CN113217109A - Waveform completion method for rockburst mine microseismic monitoring system - Google Patents
Waveform completion method for rockburst mine microseismic monitoring system Download PDFInfo
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Abstract
A method for completing a waveform of a microseismic monitoring system of a rock burst mine comprises the steps of firstly, obtaining a waveform missing interval; selecting the time t corresponding to the first trough before the missing waveform intervalmAnd the first acquisition point t before the missing waveform intervalMData point between and calculate the rate of change a of the vibration speed between two pointsmSelecting the time t corresponding to the first trough after the missing waveform intervalnAnd the first acquisition point t after the missing waveform intervalNData point between and calculate the rate of change a of the vibration speed between two pointsn(ii) a For tmTo tMAcceleration a betweenmFitting with t to obtain a functional relation am(t) analogously to obtain an(t);am(t) and an(t) the integral over time t is the vibration velocity VmaxTo obtain tXAnd utilize am(t)、an(t) complementing the waveform missing part. The method can improve the application range and the application precision of the microseismic monitoring system and improve the microseismic monitoring and early warning level of the rock burst mine.
Description
Technical Field
The invention belongs to the field of coal rock dynamic disaster monitoring, and particularly relates to a waveform completion method for a micro-seismic monitoring system, in particular to a waveform completion method for a micro-seismic monitoring system of a rock burst mine.
Background
Rock burst is a typical mine dynamic phenomenon and has great harmfulness. Statistics show that 135 rock burst mines are mined in 13 provinces and autonomous regions in China at present, the rock burst mines tend to increase year by year, and rock burst accidents are more serious. The microseism monitoring method is a main means for monitoring dynamic phenomena of rock burst mines, the microseism technology is known as one of the most effective and most development potential monitoring methods for predicting and forecasting coal rock dynamic disasters, particularly coal mine dynamic disasters, and the microseism monitoring method is widely applied to rock burst mines in China.
The microseism sensor is generally a magnetoelectric speed sensor, and the working principle of the microseism sensor is that the speed quantity is converted into an electric signal by utilizing electromagnetic induction, and the microseism sensor is matched with a signal acquisition station, a signal recorder and the like of a microseism monitoring system to work and is used for measuring the coal wall vibration speed. The microseismic sensor has higher precision, such as an SOS microseismic monitoring system imported from Poland,the vibration speed range is generally 1 × 10-6~6.2×10-3m/s, the mine earthquake with the minimum energy of 100J can be monitored. For microseismic sensors, high precision means that the measuring range is small, so that most of rock burst mines are faced with the condition that the measuring range of the microseismic sensors is too small when a large-energy mine earthquake event occurs, and the monitored waveforms are incomplete, namely, the waveforms are lost.
At present, a corresponding method is not available in the field of microseismic monitoring to deal with the situation that the waveform acquired by a microseismic sensor is incomplete, so that the coal wall vibration speed is inaccurate, the mine earthquake energy is not accurately calculated, and the requirement of high-precision microseismic monitoring of a rock burst mine cannot be met.
Disclosure of Invention
The invention aims to provide a waveform completion method for a microseismic monitoring system of a rock burst mine, which can improve the application range and the application precision of the microseismic monitoring system and improve the microseismic monitoring and early warning level of the rock burst mine.
