CN108535774A - A kind of method and device quickly identifying seismic phase using controlled source excitation seismic signal - Google Patents

A kind of method and device quickly identifying seismic phase using controlled source excitation seismic signal Download PDF

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CN108535774A
CN108535774A CN201810227705.5A CN201810227705A CN108535774A CN 108535774 A CN108535774 A CN 108535774A CN 201810227705 A CN201810227705 A CN 201810227705A CN 108535774 A CN108535774 A CN 108535774A
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seismic
signal
source
controlled source
phase
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CN108535774B (en
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刘康
游庆瑜
李志伟
王宝善
姚华建
肖雪
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Tongji University
Institute of Geology and Geophysics of CAS
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Institute of Geology and Geophysics of CAS
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    • 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. analysis, for interpretation, for correction
    • G01V1/30Analysis
    • G01V1/307Analysis for determining seismic attributes, e.g. amplitude, instantaneous phase or frequency, reflection strength or polarity
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01VGEOPHYSICS; GRAVITATIONAL MEASUREMENTS; DETECTING MASSES OR OBJECTS; TAGS
    • G01V2210/00Details of seismic processing or analysis
    • G01V2210/60Analysis
    • G01V2210/63Seismic attributes, e.g. amplitude, polarity, instant phase

Abstract

The method and device provided by the invention that seismic phase is quickly identified using controlled source excitation seismic signal, the linear frequency modulation seismic signal excited to controlled source using Fourier Transform of Fractional Order carries out quick seismic phase identification, inherit the linear behavio(u)r of conventional Fourier transform, the interference of cross term when can inhibit time frequency analysis well, the time-frequency distributions feature of the linear frequency modulation seismic signal of controlled source excitation can be improved, it is analysis object with impulse function, improve the signal-to-noise ratio of seismic phase, it identifies seismic phase then, more reliable data basis is provided for geologic interpretation.

Description

A kind of method and device quickly identifying seismic phase using controlled source excitation seismic signal
Technical field
The present invention relates to field of seismic exploration, and in particular to a kind of quickly to identify shake using controlled source excitation seismic signal The method and device of phase.
Background technology
In seismic prospecting, observation technology plays a crucial role.It is controllable that accurate controlled source can generate frequency Elastic wave, since frequency accuracy is very high, wave detector can be in the inscribed collection of letters number of very narrow bandwidth;Pass through the precision control of waveform phase System further increases signal-to-noise ratio with Signal averaging technology, realizes that smaller power carries out remote earthquake data acquisition.It is accurate controllable Seismic source apparatus be capable of continuous-stable it is long when operate, compared to man-made explosions such as explosion, hammerings, there is prodigious application prospect.
The seismic signal of controlled source excitation is a kind of linear frequency modulation (Linear Frequency Modulation, LFM) Signal, a signal frequency not instead of definite value, changes, we are difficult to be found from its time-domain with the change of time The seismic phase of certain seismic wave;And traditional Fourier transformation (Fourier Transform, FT) method is utilized, it can not be from its frequency The information of LFM signal parameters is obtained on domain.
Therefore, a kind of quick phase identification method is found, time frequency analysis is carried out to the seismic signal of controlled source excitation, It can just solve the above problems, improve the explanation accuracy of seismic prospecting, in the past in the research of Time-Frequency Analysis Method, Chen Yuhong Deng (2006) comparative analysis Hilbert transform, Hilbert-Huang transform, sine curve fitting, Ricker wavelet matching, in short-term A variety of methods such as Fourier transform, wavelet transformation, and from temporal resolution, frequency resolution, to multi-frequency component signal adapt to The various aspects such as ability elaborate the advantage and disadvantage of various methods.Such as certain nonlinear transformations can bring serious cross term interference, Seriously interfere explanation of the people to signal time-frequency characteristic;For suppressing crossterms, it has to be to sacrifice time frequency resolution Cost, and calculation amount is huge.In addition, above method research is primarily adapted for use in non-linear, non-stationary signal, rather than controllably shake The linear FM signal that source generates.In the signal research excited to controlled source, Yang Wei etc. (2013) has carried out cross-correlation, short Four kinds of methods processing analyses such as Shi Xiangguan, relevant and deconvolution, and respectively from repeatability, walk when section, spectrum signature and letter Make an uproar than etc. research compared and analyzed to handling result, the ground that Primary Study Method of Mathematical Physics excites controlled source The recognition capability of signal is shaken, but various methods have certain limitation, are not well positioned to meet exploration needs.
Invention content
In view of this, a kind of method and device quickly identifying seismic phase using controlled source excitation seismic signal is provided, Using the time-frequency convert of Method of Mathematical Physics, the resolution capability of seismic phase can be improved, and more accurately calculates the arrival time difference of seismic phase, And then more reliable data basis is provided for geologic interpretation, improve the recognition capability of seismic phase.
