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Alpha limit set

Now let jt ) be a sequence of real numbers which tends to negative infinity as n tends to infinity. If P = ir(x, t ) converges to a point P, then P is said to be an alpha limit point of x. The set of all such alpha limit points is called the alpha limit set of x, denoted a(x). It enjoys similar properties if the trajectory lies in a compact set for t < 0. [Pg.8]

Theorem C.7 bears a strong resemblance to the Poincare-Bendixson theorem stated in Chapter 1. It will be used in Chapter 4 for the case where (C.l) is a competitive system, that is, for a system (C.l) where -/ is cooperative. Note that the omega (alpha) limit set of a competitive system is the alpha (omega) limit set of the time-reversed cooperative system, so Theorems C.5, C.6, and C.7 apply to competitive systems. Unlike cooperative systems, competitive systems can have attracting periodic orbits. For more on the Poincare-Bendixson theory of competitive and cooperative systems in see [S3], [SWl], and [ZS]. [Pg.275]

We review the basic definitions and set up the semidynamical system appropriate for systems of the form (D.l). Let A" be a locally compact metric space with metric d, and let be a closed subset of X with boundary dE and interior E. The boundary, dE, corresponds to extinction in the ecological problems. Let tt be a semidynamical system defined on E which leaves dE invariant. (A set B in A" is said to be invariant if n-(B, t) = B.) Dynamical systems and semidynamical systems were discussed in Chapter 1. The principal difficulty for our purposes is that for semidynamical systems, the backward orbit through a point need not exist and, if it does exist, it need not be unique. Hence, in general, the alpha limit set needs to be defined with care (see [H3]) and, for a point x, it may not exist. Those familiar with delay differential equations are aware of the problem. Fortunately, for points in an omega limit set (in general, for a compact invariant set), a backward orbit always exists. The definition of the alpha limit set for a specified backward orbit needs no modification. We will use the notation a.y(x) to denote the alpha limit set for a given orbit 7 through the point x. [Pg.278]

According to Theorem C.6, the limit set can be deformed to a compact invariant set A, without rest points, of a planar vector field. By the Poin-care-Bendixson theorem, A must contain at least one periodic orbit and possibly entire orbits which have as their alpha and omega limits sets distinct periodic orbits belonging to A. Using the fact that A is chain-recurrent, Hirsch [Hil] shows that these latter orbits cannot exist. Since A is connected it must consist entirely of periodic orbits that is, it must be an annulus foliated by closed orbits. Monotonicity is used to show... [Pg.274]

Figure 2.9. The confidence interval for an individual result CI( 3 ) and that of the regression line s CLj A are compared (schematic, left). The information can be combined as per Eq. (2.25), which yields curves B (and S, not shown). In the right panel curves A and B are depicted relative to the linear regression line. If e > 0 or d > 0, the probability of the point belonging to the population of the calibration measurements is smaller than alpha cf. Section 1.5.5. The distance e is the difference between a measurement y (error bars indicate 95% CL) and the appropriate tolerance limit B this is easy to calculate because the error is calculated using the calibration data set. The distance d is used for the same purpose, but the calculation is more difficult because both a CL(regression line) A and an estimate for the CL( y) have to be provided. Figure 2.9. The confidence interval for an individual result CI( 3 ) and that of the regression line s CLj A are compared (schematic, left). The information can be combined as per Eq. (2.25), which yields curves B (and S, not shown). In the right panel curves A and B are depicted relative to the linear regression line. If e > 0 or d > 0, the probability of the point belonging to the population of the calibration measurements is smaller than alpha cf. Section 1.5.5. The distance e is the difference between a measurement y (error bars indicate 95% CL) and the appropriate tolerance limit B this is easy to calculate because the error is calculated using the calibration data set. The distance d is used for the same purpose, but the calculation is more difficult because both a CL(regression line) A and an estimate for the CL( y) have to be provided.
For the composition Pd2H there are no atoms in the alpha phase. We have set the composition 0.5 H/Pd ratio as the limit of the beta phase in accord with the numerology of the model. Consideration of the d-band places this figure at 0.60. However, the hydrogen atoms themselves will modify the lattice and it is difficult to get a consistent model of the beta phase which gives it a composition other than H/Pd = 0.5 (6). Obviously the neutron diffraction data require a composition Pd/H = 0.5. [Pg.116]

The two principal disadvantages of using Po as an export tracer are its half-hfe and the labor-intensive nature of its measurements. The half-life of °Po (138 d) is substantially greater than the timescale for seasonal phytoplankton blooms. Consequently, the amplitude of the seasonal cycle of scavenging and export will be damped by the time constant for °Po production and decay. Application of the °Po method requires independent determination of °Pb and °Po concentrations, both of which are labor intensive. Typically, °Po is determined by isotope dilution alpha spectrometry, and °Pb isolated from the sample is set aside for several months to permit ingrowth of °Po, which is measured a second time to evaluate the concentration of °Pb. Despite these limitations, if further studies confirm that Po is a more specific tracer than thorium for POC, and if it can be demonstrated... [Pg.3109]

EPA sets health-based limits on radiation in air, soil, and water. Federal government agencies are required to meet EPA standards the same as commercial industries. Using its authority under the Safe Drinking Water Act, EPA limits the amount of radiation in community water systems by establishing maximum contaminant levels. Maximum Contaminant Levels limit the amount of activity from alpha emitters, like plutonium, to 15 picocuries per liter. [Pg.266]

In case of the metallocene-catalyzed random copolymer of ethylene and alpha-olefin (POP and POE), incorporating more comonomer along the polymer backbone reduces density and crystallinity and hence, increases flexibility and softness. However, as the density is decreased, the melting point, crystallization peak temperature and heat resistance decrease and cycle times in injection molding increase. These deficiencies have limited the use of POEs in applications where heat resistance, high temperature compression set, and faster cycle times are desired. [Pg.92]

In the above equation, Zg, is the required percentile of the distribution and will be considered as a variable for adjustment. In details, to set the lower control limit and upper control limit, the pth percentile and the th percentile are considered so as to give the preset alpha value of 0.0027. [Pg.516]

If fluids are limited, the kidneys set into play a mechanism which conserves water. They secrete renin, an enzyme which initiates the conversion of a bloodborne protein (an alpha-globulin) to angiotension II, a hormonelike substance. The latter substance stimulates the adrenal cortex to secrete aldosterone—a hormone which causes the retention of water and sodium by the kidney and a reduction in the amount of urine volume. [Pg.989]


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See also in sourсe #XX -- [ Pg.8 ]




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