In order to achieve the purpose, the invention provides a waveform completion method of a rock burst mine microseismic monitoring system, which is based on the principle of least square method and comprises the following steps:
(1) obtaining waveform missing intervals according to waveform files acquired by a microseismic monitoring system and the maximum measuring range of a microseismic sensor, and naming each interval as C according to time sequence1、C2、C3、……、Cn;
In time order, C1The time and the vibration speed corresponding to the first wave trough are respectively tm1、vm1;C1The time and the vibration speed corresponding to the first wave trough are respectively tn1、vn1;C2The time and the vibration speed corresponding to the first wave trough are respectively tm2、vm2;C2The time and the vibration speed corresponding to the first wave trough are respectively tn2、vn2;C3The time and the vibration speed corresponding to the first wave trough are respectively tm3、vm3;C3The time and the vibration speed corresponding to the first wave trough are respectively tn3、vn3;……;CnThe time and the vibration speed corresponding to the first wave trough are respectively tmn、vmn;CnThe time and the vibration speed corresponding to the first wave trough are respectively tnn、vnn;
C1The time and the vibration speed of the previous acquisition point of the waveform loss are respectively tM1、vM1;C1The time and the vibration speed of the first acquisition point after the waveform is lost are respectively tN1、vN1;C2The time and the vibration speed of the previous acquisition point of the waveform loss are respectively tM2、vM2;C2The time and the vibration speed of the first acquisition point after the waveform is lost are respectively tN2、vN2;C3The time and the vibration speed of the previous acquisition point of the waveform loss are respectively tM3、vM3;C3The time and the vibration speed of the first acquisition point after the waveform is lost are respectively tN3、vN3;……;CnThe time and the vibration speed of the previous acquisition point of the waveform loss are respectively tMn、vMn;CnThe time and the vibration speed of the first acquisition point after the waveform is lost are respectively tNn、vNn;
(2) If the sampling frequency of the microseismic sensor is known to be f, the sampling interval delta t is 1/f; selecting tm1、tM1T isN1、tn1T ism2、tM2T isN2、tn2T ism3、tM3T isN3、tn3… …, tmn、tMnT isNn、tnnThe vibration acceleration a between two adjacent sampling points is obtained by calculation, and a is delta v/delta t according to tm1To tM1Calculating the intermediate data point to obtain tm1To tM1The value of the intermediate acceleration a with the time t; calculating to obtain t by the same methodN1、tn1T ism2、tM2T isN2、tn2T ism3、tM3T isN3、tn3… …, tmn、tMnT isNn、tnnThe value of the respective acceleration a with the time t;
(3) based on the principle of least square method, using the pairs tm1To tM1Acceleration a betweenm1Fitting with time t to obtain am1Functional relation a with tm1(t); by the same token obtain an1(t)、am2(t)、an2(t)、am3(t)、an3(t)、……、amn(t)、ann(t);
(4) The principle that the peak vibration velocity after the completion of the waveform at the same time point is equal, namely am1(t) and an1(t) the peak velocities found are the same, function am1(t)、an1(t) the integral over time t is the peak vibration velocity V after the completion of the waveformmax1Is provided with Vmax1Corresponds to a time tx1To a, am1(t)、an1(t) the two functions are respectively integrated along the time axis to obtain an equation:solve to obtain tx1(ii) a Will tx1Carry-in typeOr formulaNamely obtainSimultaneously by the functional formula am1(t)、an1(t) completing the waveform missing interval;
in the same way, a is obtainedm2(t) and an2(t) between am3(t) and an3(t) between … …, amn(t) and ann(t) each of (V) corresponds tomax2,tx2)、(Vmax3,tx3)、……、(Vmaxn,txn) Simultaneously by functional formula am2(t)、an2(t)、am3(t)、an3(t)、……、amn(t)、ann(t) complementing the waveform-missing region.
Further, the fitting in step (3) is a piecewise fitting.
Preferably, the microseismic sensor in the step (1) is a microseismic sensor in an SOS microseismic monitoring system, and the sampling frequency f in the step (2) is 500 Hz.
The invention provides a waveform completion method based on the least square method, the principle is simple, the operability is strong, the calculation process involved in the method is easy to realize by programming, and the method is convenient to popularize and use; the method can fill the technical blank in the field of micro-seismic monitoring in the aspect of waveform completion, and can improve the use precision and the use range of a micro-seismic monitoring system; the method has important effects on accurately evaluating the mine earthquake risk and improving the monitoring and early warning efficiency of dynamic disasters such as rock burst and the like.
