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Theory

 
APPROPRIATENESS OF CONNECTION OF SEISMIC WAVES, EMITTED BY THE EARTHQUAKE CENTER


   Mechanical system of process investigation into the destroying center is considered as limited volume, including the breaking area, deformed by the forces, applied on its external surface [16,18], fig. 16

Extension displacements into the deformed body of the break surface leads to the energetic changes. They are the reasons, that on the break surface owing to the media mechanical properties the release of external tension field elastic energy is taking place.

One part of it is converted to the displacement fields energy, accompanying the breakage i.e. into the energy of own stress field, the other part is consumed for the irreversible processes into the breakage area. In the process of break extension kinetic energy is dispersed.


Fig.11.
Limited volume with the developing crack.
B and C - crack tops.


   Let’s assume that the coordinate system is choused so, that the limited fault area including the beginning of XYZ coordinate system be located into the XZ plane, and normal is oriented along the Y-axis. Breakage faces are displaced one towards another in the XZ plane in the X direction. Let’s consider the crack received in the process of its wave developing with the frequency of f waves per second (Fig.16).

If B point of crack’s top is moving towards to Z by the velocity of VCR, it is moved off at the distance of VCR for one second. At the crack developing in the direction of Z, crack’s top is emitting energy in the form of ultrasonic oscillations, which could be fixed by the device in the point A. Interval between the waves consecutively emitted by the crack’s top is equal to 1/f sec. For this time B top of the crack would pass the distance of VCR/f cm, i.e. VCR x T, where T= is the emitting wave period. That’s why the wave must be pass long way and device in the point A will fix a large interval of time between the two waves crest coming one after another,
(35)


where Vsound is the velocity of ultrasonic waves coming to the receiver into the A point. In other words, device discovered frequency lower than the cracks frequency:

(36)


The ratio of observed emission frequency to the released frequency is equal to:


(37)


In the formula (55) it is possible to use the wave length λ, i.e. the distance between the consecutive wave crests received by the following relation:


(38)


in this case:


(39)


This formula indicates, that the remoteness of top’s B point means the further crack’s developing and lead to the increasing of the wavelength coming to the receiver A.


Converting formula (45) the following relation is possible to receive:


(40)


By the designating Vc / Vsound by Z, i.e. the value, characterizing the relation of the difference between the observed and emitted wavelength top to the emitted wavelength, we shall receive the expression according to which it will be possible to judge about the time of fault (destroying) beginning when the crack reaches to its critical dimensions, which would lead to the noticeable quantity fall of the Vcr in the direction of Z.

Simultaneously, along with the ceasing of crack’s developing in the detection of Z the crack’s developing in the direction X is taking place. At that moment Ucr acquires its minimal significance, which is well observed at the experimental researchers described below.

Probably this is explained by this fact, that the micro cracks united to the arterial cracks, i.e. the stage of avalanched increasing cracking formation (AIC) is taking place.

So, we had received the following expression:


(41)


For the point C, approaching to the receiver A of the crack’s top, all the above mentioned formulas, will be correct at the condition that Vcr will be everywhere substituted by ­Vcr. Hence, the point C approaching to the receiver would lead to the frequency increasing that is equivalent to the wavelength decreasing and in this case formula (59) will be as follows;


(42)


(43)


i.e. the relation of the crack speed allocation in the solid body to the sound speed in the same environment is directly proportional to the difference of observed dimesions and emitted crack waves to the emitted wave length.

Let’s investigate the received appropriateness (43), when is assuming the extremes meanings.

At Z=0 we have: , i.e. Ucr = 0


At the same time , where from λH = λemiss .


n is coming from the experimental graphics, described below. In this case Vcr/Vsound = n = min and, hence, the crack’s developing has been continued with the minimal velocity of Ucr, which is proceeding to the crack velocity sudden leap into the solid Vcr=max.

At Vcr=max. = N we have:


,


where from
(44)


Hence, at its start point of crack’s developing Ucr has the tendency to increasing up to maximum and then decreases up to its minimal significance. After the definite period of time t increases by the sudden leap up to its maximum significance. Observed wave has the value of (1+N) time exceed the value of wave emitted by the crack.

So, the sharp increasing of observed wave’s length that is corresponds to the sudden leap of Z=Vcr/Vsound shows the destroying time coming.

Horizontal area on the plots (Fig.28) which proceeds the Z sharp increasing corresponds to the period of time before the destroying start point.

In is known that the most of materials subjected to mechanical influence possess by the acoustic emission (AE), i.e. where the destroying and deformation of the materials’ molecular structures are taking place.

Short-time mechanical waves impulse, generating into the area of material’s structural integrity destroying, are spreeded into the construction of the object, which is subjected to the mechanical forces and could be detected on its surface by the help of the appropriate apparatus.

By the determination of Z according to formula (42) and (43) it would be possible to predict the materials (construction) and rocks ultimate strength condition.

