BIFURCATION STRUCTURE IN PARAMETER PLANE OF GEAR SYSTEM

2006 ◽  
Vol 42 (03) ◽  
pp. 68
Author(s):  
Zhiying GAO
1991 ◽  
Vol 01 (02) ◽  
pp. 339-348 ◽  
Author(s):  
C. MIRA ◽  
J. P. CARCASSÈS ◽  
M. BOSCH ◽  
C. SIMÓ ◽  
J. C. TATJER

The areas considered are related to two different configurations of fold and flip bifurcation curves of maps, centred at a cusp point of a fold curve. This paper is a continuation of an earlier one devoted to parameter plane representation. Now the transition is studied in a thee-dimensional representation by introducing a norm associated with fixed or periodic points. This gives rise to complete information on the map bifurcation structure.


1991 ◽  
Vol 01 (01) ◽  
pp. 183-196 ◽  
Author(s):  
J. P. CARCASSES ◽  
C. MIRA ◽  
M. BOSCH ◽  
C. SIMÓ ◽  
J. C. TATJER

This paper is devoted to the bifurcation structure of a parameter plane related to one- and two-dimensional maps. Crossroad area and spring area correspond to a characteristic organization of fold and flip bifurcation curves of the parameter plane, involving the existence of cusp points (fold codimension-two bifurcation) and flip codimension-two bifurcation points. A transition "mechanism" (among others) from one area type to another one is given from a typical one-dimensional map.


1998 ◽  
Vol 08 (07) ◽  
pp. 1413-1435 ◽  
Author(s):  
J. Farjas ◽  
R. Herrero ◽  
F. Pi ◽  
G. Orriols

The response of a self-oscillating opto-thermal device irradiated with modulated light is investigated both numerically and experimentally. The subharmonic bifurcation structure of the amplitude-frequency parameter plane is analyzed and a variety of local and global codimension-2 bifurcations are characterized. A detailed study of the dynamics transformation around these points is also provided.


1996 ◽  
Vol 06 (08) ◽  
pp. 1463-1480
Author(s):  
NATHALIE GICQUEL

This paper concerns the bifurcation properties of a D.P.C.M. transmission system with an order-2 transversal predictor. These properties are related to the organization of some bifurcation curves in a parameter plane.


1991 ◽  
Vol 01 (04) ◽  
pp. 823-838 ◽  
Author(s):  
DANIÈLE FOURNIER-PRUNARET

The considered endomorphism is [Formula: see text] This paper studies the bifurcations structure in the parameter plane (a, b). A mixing is made to appear between two types of structures: the "boxes in files" structure, which exists for the diffeomorphism of the circle onto itself, and the "box within a box" structure, which appears for the quadratic one-dimensional endomorphism.


1993 ◽  
Vol 03 (04) ◽  
pp. 903-919 ◽  
Author(s):  
C. MIRA ◽  
H. KAWAKAMI ◽  
R. ALLAM

In a parameter plane defined by two parameters of a map, the dovetail bifurcation structure is a bifurcation curve organization, for which two fold cusps have a fold bifurcation segment in common. This gives rise to the association of either a crossroad area with a saddle area or a spring area with a saddle area. This paper describes this structure in the parameter plane for different configurations, and in the corresponding three-dimensional representations of the plane sheets. Then it identifies six different qualitative changes of this structure when a third parameter varies.


2021 ◽  
Vol 31 (16) ◽  
Author(s):  
Iryna Sushko ◽  
Viktor Avrutin ◽  
Laura Gardini

We consider the well-known Lozi map, which is a 2D piecewise linear map depending on two parameters. This map can be considered as a piecewise linear analog of the Hénon map, allowing to simplify the rigorous proof of the existence of a chaotic attractor. The related parameter values belong to a part of the parameter plane where the map has two saddle fixed points. In the present paper, we investigate a different part of the parameter plane, namely, the vicinity of the curve related to a center bifurcation of the fixed point. A distinguishing property of the Lozi map is that it is conservative at the parameter value corresponding to this bifurcation. As a result, the bifurcation structure close to the center bifurcation curve is quite complicated. In particular, an attracting fixed point (focus) can coexist with various attracting cycles, as well as with chaotic attractors, and the number of coexisting attractors increases as the parameter point approaches the center bifurcation curve. The main result of the present paper is related to the rigorous description of this bifurcation structure. Specifically, we obtain, in explicit form, the boundaries of the main periodicity regions associated with the pairs of complementary cycles with rotation number [Formula: see text]. Similar approach can be applied to other periodicity regions. Our study contributes also to the border collision bifurcation theory since the Lozi map is a particular case of the 2D border collision normal form.


1994 ◽  
Vol 04 (03) ◽  
pp. 737-739 ◽  
Author(s):  
M.W. OLESEN ◽  
C. KNUDSEN

A three-parameter numerical bifurcation analysis of the forced Brusselator model is performed. Keeping one parameter fixed the bifurcation structure in the frequency-amplitude parameter plane may, or may not, contain Arnol’d tongues. The bifurcation scenario that destroys the dominant Arnol’d tongues is described.


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