Drawings
FIG. 1 is a waveform of the microseismic system monitoring of the first embodiment, wherein C represents a waveform missing interval (t)m,vm)、(tn,vn) Respectively representing the time and the vibration speed of the first trough before and after the waveform missing interval;
FIG. 2 is a schematic diagram of the completion of the missing waveform interval in the first embodiment, VmaxIndicates the peak vibration velocity, t, after completion of the missing waveform sectionxRepresents VmaxA corresponding time; (t)M,vM)、(tN,vN) Respectively representing the time and the vibration speed of a first acquisition point before the waveform missing interval and after the waveform missing interval;
FIG. 3 is a fitting curve and a functional relation of the acceleration polynomial before the waveform is missing according to the first embodiment;
FIG. 4 is a fitting curve and a functional relation of the acceleration polynomial after the waveform is absent according to the first embodiment;
FIG. 5 is a microseismic system monitoring waveform of the second embodiment, C1、C2Indicates the waveform-missing region (t)m1,vm1)、(tn1,vn1) Respectively represent C1Wave form deletion interval front and C1Time and vibration speed at the first trough after the waveform missing interval; (t)m2,vm2)、(tn2,vn2) Respectively represent C2Wave form deletion interval front and C2Time and vibration speed at the first trough after the waveform missing interval;
FIG. 6 is a schematic diagram of the completion of the missing waveform interval according to the second embodiment, Vmax1、Vmax2Indicates the peak vibration velocity, t, after completion of the missing waveform sectionx1、tx2Represents Vmax1、Vmax2Respectively corresponding time; (t)M1,vM1)、(tN1,vN1) Respectively represent C1Wave form before deletion, C1Time and vibration speed of the first acquisition point after the waveform is lost; (t)M2,vM2)、(tN2,vN2) Respectively represent C2Wave form before deletion, C2Time and vibration speed of the first acquisition point after the waveform is lost;
FIG. 7 is C of the second embodiment1Fitting a curve and a function relation of an acceleration polynomial before waveform deletion;
FIG. 8 is C of the second embodiment1Linearly fitting a straight line and a function relation by the acceleration after the waveform is lost;
FIG. 9 shows a view of a second embodiment C2Fitting a curve and a function relation of an acceleration polynomial before waveform deletion;
FIG. 10 shows a view of a second embodiment C2And fitting a curve and a function relation of the acceleration polynomial after the waveform is absent.
Detailed Description
The invention is further described with reference to the following figures and specific examples.
Example one
As shown in figure 1, the invention discloses a waveform completion method of a microseismic monitoring system of a rock burst mine, which is based on the principle of least square method and comprises the following steps:
(1) waveform file and SOS micro-seismic monitor according to micro-seismic monitoring systemAcquiring a waveform missing interval at the maximum measuring range of a microseismic sensor in a measuring system, wherein C is the missing interval; according to the time sequence, the time and the vibration speed corresponding to the first wave trough before C are respectively tm、vm(ii) a The time and the vibration speed corresponding to the first trough after C are respectively tn、vn(ii) a The time and the vibration speed of the previous acquisition point of the C waveform lack are respectively tM、vM(ii) a The time and the vibration speed of the first acquisition point after the C waveform is lost are respectively tN、vN;
(2) The sampling frequency f of a microseismic sensor in the SOS microseismic monitoring system is 500Hz, and the sampling interval delta t is 0.002 s; as shown in fig. 2, t is selectedm、tMAnd tN、tnThe vibration acceleration a between two adjacent sampling points is obtained through calculation, and a is delta v/delta t;
according to tmTo tMInter data points and formula am=(vm+1-vm) T is calculated asmTo tMThe value of the inter-acceleration a with time t is:
[(2.722,0.010488),(2.724,0.005776),(2.726,0.0076),(2.728,0.006992),(2.73,0.007144),(2.732,0.00684),(2.734,0.035872),(2.736,0.096064),(2.738,0.113848),(2.74,0.123576),(2.742,0.120688)];
according to tNTo tnInter data points and formula an=(vn+1-vn) T is calculated asnTo tNThe value of the inter-acceleration a with time t is:
[(2.766,-0.1022959915),(2.768,-0.1097440035),(2.77,-0.112631996808953),(2.772,-0.106551999124349),(2.774,-0.0948480010265485),(2.776,-0.071591988671571)];
(3) due to tmTo tMAt time taWhere significant segmentation occurs, a segmentation fit is selected; based on the principle of least square method, for taTo tMAcceleration a betweenmFitting with time t to obtain amFunctional relation a with tm(t), the results are shown in FIG. 3; same principle and process as above for tnTo tNAcceleration a betweennFitting with time t to obtain anFunctional relation a with tn(t), the results are shown in FIG. 4;
(4) the principle that the peak vibration velocity after the completion of the waveform at the same time point is equal, namely am(t) and an(t) the peak velocity V obtainedmaxAre identical, function am(t)、an(t) the integral over time t is the peak vibration velocity V after the completion of the waveformmaxIs provided with VmaxCorresponds to a time txTo a, am(t)、an(t) the two functions are respectively integrated along the time axis to obtain an equation:solve to obtain tx(ii) a Will txCarry-in typeOr formulaCan obtainSimultaneously by the functional formula am(t)、an(t) complementing the waveform-missing region.
