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Asymptotic theory

Although at the time of its publication (1928) the asymptotic theory of Li6nard was not given serious consideration, about 20 years later it became of importance in the development of the asymptotic theory (see Part IV). [Pg.338]

Arcsine distribution, 105, 111 Assumption of molecular chaos, 17 Asymptotic theory, 384 of relaxation oscillations, 388 Asynchronous excitation, 373 Asynchronous quenching, 373 Autocorrelation function, 146,174 Autocovariance function, 174 Autonomous problems, 340 nonresonance oscillations, 350 resonance oscillations, 350 Autonomous systems, 356 problems of, 323 Autoperiodic oscillation, 372 Averages, 100... [Pg.769]

Optimal flow method, 261 Optimization non-constrained, 286 of functionals, 305 Ordinary value, 338 Orthogonalization, Schmidt," 65 Osaki, S., 664 Oscillation hysteresis, 342 Oscillations autoperiodic, 372 discontinuous theory, 385 heteroperiodic, 372 piecewise linear, 390 relaxation asymptotic theory, 388 relaxation, 383 Oscillatory circuit, 380 "Out field, 648 existence of, 723... [Pg.780]

Rate of change of observables, 477 Ray in Hilbert space, 427 Rayleigh quotient, 69 Reduction from functional to algebraic form, 97 Regula fold method, 80 Reifien, B., 212 Relative motion of particles, 4 Relative velocity coordinate system and gas coordinate system, 10 Relativistic invariance of quantum electrodynamics, 669 Relativistic particle relation between energy and momentum, 496 Relativistic quantum mechanics, 484 Relaxation interval, 385 method of, 62 oscillations, 383 asymptotic theory, 388 discontinuous theory, 385 Reliability, 284... [Pg.782]

Kutateladze, S. S., and A. I. Leont ev, 1966, Some Applications of the Asymptotic Theory of the T urbu-lent Boundary Layer, Proc. 3rd Int. Heat Transfer Conf, vol. 3, pp. 1-6, AIChE, New York. (5) Kutateladze, S. S., and L. G. Malenkov, 1974, Heat Transfer at Boiling and Barbotage Similarity and Dissimilarity, Proc. 5th Int. Heat Transfer Conf., Tokyo, vol. IV, p. 1. (2)... [Pg.542]

Carroll RJ, Cline DBH An asymptotic theory for weighted least squares with weights estimated by replication. Bio-metrika (1988) 75 35-43. [Pg.178]

At the Curie point, the Weiss theory predicts that for T > Te, in the absence of an external field, the spin order vanishes completely. Actually there is considerable short-range order just above Te, as has been verified by neutron diffraction experiments (405,675). It is the problem of short-range order that is tackled by the more exact quantum statistics mentioned in connection with equation 94. At very high temperatures (T Te), there is no short-range order, and the experimental curve approaches the Curie-Weiss curve asymptotically. Theory shows that the possibility of short-range ordering lowers the... [Pg.85]

For dense layers in good solvents, the asymptotic theory of Milner et al. (1988) applies, but with L = hjl. Density profiles are truncated according to... [Pg.203]

G. G. Stokes, Trans. Cambridge Philos. Soc. 10, 106 (1864) R. B. Dingle, Asymptotic Expansions Their Derivation and Interpretation, Academic Press, London, 1973 for a very recent development on the study of Stokes phenomenon, see, for example, B. Y. Sternin and V. E. Shatalov, Borel-Laplace Transform and Asymptotic Theory, CRC Press, Boca Raton, EL, 1996. [Pg.434]

See also H. K. Cheng, An Analytic, Asymptotic Theory of Shock Supported Arrhen ius Reactions and Ignition Delay in Gas, unpublished (1970) for an early version of the study in [48]. The work in [47] involves a double limit that also describes slight merging of the shock with the reaction zone. [Pg.197]

Matgolis, S. B., An asymptotic theory of heterogeneous condensed combustion. Combust. Set. Tech., 43,197 (1985). [Pg.218]

