CN114942472A - Offset imaging method and equipment based on uplink ray tracing strategy - Google Patents

Offset imaging method and equipment based on uplink ray tracing strategy Download PDF

Info

Publication number
CN114942472A
CN114942472A CN202210330865.9A CN202210330865A CN114942472A CN 114942472 A CN114942472 A CN 114942472A CN 202210330865 A CN202210330865 A CN 202210330865A CN 114942472 A CN114942472 A CN 114942472A
Authority
CN
China
Prior art keywords
imaging
ray tracing
seismic
uplink
shot
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
CN202210330865.9A
Other languages
Chinese (zh)
Inventor
黄建平
张东林
杨继东
苏来源
徐洁
杨秀金
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
China University of Petroleum East China
Original Assignee
China University of Petroleum East China
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by China University of Petroleum East China filed Critical China University of Petroleum East China
Priority to CN202210330865.9A priority Critical patent/CN114942472A/en
Publication of CN114942472A publication Critical patent/CN114942472A/en
Pending legal-status Critical Current

Links

Images

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01VGEOPHYSICS; GRAVITATIONAL MEASUREMENTS; DETECTING MASSES OR OBJECTS; TAGS
    • G01V1/00Seismology; Seismic or acoustic prospecting or detecting
    • G01V1/28Processing seismic data, e.g. for interpretation or for event detection
    • G01V1/282Application of seismic models, synthetic seismograms

Landscapes

  • Engineering & Computer Science (AREA)
  • Remote Sensing (AREA)
  • Physics & Mathematics (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Acoustics & Sound (AREA)
  • Environmental & Geological Engineering (AREA)
  • Geology (AREA)
  • General Life Sciences & Earth Sciences (AREA)
  • General Physics & Mathematics (AREA)
  • Geophysics (AREA)
  • Geophysics And Detection Of Objects (AREA)

Abstract

The invention discloses an offset imaging method and equipment based on an uplink ray tracing strategy, and relates to the technical field of geological exploration. The imaging steps are as follows: s1: acquiring input parameters, wherein the input parameters comprise a P-wave velocity parameter field, an anisotropy parameter field and an observation shot record; s2: generating a shot point x by adopting the following imaging expression according to the input parameters s Corresponding imaging results. The method can solve the false image problem of the traditional frequency domain Gaussian beam migration imaging method, can enable the diffracted wave energy to be more convergent, further generates a clearer imaging result, develops the time-space domain VTI medium Gaussian beam migration imaging technology based on the uplink ray tracing strategy, provides high-precision imaging guarantee for the seismic data processing of a complicated structural area, and improves the quality and reliability of subsequent interpretation work.