In a first aspect, the present invention provides a kind of method quickly identifying seismic phase using controlled source excitation seismic signal, institute The method of stating includes:
Using seismic detector acquisition controlled source in the earthquake initial data of research area excitation, the ground of controlled source excitation is obtained Signal S (i, j) is shaken, i indicates that seismographic number, j indicate the number of controlled source excitation;
Using the seismic signal that the seismic detector adjacent with the controlled source acquires as source signal S (0, j), selective exitation Any secondary source signal carry out the time-frequency characteristics of Short Time Fourier Transform analysis source signal, obtain source signal it is effective when Between range and frequency range;
Source signal S (0, j) is intercepted according to effective time range, using discrete cosine transform to the shake after interception Source signal carries out spectrum analysis and extracts the filtered source signal Stf (0, j) of the acquisition of the wavefield signals in effective frequency range;
The optimal rotation that Fourier Transform of Fractional Order calculates source signal is carried out to filtered source signal Stf (0, j) Angle αopt
The seismic signal of controlled source excitation is intercepted according to effective time range, and according to effective frequency model It encloses and is filtered, carry out Fourier Transform of Fractional Order successively using the optimal rotation angle, obtain the shake of different earthquake instrument record Phase;
Arrival time difference and apparent velocity are determined using the seismic phase.
It is described former in the earthquake of research area excitation using seismic detector acquisition controlled source as a kind of possible realization method Beginning data, obtain the seismic signal S (i, j) of controlled source excitation, and i indicates that seismographic number, j indicate controlled source excitation Number, including:
In the preset range of controlled source layout points, one seismic detector is set, it is certain further according to needing to be separated by research area Distance lay seismic detector, according to seismic detector at a distance from controlled source from the near to the remote, it is 0,1,2 that seismic detector, which is numbered, 3 ... ... the natural numbers being sequentially increased;According to the number that controlled source excites, the natural number for being denoted as 1,2,3 ... ... and being sequentially increased; The seismic signal of the controlled source excitation of seismic detector record is denoted as S (i, j), and i indicates that seismographic number, i=0 are indicated controllable Beside focus, j indicates the number of controlled source excitation.
As a kind of possible realization method, the seismic signal acquired with the seismic detector adjacent with the controlled source As source signal S (0, j), any secondary source signal of selective exitation carries out Short Time Fourier Transform, analyzes the focus letter Number time-frequency characteristics, obtain the effective time range and frequency range of the source signal, including:
It is used as source signal with S (0, j), chooses any time in S (0, j) source signal, as third time S (0,3) carries out Short Time Fourier Transform.
Short Time Fourier Transform is carried out using the first formula, S (0,3) is converted into T/F by temporal-spatial field Domain, first formula are:
In formula, STFT (t, f) indicates the time-frequency domain after Short Time Fourier Transform as a result, S (τ) table in integral term Show the time series of source signal, for signal time from 0 to T, g (τ-t) is window function, and window when t is constantly changes t, obtains third The source signal S (0,3) of secondary excitation is in the corresponding frequency f of different t;
The strongest frequency range of energy, origin coordinates is selected to be denoted as (t from T/F area image1,f1), end coordinate It is denoted as (t2,f2), t1~t2As effective time range, f1~f2As effective frequency range, and to all seismic signal S (i, J) it is applicable in.
It is described that the source signal is intercepted according to effective time range as a kind of possible realization method, profit Spectrum analysis is carried out to the source signal after interception with discrete cosine transform and extracts the wavefield signals in effective frequency range being filtered Source signal Stf (0, j) after wave, including:
Any time in S (0, j) source signal is chosen, t is intercepted1~t2The signal of period, is denoted as St (m), and m indicates to cut The sampling number of signal after taking, m=1 ..., M carry out frequency spectrum point using discrete cosine transform to the source signal after interception Analysis, and extract effective frequency range f1~f2Interior wavefield signals obtain filtered source signal, are denoted as Stf (0, j);
Discrete cosine transform is carried out using the second formula to St (m), second formula is:
In formula, DCT (k) indicate discrete cosine transform as a result, k be sampling number identical with m values,
Remember fsAbscissa for seismographic data sampling rate, DCT (k) is
By f in DCT (k)1~f2Data except range replace with 0, obtain after frequency filtering as a result, being denoted as DCTf (k);
Inverse discrete cosine transform is carried out to DCTf (k), obtains filtered source signal Stf (0, j).
It is described that Fourier Transform of Fractional Order calculating is carried out to filtered source signal as a kind of possible realization method The optimal rotation angle α of source signalopt, including:
The source signal for selecting any time in filtered source signal Stf (0, j) carries out fractional order using third formula Fourier transformation, the third formula are:
In formula, n is integer, and FrFT is the function about u and conversion angle α, and the value range of α is (- π, π);
The step of optimal rotation angle for calculating source signal, specifically includes as follows:
Using the optimal rotation angle α of the 4th formula computational theorytheory, the 4th formula is:
F in formulasFor seismographic data sampling rate, f1~f2For the effective frequency range of source signal;
With αtheoryCentered on, it is d that step-length is arranged in the range of ± r, and r is a percentage, is believed filtered focus Number Stf (0, j) carries out the iterative calculation of Fourier Transform of Fractional Order;
It is optimal rotation angle α to select the rotation angle for keeping peak value of pulse highest, convergence bestopt, the αoptTo all Seismic signal, that is, S (i, j) is applicable in.
As a kind of possible realization method, to the seismic signal of controlled source excitation according to effective time range into Row interception, and be filtered according to effective frequency range, Fourier Transform of Fractional Order is carried out successively using the optimal rotation angle, The seismic phase of different earthquake instrument record is obtained, including:
To the seismic signal S (i, j) of all controlled sources excitation, t is intercepted1~t2The signal of time range;
Using discrete cosine transform and its inverse transformation, f is extracted1~f2The signal of frequency range is denoted as Stf (i, j);
According to optimal rotation angle αopt, Fourier Transform of Fractional Order is carried out to Stf (i, j), obtains each seismic detector acquisition The impulse function FrFT (i, j) for the seismic signal that controlled source excites every time;
The same seismographic FrFT (i, j) is overlapped, the controlled source excitation of each seismic detector acquisition is obtained The seismic phase of seismic signal, is denoted as FrFT (i).
