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Stable leading manifold

If hydrogen adds to 7 in accord with the mechanism depicted in Scheme 12.2, then the final hydrogenation product should be /V-acctyl-(.S>phenylalaninc ethyl ester (10, Scheme 12.3). Halpem found, however, that the predominant product in the presence of CHIRAPHOS was the //-enantiomer (10", Scheme 12.3) Based on this result and other evidence, it was possible for Halpem to say that 7 and 7" form as an equilibrium mixture rapidly and reversibly from reaction of 5 and 6. Although 7 is more stable than 7", and thus is part of what Halpem termed the major manifold shown in Scheme 12.3, the less stable minor manifold isomer (7") reacts much faster during rate-determining oxidative addition of H2, eventually leading to the //-amino acid derivative. [Pg.530]

Here the fixed point is asymptotically stable. All trajectories apart belonging to the non-leading manifold x = 0 enter O along the leading direction... [Pg.117]

If Lk < 0, then for the original multi-dimensional map (10.4.1), the fixed point is also a stable focus. Moreover, its leading manifold coincides with the center manifold. This means that all positive semi-trajectories, excluding those in the non-leading manifold tend to O along spirals which are... [Pg.129]

Remark. In the multi-dimensional case where besides the central coordinates there are also the stable ones, the unstable set consists of three curves, whereas the stable set is a bimch consisting of three semi-planes intersecting along the non-leading manifold as shown in Fig. 10.5.4, for the three-dimensional example. [Pg.142]

Fig 11.5.4. supercritical Andronov-Hopf bifurcation in R . The stable focus (the leading manifold jg two-dimensional) in (a) becomes a saddle-focus in (b). A stable periodic orbit is the edge of the unstable manifold W. ... [Pg.235]

Although unstable, this periodic orbit is an example of classical motion which leaves the molecule bounded. Other periodic and nonperiodic trajectories of this kind may exist at higher energies. The set of all the trajectories of a given energy shell that do not lead to dissociation under either forwarder backward-time propagation is invariant under the classical flow. When all trajectories belonging to this invariant set are unstable, the set is called the repeller [19, 33, 35, 48]. There also exist trajectories that approach the repeller in the future but dissociate in the past, which form the stable manifolds of the repeller Reciprocally, the trajectories that approach the... [Pg.543]

Here, we mention only two possibilities, though we could have other cases. The hrst is that the condition of normal hyperbolicity breaks down for some NHIMs. Then, what happens to those NHIMs Do they bifurcate into other NHIMs, or do they disappear at all The second possibility is that intersections between the stable and unstable manifolds of NHIMs change into tangency. This could lead to bifurcation in the way NHIMs are connected by their stable and unstable manifolds. [Pg.341]

Equation (64) shows that the distance d x,a) exhibits an oscillatory dependence as a function of x. In other words, d x, a) changes between plus and minus values as initial conditions shift on the separatrix. This means that the stable and unstable manifolds have transverse intersections. See Fig. 14 showing how the oscillatory change of the integral implies the occurrence of transverse intersections. The existence of transverse intersections between stable and unstable manifolds leads to horseshoe dynamics—that is, chaos. Thus, the Melnikov integral given by Eq. (64) indicates that this system exhibits chaotic behavior. [Pg.368]

The extreme toxicity of lead results from the manifold modes of activity. In the stable state, >90% of total body lead is stored in the skeleton. Lead appears to have the capacity to seek out areas of active bone formation, where it occupies lattice interstices or exchanges with calcium in the bone... [Pg.2357]

The phase portrait has an interesting biological interpretation. It shows that one species generally drives the other to extinction. Trajectories starting below the stable manifold lead to eventual extinction of the sheep, while those starting above lead to eventual extinction of the rabbits. This dichotomy occurs in other models of competition and has led biologists to formulate the principle of com-... [Pg.158]

In order to make more direct correspondence between tangency and global changes in the dynamical behavior, we propose to use different methods to characterize chaos. The first one focuses attention on how normally hyperbolic invariant manifolds are connected with each other by their stable and unstable manifolds. Then, crisis would lead to a transition in their connections. The second one is to characterize chaos based on how unstable manifolds are folded as they approach normally hyperbolic invariant manifolds. Then, crisis would manifest itself as a change in their folding patterns. Let us explain these ideas in more detail. [Pg.176]


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See also in sourсe #XX -- [ Pg.128 ]




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