Seismic migration method and device for steep-dip stratums and fractures

A steep dip, stratigraphic technology, applied in seismic signal processing and other directions, can solve the problems of extremely high accuracy of velocity models, inability to achieve dual-reflection wave migration imaging, inability to provide velocity modeling methods, etc., to achieve good amplitude preservation and The effect of lateral shift adaptability

Active Publication Date: 2012-07-04
PETROCHINA CO LTD
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AI Technical Summary

Problems solved by technology

[0005] First of all, the traditional Kirchhoff integration method and the one-way wave prestack depth migration method can only image one reflection wave due to the limitation of their own algorithms, and cannot realize the migration imaging of double reflection waves related to steep-dipping formations and fractures;
[0006] Secondly, although reverse time migration is based on the direct solution of the two-way acoustic wave equation, it can accurately image different types of seismic waves including double reflection waves, and has no dip angle limitation, but in the face of actual seismic data with steep dip angles There are still many difficulties in fracture migration imaging: because reverse time migration is full-wavefield imaging, the energy of the primary reflection wave is not suppressed, and the energy of the primary wave is much stronger than that of the double reflection wave, which will cover up the The imaging energy of double-reflection waves related to steep-dipping fractures; at the same time, reverse time migration requires a very large amount of calculation and requires extremely high accuracy of the velocity model, but reverse time migration itself cannot provide an effective velocity modeling method

Method used

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  • Seismic migration method and device for steep-dip stratums and fractures
  • Seismic migration method and device for steep-dip stratums and fractures
  • Seismic migration method and device for steep-dip stratums and fractures

Examples

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example 1

[0108] Such as Figure 3a Shown is a formation velocity model with a steep dip angle, in which the velocity of the first formation 31 is 2000 m / s, and the velocity of the second formation 32 is 4000 m / s. Using the conventional Kirchhoff integration method and the one-way wave prestack depth migration method can only The imaging of the first horizontal reflection interface 34 and the second horizontal reflection interface 35 is obtained, but the formation interface 33 with a steep dip angle cannot be imaged. and Figure 3b Shown is the corresponding double-reflection prestack depth migration results of the model. It can be seen that the method of the present invention can well realize the imaging of the strata with steep dip angles. Imaging of reflective interfaces.

example 2

[0110] Such as Figure 4a Shown is the fracture velocity model, wherein the velocity of the first formation 41 is 1500 m / s, the velocity of the second formation 42 is 3500 m / s, and the fracture 43 is filled according to the actual conditions of the gas-bearing medium, the specific filling conditions As shown in Table 1:

[0111] Table 1

[0112]

[0113] Using the conventional Kirchhoff integration method and the one-way wave prestack depth migration method can only obtain the imaging of the horizontal reflection interface 44 , but cannot image the fracture 43 . and Figure 4b Shown is the double-reflection prestack depth migration result corresponding to the fracture model, and it can be seen that the method of the embodiment of the present invention can well realize imaging for fractures.

[0114] The embodiment of the present invention utilizes the double-reflection pre-stack migration method to realize seismic imaging for strata with steep dip angles and fractures. ...

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Abstract

The invention provides a seismic migration method and device for steep-dip stratums and fractures. The method comprises the following steps: inputting seismic data; defining an underground horizontal reflection layer of a foundation; generating CDG (common detector gather) seismic data; carrying out layer-by-layer continuation processing on CSG (common-shot-gather) seismic data by using an amplitude-preserved Fourier finite-difference continuation operator; calculating travel time in the migration of a HV-type dual-reflected wave by using a finite-difference travel-time calculating method; carrying out layer-by-layer imaging on the HV-type dual-reflected wave; carrying out layer-by-layer continuation processing on the CDG seismic data by using the amplitude-preserved Fourier finite-difference continuation operator; calculating travel time in the migration of a VH-type dual-reflected wave by using the finite-difference travel-time calculating method; carrying out layer-by-layer imaging on the VH-type dual-reflected wave; carrying out superimposed imaging on the migration results of the HV-type dual-reflected wave and the VH-type dual-reflected wave so as to obtain an imaging result of steep-dip stratums and fractures in a target zone. The method disclosed by the invention has high calculation efficiency and can be used for obtain a high-quality imaging result of steep-dip stratums and fractures.

Description

technical field [0001] The present invention relates to a seismic data pre-stack depth migration imaging method for steep-dip strata and fractures, specifically a seismic migration method and device for steep-dip strata and fracture imaging using a double-reflection pre-stack migration method . Background technique [0002] For a long time, the problem of seismic imaging of steep-dip strata and fractures has been the bottleneck restricting the process of seismic exploration in complex structural areas, especially fracture imaging is of great significance for natural gas exploration. There are many difficulties when imaging problems. [0003] The traditional prestack depth migration method generally uses the primary reflection wave for imaging, and treats other types of seismic waves as noise. The so-called primary reflection wave such as Figure 1a As shown, the propagation path of its wave field is: shot point 10-underground reflection layer 12-receiver point 14. If one re...

Claims

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Application Information

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Patent Type & Authority Applications(China)
IPC IPC(8): G01V1/28
Inventor 王宇超吕彬雍学善胡自多苏勤
Owner PETROCHINA CO LTD
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