It is described to determine arrival time difference and apparent velocity using the seismic phase as a kind of possible realization method, including:
Using all seismographic seismic phase FrFT (i), the sampling period where remembering their peak value of pulse is u (i), with Sampling period u (0) where the adjacent seismographic seismic phase peak value of pulse of the controlled source is zero moment;
The arrival time difference of seismic phase is calculated using the 5th formula, the 5th formula is:
Δ t (i) is the arrival time difference of the seismic phase of No. i-th seismic detector acquisition in formula;
The apparent velocity of seismic phase is calculated using the 6th formula, the 6th formula is:
In formula, v (i) is the apparent velocity of the seismic phase of No. i-th seismic detector acquisition, and d (i) is No. i-th seismic detector and controlled source Distance, No. 0 seismic detector is the seismic detector adjacent with controlled source, it is believed that No. 0 seismic detector be at a distance from controlled source 0。
Second aspect, the present invention provide a kind of device quickly identifying seismic phase using controlled source excitation seismic signal, institute Stating device includes:
Collecting unit, for, in the earthquake initial data of research area excitation, obtaining can using seismic detector acquisition controlled source The seismic signal S (i, j) of epicenter excitation is controlled, i indicates that seismographic number, j indicate the number of controlled source excitation;
Short Time Fourier Transform unit, for using the seismic signal that seismic detector corresponding with the controlled source acquires as Source signal S (0, j), any secondary source signal of selective exitation carry out the time-frequency spy of Short Time Fourier Transform analysis source signal Sign, obtains the effective time range and frequency range of source signal;
Interception unit, for being intercepted according to effective time range to source signal, using discrete cosine transform to cutting Source signal after taking carries out spectrum analysis and extracts the filtered source signal Stf of the acquisition of the wavefield signals in effective frequency range (0,j);
Fourier Transform of Fractional Order unit calculates shake for carrying out Fourier Transform of Fractional Order to filtered source signal The optimal rotation angle α of source signalopt
Seismic phase acquiring unit, the seismic signal for being excited to the controlled source are cut according to effective time range It takes, and is filtered according to effective frequency range, Fourier Transform of Fractional Order is carried out successively using the optimal rotation angle, obtain The seismic phase of different earthquake instrument record;
Determination unit, for determining arrival time difference and apparent velocity using the seismic phase.
The method and device provided by the invention that seismic phase is quickly identified using controlled source excitation seismic signal, utilizes score Rank Fourier transformation to carry out quick seismic phase identification to the linear frequency modulation seismic signal that controlled source excites, and inherits traditional Fu In leaf transformation linear behavio(u)r, the interference of cross term when can inhibit time frequency analysis well can improve controlled source excitation Linear frequency modulation seismic signal time-frequency distributions feature, be analysis object with impulse function, improve the signal-to-noise ratio of seismic phase, identification shake Phase then, for geologic interpretation provides more reliable data basis.
Description of the drawings
Fig. 1 is the method for quickly identifying seismic phase using controlled source excitation seismic signal provided in the embodiment of the present invention Flow diagram;
Fig. 2 is in the method for quickly identifying seismic phase using controlled source excitation seismic signal provided in the embodiment of the present invention The temporal-spatial field schematic diagram of source signal;
Fig. 3 is in the method for quickly identifying seismic phase using controlled source excitation seismic signal provided in the embodiment of the present invention The time-frequency domain schematic diagram of source signal;
Fig. 4 is in the method for quickly identifying seismic phase using controlled source excitation seismic signal provided in the embodiment of the present invention The spectrum diagram of source signal within the scope of effective time;
Fig. 5 is in the method for quickly identifying seismic phase using controlled source excitation seismic signal provided in the embodiment of the present invention Use the source signal schematic diagram in discrete cosine transform and inverse transformation extraction effective frequency range;
Fig. 6 is in the method for quickly identifying seismic phase using controlled source excitation seismic signal provided in the embodiment of the present invention Impulse function shows obtained from the Fourier Transform of Fractional Order carried out to source signal using theoretical rotation angle and optimal rotation angle It is intended to;
Fig. 7 is in the method for quickly identifying seismic phase using controlled source excitation seismic signal provided in the embodiment of the present invention The schematic diagram of the seismic phase of all seismic signals of identification;
Fig. 8 is in the method for quickly identifying seismic phase using controlled source excitation seismic signal provided in the embodiment of the present invention Using four seismographic position views.
Fig. 9 is the device for exciting seismic signal quickly to identify seismic phase using controlled source provided in the embodiment of the present invention Structure diagram.
Specific implementation mode
In order to enable those skilled in the art to better understand the solution of the present invention, below in conjunction in the embodiment of the present invention Attached drawing, technical scheme in the embodiment of the invention is clearly and completely described, it is clear that described embodiment is only The embodiment of a part of the invention, instead of all the embodiments.Based on the embodiments of the present invention, ordinary skill people The every other embodiment that member is obtained without making creative work should all belong to the model that the present invention protects It encloses.
Term " first ", " second ", " third " in description and claims of this specification and above-mentioned attached drawing, " Four " etc. be for distinguishing similar object, without being used to describe specific sequence or precedence.It should be appreciated that using in this way Data can be interchanged in the appropriate case, so that the embodiments described herein can be in addition to illustrating or describing herein Sequence other than appearance is implemented.In addition, term " comprising " and " having " and their any deformation, it is intended that covering is non-exclusive Include to be not necessarily limited to clearly arrange for example, containing the process of series of steps or unit, method, system, product or equipment Those of go out step or unit, but may include not listing clearly or solid for these processes, method, product or equipment The other steps or unit having.