Example two
As shown in fig. 5, the waveform completion method for the microseismic monitoring system of the rock burst mine, which is disclosed by the invention, is based on the principle of the least square method and comprises the following steps:
(1) obtaining a waveform missing interval according to a waveform file of the microseismic monitoring system and the maximum measuring range of the SOS microseismic monitoring system, C1、C2Is a deletion interval;
in time order, C1The time and the vibration speed corresponding to the first wave trough are respectively tm1、vm1;C1The time and the vibration speed corresponding to the first wave trough are respectively tn1、vn1;C2First wave trough pairThe time and vibration speed are tm2、vm2;C2The time and the vibration speed corresponding to the first wave trough are respectively tn2、vn2;
C1The time and the vibration speed of the previous acquisition point of the waveform loss are respectively tM1、vM1;C1The time and the vibration speed of the first acquisition point after the waveform is lost are respectively tN1、vN1;C2The time and the vibration speed of the previous acquisition point of the waveform loss are respectively tM2、vM2;C2The time and the vibration speed of the first acquisition point after the waveform is lost are respectively tN2、vN2;
(2) The general sampling frequency f of the SOS microseismic monitoring system is 500Hz, and the sampling interval delta t is 0.002 s; as shown in FIG. 6, t is selectedm1、tM1T isN1、tn1T ism2、tM2T isN2、tn2The data points in between are obtained by obtaining the vibration acceleration a between two adjacent sampling points, wherein a is delta v/delta t;
according to tm1To tM1Inter data points and formula am1=(vm1+1-vm1) T is calculated asm1To tM1The value of the inter-acceleration a with time t is:
[(4.148,0.00836),(4.15,0.008208),(4.152,0.008056),(4.154,0.008056),(4.156,0.007448),(4.158,0.0076),(4.16,0.007752),(4.162,0.007752),(4.164,0.0076),(4.166,0.00836),(4.168,0.008664),(4.17,0.008512),(4.172,0.008512),(4.174,0.00836),(4.176,0.008208),(4.178,0.007904),(4.18,0.007904),(4.182,0.007752),(4.184,0.0076),(4.186,0.007448),(4.188,0.007296),(4.19,0.00684),(4.192,0.007144),(4.194,0.00684),(4.196,0.006688),(4.198,0.006536),(4.2,0.006384),(4.202,0.006536),(4.204,0.00608),(4.206,0.012616),(4.208,0.019456),(4.21,0.019456),(4.212,0.019608),(4.214,0.018696),(4.216,0.01748),(4.218,0.016416),(4.22,0.01596),(4.222,0.016416),(4.224,0.017176),(4.226,0.018392),(4.228,0.019608),(4.23,0.020368),(4.232,0.020672),(4.234,0.020368),(4.236,0.020064),(4.238,0.020064),(4.24,0.021128),(4.242,0.022344)];
according to tn1To tN1Inter data points and formula an1=(vn1+1-vn1) T is calculated asn1To tN1The value of the inter-acceleration a with time t is:
[(4.29,-0.010336),(4.292,-0.010184),(4.294,-0.00988),(4.296,-0.00988),(4.298,-0.00988),(4.3,-0.009424),(4.302,-0.009424),(4.304,-0.009272),(4.306,-0.00912),(4.308,-0.008968),(4.31,-0.008968),(4.312,-0.008816),(4.314,-0.008512),(4.316,-0.015048),(4.318,-0.025688),(4.32,-0.014592),(4.322,-0.015808),(4.324,-0.014592),(4.326,-0.013984),(4.328,-0.013832),(4.33,-0.013984),(4.332,-0.014288),(4.334,-0.014896),(4.336,-0.0152),(4.338,-0.014896),(4.34,-0.01444),(4.342,-0.013832),(4.344,-0.013528),(4.346,-0.013072),(4.348,-0.013376),(4.35,-0.013832),(4.352,-0.014288),(4.354,-0.014896),(4.356,-0.0152),(4.358,-0.0152),(4.36,-0.015048),(4.362,-0.015352),(4.364,-0.015504),(4.366,-0.016264),(4.368,-0.017328),(4.37,-0.018696),(4.372,-0.019456),(4.374,-0.020064),(4.376,-0.020368),(4.378,-0.00532),(4.38,-0.000141)];
according to tm2To tM2Inter data points and formula am2=(vm2+1-vm2) T is calculated asm2To tM2The value of the inter-acceleration a with time t is:
