Read e-book online Analysis and Simulation of Chaotic Systems PDF

By Frank C. Hoppensteadt

ISBN-10: 1475722753

ISBN-13: 9781475722758

ISBN-10: 147572277X

ISBN-13: 9781475722772

Starting with sensible mathematical or verbal versions of actual or organic phenomena, the writer derives tractable versions for extra mathematical research or machine simulations. For the main half, derivations are in line with perturbation equipment, and the vast majority of the textual content is dedicated to cautious derivations of implicit functionality theorems, the tactic of averaging, and quasi-static country approximation tools. The duality among balance and perturbation is built and used, depending seriously at the proposal of balance less than chronic disturbances. proper themes approximately linear structures, nonlinear oscillations, and balance tools for distinction, differential-delay, integro-differential and traditional and partial differential equations are constructed in the course of the ebook. For the second one variation, the writer has restructured the chapters, putting precise emphasis on introductory fabrics in Chapters 1 and a pair of as special from presentation fabrics in Chapters three via eight. moreover, extra fabric on bifurcations from the viewpoint of canonical versions, sections on randomly perturbed structures, and a number of other new computing device simulations were further.

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4. Linear Systems with Periodic Coefficients 15 This result is especially helpful in determining the behavior of x(t) as t ~ For example, if all of the eigenvalues of R have negative real parts, then x(t) ~ 0 as t ~ 00. However, this theorem is difficult to apply since it is usually difficult to find the matrix R. An interesting consequence of Floquet's Theorem is that any periodic system can be transformed into one having constant coefficients. In fact, the change of variables x = P(t)y takes the problem 00.

An interesting consequence of Floquet's Theorem is that any periodic system can be transformed into one having constant coefficients. In fact, the change of variables x = P(t)y takes the problem 00. dx/dt = A(t)x into the linear system dy/dt = Ry A very useful example is the system ~ [Xl] dt x 2 = [coswt - sinwt]B[coswt sin wt cos wt sin wt -sinwt] coswt [Xl] X2 where B is a 2 x 2 matrix of constants. 1 Hill's Equation The equation where p is a continuous periodic function, is known as Hill's equation.

Then Lienard's equation has a unique periodic solution. All solutions in the plane approach this orbit except for the unstable equilibrium x = 0, Y = O. Proof. The proof results from the above lemma (2). With condition H' the mapping Yo -+ Yl(YO) is monotone decreasing. Since the previous theorem shows this mapping has a fixed point, it must be unique. This completes the • proof [see also Ref. 1]. Example of van der Pol's Equation. We can use these results to study van der Pol's equation d2x dt 2 + A(x 2 - dx 1) dt +x = 0 Ji In this case, F(x) = A(x 3 /3 - x) and a = ß = The last theorem shows that there is a unique periodic solution of van der Pol's equation for any choice of the parameter A (A > 0).

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Analysis and Simulation of Chaotic Systems by Frank C. Hoppensteadt


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