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Asymptotic normal form

The system (C.2.24) is the asymptotic normal form appearing in the study [129] of local codimension-three bifurcations of equilibria and periodic orbits of systems with a symmetry (see Sec. C.4). When H = 0, system (C.2.24) is the Shimizu-Morioka model [127], [191]... [Pg.469]

An analogous algorithm can be applied to the multi-dimensional case. The limit of the rescaled system as governing parameters tend to zero gives a description in the main order of the behavior of the system near a bifurcation point. Such a limit system is called an asymptotic normal form. [Pg.490]

The situation becomes different when one considers normal forms of higher dimensions. Three- (and higher) dimensional asymptotic normal forms may exhibit non-trivial dynamics by themselves. For example, a homoclinic loop to the saddle-focus was found in the asymptotic normal form... [Pg.490]

C.4. 53. Below we present (following [185]) a list of asymptotic normal forms which describe the trajectory behavior of a triply-degenerate equilibrium state near a stability boundary in systems with discrete symmetry. We say there is a triple instability when a dynamical system has an equilibrium state such that the associated linearized problem has a triplet of zero eigenvalues. In such a case, the analysis is reduced to a three-dimensional system on the center manifold. Assuming that (x, y, z) are the coordinates in the three-dimensional center manifold and a bifurcating equilibrium state resides at the origin, we suppose also that our system is equivariant with respect to the transformation (x,y,z) <- (-X, -y, z). [Pg.501]

The asymptotic normal form is a finite limit of the system (C.4.19) as /X 0. Note that different choices of proportion between the scaling factors Sx and r yield different normal forms. [Pg.502]

By repeating this procedure we can get a hierarchy of the asymptotic normal forms. Let us denote... [Pg.504]

Pisarevskii, V., Shilnikov, A. L. and Turaev, D. V. [1998] Asymptotic normal forms for equilibria with a triplet of zero charactersitic exponents in systems with symmetry . Regular and Chaotic Dynamics 3(1), 19-27. [Pg.573]

The beauty of this completely random approach to the analyte detection limit is the direct applicability of the statistical hypothesis testing formalism. Also, long-term trends in calibration slope or backgrounds have little influence. One important assumption is made that the form of the calibration curve [Equation 2c] is fixed. Also, a subtle change has occurred, the operation is no longer linear, with A in the denominator. Thus, the distribution of x is only asymptotically normal, as the relative standard deviation of becomes smaller. [Pg.55]

Plot the given lab-scale data using both the normal and the logarithmic forms of the Freundlich equation (see Figures 91 and 92). Plot the normal form to check if the data approach an asymptote representing a maximum capacity. Plot the logarithmic form and check to determine how straight the line is. [Pg.586]

By combining the exponential form of the electronic normalized density for the asymptotic density form in the valence electrons region with the electronegativity main domain frontier contribution above, the effective Wang-Parr (WP) electronegativity expression may be written as ... [Pg.262]

ILS experiments indicate a semi-rigid behavior for the PDA chains. Therefore we can expect to observe the form factor of the Porod-Kratky chain. More precisely, the q scattering behavior of a rod like molecule should be measured since the normalize form factor P( of an infinitely long worm-like chain has the asymptotic form ... [Pg.272]

When long drying time is required to reach asymptotic moisture in the cake. On Drum Filters, for example, the ratio of dry to form cannot normally exceed 1.5 since it is determined by its geometry and the number of circumferential compartments. [Pg.210]

After normalization to the asymptotic baseline, g2(r) decays from two to unity if measured with a perfect instrument. A real instrument always suffers from some loss of coherence, and for a monodisperse solution of ideal, non-interacting solute molecules the intensity autocorrelation function g2(r) takes the form... [Pg.225]