Description

Offset imaging method and equipment based on uplink ray tracing strategy
Technical Field
The invention relates to the technical field of geological exploration, in particular to an offset imaging method based on an uplink ray tracing strategy.
Background
Conventional frequency domain gaussian beam migration methods may produce weak illumination and strong artifacts in complex deep structures due to inaccuracies in paraxial ray tracing of the backward wavefield. For the traditional time-space domain acoustic wave medium Gaussian beam migration method, the complexity of the underground medium is not considered, so that diffracted wave energy is not converged, and the imaging result is poor. Therefore, in order to obtain a high-precision imaging result, it is necessary to further increase the diffracted wave energy.
Based on the method, the invention provides a time-space domain VTI medium Gaussian beam offset imaging method based on an uplink ray tracing strategy.
Disclosure of Invention
The present invention is directed to provide an offset imaging method based on an up-ray tracing strategy, so as to solve the problems mentioned in the background art.
In order to achieve the purpose, the invention provides the following technical scheme: an offset imaging method based on an uplink ray tracing strategy comprises the following imaging steps:
s1: acquiring input parameters, wherein the input parameters comprise a P-wave velocity parameter field, an anisotropy parameter field and an observation shot record;
s2: generating a shot point x by adopting the following imaging expression according to the input parameters s The corresponding imaging results are:
Figure BDA0003570849490000021
wherein, I (x) 0 ) Representing the result of offset imaging, i being the unit of an imaginary number, ω m For observing dominant frequencies, x, of the data s Indicating shot point, x r In order to receive the coordinates of the point,
Figure BDA0003570849490000022
is the attitude, P U For observing the shot record, ω is the circular frequency of the seismic wavelet, t is the propagation time of the seismic wavelet, τ is the travel time, P(s), Q(s) are the basic solutions of the dynamical ray tracing equation, n is the normal direction of the ray coordinate system, p is the normal direction of the ray coordinate system z For slowness in the Z direction,. epsilon.is the initial parameter of the Gaussian beam,. v is the propagation velocity of the seismic wave, and s isTangential direction of ray coordinate system, s 0 Is a tangential coordinate value of the initial position, () * Represents a conjugation;
s3: and (4) superposing the imaging results corresponding to the shot points, and generating and outputting an offset imaging result.
In the present embodiment, preferably, the imaging expression described in step S2 is obtained in advance based on the following steps:
n1: in a two-dimensional ray coordinate system (s, n), considering the acoustic medium, the seismic forward wavefield, represented by a Gaussian beam, is then represented as:
Figure BDA0003570849490000023
wherein, W (1) Is a seismic forward wavefield;
n2: kinetic ray tracing under a VTI medium is utilized to obtain Gaussian beam amplitude and travel time information;
n3: the backward propagation process from the receiving point to the underground imaging point according to the observation shot record can be realized by an uplink ray tracing strategy, and the seismic backward wave field can be expressed as:
Figure BDA0003570849490000024
wherein, W (2) Is the seismic backward wave field, T is the total time of seismic wave propagation, G is the Green function, T 0 Is an initial time, x 0 Is a point of imaging in the ground,
under high frequency approximation, the derivative expression of the green function can be simplified as:
Figure BDA0003570849490000031
n4: an expression that approximately characterizes the green's function is made using a superimposed form of a series of gaussian bundles:
Figure BDA0003570849490000032
the seismic backward wavefield can be simplified to:
Figure BDA0003570849490000033
the time domain part of the expression is transformed by fourier transform:
Figure BDA0003570849490000034
n5: in a time window, when the phase of the positive wave field and the phase of the negative wave field are the same, the cross-correlation output of the positive wave field and the negative wave field reaches the maximum value, and the noise influence is reduced by superposing multi-shot data, so that a time-space domain VTI medium Gaussian beam migration method formula based on an uplink ray tracing strategy can be obtained:
Figure BDA0003570849490000035
wherein t ∈ [ t ] 1 ,t 2 ]Represents a time window;
and substituting the positive and negative wave field expressions to obtain a final imaging expression.
In this embodiment, preferably, the dynamic ray tracing equation under the VTI medium in step N2 is:
Figure BDA0003570849490000036
wherein W, V, H are respectively:
Figure BDA0003570849490000041
wherein p is n G is a path function for slowness in the normal direction.
In combination with the above offset imaging method based on the upward ray tracing policy, the technical solution of the present invention further provides an electronic device, which includes a memory, a processor, and a computing program stored in the memory and capable of being executed on the processor, wherein when the processor executes the computing program, the above offset imaging method based on the upward ray tracing policy is implemented.
