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Oscillation Types and Bifurcations of a Nonlinear Second-Order Differential-Difference Equation
Authors:Wolf Bayer  Uwe an der Heiden
Institution:(1) Mathematical Institute, University of Witten/Herdecke, D-58448 Witten, Germany
Abstract:This paper considers the second-order differential difference equation

$$X\left( t \right) = f\left( {X\left( {t - \tau } \right)} \right) - X\left( t \right)$$
with the constant delay tau > 0 and the piecewise constant function 
$$f:\mathbb{R} \to \{ a,b\} $$
with

$$\begin{gathered}  f:\mathbb{R} \to \{ a,b\}  \hfill \\  f\left( \xi  \right): = \left\{ {_a^a } \right.{\text{ }}_{{\text{if }}}^{{\text{if }}} {\text{ }}_\xi ^\xi  {\text{ }}_ \geqslant ^{\text{ < }} {\text{ }}_\Theta ^\Theta   \hfill \\ \end{gathered} $$
Differential equations of this type occur in control systems, e.g., in heating systems and the pupil light reflex, if the controlling function is determined by a constant delay tau > 0 and the switch recognizes only the positions ldquoonrdquo f(>) = a] and ldquooffrdquo f(>) = b], depending on a constant threshold value THgr. By the nonsmooth nonlinearity the differential equation allows detailed analysis. It turns out that there is a rich solution structure. For a fixed set of parameters a, b, THgr, tau, infinitely many different periodic orbits of different minimal periods exist. There may be coexistence of three asymptotically stable periodic orbits (ldquomultistability of limit cyclesrdquo). Stability or instability of orbits can be proven.
Keywords:nonlinear differential-difference equations  periodic orbits  bifurcations  second-order control system
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