[(4.42,0.010032),(4.422,0.010336),(4.424,0.010944),(4.426,0.010944),(4.428,0.010488),(4.43,0.010488),(4.432,0.010336),(4.434,0.010336),(4.436,0.009728),(4.438,0.009728),(4.44,0.009728),(4.442,0.009576),(4.444,0.009272),(4.446,0.00912),(4.448,0.008968),(4.45,0.008816),(4.452,0.008664),(4.454,0.008664),(4.456,0.008208),(4.458,0.008208),(4.46,0.008056),(4.462,0.008208),(4.464,0.007904),(4.466,0.0076),(4.468,0.007448),(4.47,0.007448),(4.472,0.007296),(4.474,0.007144),(4.476,0.006992),(4.478,0.006688),(4.48,0.00684),(4.482,0.00684),(4.484,0.006384),(4.486,0.006384),(4.488,0.006232),(4.49,0.006232),(4.492,0.005928),(4.494,0.005928),(4.496,0.005776),(4.498,0.005624),(4.5,0.005472),(4.502,0.006992),(4.504,0.034808),(4.506,0.044232),(4.508,0.041344),(4.51,0.040584),(4.512,0.03952),(4.514,0.000106)];
according to tN2To tn2Inter data points and formula an2=(vn2+1-vn2) T is calculated asN2To tn2The value of the inter-acceleration a with time t is:
[(4.568,-0.01064),(4.57,-0.01064),(4.572,-0.010336),(4.574,-0.010184),(4.576,-0.010184),(4.578,-0.00988),(4.58,-0.00988),(4.582,-0.009576),(4.584,-0.009576),(4.586,-0.009272),(4.588,-0.009272),(4.59,-0.00912),(4.592,-0.008968),(4.594,-0.008968),(4.596,-0.008664),(4.598,-0.008664),(4.6,-0.008512),(4.602,-0.008208),(4.604,-0.008208),(4.606,-0.008056),(4.608,-0.007904),(4.61,-0.007904),(4.612,-0.007752),(4.614,-0.0076),(4.616,-0.007448),(4.618,-0.007448),(4.62,-0.007144),(4.622,-0.006992),(4.624,-0.006992),(4.626,-0.00684),(4.628,-0.007904),(4.63,-0.033896),(4.632,-0.033744),(4.634,-0.019608),(4.636,-0.0228),(4.638,-0.022192),(4.64,-0.02204),(4.642,-0.021736),(4.644,-0.021584),(4.646,-0.020824),(4.648,-0.020368),(4.65,-0.019912),(4.652,-0.019152),(4.654,-0.018392),(4.656,-0.01748),(4.658,-0.016568),(4.66,-0.015352),(4.662,-0.002584),(4.664,-0.000133)];
(3) due to tm1To tM1At time ta1Where significant segmentation occurs, a segmentation fit is selected; based on the principle of least square method, for ta1To tM1Acceleration a betweenm1Fitting with time t to obtain am1Functional relation a with tm1(t), the results are shown in FIG. 7;
same principle and process as above for tb1To tN1Acceleration a betweenn1Fitting with time t to obtain an1Functional relation a with tn1(t), the results are shown in FIG. 8;
same principle and process as above for ta2To tM2Acceleration a betweenm2Fitting with time t to obtain am2Functional relation a with tm2(t), the results are shown in FIG. 9;
same principle and process as above for tb2To tN2Acceleration a betweenn2Fitting with time t to obtain an2Functional relation a with tn2(t), the results are shown in FIG. 10;
(4) the principle that the peak vibration velocity after the completion of the waveform at the same time point is equal, namely am1(t) and an1(t) the peak velocity V obtainedmax1Are identical, function am1(t)、an1(t) the integral over time t is the peak vibration velocity V after the completion of the waveformmax1Is provided with Vmax1Corresponds to a time tx1To a, am1(t)、an1(t) the two functions are integrated along the time axis respectively to obtain the equation:solving the available tx1(ii) a Will tx1Carry-in typeOr formulaCan obtainSimultaneously by the functional formula am1(t)、an1(t) completing the waveform of the missing section;
the principle that the peak vibration velocity after the completion of the waveform at the same time point is equal, namely am2(t) and an2(t) the peak velocity V obtainedmax2Are identical, function am2(t)、an2(t) the integral over time t is the peak vibration velocity V after the completion of the waveformmax2Is provided with Vmax2Corresponds to a time tx2To a, am2(t)、an2(t) the two functions are integrated along the time axis respectively to obtain the equation:solving the available tx2(ii) a Will tx2Carry-in typeOr formulaCan obtainSimultaneously by the functional formula am2(t)、an2(t) filling the waveform of the missing section.
