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Elementary solution

Initial conditions for the total molecular wavefunction with n = I (including electronic, vibrational and rotational quantum numbers) can be imposed by adding elementary solutions obtained for each set of initial nuclear variables, keeping in mind that the xi and 5 depend parametrically on the initial variables... [Pg.325]

CHALLENGING MATHEMATICAL PROBLEMS WITH ELEMENTARY SOLUTIONS, A.M. Yaglom and I.M. Yaglom. Over 170 challenging problems on probability theory, combinatorial analysis, points and lines, topology, convex polygons, many other topics. Solutions. Total of 445pp. 5S 8b. Two-vol. set. [Pg.129]

The most widely used theoretical framework for elementary solution and interfacial reactions is activated complex theory (ACT), also referred to as absolute reaction rate theory, or transition-state theory (TST). The term activated complex refers to a high-energy ground-state species formed from reactants, for example. [Pg.71]

Figure 2.12 illustrates schematically the essential features of the thermodynamic formulation of ACT. If it were possible to evaluate A5 ° and A// ° from a knowledge of the properties of aqueous and surface species, the elementary bimolecular rate constant could be calculated. At present, this possibility has been realized for only a limited group of reactions, for example, certain (outer-sphere) electron transfers between ions in solution. The ACT framework finds wide use in interpreting experimental bimolecular rate constants for elementary solution reactions and for correlating, and sometimes interpolating, rate constants within families of related reactions. It is noted that a parallel development for unimolecular elementary reactions yields an expression for k analogous to equation 128, with appropriate AS °. [Pg.73]

This set of four operators forms a solvable Lie algebra, as we pointed out above, and the proposed Eq. (5) must have an elementary solution. In order to find it, we propose again ... [Pg.149]

The calculations presented here show that many different factors must be considered in estimating the rate constant. Nevertheless, electron transfer theory is remarkably successful in describing this elementary solution reaction. Theory has gone much further than described here, especially in developing the quantum-mechanical description of electron transfer. More details can be found in recent reviews [29, 30]. There are other related topics which have not been discussed in this section. They include, for example, photo-induced electron transfer [30], and the Marcus cross-relation [5]. [Pg.358]

One elementary solution of set of Eqs. (37) is obtained for the zero initial phase mismatch 0 = 0 and the initial amplitudes satisfying the condition ) i = Nrfj. The solution reads as... [Pg.511]

The book has been organized into three parts to address the major issues in cosmochemistry. Part I of the book deals with stellar structure, nucleosynthesis and evolution of low and intermediate-mass stars. The lectures by Simon Jeffery outline stellar evolution with discussion on the basic equations, elementary solutions and numerical methods. Amanda Karakas s lectures discuss nucleosynthesis of low and intermediate-mass stars covering nucleosynthesis prior to the Asymptotic Giant Branch (AGB) phase, evolution during the AGB, nucleosynthesis during the AGB phase, evolution after the AGB and massive AGB stars. The slow neutron-capture process and yields from AGB stars are also discussed in detail by Karakas. The lectures by S Giridhar provide some necessary background on stellar classification. [Pg.427]

In the third step, an elementary solution of the system in appropriate mathematical form is chosen for the initial disturbance. Typically the complex form of the Fourier representation of periodic functions, although the more cumbersome form of an expansion in a series of sine and cosine termis may equally well be used. For example, the elementary solution might be chosen to be the normal mode... [Pg.315]

The method introduced here is known as the method of Green s functions or the kernel method. The function (5.96) is in fact the Green s function, or elementary solution, to the diffusion equation. The general solution to the diffusion equation for a system with an arbitrary source distribution can be constructed from these elementary solutions by applying (5.97). [Pg.186]

General Solution for 0(r) for Infinite Media. The general solution to Eq. (7.251) is obtained by superimposing the elementary solutions... [Pg.380]

The directed flux in an infinite medium wherein the spatial distribution of neutrons is given by a single variable x, and therefore by a single angle dy has been given by Wilson. In this special case Xyd) is symmetric in X and 6y and the elementary solution for 4> XyB) may be written in the form... [Pg.382]