Compared with the prior art, the invention has the beneficial effects that:
the migration imaging method based on the uplink ray tracing strategy can solve the false image problem of a traditional frequency domain Gaussian beam migration imaging method, enables diffracted wave energy to be more convergent, further generates a clearer imaging result, develops a time-space domain VTI medium Gaussian beam migration imaging technology based on the uplink ray tracing strategy, provides high-precision imaging guarantee for seismic data processing of a complex structure area, and improves quality and reliability of subsequent interpretation work.
Drawings
FIG. 1 is a schematic flow chart provided by an embodiment of the present disclosure;
FIG. 2 is a true velocity field of the dimple model;
FIG. 3 is an anisotropy parameter field ε of the dimple model;
FIG. 4 is an anisotropy parameter field δ of the dimple model;
FIG. 5 is an anisotropic observation initial shot record of the dimple model;
FIG. 6 shows the result of Gaussian beam shift imaging of a conventional frequency domain VTI medium;
FIG. 7 shows the time-space domain acoustic medium Gaussian beam shift imaging results;
fig. 8 shows the imaging results provided in the examples of the present specification.
Detailed Description
In order to make the objects, technical solutions and advantages of the present application more apparent, the technical solutions of the present application will be described in detail and completely with reference to the following specific embodiments of the present application and the accompanying drawings. It should be apparent that the described embodiments are only some of the embodiments of the present application, and not all of the embodiments. All other embodiments obtained by a person skilled in the art based on the embodiments in the present specification without any inventive step are within the scope of the present application.
First, the implementation of the upstream ray tracing policy and the VTI medium used in the embodiments of the present specification will be specifically explained.
In a two-dimensional ray coordinate system (s, n), considering the acoustic medium, the seismic forward wavefield, represented by a Gaussian beam, can be written as:
Figure BDA0003570849490000051
wherein, W (1) For the seismic forward wavefield, i is in imaginary units,
Figure BDA0003570849490000052
is the space azimuth angle, omega is the circular frequency of the seismic wavelet, epsilon is the initial parameter of the Gaussian beam, v is the propagation velocity of the seismic wave, s is the tangential direction of the ray coordinate system, n is the normal direction of the ray coordinate system, s 0 The tangential coordinate value of the initial position, t is the propagation time of the seismic wavelet, tau is the travel time, and P(s), Q(s) are the basic solutions of the dynamic ray tracing equation.
In an isotropic medium, ray center coordinate systems are mutually orthogonal, but when the anisotropic medium is considered, the ray direction is no longer perpendicular to a wave front surface, at this time, if the isotropic ray tracing theory is continuously adopted, travel time and amplitude information calculation are inaccurate, and finally the precision of the offset imaging result of the text is reduced, so that a weight along the ray direction needs to be introduced to process the non-orthogonality, the related parameter information of the ray tracing calculation is relatively accurate, the central ray wave field proximity of the VTI medium is further accurately constructed, favorable conditions are provided for the subsequent offset imaging result, and a dynamic ray tracing equation set under the VTI medium is considered:
Figure BDA0003570849490000061
wherein W, V, H is:
Figure BDA0003570849490000062
wherein p is n For slowness in the normal direction, G is a function of the degree.
The backward propagation process from the receiving point to the underground imaging point according to the observation shot record can be realized by an uplink ray tracing strategy, and the seismic backward wave field can be expressed as:
Figure BDA0003570849490000063
wherein, W (2) Is the seismic backward wavefield, T is the total time of seismic wave propagation, x r To receive point coordinates, P U For observing shot records, G is the Green function, t 0 Is an initial time, x 0 Is a subsurface imaging point.
Under high frequency approximation, the derivative expression of the green function can be simplified as:
Figure BDA0003570849490000064
wherein, ω is m For observing the dominant frequency, p, of the data z Is the slowness in the Z direction.
An expression that approximately characterizes the green's function is made using a superimposed form of a series of gaussian bundles:
Figure BDA0003570849490000065
the seismic backward wavefield can be simplified to:
Figure BDA0003570849490000066
the time domain part of the expression is transformed by fourier transform:
Figure BDA0003570849490000071
wherein (C) * Representing conjugation.
