celtic stone
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2019 ◽  
Vol 61 (10) ◽  
pp. 773-786 ◽  
Author(s):  
A. S. Gonchenko ◽  
S. V. Gonchenko ◽  
A. O. Kazakov ◽  
E. A. Samylina

2018 ◽  
Vol 28 (11) ◽  
pp. 1830036 ◽  
Author(s):  
A. S. Gonchenko ◽  
S. V. Gonchenko ◽  
A. O. Kazakov ◽  
A. D. Kozlov

The paper is devoted to topical issues of modern mathematical theory of dynamical chaos and its applications. At present, it is customary to assume that dynamical chaos in finite-dimensional smooth systems can exist in three different forms. This is dissipative chaos, the mathematical image of which is a strange attractor; conservative chaos, for which the entire phase space is a large “chaotic sea” with randomly spaced elliptical islands inside it; and mixed dynamics, characterized by the principal inseparability in the phase space of attractors, repellers and conservative elements of dynamics. In the present paper (which opens a series of three of our papers), elements of the theory of pseudohyperbolic attractors of multidimensional maps and flows are presented. Such attractors, as well as hyperbolic ones, are genuine strange attractors, but they allow the existence of homoclinic tangencies. We describe two principal phenomenological scenarios for the appearance of pseudohyperbolic attractors in one-parameter families of three-dimensional diffeomorphisms, and also consider some basic examples of concrete systems in which these scenarios occur. We propagandize new methods for studying pseudohyperbolic attractors (in particular, the method of saddle charts, the modified method of Lyapunov diagrams and the so-called LMP-method for verification of pseudohyperbolicity of attractors) and test them on the above examples. We show that Lorenz-like attractors in three-dimensional generalized Hénon maps and in a nonholonomic model of Celtic stone as well as figure-eight attractors in the model of Chaplygin top are genuine (pseudohyperbolic) ones. Besides, we show an example of four-dimensional Lorenz model with a wild spiral attractor of Shilnikov–Turaev type that was found recently in [Gonchenko et al., 2018].


2018 ◽  
Vol 45 (2) ◽  
pp. 155-167 ◽  
Author(s):  
Jan Awrejcewicz ◽  
Grzegorz Kudra

2013 ◽  
Vol 18 (5) ◽  
pp. 521-538 ◽  
Author(s):  
Alexander S. Gonchenko ◽  
Sergey V. Gonchenko ◽  
Alexey O. Kazakov

2012 ◽  
pp. 507-518 ◽  
Author(s):  
A. S. Gonchenko ◽  
◽  
S. V. Gonchenko ◽  
A. O. Kazakov ◽  
◽  
...  

2012 ◽  
Vol 19 (5) ◽  
pp. 1115-1123 ◽  
Author(s):  
J. Awrejcewicz ◽  
G. Kudra

The integral model of dry friction components is built with assumption of classical Coulomb friction law and with specially developed model of normal stress distribution coupled with rolling resistance for elliptic contact shape. In order to avoid a necessity of numerical integration over the contact area at each the numerical simulation step, few versions of approximate model are developed and then tested numerically. In the numerical experiments the simulation results of the Celtic stone with the friction forces modelled by the use of approximants of different complexity (from no coupling between friction force and torque to the second order Padé approximation) are compared to results obtained from model with friction approximated in the form of piecewise polynomial functions (based on the Taylor series with hertzian stress distribution). The coefficients of the corresponding approximate models are found by the use of optimization methods, like as in identification process using the real experiment data.


2011 ◽  
Vol 21 (10) ◽  
pp. 2905-2917 ◽  
Author(s):  
GRZEGORZ KUDRA ◽  
JAN AWREJCEWICZ

In this paper, for the first time, the complete set of Tangens hyperbolicus approximations of model of dry friction coupled with rolling resistance for circular contact area between interacting bodies is proposed. The developed approximations are compared with corresponding Padé approximants of the first and second order well known from the literature and with the numerical solution of the exact integral model as well. It is shown that Tangens hyperbolicus approximants are closest to the exact solution. Then the approximated models are applied to the celtic stone dynamics, however with the significant simplifying assumption of circular contact between stone and the table, presenting differences between them again. Certain specific approximations and regularizations of the friction and rolling resistance models enabling and facilitating their application to the real problem are shown. The analysis of the response dependence on initial conditions is performed by the use of a special kind of diagram.


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