20.02.2013 Views

PROBLEMS OF GEOCOSMOS

PROBLEMS OF GEOCOSMOS

PROBLEMS OF GEOCOSMOS

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

Proceedings of the 7th International Conference "Problems of Geocosmos" (St. Petersburg, Russia, 26-30 May 2008)<br />

We will proceed from the assumption that average amplitude of fluctuations is proportional to<br />

fluctuations describe by Gaussian-distributed value � t ( 0;<br />

D)<br />

(details see in [9]). Then<br />

N and<br />

d N<br />

dt<br />

N<br />

� � � � �<br />

� ( t)<br />

t<br />

N .<br />

In this case probability density will have on of two forms:<br />

R<br />

It follows that the solution of the stochastic equation for N will have the similar form. The appearance of<br />

local minimum in aftershocks distribution shows that exponential decay of aftershocks is the least probable<br />

event. The most probable should be jumps (jerks) of aftershocks. Thus overshoots of N are the result of<br />

stochastic relaxation. Just stochasticity of relaxation process leads to appearance of «long tail» in aftershock<br />

distribution. The reorganization of relaxation process is an example of noise-induced transitions.<br />

It is clear that forshocks distribution should also have jumps. In fact we observe just such behaviour (see<br />

the picture above).<br />

7. PROSPECTS. The consistent examination of the DD-scenario has led us to investigation of the role<br />

of surface tension variations in earthquakes generation process. Prospects are not in the future development<br />

of DD-model but in integration of DD-model with alternative models of earthquake generation process in<br />

which diffusion of fluids is not considered as the main factor - dry dilatancy models and stick-slip models.<br />

The integration should be based on the Gibbs thermodynamic theory. The basis of the Gibbs theory of<br />

capillarity is the concepts of discontinuity surface and surface tension. The Gibbs energy can change not only<br />

due to surface area variations but also due to internal fluctuations of surface tension. Thus the problem is to<br />

investigate noise-induced transitions in thermodynamic systems.<br />

References.<br />

1. Brace W.F., Byerlee J.D. (1966), Stick-slip as a mechanism of earthquake, Science, 153, 990-992.<br />

2. Gibbs J.W. (1982), Thermodynamics, Nayka, Moskow, 536 p., [in Russian]; Gibbs J.W. (1878), Trans.<br />

Conn. Acad., v. 3, p. 343.<br />

3. Gratzinsky V. at al. (1967), On radioactive gas emission from rocks under action of ultrasonic, Physics of<br />

Earth, № 10, 91-94, [in Russian].<br />

4. Gupta H., Rastogi B.(1976), Dams and Earthquakes. Elsevier Publishing.<br />

5. Earthquake prediction (1983), No. 3, Donish, Dushanbe, 226 p., [in Russian].<br />

6. Makarenko V., Groza A. (1991), Earthquake Precursors and Acoustic Fields, The Journal of Geophysics,<br />

No. 1, v. 13, pp.3-14., [in Russian]<br />

7. Mandelbrot B. (1982), The Fractal Geometry of Nature. New York: W. H. Freeman and Co.<br />

8. Mogi K. (1985), Earthquake Prediction, Academic Press.<br />

9. Nicolis G., Prigogine I., Self-organization in nonequilibrium system, A Wiley-Interscience Publication.<br />

10. Tzarev V., Kuznetzov O. (1978), Experimental study of physical-chemical processes in rocks at small<br />

elastic deformations, [in Russian], Physics of the Earth, № 6, 94-101.<br />

11. Scholz C.H., Syke L.R., Aggarwal Y.P (1973), Earthquake prediction: a physical basis, Science, 181,<br />

803-809.<br />

411

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!