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Saddle switching

Saddle switching and structural stability) Consider the system... [Pg.184]

It can be seen from the figure that the optimal force switches on at the moment when the system leaves S5 along its unstable manifold. The optimal force returns to zero when the system reaches the saddle cycle SI. [Pg.509]

Secondly, the chaotic state of a resonant system is an infinite collection of unstable periodic motions (see Figure 14.9). The basic idea of the controlling chaos is to switch a chaotic system by a small perturbation among many different periodic orbits. Ott, Grebogy and Yorke [10] developed a scheme in which a chaotic system can be forced to follow one particular unstable periodic orbit. The problem is to calculate the perturbation that will shift the system towards the desired periodic orbit. This process is similar to balancing a marble on a saddle. To keep the marble from rolling off, one needs to move the saddle quickly from side to side. And... [Pg.272]

The seven bullet tanks were equipped with a simple sprinkler system that could be switched on to spray individual tanks. Each bullet tank was equipped with safety relief valves and pneumatically operated plug valves for isolation of the inlet and outlet valves by remote control. The tanks rested on concrete saddles, but were not anchored. [10]... [Pg.102]

Please note the important difference between the saddle-node and transcritical bifurcations in the transcritical case, the two fixed points don t disappear after the bifurcation—instead they just switch their stability. [Pg.51]

The OPT occurs at p = 1 via a subcritical Hopf-type bifurcation where the system settles to a uniform precession state with a small reorientation amplitude (A 7T so that 0 system switches back to the unperturbed state at p = p] 0.88 where a saddle-node bifurcation occurs. The trajectory in the ux, Uy) plane is a circle whereas, in a coordinate system that rotates with frequency /o around the z axis, it is a fixed point. The time Fourier spectra of the director n have one fundamental frequency /o, whereas 0 , 4> and A do not depend on time. [Pg.101]

The testing of an installation implies the use of instruments to obtain readings. However, a test is unlikely to identify a cracked socket outlet, a chipped or loose switch plate or a missing conduit-box lid or saddle, so it is also necessary to make a visual inspection of the installation. [Pg.301]

The table movement (x axis) is manual via the handwheel, or hydraulic for automatic reciprocation. The saddle cross-slide movement (y axis) and wheel downfeed (z axis) are controlled by digital AC servo motors. Table reversal is set by adjustable table dogs and proximity switches in the saddle. [Pg.147]


See other pages where Saddle switching is mentioned: [Pg.16]    [Pg.16]    [Pg.6]    [Pg.485]    [Pg.262]    [Pg.382]    [Pg.332]    [Pg.332]    [Pg.275]    [Pg.285]    [Pg.378]    [Pg.275]    [Pg.285]    [Pg.196]    [Pg.94]    [Pg.386]    [Pg.220]    [Pg.220]    [Pg.174]    [Pg.120]    [Pg.132]    [Pg.245]    [Pg.155]    [Pg.205]    [Pg.1216]    [Pg.508]    [Pg.111]    [Pg.128]    [Pg.162]    [Pg.229]    [Pg.332]    [Pg.723]    [Pg.205]    [Pg.163]    [Pg.59]   
See also in sourсe #XX -- [ Pg.184 ]




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