In the offset algorithm, the imaging conditions are very critical, and the final imaging quality is directly influenced. In a time window, when the phase of the positive wave field and the phase of the negative wave field are the same, the cross-correlation output of the positive wave field and the negative wave field reaches the maximum value, and the noise influence is reduced by superposing multi-shot data, so that a time-space domain VTI medium Gaussian beam migration method formula based on an uplink ray tracing strategy can be obtained:
Figure BDA0003570849490000072
wherein, I (x) 0 ) Representing offset imaging results, x s Denotes the shot point, t ∈ [ t [ ] 1 ,t 2 ]Representing a time window.
Substituting the positive and negative wave field expression to obtain the final I (x) 0 ) The expression is as follows:
Figure BDA0003570849490000073
the above sections specifically describe the implementation of the VTI medium and the upstream ray tracing strategy used in the embodiments of the present specification.
Based on the foregoing, an embodiment of the present specification provides a time-space domain VTI medium gaussian beam offset imaging method based on an uplink ray tracing strategy, which specifically includes:
s1: acquiring input parameters, wherein the input parameters comprise a P-wave velocity parameter field, an anisotropy parameter field and an observation shot record;
s2: generating a shot point x by adopting the following imaging expression according to the input parameters s The corresponding imaging results are:
Figure BDA0003570849490000081
wherein, I (x) 0 ) Representing the result of offset imaging, i being the unit of an imaginary number, ω m For observing dominant frequencies, x, of the data s Indicating shot point, x r In order to receive the coordinates of the point,
Figure BDA0003570849490000082
is the attitude, P U For observing the shot record, ω is the circular frequency of the seismic wavelet, t is the propagation time of the seismic wavelet, τ is the travel time, P(s), Q(s) are the basic solutions of the dynamical ray tracing equation, n is the normal direction of the ray coordinate system, p is the normal direction of the ray coordinate system z For slowness in the Z direction,. epsilon.is the initial parameter of the Gaussian beam,. v.is the propagation velocity of the seismic wave,. s.is the tangential direction of the ray coordinate system,. s 0 Is a tangential coordinate value of the initial position, () * Represents a conjugation;
s3: and superposing the imaging results corresponding to the shot points, and generating and outputting an offset imaging result.
As shown in fig. 1, the process specifically includes the following steps:
acquiring input parameters, wherein the input parameters comprise a P-wave velocity parameter field, an anisotropy parameter field and an observation shot record;
calculating travel time and amplitude information of a Gaussian beam under a VTI medium by an anisotropic ray tracing theory;
and superposing the multi-shot data by using the offset imaging formula to obtain an imaging result.
A description of the practical effects of the embodiments of the present invention in the model is given below.
The method provided by the invention is applied to imaging of a hollow model, and a relatively ideal imaging effect is achieved. The real velocity model (shown in fig. 2, namely, the P-wave velocity parameter field), the anisotropy parameter field epsilon (shown in fig. 3), and the anisotropy parameter field delta (shown in fig. 4); establishing a mobile receiving observation system, and inputting a real velocity field and an observation shot record obtained by anisotropic forward modeling (a first shot result is shown in figure 5); and cross-correlating the forward-transmission wave field and the backward-transmission wave field by adopting a cross-correlation imaging condition to obtain a traditional frequency domain VTI medium Gaussian beam migration imaging result (shown in figure 6), a time-space domain acoustic wave medium Gaussian beam migration imaging result (shown in figure 7) and an imaging result provided by the embodiment of the specification (shown in figure 8).
In fig. 6, the frequency domain gaussian beam shifting method produces some shifting artifacts (shown by the arrows). In fig. 7 and 8, it can be seen that all reflection interfaces can be clearly imaged due to the upward ray tracing strategy adopted by the temporal backward wave field. Compared with the Gaussian beam shift imaging result of the time-space domain acoustic wave medium, the energy of the anisotropic diffraction layer is more converged (shown in a box of FIG. 8).
Correspondingly, an embodiment of the present application further provides an electronic device, which includes a memory, a processor, and a computer program stored in the memory and executable on the processor, wherein the processor implements the above-mentioned offset imaging method based on the upward ray tracing policy when executing the computer program.
Although embodiments of the present invention have been shown and described, it will be appreciated by those skilled in the art that changes, modifications, substitutions and alterations can be made in these embodiments without departing from the principles and spirit of the invention, the scope of which is defined in the appended claims and their equivalents.