Figure 1. Spin-dependent terms Cq, —7, in Legendre expansion coefficients as functions of the interfragment distance R dashed curves from Asymptotic Theory (AT) solid curves from AT corrected to fit ah initio data. Figure 1. Spin-dependent terms Cq, —7, in Legendre expansion coefficients as functions of the interfragment distance R dashed curves from Asymptotic Theory (AT) solid curves from AT corrected to fit ah initio data.
TABLE I. Fitting quality of Asymptotic Theory after the correetion linear eonfiguration... [Pg.26]

Figure. 8. Exchange integrals I n of the Asymptotic Theory for p electrons asymptotic integrals are for the interactions of electrons from tire outer AO 2p of O with electrons from the outer MO Iti (right panel) and with electrons from the inner MO 3o (left panel) of OH. Figure. 8. Exchange integrals I n of the Asymptotic Theory for p electrons asymptotic integrals are for the interactions of electrons from tire outer AO 2p of O with electrons from the outer MO Iti (right panel) and with electrons from the inner MO 3o (left panel) of OH.
Wo consider a small parameter of expansion of the asymptotic theory... [Pg.135]

Both of these solutions for the number of expected parameters (Eqs. (5.29) and (5.31)) have been derived from asymptotic theory (27). [Pg.156]

No exact theory for protein ultrafiltration is available to test the asymptotic theory against therefore, its validity can only be inferred by how well it correlates data. The test of the data used only one adjustable parameter, the protein dlffusivity. The value calculated for D for BSA systems was compared with that in the literature. For calf serum there are no published diffusion data, and internal consistancy of results was the primary criterion for success. A patterned ear h program was used to find the least value of the sum Z[(P - several sets of... [Pg.89]

Before we turn to other topics, it is worth considering the physical events that lead to separation. There are two plausible ways to explain the phenomenon. A common feature of these two mechanisms is that viscous effects play a critical role. Experimentally, we find that separation (or at least the downstream recirculating wake that we associate with separation) usually occurs for Reynolds numbers larger than some critical value, and we infer from this that separation is basically a large-Reynolds-number phenomenon. Indeed, this point of view is consistent with the fact that separation can be predicted by boundary-layer theory, which is an asymptotic theory for Re -> oo. In spite of this, separation is a phenomenon that we can explain only by considering the consequences of viscous contributions to the motion of the fluid. [Pg.732]

Sometimes, the distribution of the statistic must be derived under asymptotic or best case conditions, which assume an infinite number of observations, like the sampling distribution for a regression parameter which assumes a normal distribution. However, the asymptotic assumption of normality is not always valid. Further, sometimes the distribution of the statistic may not be known at all. For example, what is the sampling distribution for the ratio of the largest to smallest value in some distribution Parametric theory is not entirely forthcoming with an answer. The bootstrap and jackknife, which are two types of computer intensive analysis methods, could be used to assess the precision of a sample-derived statistic when its sampling distribution is unknown or when asymptotic theory may not be appropriate. [Pg.354]

Focusing on the case of two hexagonal layers (i.e., a basal plane and one overlayer of sites), all sites in such a configuration are of valency u = 4, as noted previously. This valency is the same as for a one-layer, square-planar lattice. Accordingly, the asymptotic theory of Montroll, and den Hollendar and Kasteleyn can be used to compute values of (n) corresponding to the... [Pg.336]

Hardy, G.H. (1940). Ramanujan, Chapter VIII Asymptotic theory of partitions. Chelsea Publ. Co., New York. [Pg.845]


See other pages where Asymptotic theory is mentioned: [Pg.384]    [Pg.388]    [Pg.388]    [Pg.93]    [Pg.65]    [Pg.77]    [Pg.114]    [Pg.332]    [Pg.35]    [Pg.131]    [Pg.131]    [Pg.148]    [Pg.154]    [Pg.254]    [Pg.308]    [Pg.710]    [Pg.768]    [Pg.930]    [Pg.105]    [Pg.175]    [Pg.243]   


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