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Lamerey diagram

If li < 0, then the fixed point at the origin is stable for // < 0 and attracts all trajectories from any small neighborhood. When > 0, the fixed point becomes imstable and the stable period-two point bifurcates from it see Fig. 11.4.1 illustrating the corresponding Lamerey diagrams. [Pg.213]

Let us now consider the case A < 0 in more detail. First, let us examine the associated Lamerey diagram (Fig. 13.2.6) with A < 0 when i/ > 1 (A -h7 < 0). Just as in the orientable case, a stable fixed point exists for // > 0 indeed, the map T is decreasing and contracting, so the interval [0, a p) = T(0)] is mapped into the inside itself by T, which implies the existence of a unique stable fixed point on this interval by virtue of the Banach contraction mapping principle. [Pg.339]

Fig. 13.2.6. Lamerey diagram of the Poincare map for the non-orientable separatrix loop with (Tq < 0. Fig. 13.2.6. Lamerey diagram of the Poincare map for the non-orientable separatrix loop with (Tq < 0.
Fig. 13.2.7. Lamerey diagram for the non-orientable separatrix loop to a seuidle with (Tq > 0. Fig. 13.2.7. Lamerey diagram for the non-orientable separatrix loop to a seuidle with (Tq > 0.
Fig. 13.3.2. Lamerey diagram corresponding to the double separatrix loop. Fig. 13.3.2. Lamerey diagram corresponding to the double separatrix loop.
The Lamerey diagrams for this map are shown in Fig. 13.6.5. The right-hand side of the map is either monotonically increasing (when —n/2 < (j) < tt/2), or monotonically decreasing (when 7t/2 < < < Sir/2). Such maps may have only... [Pg.388]


See other pages where Lamerey diagram is mentioned: [Pg.112]    [Pg.113]    [Pg.122]    [Pg.193]    [Pg.210]    [Pg.220]    [Pg.337]    [Pg.338]    [Pg.338]    [Pg.339]    [Pg.363]    [Pg.389]    [Pg.112]    [Pg.113]    [Pg.122]    [Pg.193]    [Pg.210]    [Pg.220]    [Pg.337]    [Pg.338]    [Pg.338]    [Pg.339]    [Pg.363]    [Pg.389]   
See also in sourсe #XX -- [ Pg.116 , Pg.480 , Pg.490 , Pg.561 , Pg.578 , Pg.581 , Pg.588 ]




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