Claims (4)

1. An offset imaging method based on an uplink ray tracing strategy is characterized in that: the imaging steps are as follows:
s1: acquiring input parameters, wherein the input parameters comprise a P-wave velocity parameter field, an anisotropy parameter field and an observation shot record;
s2: generating a shot point x by adopting the following imaging expression according to the input parameters s The corresponding imaging results are:
Figure FDA0003570849480000011
wherein, I (x) 0 ) Representing the result of offset imaging, i being the unit of an imaginary number, ω m For observing dominant frequencies, x, of the data s Indicating shot point, x r In order to receive the coordinates of the point,
Figure FDA0003570849480000012
is attitude angle, P U For observing the shot record, ω is the circular frequency of the seismic wavelet, t is the propagation time of the seismic wavelet, τ is the travel time, P(s), Q(s) are the basic solutions of the dynamical ray tracing equation, n is the normal direction of the ray coordinate system, p is the normal direction of the ray coordinate system z For slowness in the Z direction,. epsilon.is the initial parameter of the Gaussian beam, v is the propagation velocity of the seismic wave, s is the tangential direction of the ray coordinate system, s 0 Is a tangential coordinate value of the initial position, () * Represents a conjugation;
s3: and superposing the imaging results corresponding to the shot points, and generating and outputting an offset imaging result.
2. The offset imaging method based on the up-ray tracing strategy according to claim 1, wherein: the imaging expression described in step S2 is obtained in advance based on the following steps:
n1: in a two-dimensional ray coordinate system (s, n), considering the acoustic medium, the seismic forward wavefield, represented by a Gaussian beam, is then represented as:
Figure FDA0003570849480000013
wherein, W (1) Is a seismic forward wavefield;
n2: the amplitude and travel time information of the Gaussian beam is obtained by using dynamic ray tracing under a VTI medium;
n3: the backward propagation process from the receiving point to the underground imaging point according to the observation shot record can be realized by an uplink ray tracing strategy, and the seismic backward wave field can be expressed as:
Figure FDA0003570849480000021
wherein the content of the first and second substances,W (2) is the seismic backward wave field, T is the total time of seismic wave propagation, G is the Green function, T 0 Is an initial time, x 0 Is a point of imaging in the subsurface,
under high frequency approximation, the derivative expression of the green function can be simplified as:
Figure FDA0003570849480000022
n4: an expression that approximately characterizes the green's function is made using a superimposed form of a series of gaussian bundles:
Figure FDA0003570849480000023
the seismic backward wavefield can be simplified to:
Figure FDA0003570849480000024
the time domain part of the expression is transformed by fourier transform:
Figure FDA0003570849480000025
n5: in a time window, when the phase of the positive wave field and the phase of the negative wave field are the same, the cross-correlation output of the positive wave field and the negative wave field reaches the maximum value, and the noise influence is reduced by superposing multi-shot data, so that a time-space domain VTI medium Gaussian beam migration method formula based on an uplink ray tracing strategy can be obtained:
Figure FDA0003570849480000026
wherein t ∈ [ t ] 1 ,t 2 ]Represents a time window;
and substituting the positive and negative wave field expressions to obtain a final imaging expression.
3. The offset imaging method based on the up-ray tracing strategy according to claim 2, wherein: the system of the dynamic ray tracing equation under the VTI medium described in the step N2 is as follows:
Figure FDA0003570849480000031
wherein W, V, H are respectively:
Figure FDA0003570849480000032
wherein p is n For slowness in the normal direction, G is a function of the degree.
4. An electronic device, characterized in that: comprising a memory, a processor and a computing program stored on the memory and executable on the processor, wherein the processor implements the method according to any of claims 1-3 when executing the computing program.
CN202210330865.9A 2022-03-29 2022-03-29 Offset imaging method and equipment based on uplink ray tracing strategy Pending CN114942472A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN202210330865.9A CN114942472A (en) 2022-03-29 2022-03-29 Offset imaging method and equipment based on uplink ray tracing strategy

