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Date: 5-7-2018
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The Burridge-Knopoff model is a system of differential equations used to model earthquakes using points on a straight line, each of mass , that interact with each other via springs, and in which all masses are subject to a force that is proportional to the distances of the masses from their equilibrium position and to a friction force , where is the velocity,
REFERENCES:
Burridge, R. and Knopoff, L. Bull. Seis. Soc. Amer. 57, 341, 1967.
de Sousa Vieira, M. Phys. Rev. Lett. 82, 201, 1999.
de Sousa Vieira, M. "A Simple Deterministic Self-Organized Critical System." 23 Jan 2000. http://arxiv.org/abs/cond-mat/9907201.
Ferguson, C. D.; Klein, W.; and Rundle., J. B. Computers Physics 12, 34 1998.
Hähner, P. and Drossinos, Y. Physica A 260, 391, 1998.
Muratov, C. B. "Traveling Wave Solutions in the Burridge-Knopoff Model." 14 Jan 1999. http://arxiv.org/abs/patt-sol/9901003.
Place, D. and Villedieu, P. J. Comput. Phys. 150, 332,1999.
Webman, I.; Gruver, J. L.; and Havlin, S. "Sliding Objects with Random Friction." 12 Apr 1999. http://arxiv.org/abs/cond-mat/9904148.
Trott, M. The Mathematica GuideBook for Programming. New York: Springer-Verlag, pp. 12-13, 2004. http://www.mathematicaguidebooks.org/.
Xu, H.-J and Knopoff, L. Phys. Rev. E 50, 3577, 1994.
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