24 research outputs found
Existence and uniqueness of monotone wavefronts in a nonlocal resource-limited model
We are revisiting the topic of travelling fronts for the food-limited (FL)
model with spatio-temporal nonlocal reaction. These solutions are crucial for
understanding the whole model dynamics. Firstly, we prove the existence of
monotone wavefronts. In difference with all previous results formulated in
terms of `sufficiently small parameters', our existence theorem indicates a
reasonably broad and explicit range of the model key parameters allowing the
existence of monotone waves. Secondly, numerical simulations realized on the
base of our analysis show appearance of non-oscillating and non-monotone
travelling fronts in the FL model. These waves were never observed before.
Finally, invoking a new approach developed recently by Solar , we prove
the uniqueness (for a fixed propagation speed, up to translation) of each
monotone front.Comment: 20 pages, submitte
Mackey-Glass type delay differential equations near the boundary of absolute stability
For equations with -nonlinearity which has negative Schwarzian derivative and
satisfies for , we prove convergence of all solutions to
zero when both and are less than some constant
(independent on ). This result gives additional insight to the
conjecture about the equivalence between local and global asymptotical
stabilities in the Mackey-Glass type delay differential equations.Comment: 16 pages, 1 figure, accepted for publication in the Journal of
Mathematical Analysis and Application
The peak-and-end rule and differential equations with maxima: a view on the unpredictability of happiness
In the 1990s, after a series of experiments, the behavioral psychologist and
economist Daniel Kahneman and his colleagues formulated the following Peak-End
evaluation rule: "The remembered utility of pleasant or unpleasant episodes is
accurately predicted by averaging the Peak (most intense value) of instant
utility (or disutility) recorded during an episode and the instant utility
recorded near the end of the experience", (D. Kahneman et al., 1997, QJE, p.
381). Hence, the simplest mathematical model for time evolution of the
experienced utility function can be given by the scalar differential
equation where
represents exogenous stimuli, is the maximal duration of the experience,
and are some averaging weights. In this work, we study
equation and show that, for a range of parameters and a
periodic sine-like term , the dynamics of can be completely described
in terms of an associated one-dimensional dynamical system generated by a
piece-wise continuous map from a finite interval into itself. We illustrate our
approach with two examples. In particular, we show that the hedonic utility
(`happiness') can exhibit chaotic behavior.Comment: 28 pages, 6 figures, submitte
On the geometry of wave solutions of a delayed reaction-diffusion equation
The aim of this paper is to study the existence and the geometry of positive
bounded wave solutions to a non-local delayed reaction-diffusion equation of
the monostable type.Comment: 25 pages, several important modifications are made. Some references
added to the previous versio
Traveling waves for a model of the Belousov-Zhabotinsky reaction
Following J.D. Murray, we consider a system of two differential equations
that models traveling fronts in the Noyes-Field theory of the
Belousov-Zhabotinsky (BZ) chemical reaction. We are also interested in the
situation when the system incorporates a delay . As we show, the BZ
system has a dual character: it is monostable when its key parameter and it is bistable when . For , and for each
admissible wave speed, we prove the uniqueness of monotone wavefronts. Next, a
concept of regular super-solutions is introduced as a main tool for generating
new comparison solutions for the BZ system. This allows to improve all
previously known upper estimations for the minimal speed of propagation in the
BZ system, independently whether it is monostable, bistable, delayed or not.
Special attention is given to the critical case which to some extent
resembles to the Zeldovich equation.Comment: 23 pages, to appear in the Journal of Differential Equation
Pushed traveling fronts in monostable equations with monotone delayed reaction
We study the existence and uniqueness of wavefronts to the scalar
reaction-diffusion equations with monotone delayed reaction term and . We are mostly interested in the situation when the graph of is not
dominated by its tangent line at zero, i.e. when the condition , is not satisfied. It is well known that, in such a case, a
special type of rapidly decreasing wavefronts (pushed fronts) can appear in
non-delayed equations (i.e. with ). One of our main goals here is to
establish a similar result for . We prove the existence of the minimal
speed of propagation, the uniqueness of wavefronts (up to a translation) and
describe their asymptotics at . We also present a new uniqueness
result for a class of nonlocal lattice equations.Comment: 17 pages, submitte
Slowly oscillating wave solutions of a single species reaction-diffusion equation with delay
We study positive bounded wave solutions u(t,x)=ϕ(ν⋅x+ct), ϕ(−∞)=0, of equation ut(t,x)=δu(t,x)−u(t,x)+g(u(t−h,x)), x∈Rm(*). It is supposed that Eq. (∗) has exactly two non-negative equilibria: u1≡0 and u2≡κ>9. The birth function g∈C(R+,R+) satisfies a few mild conditions: it is unimodal and differentiable at 0,κ. Some results also require the positive feedback of g:[g(maxg),maxg]→R+ with respect to κ. If additionally ϕ(+∞)=κ, the above wave solution u(t,x) is called a travelling front. We prove that every wave ϕ(ν⋅x+ct) is eventually monotone or slowly oscillating about κ. Furthermore, we indicate c∗∈R+∪+∞ such that (∗) does not have any travelling front (neither monotone nor non-monotone) propagating at velocity c>c∗. Our results are based on a detailed geometric description of the wave profile ϕ. In particular, the monotonicity of its leading edge is established. We also discuss the uniqueness problem indicating a subclass G of ’asymmetric’ tent maps such that given g∈G, there exists exactly one travelling front for each fixed admissible speed