In conjunction with shown in Fig. 1, the present invention provides a kind of method quickly identifying seismic phase using controlled source excitation seismic signal, The method includes:
S101, the earthquake initial data excited in research area using seismic detector acquisition controlled source, are obtained controlled source and swashed The seismic signal S (i, j) of hair, i indicate that seismographic number, j indicate the number of controlled source excitation.
S102, source signal S (0, j) is used as using the seismic signal that the seismic detector adjacent with the controlled source acquires, selected Any secondary source signal for selecting excitation carries out Short Time Fourier Transform, analyzes the time-frequency characteristics of source signal, obtains source signal Effective time range and frequency range.
S103, source signal is intercepted according to effective time range, using discrete cosine transform to the shake after interception Source signal carries out spectrum analysis and extracts the wavefield signals in effective frequency range, obtains filtered source signal Stf (0, j);
S104, Fourier Transform of Fractional Order is carried out to filtered source signal, calculates the optimal rotation angle of source signal αopt
S105, the seismic signal of controlled source excitation is intercepted according to effective time range, and according to effective Frequency range is filtered, and Fourier Transform of Fractional Order is carried out successively using the optimal rotation angle, obtains different earthquake instrument note The seismic phase of record.
S106, arrival time difference and apparent velocity are determined using the seismic phase.
Step 101, a seismic detector is set specifically in the preset range of controlled source layout points (in such as several meters), then The laying seismic detector separated by a distance in research area as needed;According to seismic detector at a distance from controlled source from the near to the remote, It is 0,1,2,3 that seismic detector, which is numbered, ... ... the natural number being sequentially increased;According to the number that controlled source excites, it is denoted as 1, 2,3 ... ... the natural numbers being sequentially increased;The seismic signal of the controlled source excitation of seismic detector record is denoted as S (i, j), and i indicates ground The number of instrument is shaken, i=0 indicates that beside controlled source, j indicates the number of controlled source excitation.
Step 102, source signal is specifically used as with S (0, j), it is short chooses any time in S (0, j) source signal progress When Fourier transformation.
Wherein, the time-frequency characteristics of the analysis source signal of this step, obtain the effective time range and frequency of source signal The specific steps of range include as follows:The first formula is used to carry out Short Time Fourier Transform first, it chooses in S (0, j) any time Source signal, such as third time excitation source signal S (0,3), S (0,3) is converted into T/F by temporal-spatial field Domain, first formula are:
In formula, STFT (t, f) indicates the time-frequency domain after Short Time Fourier Transform as a result, S (τ) table in integral term Show the time series of source signal, i.e. S (0,3), for signal time from 0 to T, g (τ-t) is window function, window when t is.
And then constantly change t, you can obtain S (0,3) in the corresponding frequency f of different t;
The strongest frequency range of energy, origin coordinates is finally selected to be denoted as (t from T/F area image1,f1), cut-off Coordinate is denoted as (t2,f2), t1~t2As effective time range, f1~f2As effective frequency range, and to all seismic signals, That is S (i, j), is all suitable for.
Step 103, any time in S (0, j) source signal is specifically chosen, such as third time excites, i.e. S (0,3), interception t1~t2The signal of period, is denoted as St (m), and m indicates that the sampling number of the signal after interception, m=1 ..., M recycle discrete Cosine transform carries out spectrum analysis to the source signal after interception, and extracts effective frequency range f1~f2Interior wavefield signals, are filtered Source signal after wave is denoted as Stf (0, j).
Wherein, this step using discrete cosine transform to after interception source signal carry out spectrum analysis, and extract have The wavefield signals in frequency range are imitated, the specific steps for obtaining filtered source signal include as follows:Second is used to St (m) first Formula carries out discrete cosine transform, and second formula is:
In turn by f in DCT (k)1~f2Data except range replace with 0, obtain after frequency filtering as a result, being denoted as DCTf(k);
Inverse discrete cosine transform finally is carried out to DCTf (k), filtered source signal is obtained, is denoted as Stf (0, j).
Step 104, any filtered source signal is specifically selected, i.e. any focus letter in Stf (0, j) Number, such as third time excites, i.e. Stf (0,3), carries out Fourier Transform of Fractional Order using third formula, the third formula is:
In formula, n is integer, and FrFT is the function about u and conversion angle α, and the value range of α is (- π, π);
Wherein, the step of optimal rotation angle of the calculating source signal of this step specifically includes as follows:
First α is denoted as using the optimal rotation angle of the 4th formula computational theorytheory, the 4th formula is:
F in formulasFor seismographic data sampling rate, f1~f2For the effective frequency range of source signal;
And then in αtheoryCentered on, as in ± 5% range in the range of ± r, setting step-length for d (general very little, 10-5 Magnitude), the iterative calculation of Fourier Transform of Fractional Order is carried out to Stf (0,3);
The rotation angle that finally selection keeps peak value of pulse highest, convergence best is optimal rotation angle, is denoted as αopt。αoptIt is right All seismic signals, i.e. S (i, j), are all suitable for.
Operation is carried out by Fourier Transform of Fractional Order, Fourier Transform of Fractional Order is a kind of linear transformation, can will very The interference of suppressing crossterms well, and operation time is short, efficient, more easy programming is realized on computers, reduces method It is applicable in threshold.
