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Multi bifurcation

Next, consider the case with p = 0.02014. The traverse across Fig. 12.6(a) as r is varied now also cuts the region of multi stability. It passes above the cusp point C (see Fig. 12.5), giving rise to two turning points in the stationary-state locus, but below the double-zero eigenvalue point M. There are still four intersections with the Hopf curve, so there are four points of Hopf bifurcation. The Hopf point at highest r is now a subcritical bifurcation. The dependence of the reaction rate on r for this system is shown in Fig. 12.6(d). [Pg.329]

Specifically, in Chapter 3 we create a surface for a transcendental function /(a, y) as an elevation matrix whose zero contour, expressed numerically as a two row matrix table of values, solves the nonlinear CSTR bifurcation problem. In Chapter 6 we investigate multi-tray processes via matrix realizations in Chapter 5 we benefit from the least squares matrix solution to find search directions for the collocation method that helps us solve BVPs and so on. Matrices and vectors are everywhere when we compute numerically. That is, after the laws of physics and chemistry and differential equations have helped us find valid models for the physico-chemical processes. [Pg.534]

Bifurcation Multi-laminating Diffusive Mixing Most Relevant Citations... [Pg.98]

Mixer 35 [M 35] Bifurcation Multi-laminating Micro Mixer... [Pg.99]

Mixer type Bifurcation multi-laminating micro mixer Channel width 49-58 pm... [Pg.100]

Fig. 5.43. Schematic bifurcation diagram for CH3CHO + O2 reaction showing separate branches corresponding to dark reaction and steady glow, with upper branch losing stability at a Hopf bifurcation as Ta is reduced to give limit cycle (cool-flame) oscillations. The simple limit cycle also loses stability as is reduced further and a complex oscillation corresponding to the multi-stage ignition will emerge but cannot be adequately represented... Fig. 5.43. Schematic bifurcation diagram for CH3CHO + O2 reaction showing separate branches corresponding to dark reaction and steady glow, with upper branch losing stability at a Hopf bifurcation as Ta is reduced to give limit cycle (cool-flame) oscillations. The simple limit cycle also loses stability as is reduced further and a complex oscillation corresponding to the multi-stage ignition will emerge but cannot be adequately represented...
The bifurcation mechanisms for formation of multi-slip fault zones suggest that maximum fault zone thickness will often correspond to the strike-normal distance between the traces of two overlapping slip surfaces (Fig. 2c). Fault overlaps and their breached equivalents occur on faults of all sizes as do, by implication, paired and multi-slip surface fault zones. Complex and paired slip surface fault zone structures will occur on scales below that resolvable by even high quality seismic data (lateral resolution is no better than 50-100 m at North Sea reservoir depths). The possible impact of sub-seismic complexity and paired slip surfaces on connectivity and sealing across faults offsetting an Upper Brent type sequence are briefly considered below. [Pg.65]

Fig. 16.1. Curved multi-planar reconstruction of CT of the thoracic aorta, clearly demonstrating the origin arrowhead) and bifurcation into intercostal branches and bronchial artery arrow) of right inter-costobronchial trunk... Fig. 16.1. Curved multi-planar reconstruction of CT of the thoracic aorta, clearly demonstrating the origin arrowhead) and bifurcation into intercostal branches and bronchial artery arrow) of right inter-costobronchial trunk...
Chapter 8. Bifurcation Phenomenon and Multi-stability which can be simplified to the model reaction system... [Pg.131]

Similar oscillation using a single capillary in place of membrane for the first time has also been reported recently using solutions of non-electrolytes [15]. Current is the bifurcation parameter as in the previous case. Multi-periodic oscillations are observed in case of solution of urea. In the above case, the electro-osmotic flow in one direction and hydrodynamic flow in the other direction are responsible for oscillations. Nonlinearity is imposed by concentration difference across the membrane. This point will be discussed in greater depth in the subsequent section. [Pg.192]

In the non-linear region, exotic non-equilibrium phenomena such as bifurcation from steady state to bistability and oscillations (in time and space) are observed. New mathematical methodology based on non-linear dynamics has been evolved for investigating such phenomena as discussed in Chapter 8. The essential point to note is that such complex phenomena arise when more than three forces are evolved in addition to the occurrence of multi-process as discussed in Parts Two and Three. Bifurcation process... [Pg.316]

Equilibrium state —Linear steady state close to equilibrium —Steady state —> Non-linear steady state — Bifurcation phenomena —> Multi-stability —> Temporal and spatio-temporal oscillations —> More complex situations (chaos, turbulence, pattern formation, fractal growth). All these stages have been discussed in different chapters of the book. [Pg.350]


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See also in sourсe #XX -- [ Pg.98 ]




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BIFURCATION PHENOMENON AND MULTI-STABILITY

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Bifurcation Multi-laminating Diffusive Mixing

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