to claim 18, further comprising in said working memory of said computer a subroutine for combining by summing or weighted summing said high-frequency and said low-frequency data, the optimum low-frequency plus high-frequency information being recovered by adding the stream of low-frequency data and interpolated low-frequency data to the stream of high-frequency data.

20. Device according to claim 19, wherein said computer further comprises in said working memory a subroutine for weighting low-frequency signals, weighted low-frequency signals, high-frequency signals operands, said weighting subroutine enabling prior to said addition the application of multiplication coefficients variable in time and representing different absorption by the environment of the reflected vibrations according to their mean frequency in the frequency band in question.