Step 105, specifically first according to the step of step 103 intercepted according to effective time range to source signal Suddenly, to the seismic signal of all controlled sources excitation, i.e. S (i, j) intercepts t1~t2The signal of time range;
And then the specific steps of the filtered source signal of acquisition according to step 103, using discrete cosine transform and its F is extracted in inverse transformation1~f2The signal of frequency range is denoted as Stf (i, j);
Then the optimal rotation angle α calculated according to step 104opt, Fourier Transform of Fractional Order is carried out to Stf (i, j), is obtained The impulse function for the seismic signal that the controlled source acquired to each seismic detector excites every time, is denoted as FrFT (i, j);
Finally the same seismographic FrFT (i, j) is overlapped, the controlled source for obtaining each seismic detector acquisition swashs The seismic phase of the seismic signal of hair, is denoted as FrFT (i).
Operation is carried out by Fourier Transform of Fractional Order, the interference of suppressing crossterms can improve controlled source excitation The time-frequency characteristics of linear frequency modulation seismic signal, and operation time is short, it is efficient, it is analysis object with impulse function, and pass through The same seismographic FrFT (i, j) of multiple stacking, enhances signal-to-noise ratio, improves the resolution capability of seismic phase, contribute to more accurate Really calculate the arrival time difference of seismic phase.
In step 106, first with all seismographic seismic phases, i.e. FrFT (i) remembers adopting where their peak value of pulse Sampling point number is u (i), when with the sampling period u (0) where the seismographic seismic phase peak value of pulse adjacent with controlled source being zero It carves;
And then the arrival time difference of seismic phase is calculated using the 5th formula, the 5th formula is:
Δ t (i) is the arrival time difference of the seismic phase of No. i-th seismic detector acquisition in formula;
The 6th formula is finally used to calculate the apparent velocity of seismic phase, the 6th formula is:
In formula, v (i) is the apparent velocity of the seismic phase of No. i-th seismic detector acquisition, and d (i) is No. i-th seismic detector and controlled source Distance, No. 0 seismic detector is the seismic detector beside controlled source, it is believed that it is 0 at a distance from controlled source.
The method for quickly identifying seismic phase using controlled source excitation seismic signal provided in the embodiment of the present invention, provides one Kind application scenarios are introduced, below by taking the seismic data of the controlled source in peaceful township of Mianzhu City of Sichuan Province excitation as an example, in conjunction with Previously described method, is described further.
S1, Fig. 2 is please referred to, seismic data, 4 seismic detectors is acquired with the sample rate of 100Hz in the wild using 4 seismic detectors Number is 0,1,2,3 respectively, wherein No. 0 is arranged beside controlled source 8m at a distance.Excitation 20 times, period are controlled source altogether 30min, wherein it is 26min to run well, it is front and back to stall 2min.Refer to Fig. 2.Remember that S (i, j) is seismic signal, i indicates earthquake The number of instrument, j indicate the number of controlled source excitation.
S2, in conjunction with shown in Fig. 3, to source signal any time in S (0, j), such as third time excites, i.e. S (0,3) is carried out S (0,3) is converted to time-frequency domain by Short Time Fourier Transform by temporal-spatial field.It can be with from T/F area image To find out, in the normal excitation period of 26min, fundamental frequency is 2~8Hz or so, and can tell 6 groups of frequency sweep modes, be 2 respectively~ 3min, 3~12min, 12~15min, 15~16min, 16~25min and 25~26min, corresponding frequency band are 2~4.1Hz, 4.1 ~6.6Hz, 6.6~8.15Hz, 8.15~6.5Hz, 6.5~4.1Hz and 4.1~2Hz.The strongest frequency range of energy is selected, Origin coordinates is denoted as (900s, 8.15Hz), and cut-off coordinate is denoted as (960s, 6.5Hz), and 900~960s is effective time range, 6.5~8.15Hz is effective frequency range, and is all suitable for the seismic signal of other seismic detectors record.
S3, any time in S (0, j) source signal is such as excited for the third time in conjunction with Fig. 4 and Fig. 5, i.e. S (0,3) interceptions Discrete cosine transform is carried out after the data of 900~960s, is denoted as DCT (k), and k is sampling number.Visible energy concentrates on 6.5~ 8.15Hz, and there is the second energy group in 13~16Hz, it is therefore desirable to it is filtered.It finds corresponding to 6.5Hz and 8.15Hz Data point is respectively 577 and 865, will be greater than the 865 and DCT (k) less than 577 to fill out being 0, the data inversion after then zeroizing It changes, obtains the filtered source signals of 6.5~8.15Hz, be denoted as Stf (0,3).
S4, in conjunction with Fig. 6, calculate theoretical rotation angle αtheory0.000025 step is arranged in ≈ 1.5543 (radian) or 89.05 ° It is long, it is scanned in 1.5~1.571 (being more than pi/2), iteration runs Fourier Transform of Fractional Order, the pulse obtained more every time The peak value size of signal, is maximized corresponding rotation angle, obtains optimal rotation angle αopt=1.555675 or 89.13 °.Pulse Symmetry, convergence and peak value, which have, to be obviously improved.
