Analysis of periodic solutions of a continuous dynamical system with delay and pumping

2009 ◽  
Vol 45 (2) ◽  
pp. 168-174
Author(s):  
A. A. Seslavin
1983 ◽  
Vol 50 (4a) ◽  
pp. 858-862 ◽  
Author(s):  
C. S. Hsu ◽  
R. S. Guttalu

An index evaluation method is discussed in this paper. It can also serve as the basis of a procedure to locate all the zeros of a vector function. An application of the procedure is made to a strongly nonlinear point-mapping dynamical system in order to locate all the periodic solutions of period one and period two, 41 in total number.


2013 ◽  
Vol 63 (4) ◽  
Author(s):  
Xiaoxia Yang ◽  
Haibo Chen

AbstractIn this paper, some existence theorems are obtained for periodic solutions of second order dynamical system with (q, p)-Laplaician by using the least action principle and the saddle point theorem. Our results improve Pasca and Tang’ results.


1999 ◽  
Vol 3 (1) ◽  
pp. 57-63 ◽  
Author(s):  
Michael I. Gil' ◽  
Sui Sun Cheng

LetCnbe the set ofncomplex vectors endowed with a norm‖⋅‖Cn. LetA,Bbe two complexn×nmatrices andτa positive integer. In the present paper we consider the nonlinear difference equation with delay of the typeuk+1=Auk+Buk−τ+Fk(uk,uk−τ),      k=0,1,2,…, whereFk:Cn×Cn→Cnsatisfies the condition‖Fk(x,y)‖Cn≤p‖x‖Cn+q‖y‖Cn,       k=0,1,2,…, wherepandqare positive constants. In this paper, absolute stability conditions for this equation are established.


2021 ◽  
Vol 2021 ◽  
pp. 1-7
Author(s):  
Junning Cai ◽  
Minzhi Wei ◽  
Liping He

In this paper, we consider the KP-MEW(3,2) equation by the bifurcation theory of dynamical systems when integral constant is considered. The corresponding traveling wave system is a singular planar dynamical system with one singular straight line. The phase portrait for c < 0 , 0 < c < 1 , and c > 1 is drawn. Exact parametric representations of periodic peakon solutions and smooth periodic solution are presented.


2019 ◽  
Vol 24 ◽  
pp. 01014 ◽  
Author(s):  
Alexander G. Tatashev ◽  
Marina V. Yashina

A deterministic continuous dynamical system is considered. This system contains two contours. The length of theith contour equalsci,i= 1, 2. There is a moving segment (cluster) on each contour. The length of the cluster, located on theith contour, equalsli,i= 1, 2. If a cluster moves without delays, then the velocity of the cluster is equal to 1. There is a common point (node) of the contours. Clusters cannot cross the node simultaneously, and therefore delays of clusters occur. A set of repeating system states is called a spectral cycle. Spectral cycles and values of average velocities of clusters have been found. The system belongs to a class of contour systems. This class of dynamical systems has been introduced and studied by A.P. Buslaev.


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