The first embodiment and the second embodiment are respectively a waveform complementing method in which the waveform missing interval is one and two, and when there are a plurality of waveform missing intervals, the waveform complementing method for the plurality of waveform missing intervals is the same as that in the second embodiment.
Claims (3)
1. A waveform completion method for a rock burst mine microseismic monitoring system is characterized by being based on the principle of least square method and comprising the following steps:
(1) obtaining waveform missing intervals according to waveform files acquired by a microseismic monitoring system and the maximum measuring range of a microseismic sensor, and naming each interval as C according to time sequence1、C2、C3、……、Cn;
In time order, C1The time and the vibration speed corresponding to the first wave trough are respectively tm1、vm1;C1The time and the vibration speed corresponding to the first wave trough are respectively tn1、vn1;C2The time and the vibration speed corresponding to the first wave trough are respectively tm2、vm2;C2The time and the vibration speed corresponding to the first wave trough are respectively tn2、vn2;C3The time and the vibration speed corresponding to the first wave trough are respectively tm3、vm3;C3The time and the vibration speed corresponding to the first wave trough are respectively tn3、vn3;……;CnThe time and the vibration speed corresponding to the first wave trough are respectively tmn、vmn;CnThe time and the vibration speed corresponding to the first wave trough are respectively tnn、vnn;
C1The time and the vibration speed of the previous acquisition point of the waveform loss are respectively tM1、vM1;C1The time and the vibration speed of the first acquisition point after the waveform is lost are respectively tN1、vN1;C2The time and the vibration speed of the previous acquisition point of the waveform loss are respectively tM2、vM2;C2The time and the vibration speed of the first acquisition point after the waveform is lost are respectively tN2、vN2;C3The time and the vibration speed of the previous acquisition point of the waveform loss are respectively tM3、vM3;C3The time and the vibration speed of the first acquisition point after the waveform is lost are respectively tN3、vN3;……;CnThe time and the vibration speed of the previous acquisition point of the waveform loss are respectively tMn、vMn;CnThe time and the vibration speed of the first acquisition point after the waveform is lost are respectively tNn、vNn;
(2) If the sampling frequency of the microseismic sensor is known to be f, the sampling interval delta t is 1/f; selecting tm1、tM1T isN1、tn1T ism2、tM2T isN2、tn2T ism3、tM3T isN3、tn3… …, tmn、tMnT isNn、tnnThe vibration acceleration a between two adjacent sampling points is obtained by calculation, and a is delta v/delta t according to tm1To tM1Calculating the intermediate data point to obtain tm1To tM1The value of the intermediate acceleration a with the time t; calculating to obtain t by the same methodN1、tn1T ism2、tM2T isN2、tn2T ism3、tM3T isN3、tn3… …, tmn、tMnBetween,tNn、tnnThe value of the respective acceleration a with the time t;
(3) based on the principle of least square method, using the pairs tm1To tM1Acceleration a betweenm1Fitting with time t to obtain am1Functional relation a with tm1(t); by the same token obtain an1(t)、am2(t)、an2(t)、am3(t)、an3(t)、……、amn(t)、ann(t);
(4) The principle that the peak vibration velocity after the completion of the waveform at the same time point is equal, namely am1(t) and an1(t) the peak velocities found are the same, function am1(t)、an1(t) the integral over time t is the peak vibration velocity V after the completion of the waveformmax1Is provided with Vmax1Corresponds to a time tx1To a, am1(t)、an1(t) the two functions are respectively integrated along the time axis to obtain an equation:solve to obtain tx1(ii) a Will tx1Carry-in typeOr formulaNamely obtainSimultaneously by the functional formula am1(t)、an1(t) completing the waveform missing interval;
in the same way, a is obtainedm2(t) and an2(t) between am3(t) and an3(t) between … …, amn(t) and ann(t) each of (V) corresponds tomax2,tx2)、(Vmax3,tx3)、……、(Vmaxn,txn) Simultaneously by functional formula am2(t)、an2(t)、am3(t)、an3(t)、……、amn(t)、ann(t) complementing the waveform-missing region.
2. The method for completing the waveform of the microseismic monitoring system for rock burst mine according to claim 1, wherein the fitting in the step (3) is a piecewise fitting.
3. The method for completing the waveform of the microseismic monitoring system of the rock burst mine according to claim 1 or 2, wherein the microseismic sensor in the step (1) is the microseismic sensor in the SOS microseismic monitoring system, and the sampling frequency f in the step (2) is 500 Hz.
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