S5, in conjunction with Fig. 7, to all seismic signals of controlled source excitation, i.e. S (i, j), interception, 900~960s signals Afterwards, discrete cosine transform and its inverse transformation are recycled, the signal of 6.5~8.15Hz frequency ranges is extracted, is denoted as Stf (i, j);So Optimal rotation angle α is utilized afterwardsopt=1.555675 or 89.13 °, Fourier Transform of Fractional Order is carried out to Stf (i, j), is obtained each The impulse function for the seismic signal that the controlled source of seismic detector acquisition excites every time, is denoted as FrFT (i, j);Finally to same The FrFT (i, j) of shake instrument is overlapped 20 times, obtains the seismic phase of the seismic signal of the controlled source excitation of each seismic detector acquisition, It is denoted as FrFT (i).
S6, in conjunction with Fig. 8, calculate the arrival time difference and apparent velocity of seismic phase.No. 0, No. 1, No. 2, No. 3 seismic detector record Seismic phase peak value of pulse where sampling period be 348,349,350,353 respectively, and then obtain 4 seismic detectors record shake The arrival time difference of phase is 0.6613s, 1.3227s, 3.3067s.No. 1, No. 2, No. 3 seismic detector distance the 0th, namely it is controllable The distance of focus is 1.411km, 3.482km, 8.489km respectively.Its orbicular spot be No. 0 seismic detector, triangle be No. 1, No. 2, No. 3 seismic detector.What seismic phase represented is longitudinal wave, and apparent velocity is 2.13km/s, 2.63km/s, 2.57km/s respectively. And then it can estimate that the longitudinal wave apparent velocity of this area is 2.4km/s.It is also found that No. 1 and No. 2 station note from Fig. 7 Secondary seismic phase has been recorded, surface wave is represented.Therefore a kind of seismic signal using controlled source excitation provided by the invention is quickly known The method of other seismic phase can improve the time-frequency characteristics of the linear frequency modulation seismic signal of controlled source excitation, be analysis with impulse function Object improves the resolution capability of seismic phase, and more accurately calculates the arrival time difference of seismic phase.
The present invention provides a kind of method that the seismic signal excited using controlled source quickly identifies seismic phase, including following step Suddenly:Using seismic detector acquisition controlled source in the earthquake initial data of research area excitation, the earthquake letter of controlled source excitation is obtained Number, it is denoted as S (i, j), i indicates that seismographic number, j indicate the number of controlled source excitation;With the ground adjacent with controlled source The seismic signal of instrument acquisition is shaken as source signal, is denoted as S (0, j), any secondary source signal of selective exitation carries out Fu in short-term In leaf transformation, analyze the time-frequency characteristics of source signal, obtain the effective time range and frequency range of source signal;Focus is believed It number is intercepted according to effective time range, spectrum analysis is carried out to the source signal after interception using discrete cosine transform, and The wavefield signals in effective frequency range are extracted, filtered source signal is obtained, are denoted as Stf (0, j);To filtered source signal Fourier Transform of Fractional Order is carried out, the optimal rotation angle of source signal is calculated, is denoted as αopt;To the earthquake letter of controlled source excitation Number, it is intercepted according to effective time range, and be filtered according to effective frequency range, recycles optimal rotation angle, successively Fourier Transform of Fractional Order is carried out, the seismic phase of different earthquake instrument record is obtained;Using seismic phase, arrival time difference and apparent velocity are calculated.Profit The linear frequency modulation seismic signal excited to controlled source with Fourier Transform of Fractional Order carries out quick seismic phase identification, inherits The linear behavio(u)r of traditional FT, the interference of cross term when can inhibit time frequency analysis well can improve controlled source excitation The time-frequency distributions feature of linear frequency modulation seismic signal is analysis object with impulse function, improves the signal-to-noise ratio of seismic phase, identifies seismic phase Then, more reliable data basis is provided for geologic interpretation.
Accordingly, in conjunction with shown in Fig. 9, present invention offer is a kind of quickly to identify seismic phase using controlled source excitation seismic signal Device, described device includes:
Collecting unit 901, for, in the earthquake initial data of research area excitation, being obtained using seismic detector acquisition controlled source The seismic signal S (i, j) of controlled source excitation, i indicate that seismographic number, j indicate the number of controlled source excitation;
Short Time Fourier Transform unit 902, the seismic signal for being acquired with seismic detector corresponding with the controlled source As source signal S (0, j), any secondary source signal of selective exitation carry out Short Time Fourier Transform analysis source signal when Frequency feature obtains the effective time range and frequency range of source signal;
Interception unit 903 utilizes discrete cosine transform pair for being intercepted according to effective time range to source signal Source signal after interception carries out spectrum analysis and extracts the filtered source signal Stf of the acquisition of the wavefield signals in effective frequency range (0,j);
Fourier Transform of Fractional Order unit 904, by being carried out based on Fourier Transform of Fractional Order to filtered source signal Calculate the optimal rotation angle α of source signalopt
Seismic phase acquiring unit 905, the seismic signal for being excited to the controlled source are carried out according to effective time range Interception, and be filtered according to effective frequency range, Fourier Transform of Fractional Order is carried out successively using the optimal rotation angle, is obtained Obtain the seismic phase of different earthquake instrument record;
Determination unit 906, for determining arrival time difference and apparent velocity using the seismic phase.
The device provided by the invention that seismic phase is quickly identified using controlled source excitation seismic signal, using in fractional order Fu Leaf transformation to carry out quick seismic phase identification to the linear frequency modulation seismic signal that controlled source excites, and inherits the linear of traditional FT Property, the interference of cross term when can inhibit time frequency analysis well, can improve the linear frequency modulation earthquake of controlled source excitation The time-frequency distributions feature of signal is analysis object with impulse function, improves the signal-to-noise ratio of seismic phase, identify seismic phase then, for ground Matter, which is explained, provides more reliable data basis.