We start our derivation by writing down the explicit form of the vacuum asymptote of a tip wavefunction (as well as its vacuum continuation in the tip body). As we have explained in Section 5.3, for the simplicity of relevant mathematics, the rather complicated normalization constants of the spherical harmonics are absorbed in the expression of the sample wavefunction. Up to 1=2, we define the coefficients of the expansion by the following expression ... [Pg.86]

Based on a sample of 65 observations from a normal distribution, you obtain a median of 34 and a standard deviation of 13.3. Form a confidence interval for the mean. (Hint Use the asymptotic distribution. See Example 4.15.) Compare your confidence interval to the one you would have obtained had the estimate of 34 been the sample mean instead of the sample median. [Pg.136]

In Figure 31 we have displayed a comparison between the calculated and observed values of dfldE for benzene. As mentioned in the main text, inclusion of the structure factor leads to a large deviation between calculations and observations. Now, the structure factor influences the normalization of the wave function, which normalization involves only the asymptotic form of the wave function. Examination of the relevant formula for dfjdE shows that it is necessary that there be very accurate... [Pg.299]

The last normalization means that one electron can be found within an interval of one energy unit centred around the value e. For the asymptotic form of ReAr) one gets (in atomic units)... [Pg.289]

The last term here does not vanish even if ma = 0. The nonhermitian part of mfj1 comes from the free-free matrix of H — E, which is characteristic of scattering theory. When channel orbital functions are normalized to unit flux, with the asymptotic forms specified above, this nonhermitian term is given by... [Pg.137]

The function / can be arbitrarily normalized, because [tan / ] is homogeneous in /. There is no constraint on the asymptotic form of trial functions, because they have no effect outside the range of the assumed short-range potential Av. Only the regular model functions wq occur explicitly in the theory, although the irregular functions w i must be consistent with the asymptotic character of the Green function, and may be used to construct it. [Pg.142]

These radical functions are normalized according to equ. (7.28c).) Knowing these asymptotic forms, it is now possible to derive the asymptotic limits for the ansatz in equ. (7.21) and the boundary condition in equ. (7.20). A comparison of these expressions will then lead to the unknown coefficients b K) in equ. (7.21) and the scattering amplitude in equ. (7.20). If one starts with the plane-wave part... [Pg.287]

In general, adsorption isotherms obtained with this and other zeolitic substrates are of Brunauer s Type I, the simple hyperbolic form also known as the Langmuir isotherm. Consequently, the asymptotic limit of adsorption is used instead of the value of Vm normally derived from the BET evaluation of specific surface area. It is, of course, not possible to define exact monolayer or multilayer adsorption in these three-dimensional interconnected pore systems. [Pg.128]

In order to elucidate the correlation method it may be recalled that the viscosity 77 approaches asymptotically to the constant value r c with decreasing shear rate q. Similarly, the characteristic time t approaches a constant value xQ and the shear modulus G has a limiting value G0 at low shear rates. Bueche already proposed that the relationship between 77 and q be expressed in a dimensionless form by plotting 77/r]0 as a function of qx. According to Vinogradov, also the ratio t/tq is a function of qxQ. If the zero shear rate viscosity and first normal stress are determined, then a time constant x0 may be calculated with the aid of Eqs. (15.60). This time constant is sometimes used as relaxation time, in order to be able to produce general correlations between viscosity, shear modulus and recoverable shear strain as functions of shear rate. [Pg.556]


See other pages where Asymptotic normal form is mentioned: [Pg.490]    [Pg.490]    [Pg.498]    [Pg.505]    [Pg.525]    [Pg.490]    [Pg.490]    [Pg.498]    [Pg.505]    [Pg.525]    [Pg.308]    [Pg.567]    [Pg.212]    [Pg.333]    [Pg.315]    [Pg.162]    [Pg.279]    [Pg.559]    [Pg.1344]    [Pg.508]    [Pg.516]    [Pg.616]    [Pg.267]    [Pg.8]    [Pg.206]    [Pg.81]    [Pg.286]    [Pg.265]    [Pg.287]    [Pg.351]   


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