The elementary solution to this equation is where the eigenvalue B is computed from (7.254). It was also shown that this solution satisfied the stationary-wave (diffusion) equation (see Sec. 7.4d). Now, the only solution of the diffusion equation (5.161) which is spherically symmetric and finite everywhere is [cf. Eq. (5.166)]... [Pg.385]

For the functions 0c(r) and ji(r) which appear in (8.95) we use first-order approximations of the solutions to the transport equation. The basis for this choice is derived from the following argument. It was shown previously in Sec. 7.4d that the elementary solution to the one-velocity transport equation for the source-free infinite multiplying... [Pg.443]

Consider first the form of the power oscillations. This feature may be studied by introducing the elementary solution... [Pg.608]

The general solution for the thermal flux in this reactor may be given as a linear combination of the elementary solutions 6 (cf. Sec. 7.4d). Thus we take for the flux at the surface of the rod at r... [Pg.711]

Coordinate systems, therefore, form a central underlying theme in this book. When presented correctly, they help us understand what types of elementary solutions are available for modeling, what their properties are, and what their potential uses might be. In the next section, we will introduce a new elementary solution, an arc tangent or 0 model that is complementary to the... [Pg.11]

Navier-Stokes equations. There are pitfalls in the preceding reasoning while true as far as the equation is concerned, the types of elementary solutions used in applications are different. To understand why, it is necessary to learn some aerodynamics. To be sure, the Navier-Stokes equations for Newtonian viscous flows do apply to both, but different limit processes are at work. For clarity, consider steady, constant density, planar, liquid flows governed by... [Pg.12]

In summary, aerodynamicists and mathematicians employ superpositions using two types of elementary solutions, namely, logarithms and arc tans. The correct multiple of the latter function is determined by Kutta s condition (Milne-Thomson, 1958 Yrh, 1969), simulating smooth flow from the trailing edge, as if the Navier-Stokes equations themselves had been solved. Thus, to use the results of so-called aerodynamic analysis models in Darcy pressure formulations, the level of circulation (that is, a suitable multiple of 0, which does not apply to Darcy flows) must be subtracted out. [Pg.17]

The formulations posed by Equations 2-7 and 2-11 are equivalent since superpositions of elementary solutions, which involve no additional assumptions, are used without loss of generality, integral equation methods were not available to Muskat and his contemporaries they were developed in aerodynamics and elasticity after the publication of his classic textbooks. The advantage in using Equation 2-11 is a practical one its completely analytical solution is available and is known as Carleman s formula (Carrier, Krook and Pearson, 1966 Estrada and Kanwal, 1987). in fact, for the general equation... [Pg.21]

Nonlinear superposition. Very often in pressure transient testing, the pressure (or flow rate) is changed in time for liquids, flow rate (or pressure) response is obtained by linear superposition of elementary solutions. For gases, superposition is not possible because nonlinear solutions are not linearly additive. How does one calculate the response when pressure or flow rate at the well vary, say stepwise, in time Fortunately, the governing equations can be numerically integrated with respect to t. It remains for us to represent stepwise changes in any particular variable using convenient mathematical devices. [Pg.119]


See other pages where Elementary solution is mentioned: [Pg.248]    [Pg.145]    [Pg.33]    [Pg.502]    [Pg.502]    [Pg.156]    [Pg.422]    [Pg.249]    [Pg.280]    [Pg.280]    [Pg.557]    [Pg.567]    [Pg.273]    [Pg.275]    [Pg.305]    [Pg.361]    [Pg.380]    [Pg.444]    [Pg.2]    [Pg.15]    [Pg.19]    [Pg.60]    [Pg.97]    [Pg.97]    [Pg.153]    [Pg.174]    [Pg.345]    [Pg.446]   
See also in sourсe #XX -- [ Pg.2 , Pg.11 , Pg.97 , Pg.345 , Pg.446 ]




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