It is apparent to those skilled in the art that for convenience and simplicity of description, the system of foregoing description, The specific work process of device and unit, can refer to corresponding processes in the foregoing method embodiment, and details are not described herein.
In embodiment provided herein, it should be understood that disclosed system, device and method can pass through Other modes are realized.For example, the apparatus embodiments described above are merely exemplary, for example, the division of the unit, Only a kind of division of logic function, formula that in actual implementation, there may be another division manner, such as multiple units or component can be with In conjunction with or be desirably integrated into another system, or some features can be ignored or not executed.Another point, it is shown or discussed Mutual coupling, direct-coupling or communication connection can be by some interfaces, the INDIRECT COUPLING of device or unit or Communication connection can be electrical, machinery or other forms.
The unit illustrated as separating component may or may not be physically separated, aobvious as unit The component shown may or may not be physical unit, you can be located at a place, or may be distributed over multiple In network element.Some or all of unit therein can be selected according to the actual needs to realize the mesh of this embodiment scheme 's.
In addition, each functional unit in each embodiment of the present invention can be integrated in a processing unit, it can also It is that each unit physically exists alone, it can also be during two or more units be integrated in one unit.Above-mentioned integrated list The form that hardware had both may be used in member is realized, can also be realized in the form of SFU software functional unit.
One of ordinary skill in the art will appreciate that all or part of step in the various methods of above-described embodiment is can It is completed with instructing relevant hardware by program, which can be stored in a computer readable storage medium, storage Medium may include:Read-only memory (ROM, Read Only Memory), random access memory (RAM, Random Access Memory), disk or CD etc..
Above to it is provided by the present invention it is a kind of using controlled source excitation seismic signal quickly identify seismic phase method and Device is described in detail, and for those of ordinary skill in the art, the thought of embodiment, is being embodied according to the present invention There will be changes in mode and application range, in conclusion the content of the present specification should not be construed as limiting the invention.

Claims (8)

1. a kind of method quickly identifying seismic phase using controlled source excitation seismic signal, which is characterized in that the method includes:
Using seismic detector acquisition controlled source in the earthquake initial data of research area excitation, the earthquake letter of controlled source excitation is obtained Number S (i, j), i indicate that seismographic number, j indicate the number of controlled source excitation;
Using the seismic signal that the seismic detector adjacent with the controlled source acquires as source signal S (0, j), selective exitation is appointed One time source signal carries out Short Time Fourier Transform, analyzes the time-frequency characteristics of source signal, obtains the effective time of source signal Range and frequency range;
Source signal S (0, j) is intercepted according to effective time range, the focus after interception is believed using discrete cosine transform It number carries out spectrum analysis and extracting the wavefield signals in effective frequency range, Stf (0, j);
Fourier Transform of Fractional Order is carried out to filtered source signal Stf (0, j), calculates the optimal rotation angle of source signal αopt
To the controlled source excitation seismic signal intercepted according to effective time range, and according to effective frequency range into Row filtering carries out Fourier Transform of Fractional Order using the optimal rotation angle, obtains the seismic phase of different earthquake instrument record successively;
Arrival time difference and apparent velocity are determined using the seismic phase.
2. the method according to claim 1 for quickly identifying seismic phase using controlled source excitation seismic signal, feature exist In the earthquake initial data excited in research area using seismic detector acquisition controlled source obtains the ground of controlled source excitation Signal S (i, j) is shaken, i indicates that seismographic number, j indicate the number of controlled source excitation, including:
In the preset range of controlled source layout points, one seismic detector is set, it is separated by a distance in research area further according to needing Lay seismic detector, according to seismic detector at a distance from controlled source from the near to the remote, it is 0,1,2,3 that seismic detector, which is numbered, ... ... The natural number being sequentially increased;According to the number that controlled source excites, the natural number for being denoted as 1,2,3 ... ... and being sequentially increased;Seismic detector The seismic signal of the controlled source excitation of record is denoted as S (i, j), and i indicates that seismographic number, i=0 indicate by controlled source Side, j indicate the number of controlled source excitation.
3. the method according to claim 2 for quickly identifying seismic phase using controlled source excitation seismic signal, feature exist In described using the seismic signal that the seismic detector adjacent with the controlled source acquires as source signal S (0, j), selective exitation Any time source signal carry out Short Time Fourier Transform, analyze the time-frequency characteristics of the source signal, obtain the focus The effective time range and frequency range of signal, including:
It is used as source signal with S (0, j), any time in S (0, j) source signal is chosen and carries out Short Time Fourier Transform;
Short Time Fourier Transform is carried out using the first formula, source signal is converted into time-frequency domain by temporal-spatial field, First formula is:
In formula, the time-frequency domain after STFT (t, f) expression Short Time Fourier Transforms is as a result, the S (τ) in integral term indicates shake The time series of source signal, for signal time from 0 to T, g (τ-t) is window function, and window when t is constantly changes t, obtains source signal In the corresponding frequency f of different t;
The strongest frequency range of energy, origin coordinates is selected to be denoted as (t from T/F area image1,f1), cut-off coordinate is denoted as (t2,f2), t1~t2As effective time range, f1~f2As effective frequency range, and it is suitable to all seismic signal S (i, j) With.