Hence, received appropriateness consisting in that: "THE RELATION OF THE CRACK SPEED ALLOCATION IN THE SOLID BODY TO THE SOUND SPEED IN THE SAME ENVIRONMENT IS DIRECTLY PROPORTIONAL TO THE DIFFERENCE OF OBSERVED DIMENTIONS AND EMMITTED CRACK WAVES TO THE EMMITTED WAVE LENGTH" allows us to predict the start point of ultimate strength condition of the materials (constructions) being under the dynamic (seismic) loads influence, in particular, it is possible to predict the TIME of EARTHQUAKE coming.

For the confirmation of the received appropriateness correction experimental investigations had been carried out directed to the samples of different nature and artificial materials loading by the gradually changed loads beginning from the loading start-point up to the sample’s complete destroying.

At the some types of rocks destroying process laboratory investigations and at the nature investigations provided into the tunnel workings, the device for the acoustic emission signals as the cracking indicator had been used. The resonance and bandwidth piezoelectric transducers had registered signals.

At the laboratory experiments testing of such rocks as garnet, obsidian, black shale, basalt as well as cement and concrete cement samples of different marks had been carried out.



EXAMPLE.

By the help of AF-5 device joint to the IN-10 acoustic impulses parameters measuring and treating blocks the concrete cement sample loading up to it complete destroying had been tested. Loading mode and some of the destroying parameters behavior in the time domain had been fixed on the magnetic disk. As the loading the acoustic emission signals filtration had been carried out as well as their amplification and storage on the magnetic disk with the formation of files of equal prescribed duration. Each file corresponds to definite time period in the real time scale. Simultaneously with the changing of interval duration the acoustic emission spectral density and signals power at the linear law of load increasing to the sample from the micro cracks complete meas


Fig. 12
Acoustic emission signals frecuency changing at the rockcracks origin and developing


On the starting stage of tool’s loading the frequency range, correspond to coherent function’s maximum was equal to 361-362 kHz. At the further insignificant increasing of external influence the acoustic energy’s shock had been taking place. Along with this the displacement of coherent function’s maximum frequency into the area of from 106 to 56 kHz up to the last avalanche destroying stage had been registered.

So, the fixed leaps in the acoustic energy changing and displacement of the coherent function’s maximum frequency ranges from the ultrasonic area to the sound one allowed to determine the duration of each destroying stage, beginning from the defects origin, their junction, macro and micro cracks developing, cracks derivation with the formation of arterial ones.

Fig. 12 illustrates the sample of acoustic emission spectral density maximum changing during the increasing of the destroying degree. The frequency, corresponding to the spectral density maximum is plotted on the ordinate; the strength loss is plotted on the abscissa.

The dependence shows that as the destroying degree increasing the spasmodic changing in frequency is taking place – from high, ultrasonic frequencies to sound ones correspond to the avalanche stage of destroying.

Based on the analyzed sample’s result let’s consider the phenomenon of the oscillations drooping at the load increasing according to linear law from the start point of micro cracks origin to the complete destroying (see the afore-sited formula),


Fig. 13
Changing of "seismic effect’s" magneting during The increase of loading beginning from the microcracks origin till estroyi estroying


Fig. 13 shows the Z changing as the load increasing (Z=0.0042) to the complete destroying (Z=0.67). The appropriateness of Z changing had been received accordin to the before mentioned formula (10). Table 1 represents the Z numerical values which is corresponding to the given oscillation frequency f.


Z numerical values Table 10
f kHz
252
182
106.4
56
9
6
3
Z
0.0042
0.276
0.416
0.474
0.839
0.391
0.67


As obvious from the Table 1 and Fig.3 the appropriate increasing of load up to the arterial micro crack formation is observed. Then the sharp decreasing of Z from 0.839 to 0.391 occurs after which – pause and rising up to 0.67 where the destroying is taking place.

This phenomenon had been repeated in the all-numerous experiments with the rocks. The precise appropriateness of Z decreasing with maximum is observed, and then its growth which lead to the blocks’ failure, i.e. to the earthquake and to the receiving of appropriateness between the values of different type of waves.

On this appropriateness of Z is possible to judge about the time of material structure’s changing and about the time of limited strength condition.

As it is known, the earthquake centers possess the possibility to inform about their preparation to the earthquake by the help of sound information. The only problem is to trap these sounds, reject interference and reinforce.

By registering the time sequence of waves coming from the developed earthquake center λ1, λ2 … according to formula (47), it would be possible to predict the earthquake’s start point moment. Sum of maximal horizontal and subsequent minimal horizontal areas in time (Fig.13) represents the period of time before the earthquake beginning, which always corresponds to the "calm" before the earthquake.

As it is known this period of time is in the range of 8 to 30 hours before the earthquake starting depending on the given region grounds.



What we claim is:

It was established previously unknown appropriateness of the connection between the lengths of observed and emitted plane (seismic) waves into the solid, destroyed under the mechanical force (static, dynamic, temperature) influence consists in that the ratio between the lengths of observed and emitted waves to the emitted wave at the crack developing into the destroying center increased up to maximum, distinguished by that after maximum the ratio sharp dropping is taking place and after some period of time before the destroying start point the sharp increasing is observed characterizing the starting of strength loss, i.e. destroying (earthquake beginning).



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  Sunday 20 May, 2012  

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