Phil. Trans. R. Soc. A (2009) 367, 4717–4739
doi:10.1098/rsta.2009.0177
Application of interval iterations to the
entrainment problem in respiratory physiology
BY JACQUES DEMONGEOT* AND JULES WAKU
TIMC-IMAG Laboratory, University J. Fourier of Grenoble,
38706 La Tronche, France
We present here some theoretical and numerical results about interval iterations.
We consider first an application of the interval iterations theory to the problem of
entrainment in respiratory physiology for which the classical point iterations theory fails.
Then, after a brief review of some of the main aspects of point iterations, we explain
what is meant by the term ‘interval iterations’. It consists essentially in replacing in the
point iterations the function to iterate by a set-valued map. We present both theoretical
and numerical aspects of this new type of iterations and we observe the dynamical
behaviours encountered, such as fixed intervals and interval limit cycles. The comparison
between point and interval iterations is carried out with respect to a parameter ε, which
determines the thickness of a neighbourhood around the function to iterate. We will
finally focus our attention on the Verhulst and Ricker functions largely used in population
dynamics, which exhibit various asymptotic behaviours.
Keywords: interval iterations; respiratory entrainment; set-valued map; invariant domain;
intervals limit cycles; population dynamics
1. Introduction
It is well known (May 1976; May & Oster 1976; Demongeot et al. 1997;
Murray 2002) that a first-order difference equation (e.g. the logistic one-
dimensional equation for a single species) allows the description of complex
dynamical behaviours in population growth modelling in many contexts and
several disciplines, such as in biology, economy and social sciences (Schaffer
et al. 1986; Demongeot & Leitner 1996; Demongeot et al. 1997; Stenseth et al.
1997; Demongeot & Waku 2005). The case of n -dimensional flows (system of
difference equations for n species) will not be treated in the following, but could
be considered as a natural generalization of the techniques here proposed. Let
the basic equation be
x
t +1
= f (x
t
). (1.1)
The variable x
t
can be referred to as the ‘population’ at time t ; f is usually
a nonlinear function, containing one or more adjustable parameters, which tune
the nonlinear behaviour of the considered system. Population here means people,
*Author for correspondence (jacques.demongeot@imag.fr).
One contribution of 17 to a Theme Issue ‘From biological and clinical experiments to mathematical
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2009 The Royal Society 4717