4. the method according to claim 3 for quickly identifying seismic phase using controlled source excitation seismic signal, feature exist In, it is described that the source signal is intercepted according to effective time range, using discrete cosine transform to the focus after interception Signal carries out spectrum analysis and extracts the filtered source signal Stf (0, j) of the acquisition of the wavefield signals in effective frequency range, including:
Any time in S (0, j) source signal is chosen, t is intercepted1~t2The signal of period is denoted as St (m), after m indicates interception Signal sampling number, m=1 ..., M, using discrete cosine transform to after interception source signal carry out spectrum analysis, and Extract effective frequency range f1~f2Interior wavefield signals obtain filtered source signal, are denoted as Stf (0, j);
Discrete cosine transform is carried out using the second formula to St (m), second formula is:
In formula, DCT (k) indicate discrete cosine transform as a result, k be sampling number identical with m values,
Remember fsAbscissa for seismographic data sampling rate, DCT (k) is
By f in DCT (k)1~f2Data except range replace with 0, obtain after frequency filtering as a result, being denoted as DCTf (k);
Inverse discrete cosine transform is carried out to DCTf (k), obtains filtered source signal Stf (0, j).
5. the method according to claim 4 for quickly identifying seismic phase using controlled source excitation seismic signal, feature exist In described to carry out the optimal rotation angle α that Fourier Transform of Fractional Order calculates source signal to filtered source signalopt, packet It includes:
The source signal for selecting any time in filtered source signal Stf (0, j) is carried out using third formula in fractional order Fu Leaf transformation, the third formula are:
In formula, n is integer, and FrFT is the function about u and conversion angle α, and the value range of α is (- π, π);
The step of optimal rotation angle for calculating source signal, specifically includes as follows:
Using the optimal rotation angle α of the 4th formula computational theorytheory, the 4th formula is:
F in formulasFor seismographic data sampling rate, f1~f2For the effective frequency range of source signal;
With αtheoryCentered on, it is d that step-length is arranged in the range of ± r, and r is a percentage, to filtered source signal Stf (0, j) carries out the iterative calculation of Fourier Transform of Fractional Order;
It is optimal rotation angle α to select the rotation angle for keeping peak value of pulse highest, convergence bestopt, the αoptTo all earthquakes Signal, that is, S (i, j) is applicable in.
6. the method according to claim 5 for quickly identifying seismic phase using controlled source excitation seismic signal, feature exist In, to the controlled source excitation seismic signal intercepted according to effective time range, and according to effective frequency range into Row filtering carries out Fourier Transform of Fractional Order successively using the optimal rotation angle, obtains the seismic phase of different earthquake instrument record, packet It includes:
To the seismic signal S (i, j) of all controlled sources excitation, t is intercepted1~t2The signal of time range;
Using discrete cosine transform and its inverse transformation, f is extracted1~f2The signal of frequency range is denoted as Stf (i, j);
According to optimal rotation angle αopt, Fourier Transform of Fractional Order is carried out to Stf (i, j), obtains the controllable of each seismic detector acquisition The impulse function FrFT (i, j) for the seismic signal that focus excites every time;
The same seismographic FrFT (i, j) is overlapped, the earthquake of the controlled source excitation of each seismic detector acquisition is obtained The seismic phase of signal, is denoted as FrFT (i).
7. the method according to claim 6 for quickly identifying seismic phase using controlled source excitation seismic signal, feature exist In, it is described to determine arrival time difference and apparent velocity using the seismic phase, including:
Using all seismographic seismic phase FrFT (i), the sampling period where remembering their peak value of pulse is u (i), with it is described Sampling period u (0) where the adjacent seismographic seismic phase peak value of pulse of controlled source is zero moment;
The arrival time difference of seismic phase is calculated using the 5th formula, the 5th formula is:
Δ t (i) is the arrival time difference of the seismic phase of No. i-th seismic detector acquisition in formula;
The apparent velocity of seismic phase is calculated using the 6th formula, the 6th formula is:
In formula, v (i) is the apparent velocity of the seismic phase of No. i-th seismic detector acquisition, d (i) be No. i-th seismic detector and controlled source away from From No. 0 seismic detector is the seismic detector adjacent with controlled source, it is believed that No. 0 seismic detector is 0 at a distance from controlled source.
8. a kind of quickly identifying the device of seismic phase using controlled source excitation seismic signal, which is characterized in that described device includes:
Collecting unit, for, in the earthquake initial data of research area excitation, controllably being shaken using seismic detector acquisition controlled source The seismic signal S (i, j) of source excitation, i indicate that seismographic number, j indicate the number of controlled source excitation;
Short Time Fourier Transform unit, for using the seismic signal that seismic detector corresponding with the controlled source acquires as focus Signal S (0, j), any secondary source signal of selective exitation carry out the time-frequency characteristics of Short Time Fourier Transform analysis source signal, Obtain the effective time range and frequency range of source signal;
Interception unit, for being intercepted according to effective time range to source signal, using discrete cosine transform to interception after Source signal carry out spectrum analysis and extract the wavefield signals in effective frequency range obtaining filtered source signal Stf (0, j);
Fourier Transform of Fractional Order unit calculates focus letter for carrying out Fourier Transform of Fractional Order to filtered source signal Number optimal rotation angle αopt
Seismic phase acquiring unit, the seismic signal for being excited to the controlled source are intercepted according to effective time range, and It is filtered according to effective frequency range, Fourier Transform of Fractional Order is carried out successively using the optimal rotation angle, obtained different The seismic phase of seismic detector record;
Determination unit, for determining arrival time difference and apparent velocity using the seismic phase.
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