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN202210330865.9A CN114942472A (en) 2022-03-29 2022-03-29 Offset imaging method and equipment based on uplink ray tracing strategy

Publications (1)

Publication Number Publication Date
CN114942472A true CN114942472A (en) 2022-08-26

Family

ID=82906894

Family Applications (1)

Application Number Title Priority Date Filing Date
CN202210330865.9A Pending CN114942472A (en) 2022-03-29 2022-03-29 Offset imaging method and equipment based on uplink ray tracing strategy

Country Status (1)

Country Link
CN (1) CN114942472A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN115993650A (en) * 2023-03-22 2023-04-21 中国石油大学(华东) Earthquake interference imaging method based on prismatic waves

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN115993650A (en) * 2023-03-22 2023-04-21 中国石油大学(华东) Earthquake interference imaging method based on prismatic waves
CN115993650B (en) * 2023-03-22 2023-06-06 中国石油大学(华东) Earthquake interference imaging method based on prismatic waves

Similar Documents

Publication Publication Date Title
Wu et al. Directional illumination analysis using beamlet decomposition and propagation
Yan et al. Improving the efficiency of elastic wave-mode separation for heterogeneous tilted transverse isotropic media
CN106932824B (en) The adaptive interlayer multiple suppression method of dimensionality reduction of land seismic prospecting data
CN111290017B (en) Surface wave exploration method for jointly extracting Rayleigh wave frequency dispersion characteristics through seismic electric wave field
CN109946741B (en) Pure qP wave least square reverse time migration imaging method in TTI medium
EA032186B1 (en) Seismic adaptive focusing
CN112327358B (en) Forward modeling method for acoustic seismic data in viscous medium
CN109856679A (en) A kind of anisotropic medium elastic wave Gaussian beam offset imaging method and system
WO2022232572A1 (en) Method and system for high resolution least-squares reverse time migration
CN104570116A (en) Geological marker bed-based time difference analyzing and correcting method
WO2013152221A1 (en) Converting a first acquired data subset to a second acquired data subset
CN112034520A (en) Anisotropic medium dynamic focusing beam offset imaging method and system
CN114942472A (en) Offset imaging method and equipment based on uplink ray tracing strategy
CN112285778B (en) Reverse time migration imaging method for pure qP waves in sticky sound TTI medium
Jia et al. Superwide-angle one-way wave propagator and its application in imaging steep salt flanks
CN110780341B (en) Anisotropic seismic imaging method
CN113866821B (en) Passive source interference offset imaging method and system based on illumination direction constraint
US12000971B2 (en) Method and system for seismic processing using virtual trace bins based on offset attributes and azimuthal attributes
CN113406700B (en) Earth surface active source reflected wave interference imaging method
Zhang et al. One-way wave propagation in the ray-centred coordinate system for vertical transversely isotropic media
CN113820742A (en) Imaging method in visco-acoustic anisotropic medium
Shiranzaei et al. Moho depth variations and Vp/Vs ratio in the Zagros (Iran) from teleseismic converted waves
Kim et al. Efficient extended least-squares reverse time migration based on an excitation amplitude imaging condition
CN113391348B (en) Common reflection point gather construction method and device for prestack inversion
CN114415239B (en) Earthquake reflection wave combined imaging method and system

Legal Events

Date Code Title Description
PB01 Publication
PB01 Publication
SE01 Entry into force of request for substantive examination
SE01 Entry into force of request for substantive examination